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Numerical AnalysisOperations ResearchOptimization·Captain: mikedeng1

Variable Metric Method for Minimization: Davidon's Rank-One Variable-Metric Update Recovers the Inverse Hessian of a Quadratic in N Steps and Then Steps to the Exact MinimumResearch Paper

Motivation

Quasi-Newton methods minimize a smooth function f:Rn→Rf:\mathbb R^n\to\mathbb Rf:Rn→R using gradients only, while building up an approximation to the inverse of the Hessian matrix from the changes of gradient they observe. They are the default algorithms of unconstrained nonlinear optimization: BFGS and its limited-memory variant L-BFGS sit inside most numerical optimization libraries and most large-scale fitting codes in statistics and machine learning.

The family starts with William C. Davidon's Argonne report ANL-5990 of 1959, Variable Metric Method for Minimization, rejected by a journal in 1957 and published only in 1991 as the first article of the SIAM Journal on Optimization, with a preface by the author (DOI 10.1137/0801001). The report's body describes a flowchart algorithm; its Appendix describes "a simplified method embodying some of the ideas" of that algorithm, in one and a half pages. That simplified method is what is now called the symmetric rank-one (SR1) update, and the Appendix contains its quadratic-termination property: on a quadratic, after at most nnn steps the trial matrix equals the inverse Hessian, and the next step lands at the minimum.

Timeline.

  • 1952: Hestenes and Stiefel's conjugate gradient method minimizes a strictly convex quadratic in at most nnn steps (J. Res. NBS 49); Davidon cites it as [2].
  • 1959: Davidon's ANL-5990, including the Appendix method treated here.
  • 1963: Fletcher and Powell simplify the body's method into the DFP update and prove its quadratic termination with exact line searches (Comput. J. 6).
  • 1967: Broyden's survey of quasi-Newton methods discusses the symmetric rank-one update (Math. Comp. 21); textbooks later analyse it under the name SR1.
  • 1980: Nocedal's limited-storage BFGS, whose termination on quadratics with exact line searches is a separate Prove2Me mission (Math. Comp. 35).

Setting

Vectors are elements of Rn\mathbb R^nRn and matrices are real n×nn\times nn×n. Fix a symmetric positive definite matrix GGG and a point ξ\xiξ, and let

f(x)=12 (x−ξ)TG (x−ξ)+c,f(x)=\tfrac12\,(x-\xi)^{\mathsf T}G\,(x-\xi)+c ,f(x)=21​(x−ξ)TG(x−ξ)+c,

a quadratic with constant Hessian GGG and minimum point ξ\xiξ. Its gradient is ∇(x)=G(x−ξ)\nabla(x)=G(x-\xi)∇(x)=G(x−ξ), display (6) of the Appendix.

The method keeps a point xkx_kxk​ and a symmetric trial matrix HkH_kHk​, which plays the role of G−1G^{-1}G−1. Write ∇k=∇(xk)\nabla_k=\nabla(x_k)∇k​=∇(xk​). One iteration is

xk+1=xk−Hk∇k(2),Hk+1=Hk+ak (Hk∇k+1)(Hk∇k+1)T(3),x_{k+1}=x_k-H_k\nabla_k \quad\text{(2)},\qquad H_{k+1}=H_k+a_k\,(H_k\nabla_{k+1})(H_k\nabla_{k+1})^{\mathsf T}\quad\text{(3)},xk+1​=xk​−Hk​∇k​(2),Hk+1​=Hk​+ak​(Hk​∇k+1​)(Hk​∇k+1​)T(3),

a full step with no line search followed by a symmetric rank-one update. With the two scalars

Nk=∇k+1THk∇k+1,Mk=∇k+1THk∇k,N_k=\nabla_{k+1}^{\mathsf T}H_k\nabla_{k+1},\qquad M_k=\nabla_{k+1}^{\mathsf T}H_k\nabla_k ,Nk​=∇k+1T​Hk​∇k+1​,Mk​=∇k+1T​Hk​∇k​,

footnote 2 of the Appendix fixes the coefficient on a quadratic to ak=(Mk−Nk)−1a_k=(M_k-N_k)^{-1}ak​=(Mk​−Nk​)−1, which makes the paper's quality measure Δ\DeltaΔ of (4) vanish. Write Sk=xk+1−xkS_k=x_{k+1}-x_kSk​=xk+1​−xk​ for the step and Dk=∇k+1−∇kD_k=\nabla_{k+1}-\nabla_kDk​=∇k+1​−∇k​ for the change of gradient. The paper writes xxx, HHH, ∇\nabla∇ for the current quantities and x+x^{+}x+, H+H^{+}H+, ∇+\nabla^{+}∇+ for the updated ones, and uses the letter NNN both for the number of variables and for the scalar NkN_kNk​; here the number of variables is nnn.

Formalization targets

Goal: termination in nnn steps

If H0H_0H0​ is symmetric and Mk≠NkM_k\ne N_kMk​=Nk​ for every k<nk<nk<n, then

Hn=G−1andxn+1=ξ.H_n=G^{-1}\qquad\text{and}\qquad x_{n+1}=\xi .Hn​=G−1andxn+1​=ξ.

This is the sentence after (8) on p. 17: "After no more than NNN steps (for which Δ=0\Delta=0Δ=0), HHH will equal G−1G^{-1}G−1 and the following step will be to the exact minimum."

Milestones

  1. Display (6): the gradient of fff is G(x−ξ)G(x-\xi)G(x−ξ).
  2. Display (8): with a=(M−N)−1a=(M-N)^{-1}a=(M−N)−1 and M≠NM\ne NM=N, H+GS=H+D=SH^{+}GS=H^{+}D=SH+GS=H+D=S.
  3. Display (7): if HGu=uHGu=uHGu=u then H+Gu=uH^{+}Gu=uH+Gu=u, for any coefficient aaa.
  4. The sentence "so that SSS becomes another such eigenvector", read along the run: if Mi≠NiM_i\ne N_iMi​=Ni​ for i<ki<ki<k, then HkGSj=SjH_kGS_j=S_jHk​GSj​=Sj​ for every j<kj<kj<k.

Further statements of the Appendix

  • Condition 1 (p. 16): if HHH is positive definite and R−1≤det⁡H+/det⁡H≤RR^{-1}\le\det H^{+}/\det H\le RR−1≤detH+/detH≤R with R>1R>1R>1, then H+H^{+}H+ is positive definite.
  • The constraint remark (p. 17): for any function and any coefficients, if H0H_0H0​ is symmetric and H0b=0H_0b=0H0​b=0, then every step is perpendicular to bbb and b⋅xkb\cdot x_kb⋅xk​ is conserved.
  • Table (5) (p. 16): for general (non-quadratic) fff, the coefficient aaa that minimizes Δ\DeltaΔ subject to condition 1, and the minimum value, on each of five ranges of MMM.

Significance

The termination theorem says that on a quadratic the rank-one update recovers the exact inverse Hessian from nnn gradient differences, without line searches and without positive definiteness of the trial matrix, and then takes the Newton step. This is the property that justifies the name "variable metric": the metric HkH_kHk​ converges to the one that makes the problem trivial. The secant equation (8) and the persistence of earlier secant equations (7) are the template for the analysis of every later quasi-Newton update, and the SR1 update remains in use in trust-region methods because it does not force positive definiteness.

The result is classical and its proof is short; what this mission adds is a machine-checked version stated in the paper's own form. In particular the hypothesis is the paper's: only that each of the first nnn coefficients is defined. Textbook statements of SR1 termination often assume in addition that the steps are linearly independent; the paper does not, and the formal goal does not either. No Lean formalization of SR1, DFP or BFGS termination was found in Mathlib or on Prove2Me. On Prove2Me, the related open targets are L-BFGS termination (Nocedal 1980) and conjugate-gradient termination (Hestenes–Stiefel 1952); the definitions here are independent of theirs.

Difficulty

Each update changes HHH by a rank-one term, and nothing in a single step forces HnH_nHn​ to be G−1G^{-1}G−1: the coefficient aka_kak​ depends on the current iterate and the update could, a priori, destroy what earlier steps achieved, as general rank-one updates do. The obvious count — nnn steps, nnn conditions — does not by itself give nnn independent conditions on HnH_nHn​; the steps produced by the method are not chosen to be independent, and the only hypothesis available is that the denominators Mk−NkM_k-N_kMk​−Nk​ are nonzero. The difficulty is to get the full conclusion from that hypothesis alone, without assuming independence, positive definiteness of H0H_0H0​, or a line search.

Formalization scope

Vectors are Fin n → ℝ with 0-based indices, matrices Matrix (Fin n) (Fin n) ℝ; uTHvu^{\mathsf T}HvuTHv is u ⬝ᵥ (H *ᵥ v) and (Hg)(Hg)T(Hg)(Hg)^{\mathsf T}(Hg)(Hg)T is vecMulVec (H *ᵥ g) (H *ᵥ g). The definition file DavidonVM.Termination.Method provides quad, grad, Nval, Mval, the run predicate IsRunWith for an arbitrary gradient field and coefficients, and IsQuadRun for the quadratic with ak=(Mk−Nk)−1a_k=(M_k-N_k)^{-1}ak​=(Mk​−Nk​)−1; DavidonVM.Termination.Delta provides the update and the quantity Δ\DeltaΔ of (4).

Committed conventions, each a reading of something the paper leaves implicit:

  • The function is an explicit quadratic with constant symmetric positive definite GGG ("in the neighborhood of a minimum"); the run's gradient field is G(x−ξ)G(x-\xi)G(x−ξ), and milestone 1 ties it to the quadratic. The goal uses positive definiteness; milestones use only symmetry where that suffices; the secant milestone needs nothing on GGG.
  • Only H0H_0H0​ is assumed symmetric (the paper, p. 4: "It is to be symmetric"); positive definiteness of H0H_0H0​ is not assumed.
  • "Steps for which Δ=0\Delta=0Δ=0" is read through footnote 2 as Mk≠NkM_k\ne N_kMk​=Nk​. Lean's real inverse gives 0−1=00^{-1}=00−1=0, so without this hypothesis the update would silently leave HHH unchanged.
  • The stopping rule "provided that NNN is greater than some preassigned ε\varepsilonε" is not modelled; the run continues for every kkk, and the goal looks at steps 0,…,n0,\dots,n0,…,n only.
  • G−1G^{-1}G−1 is Mathlib's matrix inverse, the true inverse since GGG is positive definite.

A statement of the goal with the extra hypothesis "S0,…,Sn−1S_0,\dots,S_{n-1}S0​,…,Sn−1​ are linearly independent", or with HkGSj=SjH_k G S_j=S_jHk​GSj​=Sj​ assumed, would be a weaker theorem than the paper's and is ruled out. The case n=0n=0n=0 is trivial; the hypotheses are jointly satisfiable for n=1n=1n=1 (checked locally).

Welcome contributions: proofs of the four milestones and the goal; general facts about rank-one updates (determinant and positive definiteness, Sherman–Morrison form of the inverse) that the further statements need and that are reusable for DFP, BFGS and trust-region analyses.

Selected references

  • W. C. Davidon, Variable Metric Method for Minimization, SIAM J. Optim. 1(1) (1991) 1–17 (Argonne report ANL-5990, 1959). https://doi.org/10.1137/0801001
  • M. R. Hestenes and E. Stiefel, Methods of conjugate gradients for solving linear systems, J. Res. Nat. Bur. Standards 49 (1952) 409–436. https://doi.org/10.6028/jres.049.044
  • R. Fletcher and M. J. D. Powell, A rapidly convergent descent method for minimization, Comput. J. 6 (1963) 163–168. https://doi.org/10.1093/comjnl/6.2.163
  • C. G. Broyden, Quasi-Newton methods and their application to function minimisation, Math. Comp. 21 (1967) 368–381. https://doi.org/10.1090/S0025-5718-1967-0224273-2
  • J. Nocedal, Updating quasi-Newton matrices with limited storage, Math. Comp. 35 (1980) 773–782. https://doi.org/10.1090/S0025-5718-1980-0572855-7
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Complexity TheoryOperations ResearchOptimization+1·Captain: mikedeng1

Scheduling Problems with Two Competing Agents 7: PARTITION Reduces to Two Agents Each Bounding Their Own Makespan in the Two-Machine Flow Shop and Open ShopResearch Paper

Motivation

In multi-agent scheduling, several decision makers share one processing resource, and each one cares only about the completion of its own jobs. Agnetis, Mirchandani, Pacciarelli and Pacifici (Oper. Res. 52(2), 2004) set up the two-agent version of this problem and classified its complexity for most combinations of classical objectives. Typical settings are a manufacturing cell that serves an internal and an external customer, or two departments that negotiate access to a shared machine. Most of the paper treats a single machine. Its §10 asks what happens when the shared resource is a small shop: two machines that every job must visit.

The answer is that even the simplest two-machine case is hard. In the classical single-agent setting, the two-machine flow shop makespan problem is solved by Johnson's rule (Johnson 1954) and the two-machine open shop makespan problem by Gonzalez and Sahni (1976), both in polynomial time. As soon as two agents each want their own jobs finished early, both problems become NP-hard.

Setting

There are two agents, A and B. Agent A owns jobs J1A,…,JnAAJ^A_1,\dots,J^A_{n_A}J1A​,…,JnA​A​ and agent B owns jobs J1B,…,JnBBJ^B_1,\dots,J^B_{n_B}J1B​,…,JnB​B​. Every job consists of one operation on machine M1M_1M1​ and one on machine M2M_2M2​, and pihX≥0p^X_{ih}\ge 0pihX​≥0 is the processing time of job JiXJ^X_iJiX​ on machine MhM_hMh​. A schedule gives every operation a start time. It is feasible when no operation starts before time 000, each machine processes at most one operation at a time, and the two operations of one job do not overlap in time. Processing is nonpreemptive.

  • In the flow shop F2F2F2 every job is processed first on M1M_1M1​ and then on M2M_2M2​.
  • In the open shop O2O2O2 the two operations of a job may be processed in either order.

The makespan of agent XXX, Cmax⁡XC^X_{\max}CmaxX​, is the latest completion time of an operation of one of its jobs. The recognition problem F2∥Cmax⁡A≤QA, Cmax⁡B≤QBF2\|C^A_{\max}\le Q_A,\ C^B_{\max}\le Q_BF2∥CmaxA​≤QA​, CmaxB​≤QB​ asks, for given thresholds QA,QBQ_A, Q_BQA​,QB​, whether some feasible flow shop schedule has Cmax⁡A≤QAC^A_{\max}\le Q_ACmaxA​≤QA​ and Cmax⁡B≤QBC^B_{\max}\le Q_BCmaxB​≤QB​. The problem O2∥Cmax⁡A≤QA, Cmax⁡B≤QBO2\|C^A_{\max}\le Q_A,\ C^B_{\max}\le Q_BO2∥CmaxA​≤QA​, CmaxB​≤QB​ is the same question for the open shop.

PARTITION (Problem 9.1 of the paper) asks whether a finite list of nonnegative integers p1,…,pkp_1,\dots,p_kp1​,…,pk​ can be split into two parts of equal sum P/2P/2P/2, where P=∑ipiP=\sum_i p_iP=∑i​pi​.

Formalization targets

Goal: Theorems 10.1 and 10.2

PARTITION ≤p F2 ∥ Cmax⁡A≤QA, Cmax⁡B≤QBandPARTITION ≤p O2 ∥ Cmax⁡A≤QA, Cmax⁡B≤QB,\text{PARTITION}\ \le_p\ F2\,\|\,C^A_{\max}\le Q_A,\ C^B_{\max}\le Q_B \qquad\text{and}\qquad \text{PARTITION}\ \le_p\ O2\,\|\,C^A_{\max}\le Q_A,\ C^B_{\max}\le Q_B,PARTITION ≤p​ F2∥CmaxA​≤QA​, CmaxB​≤QB​andPARTITION ≤p​ O2∥CmaxA​≤QA​, CmaxB​≤QB​,

with ≤p\le_p≤p​ polynomial-time many-one reducibility between binary-coded languages. This is how the paper proves "F2∥Cmax⁡A:Cmax⁡BF2\|C^A_{\max}:C^B_{\max}F2∥CmaxA​:CmaxB​ is NP-hard" (Theorem 10.1, p. 238) and "O2∥Cmax⁡A:Cmax⁡BO2\|C^A_{\max}:C^B_{\max}O2∥CmaxA​:CmaxB​ is NP-hard" (Theorem 10.2, p. 239).

Milestones: the two constructions

For Theorem 10.1, with ε=1/(k+1)\varepsilon=1/(k+1)ε=1/(k+1), the paper builds the instance with kkk A-jobs of times (ε,pi)(\varepsilon, p_i)(ε,pi​), one B-job of times (P/2−(k−1)ε, P/2)(P/2-(k-1)\varepsilon,\ P/2)(P/2−(k−1)ε, P/2), and thresholds QA=3P/2+εQ_A = 3P/2+\varepsilonQA​=3P/2+ε, QB=P+εQ_B = P+\varepsilonQB​=P+ε. The milestones are:

  1. under Cmax⁡B≤QBC^B_{\max}\le Q_BCmaxB​≤QB​ the B-job starts on M2M_2M2​ by P/2+εP/2+\varepsilonP/2+ε, and the A-jobs before it on M2M_2M2​ total at most P/2P/2P/2;
  2. for even PPP, PARTITION has a solution if and only if this instance meets both thresholds.

For Theorem 10.2 the instance has kkk A-jobs of time pip_ipi​ on both machines, one B-job of time P/2P/2P/2 on both machines, and thresholds QA=3P/2Q_A=3P/2QA​=3P/2, QB=PQ_B=PQB​=P. The milestones are:

  1. under Cmax⁡B≤QBC^B_{\max}\le Q_BCmaxB​≤QB​ the B-job starts at 000 on one machine and at P/2P/2P/2 on the other;
  2. PARTITION has a solution if and only if this instance meets both thresholds.

Significance

The two theorems mark the boundary of tractability of §10. The single-agent problems F2∥Cmax⁡F2\|C_{\max}F2∥Cmax​ and O2∥Cmax⁡O2\|C_{\max}O2∥Cmax​ are polynomial. Giving the second agent a single job and a deadline is already enough to make the problems NP-hard, so no extension of Johnson's rule or of the Gonzalez–Sahni algorithm solves the two-agent versions unless P = NP. The paper also observes that any other combination of the objectives it considers is NP-hard in these shops.

The theorems are proved in the paper by short reductions. As far as we know none of them is machine-checked. This mission produces checked statements of both reductions on a general two-machine shop model with real start times. It also corrects the flow shop equivalence, which as printed does not hold for odd PPP.

Difficulty

The hard direction of each equivalence goes from a feasible schedule to a partition. A schedule is a set of real start times, not a permutation. Nothing forces the jobs into a fixed order or rules out idle time. The proof has to extract a combinatorial split from interval packing: which A-jobs fit into the gap before the B-job on one machine and which fit into the gap after it. The sum of lengths of pairwise disjoint intervals inside a window must be bounded by the window's length.

In the flow shop the gap after the B-job has length P/2+kεP/2+k\varepsilonP/2+kε, which is not P/2P/2P/2. Integrality of the A-lengths is what closes the gap, and it only works when P/2P/2P/2 is an integer. In the open shop, the same argument has to cover both orders of the B-job's operations. Both reductions output rational data, so the goal also needs a scaling to integer data and a polynomial-time bound on the code map.

Formalization scope

  • Model. Jobs are numbered Fin (n_A + n_B), the A-jobs first. Start times are real numbers, and idle time and different job orders on the two machines are allowed. Flow shop feasibility is the published JohnsonFlowShop.TwoStage.IsFeasible from the Johnson (1954) series. Open shop feasibility is the definition IsOpenFeasible of this mission: no machine overlap between distinct jobs, and no time overlap between the two operations of a job. "Cmax⁡X≤QXC^X_{\max}\le Q_XCmaxX​≤QX​" is stated as "every operation of every XXX-job ends by QXQ_XQX​", so no maximum over a possibly empty set is taken.
  • Languages. The target languages hold the binary codes of instances with natural-number processing times and thresholds that have a feasible schedule meeting both thresholds. PARTITION is the published ProjSchedTW.Complexity.partitionLang (nonnegative sizes, zero allowed), and reducibility is CookPvsNP.PolyReducible. Both come from published definitions of the Neumann–Schwindt–Zimmermann and Cook series. NP-membership is not formalized.
  • Constructions. They are defined over R\mathbb RR exactly as printed. A reduction to the N\mathbb NN-coded languages has to rescale (for example by 2(k+1)2(k+1)2(k+1)). That rescaling is the solver's to choose and is not a milestone.
  • Corrections. The printed flow shop equivalence uses ⌊P/2+kε⌋=P/2\lfloor P/2+k\varepsilon\rfloor = P/2⌊P/2+kε⌋=P/2 and fails for odd PPP: p=(1)p=(1)p=(1) gives a yes-instance of the scheduling problem but has no partition. It also fails for P=0P=0P=0 and k≥2k\ge 2k≥2, where the printed p11Bp^B_{11}p11B​ is negative. Milestone 2 therefore assumes PPP even and (P≥2P\ge2P≥2 or k≤1k\le1k≤1). The goal is unaffected, because odd PPP is a PARTITION no-instance. In the open shop proof, the printed identity "∑piA+∑piB=2P\sum p^A_i+\sum p^B_i = 2P∑piA​+∑piB​=2P" is read as "each machine carries 3P/23P/23P/2 of work", and the statement is unchanged.
  • No trivialization. The flow shop and open shop languages are not restricted to the instances the constructions produce, so they cannot be decided by reading off the construction. A schedule must satisfy the machine and job non-overlap constraints, including in the open shop, where a definition without the job constraint would let a job run on both machines at once.
  • Welcome contributions. Interval-packing lemmas on R\mathbb RR, a polynomial-time bound for list arithmetic over encNats, and a scaling lemma for shop schedules are reusable beyond this mission.

Selected references

  • A. Agnetis, P. B. Mirchandani, D. Pacciarelli, A. Pacifici, Scheduling Problems with Two Competing Agents, Operations Research 52(2) (2004) 229–242. https://doi.org/10.1287/opre.1030.0092
  • S. M. Johnson, Optimal two- and three-stage production schedules with setup times included, Naval Research Logistics Quarterly 1 (1954) 61–68. https://doi.org/10.1002/nav.3800010110
  • T. Gonzalez, S. Sahni, Open shop scheduling to minimize finish time, Journal of the ACM 23(4) (1976) 665–679. https://doi.org/10.1145/321978.321985
  • M. R. Garey, D. S. Johnson, Computers and Intractability: A Guide to the Theory of NP-Completeness, W. H. Freeman, 1979.
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🏆Completed
AnalysisControl TheoryDynamical Systems+1·Captain: mikedeng1

Continuous-Time Average-Preserving Opinion Dynamics with Opinion-Dependent Communications 1: Every Proper Solution of the Discrete-Agent Model Converges to Clusters at Least 1 ApartResearch Paper

Motivation

Bounded-confidence opinion dynamics model a population in which each individual revises an opinion, represented by a real number, by looking only at opinions close to its own. The best-known example is the discrete-time model of Krause (1997), also called the Hegselmann–Krause model, in which every agent moves to the average of the opinions within distance 1 of its own. Such models are studied in the social sciences as models of consensus formation and polarization, and in control theory as prototypes of multiagent systems with state-dependent interaction topology: the communication graph is not given in advance but is determined by the state itself, which is what rendezvous algorithms for mobile robots and flocking models share (Lorenz 2007; Olfati-Saber, Fax, Murray 2007).

Blondel, Hendrickx and Tsitsiklis (SIAM J. Control Optim. 48 (2010)) study the continuous-time, symmetric counterpart of Krause's model. Each opinion is continuously attracted by every other opinion differing from it by less than 1, with an intensity proportional to the difference. Simulations show convergence to clusters, groups of agents sharing a common value, with distinct clusters at distance at least 1 and typically close to 2. This mission formalizes the first of the paper's results: convergence to clusters at least 1 apart for finitely many agents.

Timeline.

  • 1997: Krause introduces the discrete-time bounded-confidence model.
  • 2003: Jadbabaie, Lin and Morse prove convergence results for nearest-neighbour coordination with switching topologies (IEEE TAC 48).
  • 2009: Blondel, Hendrickx and Tsitsiklis analyse Krause's discrete-time model and the observed intercluster distance of about 2 (IEEE TAC 54).
  • 2010: the present paper. For the continuous-time model with n agents it proves that every proper solution converges to an equilibrium with clusters at least 1 apart (Theorem 2). It also proves that almost every initial condition is proper (Theorem 1, proof sketched) and gives a continuum-agent analysis with a sharper intercluster bound.

Setting

There are nnn agents, labelled 1,…,n1,\dots,n1,…,n. Agent iii holds a real opinion xi(t)x_i(t)xi​(t) at each time t≥0t\ge 0t≥0, and xix_ixi​ is a continuous function of time. Agent jjj is a neighbour of agent iii at time ttt when ∣xi(t)−xj(t)∣<1|x_i(t)-x_j(t)|<1∣xi​(t)−xj​(t)∣<1; the inequality is strict, and every agent is its own neighbour. The intended dynamics are

x˙i(t)=∑j: ∣xi(t)−xj(t)∣<1(xj(t)−xi(t)).(1.1)\dot x_i(t)=\sum_{j:\,|x_i(t)-x_j(t)|<1}\bigl(x_j(t)-x_i(t)\bigr).\tag{1.1}x˙i​(t)=j:∣xi​(t)−xj​(t)∣<1∑​(xj​(t)−xi​(t)).(1.1)

The right-hand side jumps whenever a pair of opinions crosses distance 1, so (1.1) usually has no differentiable solution. The model is therefore the integral equation

xi(t)=xi(0)+∫0t∑j: ∣xi(τ)−xj(τ)∣<1(xj(τ)−xi(τ)) dτ(t≥0, i=1,…,n).(2.1)x_i(t)=x_i(0)+\int_0^t\sum_{j:\,|x_i(\tau)-x_j(\tau)|<1}\bigl(x_j(\tau)-x_i(\tau)\bigr)\,d\tau\qquad(t\ge0,\ i=1,\dots,n).\tag{2.1}xi​(t)=xi​(0)+∫0t​j:∣xi​(τ)−xj​(τ)∣<1∑​(xj​(τ)−xi​(τ))dτ(t≥0, i=1,…,n).(2.1)

Solutions of (2.1) need not be unique. The two-agent initial condition (−12,12)(-\tfrac12,\tfrac12)(−21​,21​) is a fixed point, but the agents can also start attracting each other immediately. An initial condition x~∈Rn\tilde x\in\mathbb R^nx~∈Rn is proper if (a) (2.1) has exactly one solution xxx with x(0)=x~x(0)=\tilde xx(0)=x~; (b) the set of times at which xxx is not differentiable is at most countable and has no accumulation point; and (c) agents that meet stay together: xi(t)=xj(t)x_i(t)=x_j(t)xi​(t)=xj​(t) implies xi(t′)=xj(t′)x_i(t')=x_j(t')xi​(t′)=xj​(t′) for all t′≥tt'\ge tt′≥t. That solution is then a proper solution.

The set of equilibria is

F={s~∈Rn: for all i,j, s~i=s~j or ∣s~i−s~j∣≥1}.F=\bigl\{\tilde s\in\mathbb R^n:\ \text{for all } i,j,\ \tilde s_i=\tilde s_j\ \text{or}\ |\tilde s_i-\tilde s_j|\ge 1\bigr\}.F={s~∈Rn: for all i,j, s~i​=s~j​ or ∣s~i​−s~j​∣≥1}.

The average opinion is xˉ(t)=1n∑ixi(t)\bar x(t)=\frac1n\sum_i x_i(t)xˉ(t)=n1​∑i​xi​(t), and V(x(t))=∑i(xi(t)−xˉ(t))2V(x(t))=\sum_i\bigl(x_i(t)-\bar x(t)\bigr)^2V(x(t))=∑i​(xi​(t)−xˉ(t))2 is the sum of squared differences from it.

Formalization targets

Goal: Theorem 2

Every proper solution xxx of (2.1) converges to a limit in FFF:

∃ x∗∈F:lim⁡t→∞x(t)=x∗,\exists\,x^*\in F:\qquad \lim_{t\to\infty}x(t)=x^*,∃x∗∈F:t→∞lim​x(t)=x∗,

that is, all limits exist and two agents with different limits end at distance at least 1.

Milestones, in the order the argument uses them

  1. Order preservation (§2.1, p. 5218): if xi(t)≥xj(t)x_i(t)\ge x_j(t)xi​(t)≥xj​(t) for some ttt, then xi(t′)≥xj(t′)x_i(t')\ge x_j(t')xi​(t′)≥xj​(t′) for every t′≥tt'\ge tt′≥t.
  2. Proposition 1 (p. 5218): xˉ\bar xxˉ is constant, V(x(t))V(x(t))V(x(t)) is nonincreasing, and outside a countable set of times dV/dtdV/dtdV/dt is negative when x(t)∉Fx(t)\notin Fx(t)∈/F and zero when x(t)∈Fx(t)\in Fx(t)∈F.
  3. Monotone partial sums (2.3) (p. 5219): for a sorted initial condition and every kkk, outside a countable set of times the derivative of ∑i≤kxi(t)\sum_{i\le k}x_i(t)∑i≤k​xi​(t) equals ∑i≤k∑j>k: ∣xi−xj∣<1(xj−xi)≥0\sum_{i\le k}\sum_{j>k:\,|x_i-x_j|<1}(x_j-x_i)\ge 0∑i≤k​∑j>k:∣xi​−xj​∣<1​(xj​−xi​)≥0, and ∑i≤kxi(t)\sum_{i\le k}x_i(t)∑i≤k​xi​(t) is nondecreasing in ttt.
  4. Convergence of each opinion (p. 5219): every xi(t)x_i(t)xi​(t) has a limit as t→∞t\to\inftyt→∞.

Significance

The result. Theorem 2 establishes the clustering behaviour seen in simulations for every proper solution. The paper's Theorem 1 states that almost every initial condition is proper, so the conclusion covers almost every initial condition. The lower bound 1 on the distance between clusters is the baseline that the paper's continuum analysis improves to 1+min⁡{WA,WB}/max⁡{WA,WB}1+\min\{W_A,W_B\}/\max\{W_A,W_B\}1+min{WA​,WB​}/max{WA​,WB​}. Average preservation and the decrease of VVV (Proposition 1) are the structural facts that the continuum model also has.

Formalization. Theorem 2 is proved in the paper; no machine-checked version exists on Prove2Me or, as far as is known, elsewhere. The mission produces a Lean definition of solutions of a discontinuous integral equation with a state-dependent neighbour graph, and a convergence proof for it. The remaining work is to formalize the known argument, from the integral equation to the existence and location of the limit.

Difficulty

The obvious approach treats (1.1) as an ODE and differentiates along trajectories. That fails because the right-hand side is discontinuous in the state. A solution is only an integral solution, it may fail to be differentiable, and derivative identities such as (2.3) hold only outside an exceptional set of times. Every step from a derivative sign to a monotonicity or limit statement therefore has to go through the integral equation, not the differential one. A second obstacle is that pairs of agents at distance exactly 1 sit on the discontinuity of the interaction rule. This is where uniqueness fails (footnote 3 of the paper) and why conditions (a)–(c) are hypotheses. A decreasing Lyapunov function VVV alone does not give convergence of the trajectory to a single point, so Proposition 1 does not by itself settle Theorem 2.

Formalization scope

Agents are Fin n. Time is ℝ, and only values at t≥0t\ge 0t≥0 enter. A trajectory is x : ℝ → Fin n → ℝ. A solution of (2.1) is continuous on [0,∞)[0,\infty)[0,∞) and satisfies (2.1) for every t≥0t\ge 0t≥0 and every iii, with the neighbour set Finset.univ.filter (fun j => |x τ i - x τ j| < 1). The integrand is also required to be interval-integrable on [0,t][0,t][0,t]; for a continuous trajectory this always holds. Explicit readings of the paper's phrases:

  • "unique solution" in (a) is uniqueness among all solutions of (2.1), with no sortedness or differentiability assumed;
  • condition (b) is "for every TTT, the non-differentiability times in [0,T][0,T][0,T] form a finite set", which is equivalent for subsets of [0,∞)[0,\infty)[0,∞);
  • "converges to a limit" is Tendsto x atTop (𝓝 xstar) in Fin n → ℝ, with real time;
  • "with the exception of a countable set of times" is the existence of a countable set SSS outside which the derivative of V(x(t))V(x(t))V(x(t)) exists and has the stated sign;
  • "constant" and "nonincreasing" are on [0,∞)[0,\infty)[0,∞);
  • Proposition 1 assumes n≥1n\ge1n≥1 so that xˉ\bar xxˉ is meaningful.

The paper's sortedness convention ("we assume … that the components of proper initial conditions are sorted") is a hypothesis only of the partial-sum milestone. Theorem 2 is stated for every proper solution. A formalization that dropped condition (a), restricted solutions to sorted, differentiable or eventually constant trajectories, or replaced (2.1) by the differential equation would prove a different, and in parts trivial, statement. These are excluded.

The work needs interval integrals and the fundamental theorem of calculus for integrands with jumps, monotonicity from almost-everywhere derivative signs, and bounded monotone convergence. The definition of solutions of (2.1) and the equilibrium set is reusable for the stability results of the same paper (Theorem 3), which are not part of this mission. Contributions are welcome at every milestone, as are alternative convergence proofs, such as the paper's reference [9], that avoid symmetry.

Selected references

  • V. D. Blondel, J. M. Hendrickx, J. N. Tsitsiklis, Continuous-time average-preserving opinion dynamics with opinion-dependent communications, SIAM J. Control Optim. 48(8), 2010, 5214–5240. https://doi.org/10.1137/090766188
  • V. D. Blondel, J. M. Hendrickx, J. N. Tsitsiklis, On Krause's multi-agent consensus model with state-dependent connectivity, IEEE Trans. Automat. Control 54(11), 2009, 2586–2597. https://doi.org/10.1109/TAC.2009.2031211
  • A. Jadbabaie, J. Lin, A. S. Morse, Coordination of groups of mobile autonomous agents using nearest neighbor rules, IEEE Trans. Automat. Control 48(6), 2003, 988–1001. https://doi.org/10.1109/TAC.2003.812781
  • J. Lorenz, Continuous opinion dynamics under bounded confidence: a survey, Internat. J. Modern Phys. C 18(12), 2007, 1819–1838. https://doi.org/10.1142/S0129183107011789
  • R. Olfati-Saber, J. A. Fax, R. M. Murray, Consensus and cooperation in networked multi-agent systems, Proc. IEEE 95(1), 2007, 215–233. https://doi.org/10.1109/JPROC.2006.887293
  • U. Krause, Soziale Dynamiken mit vielen Interakteuren. Eine Problemskizze, in Modellierung und Simulation von Dynamiken mit vielen interagierenden Akteuren, Universität Bremen, 1997, 37–51.
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Convex OptimizationMachine LearningOperations Research+1·Captain: mikedeng1

Incremental Proximal Methods for Large Scale Convex Optimization I: With a Cyclic Order and a Diminishing Stepsize, Incremental Subgradient-Proximal Methods Converge to an Optimal SolutionResearch Paper

Motivation

Many optimization problems in machine learning, signal processing and distributed computation have an objective that is a sum of a large number mmm of component functions: one per data point, per sensor, or per processor. Evaluating the whole sum, or a subgradient of it, at every iteration is expensive when mmm is large. Incremental methods process one component at a time, cycling through the components or sampling them, and update the iterate after each one. Incremental gradient and subgradient methods go back to the training of neural networks and to least squares; incremental proximal methods replace the subgradient step of a component by a proximal step, which is more stable and handles nonsmooth terms exactly.

Bertsekas (LIDS-P-2847, 2010, rev. 2011; Math. Program. 129 (2011)) proposed a unified family that mixes the two: each component is split as Fi=fi+hiF_i=f_i+h_iFi​=fi​+hi​, a proximal step is taken on fif_ifi​ and a subgradient step on hih_ihi​, followed by a projection onto the constraint set. This mission formalizes the convergence analysis of that family under the cyclic order of component selection.

Timeline. Incremental subgradient methods were analysed by Nedić and Bertsekas (SIAM J. Optim. 12 (2001)) for cyclic and randomized orders. Incremental proximal methods were studied by Bertsekas (Optimization for Machine Learning, 2011, ch. 4). The 2011 paper combines the two analyses; its cyclic-order results are Propositions 3–6.

Setting

Let Rn\mathbb R^nRn carry the Euclidean norm ∥⋅∥\|\cdot\|∥⋅∥ and inner product x′yx'yx′y. The data are a nonempty closed convex set X⊆RnX\subseteq\mathbb R^nX⊆Rn and real-valued convex functions fi,hi:Rn→Rf_i,h_i:\mathbb R^n\to\mathbb Rfi​,hi​:Rn→R, i=1,…,mi=1,\dots,mi=1,…,m. The problem is

minimize F(x)=∑i=1mFi(x),Fi=fi+hi,subject to x∈X,\text{minimize } F(x)=\sum_{i=1}^m F_i(x),\qquad F_i=f_i+h_i,\qquad\text{subject to } x\in X,minimize F(x)=i=1∑m​Fi​(x),Fi​=fi​+hi​,subject to x∈X,

with optimal value F∗=inf⁡x∈XF(x)F^*=\inf_{x\in X}F(x)F∗=infx∈X​F(x), possibly −∞-\infty−∞, and optimal set X∗={x∗∈X:F(x∗)=F∗}X^*=\{x^*\in X:F(x^*)=F^*\}X∗={x∗∈X:F(x∗)=F∗}, possibly empty.

A subgradient ∇~f(x)\tilde\nabla f(x)∇~f(x) of a convex fff at xxx is a vector ggg with f(y)≥f(x)+g′(y−x)f(y)\ge f(x)+g'(y-x)f(y)≥f(x)+g′(y−x) for all yyy; PX(u)P_X(u)PX​(u) is the point of XXX nearest to uuu. At iteration kkk one component iki_kik​ is processed with stepsize αk>0\alpha_k>0αk​>0. The three iterations are

(19)zk=PX(xk−αk∇~fik(zk)),xk+1=PX(zk−αk∇~hik(zk)),(20)zk=xk−αk∇~fik(zk),xk+1=PX(zk−αk∇~hik(zk)),(21)zk=xk−αk∇~hik(xk),xk+1=PX(zk−αk∇~fik(xk+1)).\begin{aligned} &(19)\quad z_k=P_X\big(x_k-\alpha_k\tilde\nabla f_{i_k}(z_k)\big),&& x_{k+1}=P_X\big(z_k-\alpha_k\tilde\nabla h_{i_k}(z_k)\big),\\ &(20)\quad z_k=x_k-\alpha_k\tilde\nabla f_{i_k}(z_k),&& x_{k+1}=P_X\big(z_k-\alpha_k\tilde\nabla h_{i_k}(z_k)\big),\\ &(21)\quad z_k=x_k-\alpha_k\tilde\nabla h_{i_k}(x_k),&& x_{k+1}=P_X\big(z_k-\alpha_k\tilde\nabla f_{i_k}(x_{k+1})\big). \end{aligned}​(19)zk​=PX​(xk​−αk​∇~fik​​(zk​)),(20)zk​=xk​−αk​∇~fik​​(zk​),(21)zk​=xk​−αk​∇~hik​​(xk​),​​xk+1​=PX​(zk​−αk​∇~hik​​(zk​)),xk+1​=PX​(zk​−αk​∇~hik​​(zk​)),xk+1​=PX​(zk​−αk​∇~fik​​(xk+1​)).​

The fff-subgradient is taken at the new point, which makes the fff-part a proximal step (Proposition 1). In the cyclic order ik=(k mod m)+1i_k=(k\bmod m)+1ik​=(kmodm)+1; a block of mmm consecutive iterations is a cycle, and αk\alpha_kαk​ is constant within a cycle.

The analysis assumes that the subgradients the iteration uses are bounded by a constant ccc and that, at each cycle start k>0k>0k>0, the function values at the intermediate points of the cycle differ from those at xkx_kxk​ by at most ccc times the distance (Assumption 1 for (19), (20); Assumption 2 for (21)). Both hold, for example, when all fif_ifi​, hih_ihi​ are polyhedral or Lipschitz.

Formalization targets

Goal: Proposition 6

If αk→0\alpha_k\to0αk​→0 and ∑kαk=∞\sum_k\alpha_k=\infty∑k​αk​=∞, then

lim inf⁡k→∞F(xk)=F∗,\liminf_{k\to\infty}F(x_k)=F^*,k→∞liminf​F(xk​)=F∗,

and if moreover X∗≠∅X^*\neq\emptysetX∗=∅ and ∑kαk2<∞\sum_k\alpha_k^2<\infty∑k​αk2​<∞, then xk→x∗x_k\to x^*xk​→x∗ for some x∗∈X∗x^*\in X^*x∗∈X∗. Both parts are one item, as in the paper.

Milestones

  1. Proposition 1: the proximal iteration over XXX equals PX(xk−αk∇~f(xk+1))P_X(x_k-\alpha_k\tilde\nabla f(x_{k+1}))PX​(xk​−αk​∇~f(xk+1​)), and ∥xk+1−y∥2≤∥xk−y∥2−2αk(f(xk+1)−f(y))−∥xk−xk+1∥2\|x_{k+1}-y\|^2\le\|x_k-y\|^2-2\alpha_k(f(x_{k+1})-f(y))-\|x_k-x_{k+1}\|^2∥xk+1​−y∥2≤∥xk​−y∥2−2αk​(f(xk+1​)−f(y))−∥xk​−xk+1​∥2 for y∈Xy\in Xy∈X.
  2. Eq. (30) and Eq. (37): one-iteration estimates for (19)/(20) and for (21).
  3. Proposition 3: over one cycle, ∥xk+m−y∥2≤∥xk−y∥2−2αk(F(xk)−F(y))+αk2βm2c2\|x_{k+m}-y\|^2\le\|x_k-y\|^2-2\alpha_k(F(x_k)-F(y))+\alpha_k^2\beta m^2c^2∥xk+m​−y∥2≤∥xk​−y∥2−2αk​(F(xk​)−F(y))+αk2​βm2c2, with β=1m+4\beta=\frac1m+4β=m1​+4 for (19), (20) and β=5m+4\beta=\frac5m+4β=m5​+4 for (21).
  4. Footnote 5: nonnegative sequences with Yk+1≤Yk−Zk+WkY_{k+1}\le Y_k-Z_k+W_kYk+1​≤Yk​−Zk​+Wk​ and ∑Wk<∞\sum W_k<\infty∑Wk​<∞ have YkY_kYk​ convergent.
  5. Proof of Proposition 6: ∥xk+1−xk∥≤2αkc\|x_{k+1}-x_k\|\le2\alpha_kc∥xk+1​−xk​∥≤2αk​c.
  6. Proposition 4 (constant stepsize α\alphaα): lim inf⁡F(xk)=F∗\liminf F(x_k)=F^*liminfF(xk​)=F∗ if F∗=−∞F^*=-\inftyF∗=−∞, and lim inf⁡F(xk)≤F∗+αβm2c2/2\liminf F(x_k)\le F^*+\alpha\beta m^2c^2/2liminfF(xk​)≤F∗+αβm2c2/2 otherwise.

Significance

Proposition 6 is the exact-convergence guarantee for the cyclic incremental subgradient-proximal methods: with a diminishing, non-summable stepsize they reach the optimal value whatever the starting point, and with square-summable stepsizes the iterates converge to a single optimal solution. It covers the pure incremental subgradient method (fi=0f_i=0fi​=0) and the pure incremental proximal method (hi=0h_i=0hi​=0) as special cases, and it is the template for the randomized-order analysis of the companion mission. Proposition 4 quantifies what a constant stepsize achieves.

These results are proved in the paper. None of them, nor the underlying estimates, is formalized on the platform or, to our knowledge, in Mathlib. The mission produces machine-checked versions of the proximal-step lemma for extended-real-valued functions on a constrained set, of the cycle estimate (27) with its explicit constants, and of the deterministic supermartingale convergence lemma, all reusable for other incremental and proximal methods.

Difficulty

The obvious argument treats one cycle as one step of a subgradient method on FFF. It fails because within a cycle the subgradients are taken at the intermediate points zk+j−1z_{k+j-1}zk+j−1​ or xk+j−1x_{k+j-1}xk+j−1​, not at xkx_kxk​, and the proximal steps use subgradients at the points they produce. The error between Fj(xk)F_j(x_k)Fj​(xk​) and FjF_jFj​ at those points must be controlled through the drift of the iterates during the cycle, and the bookkeeping differs between (19)/(20) and (21), which is why β\betaβ differs. For the second part of Proposition 6, convergence of the values in the lim inf⁡\liminfliminf sense does not by itself give convergence of the iterates, and X∗X^*X∗ may contain more than one point.

Formalization scope

  • Rn\mathbb R^nRn is EuclideanSpace ℝ (Fin n). Components are Fin m (0-based), so iki_kik​ is k % m, and the paper's j=1,…,mj=1,\dots,mj=1,…,m with zk+j−1z_{k+j-1}zk+j−1​ becomes j=0,…,m−1j=0,\dots,m-1j=0,…,m−1 with z (k + j). m≥1m\ge1m≥1 is assumed (NeZero m).
  • PXP_XPX​ is a predicate (IsProj: a nearest point of XXX), not a choice function.
  • Each iteration is a relation Step between xkx_kxk​, zkz_kzk​, xk+1x_{k+1}xk+1​ and the two subgradients it uses, with the fff-subgradient at the point the paper names. A run records these subgradients, so Assumptions 1–2 bound exactly them. The assumptions are not replaced by Lipschitz continuity, which is only a sufficient condition (p. 9).
  • F∗F^*F∗ and lim inf⁡F(xk)\liminf F(x_k)liminfF(xk​) are taken in EReal; F∗=−∞F^*=-\inftyF∗=−∞ is allowed and no boundedness is assumed.
  • The standing assumptions of p. 4 (X nonempty closed convex, fi,hif_i,h_ifi​,hi​ convex), positive stepsizes, constancy within a cycle and Assumptions 1–2 (stated "throughout this section", p. 8) are explicit hypotheses of every statement, including the goal, whose sentence does not repeat them.
  • The starting point x0x_0x0​ is arbitrary, as in the paper. Assumptions 1–2 make the cycle-start conditions only for k>0k>0k>0, and the bound ∥xk+1−xk∥≤2αkc\|x_{k+1}-x_k\|\le2\alpha_kc∥xk+1​−xk​∥≤2αk​c needs xk∈Xx_k\in Xxk​∈X, which holds from k=1k=1k=1 on. Proposition 3 and the step bound are therefore stated for k>0k>0k>0 and k≥1k\ge1k≥1; this does not affect Propositions 4 and 6.
  • Proposition 1 is stated for extended-real-valued closed proper convex fff, as in the paper, using the published class Γ0\Gamma_0Γ0​ (MoreauProx.Characterization.GammaZero) and its subgradients, with relative interiors as Mathlib's intrinsicInterior.

The goal cannot be satisfied vacuously: a sorry-free check confirms that the hypotheses hold together (for n=1n=1n=1, m=2m=2m=2, X=RX=\mathbb RX=R, αk=1/(⌊k/2⌋+1)\alpha_k=1/(\lfloor k/2\rfloor+1)αk​=1/(⌊k/2⌋+1), X∗≠∅X^*\neq\emptysetX∗=∅). Restricting to Lipschitz components, to bounded-below FFF, or to x0∈Xx_0\in Xx0​∈X would state a weaker theorem and is ruled out.

Proofs of any item are welcome, as are general lemmas (the projection theorem as a variational inequality, the subdifferential sum rule under the relative-interior condition) that the proofs need.

Selected references

  • D. P. Bertsekas, Incremental Proximal Methods for Large Scale Convex Optimization, Report LIDS-P-2847, MIT, 2010 (rev. March 2011); Math. Program. 129(2) (2011) 163–195. https://doi.org/10.1007/s10107-011-0472-0
  • A. Nedić, D. P. Bertsekas, Incremental Subgradient Methods for Nondifferentiable Optimization, SIAM J. Optim. 12(1) (2001) 109–138. https://doi.org/10.1137/S1052623499362111
  • D. P. Bertsekas, Incremental Gradient, Subgradient, and Proximal Methods for Convex Optimization: A Survey, in Optimization for Machine Learning, MIT Press, 2011. https://arxiv.org/abs/1507.01030
  • D. P. Bertsekas, A. Nedić, A. E. Ozdaglar, Convex Analysis and Optimization, Athena Scientific, 2003.
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Scheduling Problems with Two Competing Agents 6: PARTITION Reduces to Two Agents Each Bounding Their Own Total Completion Time on One MachineResearch Paper

Two agents sharing one machine

In many production and service settings a single resource is shared by parties with different goals: two departments sending orders to the same machine, two customers of a contract manufacturer, or two classes of requests on one processor. Multi-agent scheduling models this directly. Each agent owns its own jobs and its own objective, and a schedule is judged by the pair of objective values it gives the two agents rather than by a single combined criterion.

Agnetis, Mirchandani, Pacciarelli and Pacifici (Oper. Res. 52(2), 2004, pp. 229–242) set up the systematic study of the two-agent single-machine problem. For each pair of classical objectives they ask how hard it is to optimise one agent's objective while the other agent's objective stays within a given bound. This mission formalises their §9, the case in which both agents minimise their own total completion time. With a single agent, minimising the total completion time is solved by sorting the jobs by length (the shortest-processing-time rule of Smith, 1956). §9 shows that two agents, each with this easiest of objectives, already give an NP-hard problem (Theorem 9.2), and that the problem is solved in pseudopolynomial time by a dynamic program (Theorem 9.3).

Setting

There are two agents, A and B. Agent A owns jobs J1A,…,JnAAJ^A_1,\dots,J^A_{n_A}J1A​,…,JnA​A​ with processing times phA∈Np^A_h\in\mathbb NphA​∈N; agent B owns jobs J1B,…,JnBBJ^B_1,\dots,J^B_{n_B}J1B​,…,JnB​B​ with processing times pkB∈Np^B_k\in\mathbb NpkB​∈N. All jobs are available at time 000 and are processed on one machine, one at a time, without interruption. Since both objectives are nondecreasing in the completion times, a schedule σ\sigmaσ is a sequence of all nA+nBn_A+n_BnA​+nB​ jobs processed back to back from time 000. The completion time Cj(σ)C_j(\sigma)Cj​(σ) of a job is the total processing time of the job and of all jobs before it. Agent A's cost is ∑hChA(σ)\sum_hC^A_h(\sigma)∑h​ChA​(σ) and agent B's cost is ∑kCkB(σ)\sum_kC^B_k(\sigma)∑k​CkB​(σ).

The recognition problem 1∥∑CiA≤QA, ∑CiB≤QB1\|\sum C^A_i\le Q_A,\ \sum C^B_i\le Q_B1∥∑CiA​≤QA​, ∑CiB​≤QB​ asks, for thresholds QA,QBQ_A,Q_BQA​,QB​, whether some schedule has

∑h=1nAChA(σ)≤QAand∑k=1nBCkB(σ)≤QB.\sum_{h=1}^{n_A}C^A_h(\sigma)\le Q_A\qquad\text{and}\qquad\sum_{k=1}^{n_B}C^B_k(\sigma)\le Q_B .h=1∑nA​​ChA​(σ)≤QA​andk=1∑nB​​CkB​(σ)≤QB​.

The source problem is PARTITION (Problem 9.1): given integers p1,…,pkp_1,\dots,p_kp1​,…,pk​ with P=∑ipiP=\sum_ip_iP=∑i​pi​, is there a set S⊆{1,…,k}S\subseteq\{1,\dots,k\}S⊆{1,…,k} with ∑i∈Spi=∑i∉Spi=P/2\sum_{i\in S}p_i=\sum_{i\notin S}p_i=P/2∑i∈S​pi​=∑i∈/S​pi​=P/2?

The paper's reduction numbers the integers so that p1≤⋯≤pkp_1\le\dots\le p_kp1​≤⋯≤pk​ and gives both agents identical job sets, kkk jobs of lengths p1,…,pkp_1,\dots,p_kp1​,…,pk​, with thresholds QA=QB=T/2Q_A=Q_B=T/2QA​=QB​=T/2, where

T=3P+4∑i=1k(k−i)pi.T=3P+4\sum_{i=1}^k(k-i)p_i .T=3P+4i=1∑k​(k−i)pi​.

Writing J[i]J[i]J[i] for the pair JiA,JiBJ^A_i,J^B_iJiA​,JiB​, an SPT schedule processes J[1],…,J[k]J[1],\dots,J[k]J[1],…,J[k] in order, each pair in either internal order; xxx denotes the total length of the pairs in which B goes first.

Formalization targets

Goal: Theorem 9.2

PARTITION ≤p 1∥∑CiA≤QA, ∑CiB≤QB\text{PARTITION}\ \le_p\ 1\|\textstyle\sum C^A_i\le Q_A,\ \sum C^B_i\le Q_BPARTITION ≤p​ 1∥∑CiA​≤QA​, ∑CiB​≤QB​

Here ≤p\le_p≤p​ is polynomial-time many-one reducibility between languages of binary codes: a polynomial-time Turing-machine-computable map on strings that sends codes of PARTITION yes-instances, and only those, to codes of yes-instances of the recognition problem. Together with the NP-completeness of PARTITION (Karp 1972) this is the statement "1∥∑CiA:∑CiB1\|\sum C^A_i : \sum C^B_i1∥∑CiA​:∑CiB​ is binary NP-hard".

Milestones of the proof

  1. Every SPT schedule has ∑CiA+∑CiB=T\sum C^A_i+\sum C^B_i=T∑CiA​+∑CiB​=T, and QA=QB=T/2Q_A=Q_B=T/2QA​=QB​=T/2.
  2. Eqs. (5) and (6): in an SPT schedule, ∑CiA=P+2∑i(k−i)pi+x\sum C^A_i=P+2\sum_i(k-i)p_i+x∑CiA​=P+2∑i​(k−i)pi​+x and ∑CiB=P+2∑i(k−i)pi+(P−x)\sum C^B_i=P+2\sum_i(k-i)p_i+(P-x)∑CiB​=P+2∑i​(k−i)pi​+(P−x).
  3. A schedule with ∑CiA≤T/2\sum C^A_i\le T/2∑CiA​≤T/2 and ∑CiB≤T/2\sum C^B_i\le T/2∑CiB​≤T/2 processes the jobs in nondecreasing order of length.
  4. For pairwise distinct p1<⋯<pkp_1<\dots<p_kp1​<⋯<pk​: PARTITION has a solution iff some schedule meets T/2T/2T/2 for both agents.

Further result: Theorem 9.3 with recursion (7)

With each agent's jobs numbered by nondecreasing length and P(i,j)P(i,j)P(i,j) the total length of J1A,…,JiA,J1B,…,JjBJ^A_1,\dots,J^A_i,J^B_1,\dots,J^B_jJ1A​,…,JiA​,J1B​,…,JjB​, the recursion

F(i,j,q)=min⁡{F(i−1,j,q)+P(i−1,j)+piA; F(i,j−1,q−P(i,j))}F(i,j,q)=\min\bigl\{F(i-1,j,q)+P(i-1,j)+p^A_i;\ F(i,j-1,q-P(i,j))\bigr\}F(i,j,q)=min{F(i−1,j,q)+P(i−1,j)+piA​; F(i,j−1,q−P(i,j))}

with F(0,0,q)=0F(0,0,q)=0F(0,0,q)=0 for q≥0q\ge0q≥0 and F=+∞F=+\inftyF=+∞ for q<0q<0q<0 yields F(nA,nB,Q)=min⁡{∑CiA:∑CiB≤Q}F(n_A,n_B,Q)=\min\{\sum C^A_i:\sum C^B_i\le Q\}F(nA​,nB​,Q)=min{∑CiA​:∑CiB​≤Q}, and +∞+\infty+∞ when no schedule meets the bound.

Significance

Theorem 9.2 fills one cell of the paper's complexity table: even when both agents use the objective that is trivial for one agent, sharing the machine makes the constrained problem NP-hard. Together with Theorem 9.3 it places 1∥∑CiA:∑CiB1\|\sum C^A_i:\sum C^B_i1∥∑CiA​:∑CiB​ exactly: NP-hard under binary encoding, solvable in pseudopolynomial time, hence not strongly NP-hard unless P = NP. The later literature on two-agent and multi-agent scheduling (for example the monograph of Agnetis, Billaut, Gawiejnowicz, Pacciarelli and Soukhal, Multiagent Scheduling, Springer 2014) cites this classification.

Neither result has a machine-checked proof that we know of. The mission adds a formal record of the reduction and of the dynamic program, reusable definitions for the two-agent total-completion-time problem, and a correction of the printed proof: the equivalence between PARTITION and the constructed instance, as printed, holds only when the integers are pairwise distinct. For p=(1,1,1,1,10)p=(1,1,1,1,10)p=(1,1,1,1,10) PARTITION has no solution, yet a schedule meets T/2=41T/2=41T/2=41 for both agents. Theorem 9.2 itself is not affected, since PARTITION remains NP-hard, but a complete formal proof needs a reduction that is correct on every input.

Difficulty

The equivalence for distinct integers rests on two facts: the overall total ∑CiA+∑CiB\sum C^A_i+\sum C^B_i∑CiA​+∑CiB​ is at least TTT for every schedule, with equality only for sequences in nondecreasing order of length; and, with distinct lengths, such a sequence is made of consecutive pairs, whose split is controlled by xxx. The naive formal argument stops at the second fact, which is false with repeated lengths: a block of equal-length jobs can be shared between the agents in ways no sequence of pairs realises. The goal adds the encoding layer: the reduction must be computable in polynomial time on a Turing machine, must handle repeated and zero sizes and odd PPP (where T/2T/2T/2 is not an integer and the language's thresholds are), and must send strings that do not code a PARTITION instance outside the target language. For Theorem 9.3, the dynamic program is correct only because some optimal schedule orders each agent's jobs by length, and the constraint makes this exchange argument less direct than for a single agent.

Formalization scope

Jobs are Fin nA ⊕ Fin nB (Sum.inl h is Jh+1AJ^A_{h+1}Jh+1A​, Sum.inr k is Jk+1BJ^B_{k+1}Jk+1B​, 0-based). Schedules, completion times and the idle-free sequence model are the published MooreLateJobs.Shared.completionTime (Moore 1968 series): a schedule is a duplicate-free list containing every job once, and completion times are real numbers. Processing times and thresholds of the language are natural numbers. Reducibility is the published CookPvsNP.PolyReducible, and PARTITION, the alphabet and the binary codes are the published ProjSchedTW.Complexity.Encoding (partitionLang, whose sizes are natural numbers including 000). The target language allows any job counts and any processing times; identical job sets are a property of the construction only.

The following readings are explicit:

  • An SPT schedule of the construction is given by a choice x:Fin k→Boolx:\mathrm{Fin}\,k\to\mathrm{Bool}x:Fink→Bool of the first agent in each pair; "feasible implies SPT" is stated as "lengths are nondecreasing along the sequence", which is what the paper's exchange argument proves.
  • The milestones take the integers already sorted, as a hypothesis; the paper's thresholds T/2T/2T/2 are real numbers in the milestones.
  • The equivalence milestone assumes p1<⋯<pkp_1<\dots<p_kp1​<⋯<pk​; the printed version with ≤\le≤ is false, as shown above.
  • In recursion (7), the terms F(−1,j,q)F(-1,j,q)F(−1,j,q) and F(i,−1,q)F(i,-1,q)F(i,−1,q) that the paper leaves undefined are +∞+\infty+∞.
  • The running time O(nAnBQ)O(n_An_BQ)O(nA​nB​Q) of Theorem 9.3 is not formalised; only the correctness of (7) is. Membership in NP is not formalised.

The goal cannot be met by a trivial reduction: PolyReducible requires the map to be computed by a polynomial-time Turing machine and to be correct on every string, and the target language contains every two-agent instance, not only those with identical job sets. Contributions welcome: the exchange lemmas for total completion time on the shared sequence model, the SPT formulas, and Turing-machine constructions for list sorting and arithmetic on binary codes, which other reductions of this series reuse.

Selected references

  • A. Agnetis, P. B. Mirchandani, D. Pacciarelli, A. Pacifici, Scheduling Problems with Two Competing Agents, Operations Research 52(2) (2004) 229–242. https://doi.org/10.1287/opre.1030.0092
  • R. M. Karp, Reducibility among Combinatorial Problems, in Complexity of Computer Computations, Plenum (1972) 85–103. https://doi.org/10.1007/978-1-4684-2001-2_9
  • W. E. Smith, Various Optimizers for Single-Stage Production, Naval Research Logistics Quarterly 3 (1956) 59–66. https://doi.org/10.1002/nav.3800030106
  • J. M. Moore, An n Job, One Machine Sequencing Algorithm for Minimizing the Number of Late Jobs, Management Science 15(1) (1968) 102–109. https://doi.org/10.1287/mnsc.15.1.102
  • S. Cook, The P versus NP Problem, Clay Mathematics Institute Millennium Problems (2000). https://www.claymath.org/wp-content/uploads/2022/06/pvsnp.pdf
  • A. Agnetis, J.-C. Billaut, S. Gawiejnowicz, D. Pacciarelli, A. Soukhal, Multiagent Scheduling: Models and Algorithms, Springer (2014). https://doi.org/10.1007/978-3-642-41880-8
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Complexity TheoryOperations ResearchOptimization+1·Captain: mikedeng1

Scheduling Problems with Two Competing Agents 2: KNAPSACK Reduces to Minimizing One Agent's Total Weighted Completion Time Under a Makespan Bound for the OtherResearch Paper

Two agents sharing one machine

In many production and logistics settings a single resource is shared by parties with different goals: two departments of a plant that send orders to the same machine, two customers of a contract manufacturer, or two classes of traffic on one processor. Multi-agent scheduling models this directly. Each agent owns its own jobs and its own objective, and a schedule is judged by the pair of objective values it gives the two agents rather than by one combined criterion.

Agnetis, Mirchandani, Pacciarelli and Pacifici (Oper. Res. 52(2), 2004, pp. 229–242) set up the systematic study of the two-agent single-machine problem. For each pair of classical objectives they ask how hard it is to optimise one agent's objective while the other agent's objective stays within a given bound. Their Table 1 lists the outcome for each pair. This mission formalises one entry, Theorem 5.2: when agent A minimises its total weighted completion time and agent B only requires its makespan to stay below a bound, the problem is NP-hard under binary encoding of the numbers. The corresponding single-agent bicriteria problem had been shown NP-hard in the strong sense by Lenstra, Rinnooy Kan and Brucker (1977); the two-agent version differs because only B's jobs are constrained.

Setting

There are two agents, A and B. Agent A owns jobs J1A,…,JnAAJ^A_1,\dots,J^A_{n_A}J1A​,…,JnA​A​; job JhAJ^A_hJhA​ has a processing time phA∈Np^A_h\in\mathbb NphA​∈N and a weight whA∈Nw^A_h\in\mathbb NwhA​∈N. Agent B owns jobs J1B,…,JnBBJ^B_1,\dots,J^B_{n_B}J1B​,…,JnB​B​ with processing times pkB∈Np^B_k\in\mathbb NpkB​∈N. All jobs are available at time 000 and are processed on one machine, one at a time, without interruption.

Because both objectives are nondecreasing in the completion times, there is no reason to leave the machine idle, so a schedule σ\sigmaσ is a sequence of all nA+nBn_A+n_BnA​+nB​ jobs processed back to back from time 000. The completion time Cj(σ)C_j(\sigma)Cj​(σ) of a job jjj is the total processing time of jjj and of all jobs sequenced before it. Agent A's cost is ∑hwhAChA(σ)\sum_{h}w^A_hC^A_h(\sigma)∑h​whA​ChA​(σ); agent B's cost is its makespan Cmax⁡B(σ)=max⁡kCkB(σ)C^B_{\max}(\sigma)=\max_kC^B_k(\sigma)CmaxB​(σ)=maxk​CkB​(σ).

The paper's recognition problem 1∥∑wiCiA≤QA, Cmax⁡B≤QB1\|\sum w_iC^A_i\le Q_A,\ C^B_{\max}\le Q_B1∥∑wi​CiA​≤QA​, CmaxB​≤QB​ asks, for given thresholds QA,QBQ_A,Q_BQA​,QB​, whether some schedule has

∑h=1nAwhAChA(σ)≤QAandCkB(σ)≤QB  for all k.\sum_{h=1}^{n_A}w^A_hC^A_h(\sigma)\le Q_A\qquad\text{and}\qquad C^B_k(\sigma)\le Q_B\ \text{ for all }k .h=1∑nA​​whA​ChA​(σ)≤QA​andCkB​(σ)≤QB​  for all k.

The source problem is KNAPSACK (Problem 5.1): given nonnegative integers u1,…,unu_1,\dots,u_nu1​,…,un​, w1,…,wnw_1,\dots,w_nw1​,…,wn​ and integers b,Wb,Wb,W, is there S⊆{1,…,n}S\subseteq\{1,\dots,n\}S⊆{1,…,n} with ∑i∈Sui≤b\sum_{i\in S}u_i\le b∑i∈S​ui​≤b and ∑i∈Swi≥W\sum_{i\in S}w_i\ge W∑i∈S​wi​≥W?

Formalization targets

Goal: Theorem 5.2

KNAPSACK ≤p 1∥∑wiCiA≤QA, Cmax⁡B≤QB\text{KNAPSACK}\ \le_p\ 1\|\textstyle\sum w_iC^A_i\le Q_A,\ C^B_{\max}\le Q_BKNAPSACK ≤p​ 1∥∑wi​CiA​≤QA​, CmaxB​≤QB​

Here ≤p\le_p≤p​ is polynomial-time many-one reducibility between languages of binary codes: a Turing-machine-computable, polynomial-time map on strings sending codes of KNAPSACK yes-instances, and only those, to codes of yes-instances of the recognition problem. Together with the NP-completeness of KNAPSACK (Garey and Johnson 1979) this is the statement "1∥∑wiCiA:Cmax⁡B1\|\sum w_iC^A_i : C^B_{\max}1∥∑wi​CiA​:CmaxB​ is binary NP-hard".

Milestones

The paper's reduction builds, from a KNAPSACK instance, the two-agent instance with piA=uip^A_i=u_ipiA​=ui​, wiA=wiw^A_i=w_iwiA​=wi​, a single B-job of length p1B=w^u^p^B_1=\hat w\hat up1B​=w^u^ (where u^=∑iui\hat u=\sum_iu_iu^=∑i​ui​, w^=∑iwi\hat w=\sum_iw_iw^=∑i​wi​), and thresholds QB=b+p1BQ_B=b+p^B_1QB​=b+p1B​, QA=w^u^+(w^−W)p1BQ_A=\hat w\hat u+(\hat w-W)p^B_1QA​=w^u^+(w^−W)p1B​. The milestones are the two directions of the proof and their combination:

  1. Eq. (1): if SSS solves KNAPSACK, every sequence with exactly the A-jobs of SSS before the B-job meets both thresholds.
  2. Eq. (2): if ∑iwiui>0\sum_iw_iu_i>0∑i​wi​ui​>0 and a sequence meets both thresholds, the A-jobs before the B-job solve KNAPSACK.
  3. Equivalence: under ∑iwiui>0\sum_iw_iu_i>0∑i​wi​ui​>0, KNAPSACK is a yes-instance iff the constructed instance is.
  4. §8: with every B-job given due date QQQ and Q′=0Q'=0Q′=0, a sequence meets ∑UiB≤Q′\sum U^B_i\le Q'∑UiB​≤Q′ (and A's bound) iff it meets Cmax⁡B≤QC^B_{\max}\le QCmaxB​≤Q, which carries the hardness over to 1∥∑wiCiA:∑UiB1\|\sum w_iC^A_i:\sum U^B_i1∥∑wi​CiA​:∑UiB​.

Significance

Theorem 5.2 fixes the complexity of one cell of the two-agent classification. It shows that the polynomial algorithm for the unweighted case 1∥∑CiA:fmax⁡B1\|\sum C^A_i:f^B_{\max}1∥∑CiA​:fmaxB​ (Theorem 5.5 of the same paper) cannot be extended to arbitrary weights unless P = NP. Through §8 it also settles 1∥∑wiCiA:∑UiB1\|\sum w_iC^A_i:\sum U^B_i1∥∑wi​CiA​:∑UiB​. The hardness is binary, not strong: the reduction produces numbers of size about w^u^\hat w\hat uw^u^, so pseudo-polynomial algorithms are not ruled out, which is consistent with the dynamic programs studied in later two-agent literature.

The result is proved in the paper; no machine-checked proof is known to exist. Formalizing it produces a complete reduction from a two-constraint knapsack problem to a scheduling recognition problem, with the encoding, the degenerate instances and the polynomial running time all made explicit. The model and the KNAPSACK language are reusable by other two-agent reductions (Theorems 9.2, 10.1 and 10.2 of the paper reduce from PARTITION in the same frame).

Difficulty

The two directions of the equivalence are short computations with completion times. The printed argument, however, is not correct as written in two places. The bounds "smaller than w^u^\hat w\hat uw^u^" and "smaller than (w^−W)p1B(\hat w-W)p^B_1(w^−W)p1B​" in the derivation of (1) hold only with equality allowed. The strict inequalities in (2) fail when ∑iwiui=0\sum_iw_iu_i=0∑i​wi​ui​=0, and then the reduction itself fails: with all ui=0u_i=0ui​=0 and W>w^W>\hat wW>w^ the KNAPSACK instance is a no-instance while the constructed instance has QA=QB=0Q_A=Q_B=0QA​=QB​=0 and every schedule meets both thresholds. A complete reduction must recognise such instances and treat them separately.

The construction also produces integer thresholds that can be negative (b<−p1Bb<-p^B_1b<−p1B​, or W>w^+1W>\hat w+1W>w^+1), while instances of the target are coded with natural numbers. Finally, the reduction must be a polynomial-time Turing machine computation over binary codes, including the decoding of arbitrary strings and the binary multiplication w^u^\hat w\hat uw^u^; that is where most of the formal work lies.

Formalization scope

  • Model. Jobs are Fin nA ⊕ Fin nB (0-based: Sum.inl h is Jh+1AJ^A_{h+1}Jh+1A​, Sum.inr k is Jk+1BJ^B_{k+1}Jk+1B​). Schedules and completion times are the published MooreLateJobs.Shared sequence model (IsSchedule, completionTime) of the Moore (1968) series: a duplicate-free list of all jobs, processed without idle time from time 000. Integer processing times are cast to R\mathbb RR.
  • Makespan bound. Cmax⁡B≤QBC^B_{\max}\le Q_BCmaxB​≤QB​ is written as CkB≤QBC^B_k\le Q_BCkB​≤QB​ for every B-job; no nonemptiness of B's job set is assumed.
  • Languages. Polynomial-time reducibility is the published CookPvsNP.PolyReducible (Cook's Definition 3, one-tape Turing machines). Codes use the published binary encoding ProjSchedTW.Complexity.Encoding (alphabet BSym, encNat, encInt) of the Neumann–Schwindt–Zimmermann series. A KNAPSACK instance is coded as the integers n,u1,…,un,w1,…,wn,b,Wn,u_1,\dots,u_n,w_1,\dots,w_n,b,Wn,u1​,…,un​,w1​,…,wn​,b,W; a target instance as the natural numbers nA,nBn_A,n_BnA​,nB​, the processing times and weights, and QA,QBQ_A,Q_BQA​,QB​. The target language allows any nA,nB≥0n_A,n_B\ge0nA​,nB​≥0; the reduction uses nB=1n_B=1nB​=1.
  • Readings of the paper. "Binary NP-hard" is formalised as the reduction from KNAPSACK, without the NP-completeness of KNAPSACK and without membership in NP. The milestone Eq. (2) and the equivalence carry the added hypothesis ∑iwiui>0\sum_iw_iu_i>0∑i​wi​ui​>0; the inequalities "smaller than" in (1) are read as ≤\le≤. Eq. (1) is stated for every order of the jobs inside SSS and inside its complement. The §8 result is stated as the encoding-free equivalence of feasible solutions, not as a reduction between languages.
  • Ruled out. The goal cannot be met by a reduction that ignores the input: the equivalence must hold for every string, and the target language is exactly the codes of yes-instances of the two-agent recognition problem with B's objective the makespan. KNAPSACK here is the two-constraint problem of Problem 5.1, not subset sum.

Contributions welcome: proofs of the two directions, of the equivalence, the treatment of the degenerate instances, and the Turing machine for the reduction, which would also serve the other binary-coded reductions on the platform.

Selected references

  • A. Agnetis, P. B. Mirchandani, D. Pacciarelli, A. Pacifici, Scheduling Problems with Two Competing Agents, Operations Research 52(2) (2004) 229–242. https://doi.org/10.1287/opre.1030.0092
  • M. R. Garey, D. S. Johnson, Computers and Intractability: A Guide to the Theory of NP-Completeness, W. H. Freeman, 1979.
  • J. K. Lenstra, A. H. G. Rinnooy Kan, P. Brucker, Complexity of Machine Scheduling Problems, Annals of Discrete Mathematics 1 (1977) 343–362. https://doi.org/10.1016/S0167-5060(08)70743-X
  • S. Cook, The P versus NP Problem, Clay Mathematics Institute Millennium Problem description. https://www.claymath.org/wp-content/uploads/2022/06/pvsnp.pdf
  • J. M. Moore, An n Job, One Machine Sequencing Algorithm for Minimizing the Number of Late Jobs, Management Science 15(1) (1968) 102–109. https://doi.org/10.1287/mnsc.15.1.102
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Control TheoryDynamical SystemsLinear algebra·Captain: mikedeng1

Lyapunov Equations, Energy Functionals, and Model Order Reduction of Bilinear and Stochastic Systems 1: States Reached from 0 Stay in Im P and Ker Q Gives Zero Output, for Gramians P, Q ≥ 0 of (3.6)Research Paper

Motivation

Balanced truncation is the standard method for reducing the state dimension of a linear control system while keeping its input–output behaviour: states that are both hard to reach and hard to observe are discarded. Its justification rests on two Gramians, the solutions PPP and QQQ of a pair of Lyapunov equations, whose quadratic forms measure how much input energy a state costs to reach and how much output energy it produces. For linear systems the facts are classical: the image of the controllability Gramian is the reachable subspace, and the kernel of the observability Gramian is the unobservable subspace.

Bilinear systems, in which the input multiplies the state, are the simplest nonlinear extension of linear control systems. Their generalized Lyapunov equations have the same form as the Lyapunov equations of linear stochastic systems with multiplicative noise, which is why Benner and Damm treat the two classes together. Balanced truncation was extended to them using the solutions of generalized Lyapunov equations (Al-Baiyat and Bettayeb, 1993; Gray and Mesko, 1998, both as cited by Benner and Damm). Benner and Damm, in Lyapunov Equations, Energy Functionals, and Model Order Reduction of Bilinear and Stochastic Systems (SIAM J. Control Optim. 49(2), 2011, doi:10.1137/09075041X), examine which of the linear-system energy interpretations survive for bilinear systems. Their Theorem 3.1 is the structural result that does survive: the kernels of the Gramians still identify states that are unreachable from the origin and states that produce no output, so these states can be eliminated without changing the transfer behaviour.

Setting

Fix n,m,p≥0n, m, p \ge 0n,m,p≥0 and real matrices A,N1,…,Nm∈Rn×nA, N_1,\dots,N_m\in\mathbb R^{n\times n}A,N1​,…,Nm​∈Rn×n, B∈Rn×mB\in\mathbb R^{n\times m}B∈Rn×m, C∈Rp×nC\in\mathbb R^{p\times n}C∈Rp×n. The bilinear control system (3.1)–(3.2) is

x˙=Ax+∑j=1mNjx uj+Bu,y=Cx,\dot x = Ax + \sum_{j=1}^m N_j x\,u_j + Bu,\qquad y = Cx,x˙=Ax+j=1∑m​Nj​xuj​+Bu,y=Cx,

with state x(t)∈Rnx(t)\in\mathbb R^nx(t)∈Rn, input u(t)=[u1(t),…,um(t)]T∈Rmu(t) = [u_1(t),\dots,u_m(t)]^T\in\mathbb R^mu(t)=[u1​(t),…,um​(t)]T∈Rm and output y(t)∈Rpy(t)\in\mathbb R^py(t)∈Rp. The homogeneous system (3.5) drops the term BuBuBu: x˙=Ax+∑jNjx uj\dot x = Ax + \sum_j N_j x\,u_jx˙=Ax+∑j​Nj​xuj​, y=Cxy = Cxy=Cx. The same mmm indexes the bilinear terms and the columns of BBB. Write x(t,x0,u)x(t, x_0, u)x(t,x0​,u) for a solution with input uuu and initial state x(0)=x0x(0) = x_0x(0)=x0​, and y(t,x0,u)=Cx(t,x0,u)y(t,x_0,u) = Cx(t,x_0,u)y(t,x0​,u)=Cx(t,x0​,u).

An admissible input is a function u:[0,∞)→Rmu:[0,\infty)\to\mathbb R^mu:[0,∞)→Rm that is integrable on every interval [0,T][0,T][0,T]. A solution with x(0)=x0x(0) = x_0x(0)=x0​ is a continuous x:[0,∞)→Rnx:[0,\infty)\to\mathbb R^nx:[0,∞)→Rn satisfying

x(t)=x0+∫0t(Ax(s)+∑j=1muj(s)Njx(s)+Bu(s)) ds(t≥0).x(t) = x_0 + \int_0^t \Big(Ax(s) + \sum_{j=1}^m u_j(s)N_jx(s) + Bu(s)\Big)\,ds\qquad (t\ge 0).x(t)=x0​+∫0t​(Ax(s)+j=1∑m​uj​(s)Nj​x(s)+Bu(s))ds(t≥0).

The generalized Lyapunov equations (3.6) are

AP+PAT+∑j=1mNjPNjT=−BBT,ATQ+QA+∑j=1mNjTQNj=−CTC.AP + PA^T + \sum_{j=1}^m N_jPN_j^T = -BB^T,\qquad A^TQ + QA + \sum_{j=1}^m N_j^TQN_j = -C^TC .AP+PAT+j=1∑m​Nj​PNjT​=−BBT,ATQ+QA+j=1∑m​NjT​QNj​=−CTC.

A solution PPP of the first is a controllability Gramian and a solution QQQ of the second an observability Gramian. "P≥0P\ge 0P≥0" means PPP is symmetric nonnegative definite; Im P\mathrm{Im}\,PImP and Ker P\mathrm{Ker}\,PKerP are its image and kernel.

Formalization targets

Goal: Theorem 3.1 (p. 695)

(a) If P≥0P\ge 0P≥0 solves the first equation of (3.6), then for every admissible input uuu

x(t,0,u)∈Im Pfor all t≥0.x(t,0,u)\in\mathrm{Im}\,P\qquad\text{for all } t\ge 0 .x(t,0,u)∈ImPfor all t≥0.

(b) If Q≥0Q\ge 0Q≥0 solves the second equation of (3.6) and x0∈Ker Qx_0\in\mathrm{Ker}\,Qx0​∈KerQ, then for the homogeneous system (3.5) and every admissible input uuu

y(t,x0,u)=Cx(t,x0,u)=0for all t≥0.y(t,x_0,u) = Cx(t,x_0,u) = 0\qquad\text{for all } t\ge 0 .y(t,x0​,u)=Cx(t,x0​,u)=0for all t≥0.

Milestones (the steps of the paper's proof, pp. 695–696)

  1. NjT Ker P⊂Ker P⊂Ker BTN_j^T\,\mathrm{Ker}\,P\subset\mathrm{Ker}\,P\subset\mathrm{Ker}\,B^TNjT​KerP⊂KerP⊂KerBT.
  2. AT Ker P⊂Ker PA^T\,\mathrm{Ker}\,P\subset\mathrm{Ker}\,PATKerP⊂KerP.
  3. Im P\mathrm{Im}\,PImP is invariant under the vector field of (3.1): z∈Im Pz\in\mathrm{Im}\,Pz∈ImP implies Az+∑jwjNjz+Bw∈Im PAz + \sum_j w_jN_jz + Bw\in\mathrm{Im}\,PAz+∑j​wj​Nj​z+Bw∈ImP for every w∈Rmw\in\mathbb R^mw∈Rm.
  4. Nj Ker Q⊂Ker Q⊂Ker CN_j\,\mathrm{Ker}\,Q\subset\mathrm{Ker}\,Q\subset\mathrm{Ker}\,CNj​KerQ⊂KerQ⊂KerC and A Ker Q⊂Ker QA\,\mathrm{Ker}\,Q\subset\mathrm{Ker}\,QAKerQ⊂KerQ.
  5. Ker Q\mathrm{Ker}\,QKerQ is invariant under the vector field of (3.5).

Significance

The result. Part (a) says that a state outside Im P\mathrm{Im}\,PImP cannot be reached from the origin by any input, so its controllability energy EcE_cEc​ is infinite; part (b) says that a state in Ker Q\mathrm{Ker}\,QKerQ is indistinguishable from the origin at the output, so its observability energy EoE_oEo​ is zero. Together they justify the first step of balanced truncation for bilinear systems (Remark 3.2 of the paper): the system can be restricted to Im P\mathrm{Im}\,PImP and projected along Ker Q\mathrm{Ker}\,QKerQ without changing its input–output map, after which the Gramians are nonsingular and can be balanced. The theorem needs neither stability of AAA nor uniqueness of the Gramians, so it applies to every nonnegative definite solution of (3.6). The rest of §3 of the paper shows that the finer, quantitative energy estimates of the linear case fail for bilinear systems; this qualitative statement is what remains exact.

Formalizing it. The theorem is proved in the paper; no machine-checked version is known. A formal proof yields a reusable invariance principle: a subspace that is invariant under every vector field z↦Az+∑jwjNjz+Bwz\mapsto Az + \sum_j w_jN_jz + Bwz↦Az+∑j​wj​Nj​z+Bw is invariant under the flow of the input-driven system, for merely integrable inputs. It also yields the linear-algebra lemmas relating kernels of nonnegative definite solutions of generalized Lyapunov equations to the system matrices, which are used throughout model reduction and stochastic stability theory.

Difficulty

The algebraic part (milestones 1, 2, 4) rests on the fact that for a nonnegative definite matrix MMM, vTMv=0v^TMv = 0vTMv=0 forces Mv=0Mv = 0Mv=0, applied to the terms of the Lyapunov equation tested against a kernel vector. The passage from the vector field to trajectories is where care is needed. The paper's sentence "x˙(t)∈Im P\dot x(t)\in\mathrm{Im}\,Px˙(t)∈ImP whenever x(t)∈Im Px(t)\in\mathrm{Im}\,Px(t)∈ImP, so Im P\mathrm{Im}\,PImP is invariant" is not by itself an argument: tangency of a vector field to a subspace implies invariance only together with a uniqueness or Gronwall-type estimate, and here the field depends on time through an input that is only integrable, so xxx is merely absolutely continuous and x˙\dot xx˙ exists only almost everywhere. A pointwise "the derivative points into the subspace" argument therefore does not apply as stated, and the step needs an estimate on the component of x(t)x(t)x(t) orthogonal to the subspace.

Formalization scope

The Lean development uses states Fin n → ℝ, matrices Matrix (Fin n) (Fin n) ℝ, the matrix–vector product *ᵥ, and indices j=1,…,mj = 1,\dots,mj=1,…,m as Fin m. Im P\mathrm{Im}\,PImP and Ker P\mathrm{Ker}\,PKerP are LinearMap.range and LinearMap.ker of Matrix.toLin' P; "P≥0P\ge 0P≥0" is Matrix.PosSemidef, which includes symmetry. Admissible inputs are integrable on every [0,T][0,T][0,T] (this contains L2[0,∞[L^2[0,\infty[L2[0,∞[, the input space of the paper's energy functionals). A solution is a function continuous on [0,∞)[0,\infty)[0,∞) whose integrand is integrable on every [0,t][0,t][0,t] and which satisfies the integral equation for all t≥0t\ge 0t≥0; no uniqueness of solutions is presupposed, and the theorem is asserted for every such solution.

Two reading decisions are fixed. First, part (b) is stated for every admissible input uuu, not only for u=0u = 0u=0 as printed in the theorem: the paper's proof concludes "x(t,x0,u)∈Ker Qx(t,x_0,u)\in\mathrm{Ker}\,Qx(t,x0​,u)∈KerQ for all t≥0t\ge0t≥0, implying y(t,x0,u)=0y(t,x_0,u) = 0y(t,x0​,u)=0", and the theorem's clause "i.e., Eo(x0)=0E_o(x_0) = 0Eo​(x0​)=0" (with EoE_oEo​ a maximum over inputs) needs this form. The ∀u\forall u∀u statement contains the printed one. Second, the clauses "i.e., Ec(x0)=∞E_c(x_0) = \inftyEc​(x0​)=∞" and "i.e., Eo(x0)=0E_o(x_0) = 0Eo​(x0​)=0", which restate the conclusions through the energy functionals (3.3)–(3.4), are not formalized.

The statements must not be trivialized: assuming PPP positive definite makes (a) empty (Im P=Rn\mathrm{Im}\,P = \mathbb R^nImP=Rn), assuming AAA stable or the Gramians unique adds hypotheses the paper does not have, and a solution notion requiring C1C^1C1 trajectories for integrable inputs would make the solution set empty. None of these is used. A local check confirms the hypotheses have content: for A=−I2A = -I_2A=−I2​, N1=0N_1 = 0N1​=0, B=e1B = e_1B=e1​, the matrix P=diag(1/2,0)P = \mathrm{diag}(1/2, 0)P=diag(1/2,0) is a nonnegative definite solution of (3.6) with e2∉Im Pe_2\notin\mathrm{Im}\,Pe2​∈/ImP.

A complete development needs Mathlib's facts on nonnegative definite matrices, interval integrals of vector-valued functions, and a Gronwall inequality with an integrable coefficient. The flow-invariance lemma for input-driven linear-in-state systems is reusable beyond this mission. Contributions welcome: proofs of the five milestones, and the passage from vector-field invariance to trajectory invariance.

Selected references

  • P. Benner, T. Damm, Lyapunov Equations, Energy Functionals, and Model Order Reduction of Bilinear and Stochastic Systems, SIAM J. Control Optim. 49(2), 686–711, 2011. https://doi.org/10.1137/09075041X
  • S. A. Al-Baiyat, M. Bettayeb, A new model reduction scheme for k-power bilinear systems, Proceedings of the 32nd IEEE Conference on Decision and Control, San Antonio, 1993, pp. 22–27 (reference [1] of Benner–Damm).
  • W. S. Gray, J. Mesko, Energy functions and algebraic Gramians for bilinear systems, Preprints of the 4th IFAC Nonlinear Control Systems Design Symposium, Enschede, 1998, pp. 103–108 (reference [25] of Benner–Damm).
  • B. C. Moore, Principal component analysis in linear systems: Controllability, observability, and model reduction, IEEE Trans. Automat. Control 26(1), 17–32, 1981. https://doi.org/10.1109/TAC.1981.1102568
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AnalysisOptimization·Captain: mikedeng1

Semismooth and Semiconvex Functions in Constrained Optimization I: The Pointwise Maximum or Minimum over a Compact Family of Continuously Differentiable Functions Is SemismoothResearch Paper

Motivation

Many objective functions in engineering design, Chebyshev approximation and game-theoretic planning are extremal-valued: they are the pointwise maximum or minimum of a family of smooth functions, E(x)=max⁡u∈Uf(x,u)E(x)=\max_{u\in U} f(x,u)E(x)=maxu∈U​f(x,u). Such a function is typically not differentiable at points where two or more members of the family are active, so gradient methods do not apply directly. In 1976 R. Mifflin introduced the class of semismooth functions to identify which nondifferentiable functions can be minimized by bundle-type and line-search methods whose convergence relies only on generalized gradients (Mifflin, IIASA RR-76-21; journal version SIAM J. Control Optim. 15 (1977), doi:10.1137/0315061). For that class to be useful it must contain the functions that actually occur in practice. §3 of the report shows that it contains min–max objectives, which is the content of this mission.

Background: F. H. Clarke defined the generalized gradient of a locally Lipschitz function and computed it for max functions (Clarke, Trans. AMS 205 (1975), Theorem 2.1). A. Feuer's Columbia dissertation (1974) proved the formulas of Theorem 1 below under stronger assumptions and a result close to semismoothness, from which Mifflin's proof of Theorem 2 is adapted (report, Remark, p. 8). Mifflin's notion of semismoothness was later extended to vector-valued maps by Qi and Sun (1993), where it became the standard hypothesis for superlinear convergence of nonsmooth Newton methods.

Setting

Let Rn\mathbb R^nRn carry the Euclidean inner product ⟨⋅,⋅⟩\langle\cdot,\cdot\rangle⟨⋅,⋅⟩ and norm ∣⋅∣|\cdot|∣⋅∣, and let F:Rn→RF:\mathbb R^n\to\mathbb RF:Rn→R. FFF is Lipschitz on a set BBB if ∣F(y)−F(z)∣≤K∣y−z∣|F(y)-F(z)|\le K|y-z|∣F(y)−F(z)∣≤K∣y−z∣ for all y,z∈By,z\in By,z∈B. Clarke's generalized directional derivative is

F0(x;d)=lim sup⁡h→0, t↓0F(x+h+td)−F(x+h)t,F^0(x;d)=\limsup_{h\to 0,\ t\downarrow 0}\frac{F(x+h+td)-F(x+h)}{t},F0(x;d)=h→0, t↓0limsup​tF(x+h+td)−F(x+h)​,

and the generalized gradient is ∂F(x)={g:⟨g,d⟩≤F0(x;d) ∀d}\partial F(x)=\{g:\langle g,d\rangle\le F^0(x;d)\ \forall d\}∂F(x)={g:⟨g,d⟩≤F0(x;d) ∀d}. When lim⁡t↓0[F(x+td)−F(x)]/t\lim_{t\downarrow 0}[F(x+td)-F(x)]/tlimt↓0​[F(x+td)−F(x)]/t exists it is the directional derivative F′(x;d)F'(x;d)F′(x;d); FFF is quasidifferentiable at xxx if F′(x;d)F'(x;d)F′(x;d) exists and equals F0(x;d)F^0(x;d)F0(x;d) for all ddd.

FFF is semismooth at xxx (Definition 1) if it is Lipschitz on a ball about xxx and, for each ddd and all sequences tk↓0t_k\downarrow 0tk​↓0, θk\theta_kθk​ with θk/tk→0\theta_k/t_k\to 0θk​/tk​→0, and gk∈∂F(x+tkd+θk)g_k\in\partial F(x+t_kd+\theta_k)gk​∈∂F(x+tk​d+θk​), the real sequence ⟨gk,d⟩\langle g_k,d\rangle⟨gk​,d⟩ has exactly one accumulation point. FFF is semiconvex at xxx with respect to XXX (Definition 2) if it is Lipschitz on a ball about xxx, quasidifferentiable at xxx, and x+d∈Xx+d\in Xx+d∈X, F′(x;d)≥0F'(x;d)\ge 0F′(x;d)≥0 imply F(x+d)≥F(x)F(x+d)\ge F(x)F(x+d)≥F(x).

In §3, B⊆RnB\subseteq\mathbb R^nB⊆Rn is open, TTT is a topological space, U⊆TU\subseteq TU⊆T is sequentially compact, f:Rn×T→Rf:\mathbb R^n\times T\to\mathbb Rf:Rn×T→R, and E:Rn→RE:\mathbb R^n\to\mathbb RE:Rn→R satisfies either (d) E(x)=max⁡u∈Uf(x,u)E(x)=\max_{u\in U}f(x,u)E(x)=maxu∈U​f(x,u) on BBB or (d′) E(x)=min⁡u∈Uf(x,u)E(x)=\min_{u\in U}f(x,u)E(x)=minu∈U​f(x,u) on BBB. The active set is A(x)={u∈U:E(x)=f(x,u)}A(x)=\{u\in U:E(x)=f(x,u)\}A(x)={u∈U:E(x)=f(x,u)}, and ∂xf(x,u)\partial_x f(x,u)∂x​f(x,u) is the generalized gradient of f(⋅,u)f(\cdot,u)f(⋅,u) at xxx. Hypotheses (a)–(c) ask that fff be continuous on B×UB\times UB×U, Lipschitz in xxx uniformly in uuu, and that ∂xf\partial_x f∂x​f be upper semicontinuous on B×UB\times UB×U; (e) and (e′) ask that fx′(x,u;d)f'_x(x,u;d)fx′​(x,u;d) exist and equal fx0(x,u;d)f^0_x(x,u;d)fx0​(x,u;d), respectively −fx0(x,u;−d)-f^0_x(x,u;-d)−fx0​(x,u;−d).

Formalization targets

Goal: Theorem 2 (p. 8)

If (a) holds, EEE has the max form (d) or the min form (d′), f(⋅,u)f(\cdot,u)f(⋅,u) is differentiable on BBB for each u∈Uu\in Uu∈U, and ∇xf\nabla_x f∇x​f is continuous and bounded on B×UB\times UB×U, then

E is semismooth on B.E\ \text{is semismooth on } B.E is semismooth on B.

Milestones

  • Proposition 1(a), (b), (d) (p. 3): ∂F(x)\partial F(x)∂F(x) is nonempty, convex and compact; F0(x;d)=max⁡{⟨g,d⟩:g∈∂F(x)}F^0(x;d)=\max\{\langle g,d\rangle:g\in\partial F(x)\}F0(x;d)=max{⟨g,d⟩:g∈∂F(x)}; ∂F\partial F∂F is bounded by the Lipschitz constant and upper semicontinuous.
  • Theorem 1 (pp. 7–8), max and min forms: EEE is Lipschitz on BBB,
∂E(x)=conv⁡⋃u∈A(x)∂xf(x,u),E′(x;d)=E0(x;d)=max⁡{⟨g,d⟩:g∈∂xf(x,u), u∈A(x)}\partial E(x)=\operatorname{conv}\bigcup_{u\in A(x)}\partial_x f(x,u),\qquad E'(x;d)=E^0(x;d)=\max\{\langle g,d\rangle:g\in\partial_x f(x,u),\ u\in A(x)\}∂E(x)=convu∈A(x)⋃​∂x​f(x,u),E′(x;d)=E0(x;d)=max{⟨g,d⟩:g∈∂x​f(x,u), u∈A(x)}

in the max form, and E′(x;d)=−E0(x;−d)=min⁡{⋯ }E'(x;d)=-E^0(x;-d)=\min\{\cdots\}E′(x;d)=−E0(x;−d)=min{⋯} in the min form.

  • Two claims from the proof of Theorem 2 (p. 8): the smoothness assumption yields (b), (c), (e), (e′) and ∂xf={∇xf}\partial_x f=\{\nabla_x f\}∂x​f={∇x​f}; and lim sup⁡k⟨gk,d⟩≤E′(x;d)\limsup_k\langle g_k,d\rangle\le E'(x;d)limsupk​⟨gk​,d⟩≤E′(x;d).
  • Theorem 3 (p. 10): a max function of functions semiconvex at xxx is semiconvex at xxx.
  • Propositions 3 and 4 (pp. 5–6): convex, concave and continuously differentiable functions are semismooth, with the corresponding semiconvexity and quasidifferentiability statements.

Significance

Theorem 2 places every min–max objective with continuously differentiable data inside the class on which Mifflin's descent algorithms, and the bundle methods that followed them, are proved to converge. Theorem 1 is the generalized-gradient form of Danskin's theorem, the standard tool for computing subgradients of max functions. Theorem 3 shows that semiconvexity, unlike pseudoconvexity, survives pointwise maximization, which is what the sufficient optimality results of §5 of the report need.

All of these results are proved in the report and in the literature since 1977; none is open. As far as is known, none of them has a machine-checked proof. Mathlib has Fréchet derivatives and convex analysis but no Clarke generalized gradient calculus, no semismoothness and no Danskin-type theorem. A formalization produces those pieces as reusable infrastructure, and checks the report's statements under exactly stated hypotheses. One printed claim already needs a correction (see Formalization scope).

Difficulty

Lipschitz continuity of EEE and the inequality lim sup⁡k⟨gk,d⟩≤E′(x;d)\limsup_k\langle g_k,d\rangle\le E'(x;d)limsupk​⟨gk​,d⟩≤E′(x;d) follow from Theorem 1 and the upper semicontinuity of ∂E\partial E∂E. The difficulty is the matching lower bound: semismoothness asks that the slopes ⟨gk,d⟩\langle g_k,d\rangle⟨gk​,d⟩ along an arbitrary sequence xk=x+tkd+θkx_k=x+t_kd+\theta_kxk​=x+tk​d+θk​, with arbitrary gk∈∂E(xk)g_k\in\partial E(x_k)gk​∈∂E(xk​), not accumulate strictly below E′(x;d)E'(x;d)E′(x;d). A generalized gradient of EEE at xkx_kxk​ is only a convex combination of gradients of the active functions at xkx_kxk​, and the active set can change discontinuously along the sequence. Upper semicontinuity of ∂E\partial E∂E alone does not prevent this; the function x2sin⁡(1/x)x^2\sin(1/x)x2sin(1/x) (p. 6) is Lipschitz and has an upper semicontinuous ∂F\partial F∂F but is not semismooth at 000. The argument has to use the continuity of ∇xf\nabla_x f∇x​f jointly in (x,u)(x,u)(x,u) and the compactness of UUU. Theorem 1 itself needs a mean value theorem for Lipschitz functions and a compactness argument over the active set, neither of which is in Mathlib in this form.

Formalization scope

Rn\mathbb R^nRn is EuclideanSpace ℝ (Fin n). F0F^0F0 is the published ClarkeGradients.Shared.genDirDeriv, a real limsup; every statement assumes the Lipschitz hypothesis of the page at the points where F0F^0F0 or ∂F\partial F∂F is used, so that this limsup is the true value. ∂F\partial F∂F is the support-set definition of the page, not Clarke's convex hull of gradient limits; the two coincide by Proposition 1(c), which is not assumed. F′(x;d)F'(x;d)F′(x;d) is a relation (HasDirDeriv), so "F′(x;d)≥0F'(x;d)\ge 0F′(x;d)≥0" means "exists and is nonnegative". "Exactly one accumulation point" is a unique cluster point, not convergence. "tk↓0t_k\downarrow 0tk​↓0" is read as "positive and tending to 000", as the report reads it in the proof of Lemma 2. "max" and "min" are attained extrema (IsGreatest, IsLeast), never suprema with default values.

EEE is a given function constrained by (d) or (d′), not a supremum; this rules out the trivializing formalization in which EEE is defined as ⨆ u ∈ U, f x u and takes the default value 000 for an empty or unbounded family. (d) and (d′) force U≠∅U\neq\emptysetU=∅. The page's "for each x∈Bx\in Bx∈B either (d) and (e) or (d′) and (e′)" is read as one form on all of BBB, as the proof of Theorem 2 treats it, and Theorem 1 is stated as two items. Hypothesis (c) is the sequential accumulation-point form in which Proposition 1(d) glosses upper semicontinuity.

The goal does not assume (b), (c), (e), (e′) or convexity of BBB; the report derives the first four from smoothness. The report claims (b) on all of BBB, which fails for non-convex open BBB (a bounded gradient gives a uniform Lipschitz constant only on convex sets). The corresponding milestone states (b) on balls contained in BBB, which is all the proof needs.

The development needs Clarke's calculus for Lipschitz functions on Rn\mathbb R^nRn (Propositions 1 and 2, a Lebourg mean value theorem), a Danskin-type theorem, and the regularity of C1C^1C1 functions. These are reusable well beyond this mission; a companion mission of the series covers Propositions 1(c), 2 and the chain rule. Contributions are welcome on any milestone, including alternative proofs of Theorem 1.

Selected references

  • R. Mifflin, Semismooth and semiconvex functions in constrained optimization, IIASA Research Report RR-76-21, December 1976. https://pure.iiasa.ac.at/id/eprint/524/ (journal version: SIAM J. Control Optim. 15(6) (1977) 959–972, https://doi.org/10.1137/0315061).
  • F. H. Clarke, Generalized gradients and applications, Trans. Amer. Math. Soc. 205 (1975) 247–262. https://doi.org/10.1090/S0002-9947-1975-0367131-6
  • A. Feuer, An Implementable Mathematical Programming Algorithm for Admissible Fundamental Functions, Ph.D. dissertation, Department of Mathematics, Columbia University, 1974.
  • G. Lebourg, Valeur moyenne pour gradient généralisé, C. R. Acad. Sci. Paris Sér. A 281 (1975) 795–797.
  • L. Qi and J. Sun, A nonsmooth version of Newton's method, Math. Programming 58 (1993) 353–367. https://doi.org/10.1007/BF01581275
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Algorithmic Game TheoryDifferential GeometryOperations Research·Captain: mikedeng1

Inefficiency of Nash Equilibria: For an Open Dense Set of C² Payoffs, Nash Equilibria Are Finite, an Efficient One Has a Player at a Vertex, and a Strong One Has at Most One Player off a VertexResearch Paper

Motivation

That noncooperative play usually wastes something is part of the folklore of game theory, with the Prisoner's Dilemma as its emblem: each player's best reply leads to an outcome that both would trade for another. Pradeep Dubey's paper turns this folklore into a theorem about smooth games. For games whose payoffs are twice continuously differentiable, and for all payoffs outside a negligible (closed, nowhere dense) set, Nash equilibria are finite in number and are Pareto-inefficient unless some player sits at a vertex of his strategy set. The same conclusion applies to Nash's mixed extensions of finite games (Nash 1951), where a vertex is a pure strategy.

The question is basic to welfare analysis of strategic interaction: market games, oligopoly, public goods and trading mechanisms (Shapley and Shubik 1977) all ask whether equilibrium outcomes can be efficient. Dubey's answer is that efficiency of an equilibrium is non-generic, so a model that delivers it is exploiting special structure.

Timeline. Nash (1951) introduced equilibrium points and multi-matrix games. Smale (1973, "Optimizing several functions") gave the first-order condition for Pareto optimality of several smooth functions: at an efficient interior point the gradients are linearly dependent. Harsanyi (1973, IJGT 2:235–250) proved that generic finite games have finitely many, indeed an odd number of, mixed equilibria. Dubey's Cowles Foundation Discussion Paper 508R (1978) stated finiteness and inefficiency; the version formalized here is the rewrite IIASA WP-83-74 (1983), published as Mathematics of Operations Research 11(1):1–8 (1986).

Setting

There are n≥2n\ge2n≥2 players N={1,…,n}N=\{1,\dots,n\}N={1,…,n}. Player iii's strategy set is the unit simplex

Si={x∈R+k(i):∑j=1k(i)xj≤1},k(i)≥1,S^i=\Big\{x\in\mathbb R^{k(i)}_+ : \sum_{j=1}^{k(i)}x_j\le1\Big\},\qquad k(i)\ge1,Si={x∈R+k(i)​:j=1∑k(i)​xj​≤1},k(i)≥1,

whose vertices (extreme points) are the origin and the unit vectors. Profiles s=(s1,…,sn)s=(s^1,\dots,s^n)s=(s1,…,sn) range over S=S1×⋯×Sn⊂Rr(n)S=S^1\times\dots\times S^n\subset\mathbb R^{r(n)}S=S1×⋯×Sn⊂Rr(n), r(n)=∑ik(i)r(n)=\sum_i k(i)r(n)=∑i​k(i).

Fix open neighbourhoods Vi⊇SiV^i\supseteq S^iVi⊇Si and V=V1×⋯×VnV=V^1\times\dots\times V^nV=V1×⋯×Vn. The space UUU consists of the C2C^2C2 functions f:V→Rf:V\to\mathbb Rf:V→R with finite C2C^2C2-norm ∥f∥=sup⁡{∥f(s)∥,∥Df(s)∥,∥D2f(s)∥:s∈V}\|f\|=\sup\{\|f(s)\|,\|Df(s)\|,\|D^2f(s)\|: s\in V\}∥f∥=sup{∥f(s)∥,∥Df(s)∥,∥D2f(s)∥:s∈V}. A game is u=(u1,…,un)∈(U)nu=(u^1,\dots,u^n)\in(U)^nu=(u1,…,un)∈(U)n. For T⊆NT\subseteq NT⊆N, (s∣e)(s|e)(s∣e) replaces sis^isi by eie^iei for i∈Ti\in Ti∈T. A profile s∈Ss\in Ss∈S is TTT-efficient if no e∈×i∈TSie\in\times_{i\in T}S^ie∈×i∈T​Si gives ui(s∣e)≥ui(s)u^i(s|e)\ge u^i(s)ui(s∣e)≥ui(s) for all i∈Ti\in Ti∈T with strict inequality for some j∈Tj\in Tj∈T. It is a Nash equilibrium if it is {i}\{i\}{i}-efficient for each iii, efficient if it is NNN-efficient, and a strong Nash equilibrium if it is TTT-efficient for every TTT. The three sets are N(u)N(u)N(u), E(u)E(u)E(u), G(u)G(u)G(u).

In the proof, Du(s)D_u(s)Du​(s) is the n×r(n)n\times r(n)n×r(n) matrix with rows Dui(s)Du^i(s)Dui(s); N∗N^*N∗ is the subspace of matrices whose iii-th row vanishes on player iii's block of columns; E∗E^*E∗ is the set of matrices with linearly dependent rows.

Formalization targets

Goal: the Theorem (p. 3)

There is an open dense set U0⊆(U)nU_0\subseteq(U)^nU0​⊆(U)n such that for u∈U0u\in U_0u∈U0​:

(a) N(u) is finite;(b) s∈N(u)∩E(u)⇒∃j, sj is a vertex;(c) s∈G(u)⇒at most one sj is not a vertex.\text{(a) } N(u)\text{ is finite};\quad \text{(b) } s\in N(u)\cap E(u)\Rightarrow \exists j,\ s^j\text{ is a vertex};\quad \text{(c) } s\in G(u)\Rightarrow \text{at most one } s^j \text{ is not a vertex}.(a) N(u) is finite;(b) s∈N(u)∩E(u)⇒∃j, sj is a vertex;(c) s∈G(u)⇒at most one sj is not a vertex.

Milestones (pp. 4–6)

For interior profiles (si∈Int⁡Sis^i\in\operatorname{Int}S^isi∈IntSi for all iii):

(i) s∈N(u)⇒Du(s)∈N∗,(ii) s∈E(u)⇒Du(s)∈E∗,\text{(i) } s\in N(u)\Rightarrow D_u(s)\in N^*,\qquad \text{(ii) } s\in E(u)\Rightarrow D_u(s)\in E^*,(i) s∈N(u)⇒Du​(s)∈N∗,(ii) s∈E(u)⇒Du​(s)∈E∗,

codim⁡N∗=r(n)\operatorname{codim}N^*=r(n)codimN∗=r(n); the linear perturbation uti(x)=u0i(x)+t∑jyijxju_t^i(x)=u_0^i(x)+t\sum_j y_{ij}x_juti​(x)=u0i​(x)+t∑j​yij​xj​ satisfies ddtD(ut,s0)∣t=0=y\frac{d}{dt}D(u_t,s_0)|_{t=0}=ydtd​D(ut​,s0​)∣t=0​=y (the computation behind (**)); claim (*) for M=N∗M=N^*M=N∗: for an open dense set of games DuD_uDu​ is transverse to N∗N^*N∗ on a compact neighbourhood V‾\underline VV​ of SSS; under that transversality S∩Du−1(N∗)S\cap D_u^{-1}(N^*)S∩Du−1​(N∗) is finite; and the Theorem restricted to interior profiles.

Companions

The Theorem (Multi-Matrix) (p. 14): for an open dense set of payoff vectors a∈(RK)na\in(\mathbb R^K)^na∈(RK)n, the mixed Nash equilibria of Πa\Pi_aΠa​ are finite, an efficient one has a player using a pure strategy, and a strong one is pure. From the example of §3: every game (P,Q)(P,Q)(P,Q) on [0,1]2[0,1]^2[0,1]2 with payoffs uP(x,y)=−[(x−a)2+(y−b)2]u_P(x,y)=-[(x-a)^2+(y-b)^2]uP​(x,y)=−[(x−a)2+(y−b)2] has a unique Nash equilibrium (p. 9); Lemma 1, E(P,Q)=rX(L(P,Q))E(P,Q)=r_X(L(P,Q))E(P,Q)=rX​(L(P,Q)) (p. 9); Lemma 2(a), an interior equilibrium is efficient iff a=ca=ca=c or b=db=db=d (p. 10).

Significance

The theorem gives the generic structure of equilibrium sets in smooth games: isolated and finitely many equilibria, and a sharp location of the only places where efficient equilibria can survive, namely the vertices. It explains why efficiency results for noncooperative models need boundary solutions or non-generic structure, and in its multi-matrix form it shows that strong equilibria of generic finite games are in pure strategies. It also supplies the finiteness of equilibria used in comparative-statics and index arguments.

On the formalization side, the result is proved on paper but has no machine-checked version. A complete development would give Lean its first generic-finiteness theorem for Nash equilibria of smooth games, a first-order Pareto condition in the form of Smale's lemma, and a parametric transversality argument in finite dimensions. The multi-matrix companion connects to the published vocabulary of finite games (agt_games), and the example of §3 is an elementary, fully explicit check of the general picture.

Difficulty

The interior case reduces, by (i) and (ii), to a dimension count: Du−1(N∗)D_u^{-1}(N^*)Du−1​(N∗) should be zero-dimensional and Du−1(N∗∩E∗)D_u^{-1}(N^*\cap E^*)Du−1​(N∗∩E∗) empty. Neither holds for every game: they hold only when DuD_uDu​ is transverse to N∗N^*N∗ and to the strata of N∗∩E∗N^*\cap E^*N∗∩E∗, and the step that requires work is showing that transversality is an open and dense condition in the C2C^2C2 topology. Density is not obtained by adding linear functions to the payoffs: a linear function has finite C2C^2C2-norm on VVV only when VVV is bounded, so perturbations must be localized. The step from interior profiles to the whole of SSS is a second difficulty. It requires repeating the argument on every product of faces of the simplices and on every subgame, and then intersecting finitely many open dense sets. Efficiency at a boundary point is not TTT-efficiency in a subgame, so the reduction has to be made with care.

Formalization scope

Players are Fin n with 2 ≤ n; block sizes k : Fin n → ℕ with 1 ≤ k i; profiles are ∀ i, Fin (k i) → ℝ. The simplex is the paper's corner simplex {x ≥ 0, ∑ x ≤ 1}, not the probability simplex; "vertex" is Set.extremePoints. The neighbourhoods ViV^iVi are taken open, and the goal is stated for every such choice, not assuming VVV bounded or convex. Payoffs are total functions; a game is ContDiffOn ℝ 2 on VVV with finite C2C^2C2-norm, which takes values in [0,∞][0,\infty][0,∞], so no junk real supremum enters. "Open dense in (U)n(U)^n(U)n" is written in ε\varepsilonε-form for the product of C2C^2C2-norm topologies; Lean's sup-type norms are equivalent to the Euclidean ones, so the open dense sets are the same. Deviations range over all strategies in ×i∈TSi\times_{i\in T}S^i×i∈T​Si, not only pure or vertex deviations.

Added hypotheses, all disclosed in the items: openness of ViV^iVi; interiority of every sis^isi on milestones (i), (ii) and the finiteness step (the proof's standing case assumption); M=N∗M=N^*M=N∗ in claim (*). The printed "By (i), N(u)⊂S∩Du−1(N∗)N(u)\subset S\cap D_u^{-1}(N^*)N(u)⊂S∩Du−1​(N∗)" is stated for interior equilibria, which is where (i) applies.

A trivializing formalization is ruled out: the open dense set must contain games arbitrarily close to every game (the zero game is a game, so it is never empty), interiority appears only in the milestones and not in the goal, and efficiency is with respect to all deviations in SSS.

Not stated: (*) for a general submanifold MMM, and the decomposition of N∗∩E∗N^*\cap E^*N∗∩E∗ into submanifolds of codimension ≥r(n)+1\ge r(n)+1≥r(n)+1, both of which need embedded submanifolds of RN\mathbb R^NRN; Remarks 1–4 (Remark 4's openness claim for strictly concave payoffs is false as printed); Lemma 2(b); §5, which the author leaves as a conjecture. Contributions welcome: a finite-dimensional parametric transversality theorem, Smale's first-order Pareto condition, and the face-by-face reduction.

Selected references

  • P. Dubey, Inefficiency of Nash Equilibria, IIASA Working Paper WP-83-74, 1983; Mathematics of Operations Research 11(1):1–8, 1986. https://doi.org/10.1287/moor.11.1.1
  • J. F. Nash, Non-Cooperative Games, Annals of Mathematics 54:286–295, 1951. https://doi.org/10.2307/1969529
  • J. C. Harsanyi, Oddness of the Number of Equilibrium Points: A New Proof, International Journal of Game Theory 2:235–250, 1973. https://doi.org/10.1007/BF01737572
  • S. Smale, Optimizing Several Functions, Manifolds — Tokyo 1973, Proceedings of the International Conference on Manifolds, University of Tokyo Press, 1975.
  • R. Abraham and J. Robbin, Transversal Mappings and Flows, W. A. Benjamin, New York, 1967.
  • L. S. Shapley and M. Shubik, Trade Using One Commodity as a Means of Payment, Journal of Political Economy 85:937–968, 1977. https://doi.org/10.1086/260617
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CombinatoricsGraph TheoryTheoretical Computer Science·Captain: mikedeng1

A c^k n 5-Approximation Algorithm for Treewidth 1: If tw(G) ≤ k, Pushed Terminal Separations Around a 3/4-Balanced Separation Glue to a Separation of Order k+1 with Sides ≤ 7/8|V|+(|B|+k+1)/2Research Paper

Motivation

Treewidth measures how closely a graph resembles a tree. Many problems that are NP-hard on general graphs can be solved in time linear in the number of vertices once a tree decomposition of bounded width is available, so computing such decompositions quickly is a basic task in algorithmic graph theory. Bodlaender, Drange, Dregi, Fomin, Lokshtanov and Pilipczuk (SIAM J. Comput. 45(2), 2016) gave an algorithm that, for a graph GGG on nnn vertices and an integer kkk, either reports that the treewidth of GGG exceeds kkk or returns a tree decomposition of width at most 5k+45k+45k+4, in time 2O(k)n2^{O(k)} n2O(k)n.

The paper's headline is that algorithm, a statement about pseudo-code and running times. This mission does not formalize it. It formalizes one of the paper's combinatorial lemmas, Lemma 6.5 (p. 369), which the algorithm's data structure uses to answer its balanced-separator query: it turns the search for a small balanced separator into two maximization problems that a dynamic program can solve.

Timeline. Robertson and Seymour (Graph Minors II, J. Algorithms 7, 1986) proved that graphs of treewidth kkk have balanced separators of size k+1k+1k+1 (Lemma 2.1 of the paper). Robertson and Seymour (Graph Minors XIII, 1995) used it in an O(33kn2)O(3^{3k} n^2)O(33kn2) approximation algorithm, Reed (1992) improved the dependence on nnn to nlog⁡nn \log nnlogn, and Bodlaender et al. (2016) reached linear time with a single-exponential dependence on kkk.

Setting

All graphs are finite and simple. For X⊆V(G)X \subseteq V(G)X⊆V(G), G∖XG \setminus XG∖X is the graph obtained by deleting XXX; its components are the vertex sets of its connected components.

A separation of GGG is a partition (L,X,R)(L, X, R)(L,X,R) of V(G)V(G)V(G) (parts may be empty) such that no edge of GGG joins LLL to RRR. Its order is ∣X∣|X|∣X∣. It is α\alphaα-balanced if ∣L∣,∣R∣≤α∣V(G)∣|L|, |R| \le \alpha|V(G)|∣L∣,∣R∣≤α∣V(G)∣.

For W⊆V(G)W \subseteq V(G)W⊆V(G) and sets of terminals TL,TRT_L, T_RTL​,TR​, a terminal separation of the induced subgraph G[W]G[W]G[W] of order ℓ\ellℓ (Definition 6.4) is a partition (L,X,R)(L, X, R)(L,X,R) of WWW with

TL⊆L,TR⊆R,no edge between L and R,∣X∣≤ℓ.T_L \subseteq L,\qquad T_R \subseteq R,\qquad \text{no edge between } L \text{ and } R,\qquad |X| \le \ell.TL​⊆L,TR​⊆R,no edge between L and R,∣X∣≤ℓ.

It is left-pushed if ∣L∣|L|∣L∣ is maximum, and right-pushed if ∣R∣|R|∣R∣ is maximum, among all terminal separations of G[W]G[W]G[W] of order ℓ\ellℓ with the same terminals.

The treewidth tw(G)\mathrm{tw}(G)tw(G) is the least width of a tree decomposition of GGG (Definition 1.1), where the width is the largest bag size minus one.

Formalization targets

Goal: Lemma 6.5

Let tw(G)≤k\mathrm{tw}(G) \le ktw(G)≤k and let (A1,B,A2)(A_1, B, A_2)(A1​,B,A2​) be a separation of GGG with ∣A1∣,∣A2∣≤34∣V(G)∣|A_1|, |A_2| \le \tfrac34|V(G)|∣A1​∣,∣A2​∣≤43​∣V(G)∣. Then there are a partition (TL,XB,TR)(T_L, X_B, T_R)(TL​,XB​,TR​) of BBB and integers k1,k2k_1, k_2k1​,k2​ with k1+k2+∣XB∣≤k+1k_1 + k_2 + |X_B| \le k+1k1​+k2​+∣XB​∣≤k+1 such that, for Gi=G[Ai∪(B∖XB)]G_i = G[A_i \cup (B \setminus X_B)]Gi​=G[Ai​∪(B∖XB​)] with terminals TL,TRT_L, T_RTL​,TR​,

  1. G1G_1G1​ and G2G_2G2​ have terminal separations of orders k1k_1k1​ and k2k_2k2​;
  2. for every left-pushed (L1,X1,R1)(L_1, X_1, R_1)(L1​,X1​,R1​) of order k1k_1k1​ in G1G_1G1​ and every right-pushed (L2,X2,R2)(L_2, X_2, R_2)(L2​,X2​,R2​) of order k2k_2k2​ in G2G_2G2​, the triple (L1∪TL∪L2, X1∪XB∪X2, R1∪TR∪R2)(L_1 \cup T_L \cup L_2,\ X_1 \cup X_B \cup X_2,\ R_1 \cup T_R \cup R_2)(L1​∪TL​∪L2​, X1​∪XB​∪X2​, R1​∪TR​∪R2​) is a terminal separation of GGG of order at most k+1k+1k+1 with
∣L1∪TL∪L2∣, ∣R1∪TR∪R2∣≤78∣V(G)∣+∣B∣+(k+1)2.|L_1 \cup T_L \cup L_2|,\ |R_1 \cup T_R \cup R_2| \le \tfrac78|V(G)| + \frac{|B| + (k+1)}{2}.∣L1​∪TL​∪L2​∣, ∣R1​∪TR​∪R2​∣≤87​∣V(G)∣+2∣B∣+(k+1)​.

Milestones

In the order of the proof, the milestones are: Lemma 2.1 (balanced SSS-separators of size k+1k+1k+1, cited from Graph Minors II); the packing step of the proof sketch of Lemma 2.2 (components holding at most 12∣S∣\tfrac12|S|21​∣S∣ of SSS each split into two sides holding at most 23∣S∣\tfrac23|S|32​∣S∣ each); the folklore 23\tfrac2332​-balanced separation of order k+1k+1k+1; the restriction of that separation to G1,G2G_1, G_2G1​,G2​, which gives part (i); four lower bounds on ∣L∩Ai∣|L \cap A_i|∣L∩Ai​∣, ∣R∩Ai∣|R \cap A_i|∣R∩Ai​∣; the dichotomy that two opposite "quadrants" have at least 18∣V(G)∣−∣B∣+(k+1)2\tfrac18|V(G)| - \tfrac{|B|+(k+1)}{2}81​∣V(G)∣−2∣B∣+(k+1)​ vertices each; the comparison of pushed separations with the restricted one; and the gluing step of part (ii).

Significance

Lemma 6.5 is what makes the paper's balanced-separator query computable: given a bag BBB that splits a component in a balanced way, a left-pushed and a right-pushed terminal separation are each the solution of a maximization problem, and the lemma guarantees that gluing them gives a separator of order k+1k+1k+1 whose sides are bounded away from ∣V(G)∣|V(G)|∣V(G)∣. The 78\tfrac7887​ constant feeds into the approximation ratio of the whole algorithm.

The proof is complete in the paper and elementary given Lemma 2.1. No part of it is formalized in Lean's Mathlib or, as far as a search of the Prove2Me catalog shows, on the platform. Lemma 2.1 itself, Robertson and Seymour's balanced-separator theorem for bounded treewidth, is not in Mathlib; a machine-checked proof of it would be reusable wherever treewidth separators are used (divide-and-conquer on tree decompositions, Lipton–Tarjan style arguments, grid-minor theorems).

Difficulty

Everything after Lemma 2.1 is counting with partitions, but the bookkeeping is the obstacle: the two separations (A1,B,A2)(A_1, B, A_2)(A1​,B,A2​) and (L,X,R)(L, X, R)(L,X,R) cut V(G)V(G)V(G) into nine pieces, the induced subgraphs G1,G2G_1, G_2G1​,G2​ overlap on B∖XBB \setminus X_BB∖XB​, and pushedness is a maximum over a family of partitions of a subset, not of V(G)V(G)V(G).

Lemma 2.1 is the hard milestone. It is a statement about tree decompositions, and any proof has to relate subtrees of the decomposition tree to components of G∖XG \setminus XG∖X for a bag XXX, infrastructure that does not yet exist in Mathlib.

Formalization scope

  • Vertices. A finite type V : Type with decidable equality; vertex sets are Finset V, V(G)V(G)V(G) is Finset.univ, ∣V(G)∣|V(G)|∣V(G)∣ is Fintype.card V. Universe 0 matches the published definition of treewidth.
  • Treewidth. "tw(G)≤k\mathrm{tw}(G) \le ktw(G)≤k" is the published RobertsonSeymour1986.GM5.TreewidthLE G k: a decomposition tree on a finite type whose bags have at most k+1k+1k+1 vertices. Definition 1.1 roots the tree; rooting does not change the width.
  • Components of G∖XG \setminus XG∖X. The component of u∉Xu \notin Xu∈/X is avoidComp G X u: the vertices reachable from uuu by a walk of GGG none of whose vertices, endpoints included, lies in XXX.
  • Partitions are pairwise disjoint triples with the given union; empty parts are allowed.
  • Induced subgraphs G[W]G[W]G[W] are encoded by their vertex set WWW: a terminal separation of G[W]G[W]G[W] is a partition of WWW, with GGG's adjacency restricted to WWW. Pushedness maximizes over partitions of WWW only.
  • "Of order ℓ\ellℓ" means ∣X∣≤ℓ|X| \le \ell∣X∣≤ℓ, as in Definition 6.4 (iii).
  • Arithmetic. Bounds with fractions or subtraction (34\tfrac3443​, 23\tfrac2332​, 78\tfrac7887​, 18∣V(G)∣−∣B∣+(k+1)2\tfrac18|V(G)| - \tfrac{|B|+(k+1)}{2}81​∣V(G)∣−2∣B∣+(k+1)​) are stated over R\mathbb RR; bounds without subtraction may be cleared of denominators in N\mathbb NN (2∣C∩S∣≤∣S∣2|C \cap S| \le |S|2∣C∩S∣≤∣S∣, 3∣L′∩S∣≤2∣S∣3|L' \cap S| \le 2|S|3∣L′∩S∣≤2∣S∣).
  • Corrections of the page. The printed bound of Lemma 6.5 has ∣X∣|X|∣X∣ where the proof derives ∣B∣|B|∣B∣; the goal states ∣B∣|B|∣B∣. The proof's "14\tfrac1441​- and 13\tfrac1331​-balanced" means 34\tfrac3443​ and 23\tfrac2332​; the milestone uses the latter.

Part (i) is part of the goal: without it, left- and right-pushed separations of the chosen orders might not exist and part (ii) would hold vacuously. Choosing XB=BX_B = BXB​=B does not trivialize the goal, because the size bound and the budget k1+k2+∣XB∣≤k+1k_1 + k_2 + |X_B| \le k+1k1​+k2​+∣XB​∣≤k+1 must hold simultaneously.

Welcome contributions: a proof of Lemma 2.1 from tree decompositions (reusable on its own), the packing lemma, and the counting milestones of the proof of Lemma 6.5.

Selected references

  • H. L. Bodlaender, P. G. Drange, M. S. Dregi, F. V. Fomin, D. Lokshtanov, M. Pilipczuk, A cknc^k nckn 5-approximation algorithm for treewidth, SIAM J. Comput. 45(2):317–378, 2016. https://doi.org/10.1137/130947374
  • N. Robertson, P. D. Seymour, Graph minors. II. Algorithmic aspects of tree-width, J. Algorithms 7(3):309–322, 1986. https://doi.org/10.1016/0196-6774(86)90023-4
  • N. Robertson, P. D. Seymour, Graph minors. XIII. The disjoint paths problem, J. Combin. Theory Ser. B 63(1):65–110, 1995. https://doi.org/10.1006/jctb.1995.1006
  • B. A. Reed, Finding approximate separators and computing tree width quickly, STOC 1992, 221–228. https://doi.org/10.1145/129712.129734
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CombinatoricsGraph Theory·Captain: mikedeng1

Three-Coloring and List Three-Coloring of Graphs Without Induced Paths on Seven Vertices 1: Every Connected P₇-Free Graph Has a Connected 2-Dominating Set of at Most Three Vertices or a K₄Research Paper

Motivation

Graph coloring asks whether vertices can be assigned colors so that adjacent vertices receive different colors. Restricting the graphs by forbidden induced paths can expose structure that is absent from general graphs. Bonomo, Chudnovsky, Maceli, Schaudt, Stein and Zhong study list three-coloring when the graph has no induced path on seven vertices, building on earlier work on coloring graphs with shorter forbidden induced paths. Their paper proves an algorithmic result, but its treatment also uses a purely graph-theoretic statement: a connected P7P_7P7​-free graph has a small connected set that reaches every vertex within two steps, unless the graph contains a four-vertex clique. This mission isolates that statement as Corollary 5 of the paper.

The structural input to the corollary is a theorem of Camby and Schaudt about connected dominating sets in PtP_tPt​-free graphs, quoted as Theorem 4 in the coloring paper. That result applies to every allowed path length ttt, rather than only to the seven-vertex case. It is a milestone here in the precise form printed in the source article. The Camby–Schaudt paper develops connected domination as a characterization of graphs without long induced paths.

Setting

A simple graph GGG has a vertex set V(G)V(G)V(G) and an undirected edge relation with no loops. The graphs in this mission are finite. The path PtP_tPt​ has ttt vertices and consecutive vertices adjacent. A graph is PtP_tPt​-free when it has no induced subgraph isomorphic to PtP_tPt​: the graph may contain a path with ttt vertices as a non-induced subgraph if extra edges join vertices of that path. This distinction matters throughout the source paper.

For a vertex set SSS, its open neighborhood N(S)N(S)N(S) consists of vertices outside SSS with a neighbor in SSS. Write Sˉ=S∪N(S)\bar S=S\cup N(S)Sˉ=S∪N(S). The set SSS is dominating when Sˉ=V(G)\bar S=V(G)Sˉ=V(G), so each vertex lies in SSS or has an edge to SSS. It is 2-dominating when Sˉ‾=V(G)\overline{\bar S}=V(G)Sˉ=V(G), meaning each vertex is at graph distance at most two from some vertex of SSS. A dominating or 2-dominating set is connected when the subgraph G[S]G[S]G[S] induced by SSS is connected. In this mission, connectedness includes nonemptiness, as in the paper's use of such sets.

A clique of size four is a set of four pairwise adjacent vertices. The notation K4⊆GK_4\subseteq GK4​⊆G below asserts the existence of such a set. Since all edges between those four vertices are present, it is also an induced complete subgraph. The notation G[S]≅Pt−2G[S]\cong P_{t-2}G[S]≅Pt−2​ means there is a graph isomorphism from the induced graph on SSS to that path.

Formalization targets

Corollary 5: a small connected 2-dominating set or a clique

For a finite, connected, P7P_7P7​-free graph GGG, the goal is

(∃S⊆V(G):∣S∣≤3,  G[S] connected,  Sˉ‾=V(G))∨K4⊆G.\left(\exists S\subseteq V(G): |S|\le 3,\;G[S]\text{ connected},\; \overline{\bar S}=V(G)\right)\quad\lor\quad K_4\subseteq G.(∃S⊆V(G):∣S∣≤3,G[S] connected,Sˉ=V(G))∨K4​⊆G.

The four-vertex clique is a genuine alternative in the claim; the mission does not assume its absence. The result is the first, structural sentence of Corollary 5. Its following sentence gives a running time for finding the set or clique and is outside this mission.

Theorem 4: connected domination across forbidden path lengths

For every t≥3t\ge 3t≥3, the cited theorem asserts that each finite connected PtP_tPt​-free graph has a connected dominating set SSS for which

G[S] is Pt−2-free∨G[S]≅Pt−2.G[S]\text{ is }P_{t-2}\text{-free}\quad\lor\quad G[S]\cong P_{t-2}.G[S] is Pt−2​-free∨G[S]≅Pt−2​.

The other milestones are statements identified in the proof of Corollary 5: a connected P3P_3P3​-free graph is complete, domination inside a dominating set yields 2-domination in the original graph, and the three non-leaf vertices work when the induced dominating graph is a P5P_5P5​. These are listed in the paper's order of use, with the quoted theorem also available as a separate target.

Significance

Corollary 5 gives a bounded set of vertices from which the rest of a connected P7P_7P7​-free graph can be reached in two steps, except when a K4K_4K4​ is present. Its bound is the concrete number three, independent of graph size. In the coloring paper this supplies a small structural seed for later restrictions on vertex palettes. A formal statement of the corollary makes that finite structural claim available independently of any coloring algorithm.

Theorem 4 has broader reuse: it links forbidden induced paths to connected dominating sets for general ttt. The remaining milestones isolate the graph facts needed to connect this general result to the seven-vertex corollary. The article and the cited theorem provide mathematical proofs; these Lean declarations are open theorem statements, with machine-checked proofs still to be supplied. This mission therefore asks for formal proofs of known graph-theoretic results, not for a new resolution of an open mathematical problem.

Difficulty

The difficult step is finding a connected dominating set whose induced graph has the much stronger path restriction in Theorem 4. Ordinary domination by itself does not impose that restriction, and replacing induced-path exclusion with exclusion of all paths would change the class of graphs. The later cases require careful handling of connectedness and the passage from domination within G[S]G[S]G[S] to distance-two domination in GGG. These issues are mathematical as well as formal: an empty set or a merely preconnected induced graph would erase the intended content.

Formalization scope

Lean represents GGG as SimpleGraph V with a finite vertex type. Vertex sets are Finset V; PtP_tPt​ is Mathlib's pathGraph t; PtP_tPt​-freeness is the absence of an induced copy using IsIndContained. The definitions of N(S)N(S)N(S), Sˉ\bar SSˉ, domination and 2-domination are shared within P7ThreeColor.Seed. A connected induced graph uses Connected, which requires at least one vertex. Four-clique existence is ¬ G.CliqueFree 4. The only added standing convention is finiteness, implicit in the source's graph algorithm and finite cardinalities. No extra colorability or clique-free hypothesis is attached to the goal.

The running-time claim in the second sentence of Corollary 5 and the paper's headline Theorem 1 are not formalized because this mission has no machine model. A statement that merely postulates a small set as a hypothesis, or substitutes ordinary domination for 2-domination, would miss the result. Contributions are welcome for proofs of the goal and milestones, reusable facts about induced paths and connected domination, and auxiliary Mathlib lemmas needed to cross between graph isomorphisms, induced subgraphs and finite sets.

Selected references

  • F. Bonomo, M. Chudnovsky, P. Maceli, O. Schaudt, M. Stein and M. Zhong, Three-coloring and list three-coloring of graphs without induced paths on seven vertices, Combinatorica, OnlineFirst 2017, DOI: 10.1007/s00493-017-3553-8.
  • E. Camby and O. Schaudt, A new characterization of PkP_kPk​-free graphs, Algorithmica 75 (2016), 205–217, DOI: 10.1007/s00453-015-9989-6; arXiv:1402.7213.
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Dynamic ProgrammingOptimizationReinforcement Learning·Captain: mikedeng1

Global Optimality Guarantees for Policy Gradient Methods 2: Under Closure, a (c, µ)-Gradient-Dominated Policy Iteration Objective Makes ℓ (κc/(1−γ), κµ/(1−γ))-Gradient DominatedResearch Paper

Motivation

Policy gradient methods optimize a parameterized control policy by gradient descent on its long-run cost. They underlie much of modern reinforcement learning, from REINFORCE and actor-critic methods to trust-region and proximal policy optimization, and they are used in operations problems such as inventory control and optimal stopping. Their objective is almost never convex in the policy parameters, even in textbook problems, so the classical guarantees of first-order optimization do not explain why they reach good policies.

Bhandari and Russo (arXiv:1906.01786v3, Operations Research, 2024, doi:10.1287/opre.2021.0014) identify structural conditions under which this non-convex landscape is benign. Their Theorem 1 shows that, for a policy class closed under policy improvement, every stationary point is globally optimal. This mission formalizes their Theorem 2, the quantitative version: approximate stationarity implies approximate optimality, a gradient dominance (Polyak–Łojasiewicz-type) inequality that yields convergence rates.

Timeline. Polyak (1963) introduced the inequality min⁡f≥f(x)−c22μ∥∇f(x)∥2\min f \ge f(x) - \frac{c^2}{2\mu}\|\nabla f(x)\|^2minf≥f(x)−2μc2​∥∇f(x)∥2 for unconstrained problems. Kakade and Langford (2002) proved the performance difference lemma for finite Markov decision processes. Fazel, Ge, Kakade and Mesbahi (2018) established gradient dominance of policy gradient for linear-quadratic control, and Agarwal, Kakade, Lee and Mahajan (2021) for tabular policies with direct and softmax parameterizations. Bhandari and Russo (preprint 2019, journal 2024) give a single condition-based argument covering general state spaces and several of these examples.

Setting

A Markov decision process has a measurable state space S\mathcal SS, feasible action sets As\mathcal A_sAs​, a bounded expected cost g(s,a)g(s,a)g(s,a), a transition kernel P(⋅∣s,a)P(\cdot\mid s,a)P(⋅∣s,a), a discount factor γ∈(0,1)\gamma\in(0,1)γ∈(0,1) and an initial distribution ρ\rhoρ. A stationary policy π\piπ maps states to feasible actions; Π\PiΠ is the set of measurable such policies. Its cost-to-go is Jπ(s)=Esπ[∑t≥0γtg(st,π(st))]J_\pi(s)=\mathbb E^\pi_s[\sum_{t\ge0}\gamma^t g(s_t,\pi(s_t))]Jπ​(s)=Esπ​[∑t≥0​γtg(st​,π(st​))], its discounted state-occupancy measure is ηπ=(1−γ)∑t≥0γt Pρπ(st∈⋅)\eta_\pi=(1-\gamma)\sum_{t\ge0}\gamma^t\,\mathbb P^\pi_\rho(s_t\in\cdot)ηπ​=(1−γ)∑t≥0​γtPρπ​(st​∈⋅), and its loss is ℓ(π)=(1−γ)∫Jπ dρ\ell(\pi)=(1-\gamma)\int J_\pi\,d\rhoℓ(π)=(1−γ)∫Jπ​dρ. An optimal policy π∗\pi^*π∗ has Jπ∗=J∗⪯JπJ_{\pi^*}=J^*\preceq J_\piJπ∗​=J∗⪯Jπ​ for every π∈Π\pi\in\Piπ∈Π.

The Bellman operator is (TπJ)(s)=g(s,π(s))+γ∫J dP(⋅∣s,π(s))(T_\pi J)(s)=g(s,\pi(s))+\gamma\int J\,dP(\cdot\mid s,\pi(s))(Tπ​J)(s)=g(s,π(s))+γ∫JdP(⋅∣s,π(s)) and TJ=min⁡a∈As[ ⋅ ]T J=\min_{a\in\mathcal A_s}[\,\cdot\,]TJ=mina∈As​​[⋅] is its optimality version. The weighted policy iteration objective is

B(πˉ∣η,J)=∫(TπˉJ) dη.\mathcal B(\bar\pi\mid\eta,J)=\int (T_{\bar\pi}J)\,d\eta .B(πˉ∣η,J)=∫(Tπˉ​J)dη.

A policy class is ΠΘ={πθ:θ∈Θ}\Pi_\Theta=\{\pi_\theta:\theta\in\Theta\}ΠΘ​={πθ​:θ∈Θ} with Θ⊆Rd\Theta\subseteq\mathbb R^dΘ⊆Rd convex, and the policy gradient objective is ℓ(θ)=ℓ(πθ)\ell(\theta)=\ell(\pi_\theta)ℓ(θ)=ℓ(πθ​). For π=πθ\pi=\pi_\thetaπ=πθ​, the map θˉ↦B(θˉ∣ηπ,Jπ)\bar\theta\mapsto\mathcal B(\bar\theta\mid\eta_{\pi},J_{\pi})θˉ↦B(θˉ∣ηπ​,Jπ​) is the single-period problem that one step of policy iteration within the class would solve.

A function fff is (c,μ)(c,\mu)(c,μ)-gradient dominated over XXX (c>0c>0c>0, μ≥0\mu\ge0μ≥0) if for all x∈Xx\in Xx∈X

min⁡x′∈Xf(x′) ≥ f(x)+min⁡x′∈X[c ⟨∇f(x),x′−x⟩+μ2∥x−x′∥22].\min_{x'\in X}f(x')\ \ge\ f(x)+\min_{x'\in X}\Big[c\,\langle\nabla f(x),x'-x\rangle+\tfrac{\mu}{2}\|x-x'\|_2^2\Big].x′∈Xmin​f(x′) ≥ f(x)+x′∈Xmin​[c⟨∇f(x),x′−x⟩+2μ​∥x−x′∥22​].

The hypotheses are Condition 0 (differentiability of B\mathcal BB in the policy and occupancy arguments), Condition 1 (closure: for every π∈ΠΘ\pi\in\Pi_\Thetaπ∈ΠΘ​ some π+∈ΠΘ\pi^+\in\Pi_\Thetaπ+∈ΠΘ​ minimizes B(⋅∣ηπ,Jπ)\mathcal B(\cdot\mid\eta_\pi,J_\pi)B(⋅∣ηπ​,Jπ​) over all of Π\PiΠ) and Condition 2.B (each single-period objective is (c,μ)(c,\mu)(c,μ)-gradient dominated over Θ\ThetaΘ). The effective concentrability coefficient κρ\kappa_\rhoκρ​ is the smallest κ\kappaκ with ∥J−J∗∥1,ρ≤κ1−γ∥J−TJ∥1,ρ\|J-J^*\|_{1,\rho}\le\frac{\kappa}{1-\gamma}\|J-TJ\|_{1,\rho}∥J−J∗∥1,ρ​≤1−γκ​∥J−TJ∥1,ρ​ for all J=JπθJ=J_{\pi_\theta}J=Jπθ​​, θ∈Θ\theta\in\Thetaθ∈Θ.

Formalization targets

Goal: Theorem 2 (p. 16)

If Conditions 0, 1 and 2.B hold and κρ<∞\kappa_\rho<\inftyκρ​<∞, then

ℓ is (κρ1−γ c, κρ1−γ μ)-gradient dominated over Θ.\ell\ \text{is}\ \Big(\frac{\kappa_\rho}{1-\gamma}\,c,\ \frac{\kappa_\rho}{1-\gamma}\,\mu\Big)\text{-gradient dominated over }\Theta .ℓ is (1−γκρ​​c, 1−γκρ​​μ)-gradient dominated over Θ.

It is stated for every κ>0\kappa>0κ>0 satisfying the concentrability inequality, which is the page's statement at κ=κρ\kappa=\kappa_\rhoκ=κρ​.

Milestones

  1. ηπ⪰(1−γ)ρ\eta_\pi\succeq(1-\gamma)\rhoηπ​⪰(1−γ)ρ (p. 7) and the element-wise inequalities TJ⪯TπJTJ\preceq T_\pi JTJ⪯Tπ​J, TJπ⪯JπTJ_\pi\preceq J_\piTJπ​⪯Jπ​, (5).
  2. The performance difference identity ℓ(π)−ℓ(πˉ)=∫[TπJπˉ−Jπˉ] dηπ\ell(\pi)-\ell(\bar\pi)=\int[T_\pi J_{\bar\pi}-J_{\bar\pi}]\,d\eta_\piℓ(π)−ℓ(πˉ)=∫[Tπ​Jπˉ​−Jπˉ​]dηπ​, (29).
  3. Lemma 6, the policy gradient theorem: ∇ℓ(θ)=∇θˉB(θˉ∣ηπθ,Jπθ)∣θˉ=θ\nabla\ell(\theta)=\nabla_{\bar\theta}\mathcal B(\bar\theta\mid\eta_{\pi_\theta},J_{\pi_\theta})|_{\bar\theta=\theta}∇ℓ(θ)=∇θˉ​B(θˉ∣ηπθ​​,Jπθ​​)∣θˉ=θ​.
  4. The closure bound of the proof of Theorem 2:
ℓ(πθ)−ℓ(π∗)≤κρ1−γ(B(θ∣ηπθ,Jπθ)−min⁡θ′∈ΘB(θ′∣ηπθ,Jπθ)).\ell(\pi_\theta)-\ell(\pi^*)\le\frac{\kappa_\rho}{1-\gamma}\Big(\mathcal B(\theta\mid\eta_{\pi_\theta},J_{\pi_\theta})-\min_{\theta'\in\Theta}\mathcal B(\theta'\mid\eta_{\pi_\theta},J_{\pi_\theta})\Big).ℓ(πθ​)−ℓ(π∗)≤1−γκρ​​(B(θ∣ηπθ​​,Jπθ​​)−θ′∈Θmin​B(θ′∣ηπθ​​,Jπθ​​)).

Companions

The remark of §3 that differentiable μ\muμ-strongly convex functions are (1,μ)(1,\mu)(1,μ)-gradient dominated and convex ones (1,0)(1,0)(1,0)-gradient dominated, and Corollary 1: under Conditions 0 and 1, convexity (strong convexity) of every single-period objective makes ℓ\ellℓ gradient dominated of degree one (two).

Significance

Gradient dominance of degree two gives linear convergence of projected gradient methods, and degree one gives sublinear rates, so Theorem 2 converts structural knowledge about one-step policy improvement into iteration complexity for the multi-period problem. The constant κρ/(1−γ)\kappa_\rho/(1-\gamma)κρ​/(1−γ) makes explicit the dependence on the initial distribution: an exploratory ρ\rhoρ with small κρ\kappa_\rhoκρ​ is what the guarantee needs. The paper instantiates the conditions for tabular MDPs, linear-quadratic control, optimal stopping with threshold policies, and finite-horizon inventory control.

The result is proved in the paper. As far as is known, none of it is machine-checked: Mathlib has convexity, strong convexity, gradients and Markov kernels but no discounted dynamic programming on general spaces, no occupancy measures and no policy gradient theorem. The formal development would supply the general-space performance difference identity and the policy gradient theorem, reusable for every other result of the paper and for related work on policy optimization.

Difficulty

The policy gradient objective ℓ(θ)\ell(\theta)ℓ(θ) is not convex, so the usual derivation of a Polyak–Łojasiewicz inequality from convexity is unavailable. Gradient dominance of the single-period objective B\mathcal BB does not transfer to ℓ\ellℓ by comparing the two functions: they differ by how a change of policy moves the state distribution, these terms do not vanish, and the minimum of B\mathcal BB over Θ\ThetaΘ is not the minimum of ℓ\ellℓ. The mismatch between ρ\rhoρ, ηπθ\eta_{\pi_\theta}ηπθ​​ and ηπ∗\eta_{\pi^*}ηπ∗​ is unavoidable, which is why a concentrability factor appears in the constants. On a general state space each identity also needs the right measurability and integrability (the measurable-selection assumption is what makes TJTJTJ measurable), and Condition 0 must be strong enough to justify a total-derivative expansion.

Formalization scope

All declarations live in PGLandscape.GradDom. S\mathcal SS and A\mathcal AA are arbitrary measurable spaces; the cost is bounded and measurable and, like the kernel, given on all of S×A\mathcal S\times\mathcal AS×A. Policies are measurable maps; the cost-to-go is a series of integrals against ttt-step kernels; ηπ\eta_\piηπ​ is a measure of total mass one. The parameter space is EuclideanSpace ℝ (Fin d), so ∇\nabla∇ is the Euclidean gradient and ∥⋅∥\|\cdot\|∥⋅∥ the ℓ2\ell_2ℓ2​ norm. J∗J^*J∗ is Jπ∗J_{\pi^*}Jπ∗​ for an optimal π∗\pi^*π∗ given as a hypothesis; no real infimum over policies is used.

Committed conventions and disclosed additions:

  • the page prints (3)–(4) without γ\gammaγ; the factor γ\gammaγ is restored, as in (6), (7) and every proof;
  • Condition 0 is the joint version the proof of Lemma 6 uses (C1C^1C1 in the pair of arguments near (θ,θ)(\theta,\theta)(θ,θ)); it implies the printed condition;
  • gradient dominance quantifies over lower bounds of the bracket instead of real minima, which need not be attained, and includes differentiability on XXX;
  • κρ\kappa_\rhoκρ​ enters as any κ>0\kappa>0κ>0 satisfying its defining inequality; Theorem 2 states c>0c>0c>0, μ≥0\mu\ge0μ≥0 explicitly; Corollary 1 assumes κρ<∞\kappa_\rho<\inftyκρ​<∞ and one strong-convexity modulus for the whole class;
  • Assumptions 1 (ηπ∗≪ρ\eta_{\pi^*}\ll\rhoηπ∗​≪ρ) and 2 (measurable selection) are hypotheses of every result, as in the paper.

A formalization that assumes gradient dominance of ℓ\ellℓ, the closure bound, or a finite state space would not be this theorem; the goal assumes only Conditions 0, 1, 2.B and concentrability.

Contributions welcome: Markov-chain lemmas for iterKernel (summability, measurability, the fixed-point equation TπJπ=JπT_\pi J_\pi=J_\piTπ​Jπ​=Jπ​), the general-space performance difference identity, and proofs of any milestone.

Selected references

  • J. Bhandari and D. Russo, Global Optimality Guarantees for Policy Gradient Methods, Operations Research, 2024. arXiv:1906.01786v3, doi:10.1287/opre.2021.0014
  • B. T. Polyak, Gradient methods for minimizing functionals, Zh. Vychisl. Mat. Mat. Fiz., 1963. doi:10.1016/0041-5553(63)90382-3
  • S. Kakade and J. Langford, Approximately optimal approximate reinforcement learning, ICML, 2002. ACM DL
  • M. Fazel, R. Ge, S. Kakade and M. Mesbahi, Global convergence of policy gradient methods for the linear quadratic regulator, ICML, 2018. arXiv:1801.05039
  • A. Agarwal, S. Kakade, J. Lee and G. Mahajan, On the theory of policy gradient methods: optimality, approximation, and distribution shift, JMLR, 2021. arXiv:1908.00261
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Algorithmic Game TheoryOperations Research·Captain: mikedeng1

The Price of Anarchy of Finite Congestion Games III: The Price of Anarchy of the Maximum Social Cost Is Theta(sqrt N)Research Paper

Motivation

In a congestion game, several users choose facilities and each facility becomes more costly as more users choose it. Such games model settings in which each participant chooses a route or collection of resources for personal use while the resulting load is shared. A pure Nash equilibrium is a stable choice of routes: no single participant can lower their own cost by switching. Stability alone gives no assurance that the resulting allocation serves the group well. The price of anarchy compares the social cost of an equilibrium with the best social cost attainable by coordinated choices.

Christodoulou and Koutsoupias studied finite congestion games with linear latency functions and several notions of social cost. For the maximum cost borne by any player, their STOC 2005 paper gives both an upper bound valid for all such games and a family of instances showing that its square-root dependence on the number of players has the right order. This mission formalizes those two claims together. The maximum criterion matters when a single heavily delayed user is significant even if the total cost of the population is moderate.

Setting

Let N≥1N\ge1N≥1 be the number of players and let EEE be a finite set of facilities. Player iii has a finite collection Σi\Sigma_iΣi​ of available pure strategies, each a subset of EEE. A profile AAA chooses one strategy Ai∈ΣiA_i\in\Sigma_iAi​∈Σi​ for every player. For a facility eee, its load ne(A)n_e(A)ne​(A) is the number of players whose chosen strategy contains eee. The latency of eee at load nnn is fe(n)f_e(n)fe​(n). Player iii pays the sum of the latencies on the facilities they chose:

ci(A)=∑e∈Aife(ne(A)).c_i(A)=\sum_{e\in A_i}f_e(n_e(A)).ci​(A)=e∈Ai​∑​fe​(ne​(A)).

A profile is a pure Nash equilibrium if no player can decrease this cost by replacing their own strategy while the others keep theirs. The paper calls latencies linear when fe(n)=aen+bef_e(n)=a_en+b_efe​(n)=ae​n+be​ with ae,be≥0a_e,b_e\ge0ae​,be​≥0; these are affine functions in standard terminology. The paper displays many calculations for the special case fe(n)=nf_e(n)=nfe​(n)=n and states the general nonnegative affine convention in its model section. The maximum social cost is MAX⁡(A)=max⁡ici(A)\operatorname{MAX}(A)=\max_i c_i(A)MAX(A)=maxi​ci​(A); the total cost is SUM⁡(A)=∑ici(A)\operatorname{SUM}(A)=\sum_i c_i(A)SUM(A)=∑i​ci​(A). The paper's average social cost is SUM⁡(A)/N\operatorname{SUM}(A)/NSUM(A)/N.

For a game with at least one pure Nash equilibrium and a positive optimal maximum cost, the maximum-cost pure price of anarchy is the largest equilibrium value of MAX⁡\operatorname{MAX}MAX divided by the smallest feasible value. The Lean targets use inequalities against every feasible comparison profile PPP rather than dividing by an optimum. This form continues to say something when an optimum has cost zero, and finite strategy sets ensure an optimum exists whenever the profile space is nonempty.

Formalization targets

Universal upper bound

For every N≥1N\ge1N≥1, every finite game with nonnegative affine latencies, every pure Nash equilibrium AAA, and every feasible profile PPP, Theorem 5's proof yields

MAX⁡(A)≤(1+5N2)MAX⁡(P).\operatorname{MAX}(A)\le \left(1+\sqrt{\frac{5N}{2}}\right)\operatorname{MAX}(P).MAX(A)≤(1+25N​​)MAX(P).

This states a numerical version of the paper's O(N)O(\sqrt N)O(N​) theorem without an unspecified constant. Taking PPP to minimize MAX⁡\operatorname{MAX}MAX gives the corresponding price-of-anarchy bound. The bound is about asymmetric games: players may have different strategy sets, and no symmetry assumption is present.

Lower-bound family

For every integer k≥2k\ge2k≥2, let N=k(k−1)+1N=k(k-1)+1N=k(k−1)+1. Theorem 6 provides an identity-latency congestion game with NNN players and kNkNkN facilities, a pure Nash profile AAA, and an optimal profile PPP for which

MAX⁡(A)=k2,MAX⁡(P)=k.\operatorname{MAX}(A)=k^2,\qquad \operatorname{MAX}(P)=k.MAX(A)=k2,MAX(P)=k.

Every feasible profile in the instance has maximum cost at least kkk. Thus the ratio is kkk, and k≥Nk\ge\sqrt Nk≥N​. The proof's explicit instance has positive comparison cost, so the lower bound cannot be satisfied by a zero-cost game. The source also says such behavior occurs in network congestion games and sketches a network realization in Figure 2; this mission's formal lower target is the finite congestion-game construction.

Significance

Together these results identify the order of growth of the worst pure equilibrium maximum cost relative to an optimum: it can grow with the population, yet for linear latencies it grows no faster than a constant times N\sqrt NN​. The upper statement applies to any feasible comparison profile, so it can also be used when a convenient benchmark is known without solving the entire optimization problem. The lower family prevents replacing the square-root dependence by a bound independent of NNN for this class of games.

The results are proved in the 2005 paper; the mission is to give them machine-checked Lean proofs in a common finite-game representation. The development also supplies reusable definitions of congestion games, loads, pure cost equilibria, and maximum social cost, together with the total-cost estimate of Theorem 1 and the intermediate bounds appearing in Theorem 5. The current draft contains statements with sorry placeholders, not completed proofs.

Difficulty

A bound on total player cost does not directly control the cost of the most expensive player sharply enough. An individual player can use several facilities whose loads interact, and bounding each load separately loses the dependence required for the square-root result. Affine coefficients add another issue: the proof printed for identity latencies writes a cardinality where the general statement needs a coefficient-weighted quantity. The lower example has an indexing discrepancy in the printed alternative strategies, so the intended Nash profile must be checked against the costs on every permitted deviation.

Formalization scope

Players are represented by Fin N; facilities by an arbitrary finite type in upper bounds and by a type with kNkNkN elements in the lower family. A profile is a function from players to finite facility sets, with feasibility stated separately. Latencies are real-valued on natural-number loads. The IsLinear predicate requires explicit nonnegative affine coefficients. Pure Nash uses a cost inequality; it is the negative-payoff version of a standard finite game's payoff equilibrium. MAX requires at least one player, and all upper-bound targets therefore require N≥1N\ge1N≥1. The lower family begins at k=2k=2k=2, where N=k(k−1)+1N=k(k-1)+1N=k(k−1)+1 is positive.

The source's number k2−k+1k^2-k+1k2−k+1 is written as k(k−1)+1k(k-1)+1k(k−1)+1 in Lean to keep natural-number subtraction inside its valid range. The two expressions agree for k≥2k\ge2k≥2. In the source's one-based indexing, the proposed alternative strategy uses a ceiling index. The printed denominator kkk makes some alternative facilities carry k+1k+1k+1 users and breaks the Nash assertion; denominator k−1k-1k−1 agrees with Figure 2's k−1k-1k−1 short-route users per layer and gives the stated costs. This correction is recorded with the lower theorem. No normalization of coefficients or artificially restricted strategy class is assumed. Contributions to the finite-game definitions, Theorem 1, the player-cost bounds, and the explicit lower instance are all in scope.

Selected references

  • G. Christodoulou and E. Koutsoupias, The Price of Anarchy of Finite Congestion Games, Proceedings of the 37th Annual ACM Symposium on Theory of Computing, 2005. DOI: 10.1145/1060590.1060600.
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Markov ChainOptimal TransportProbability·Captain: mikedeng1

Coupling and Convergence for Hamiltonian Monte Carlo 2: Lyapunov Bounds and Local Contractivity Give W_ρ(νπⁿ, ηπⁿ) ≤ e^{−cn}W_ρ(ν, η) + βⁿλⁿ⁻¹(∫ψdν + ∫ψdη)δ(C)Research Paper

Motivation

Markov chain Monte Carlo methods approximate a target probability measure by the law after nnn steps of a Markov chain. A quantitative guarantee for such a method is a bound on the distance between the law after nnn steps and the target, or between the laws of two copies of the chain started from different initial distributions. A standard route to such bounds is contractivity in a Kantorovich (Wasserstein) distance: if one step of the chain contracts the distance between any two initial laws by a factor e−c<1e^{-c}<1e−c<1, the laws converge geometrically.

For many chains of practical interest, including Hamiltonian Monte Carlo with a numerical integrator, contractivity can only be proved on a bounded region of the state space. Outside it, the integrator may be unstable, or the coupling used to prove contraction may fail. Bou-Rabee, Eberle and Zimmer (arXiv:1805.00452, Ann. Appl. Probab. 30(3), 2020) isolate a general principle that turns such local contractivity into a global distance bound. It requires two Lyapunov functions: one controls how quickly the chain can leave the region of contraction, and one controls the distance once it has left. The principle is their Theorem 2.11. It is stated for an arbitrary Markov kernel on a complete separable metric space, and they apply it to adjusted numerical HMC (their Theorem 2.12).

Setting

Let (S,ρ)(S,\rho)(S,ρ) be a complete separable metric space with Borel σ\sigmaσ-algebra B(S)\mathcal B(S)B(S), and let π(x,dy)\pi(x,dy)π(x,dy) be a Markov transition kernel on SSS. For a probability measure ν\nuν, the law after nnn steps is νπn\nu\pi^nνπn, where π0(x,⋅)=δx\pi^0(x,\cdot)=\delta_xπ0(x,⋅)=δx​ and πn+1=ππn\pi^{n+1}=\pi\pi^nπn+1=ππn. For a non-negative function fff, (πf)(x)=∫f(y) π(x,dy)(\pi f)(x)=\int f(y)\,\pi(x,dy)(πf)(x)=∫f(y)π(x,dy).

A coupling of probability measures ν,η\nu,\etaν,η on SSS is a probability measure on S×SS\times SS×S with marginals ν\nuν and η\etaη; C(ν,η)C(\nu,\eta)C(ν,η) is the set of couplings. The Kantorovich distance is

Wρ(ν,η)=inf⁡γ∈C(ν,η)∫ρ(x,y) γ(dx dy)∈[0,∞].\mathcal W_\rho(\nu,\eta)=\inf_{\gamma\in C(\nu,\eta)}\int\rho(x,y)\,\gamma(dx\,dy)\in[0,\infty].Wρ​(ν,η)=γ∈C(ν,η)inf​∫ρ(x,y)γ(dxdy)∈[0,∞].

Assumption 2.3 asks for a constant C∈(0,∞)C\in(0,\infty)C∈(0,∞) and measurable functions ψ,φ:S→(0,∞)\psi,\varphi:S\to(0,\infty)ψ,φ:S→(0,∞) such that:

  • (C1) main Lyapunov condition: for some λ∈[1,∞)\lambda\in[1,\infty)λ∈[1,∞), (πψ)(x)≤λψ(x)(\pi\psi)(x)\le\lambda\psi(x)(πψ)(x)≤λψ(x) whenever ψ(x)≤C\psi(x)\le Cψ(x)≤C;
  • (C2) global Lyapunov condition: for some β∈[1,∞)\beta\in[1,\infty)β∈[1,∞), (πφ)(x)≤βφ(x)(\pi\varphi)(x)\le\beta\varphi(x)(πφ)(x)≤βφ(x) and ρ(x,y)≤φ(x)+φ(y)\rho(x,y)\le\varphi(x)+\varphi(y)ρ(x,y)≤φ(x)+φ(y) for all x,yx,yx,y;
  • (C3) local contractivity: there are a probability space (Ω,A,P)(\Omega,\mathcal A,P)(Ω,A,P), a constant c∈(0,∞)c\in(0,\infty)c∈(0,∞) and a measurable map (X′,Y′):S×S×Ω→S×S(X',Y'):S\times S\times\Omega\to S\times S(X′,Y′):S×S×Ω→S×S. For every x,yx,yx,y, the pair (X′(x,y,⋅),Y′(x,y,⋅))(X'(x,y,\cdot),Y'(x,y,\cdot))(X′(x,y,⋅),Y′(x,y,⋅)) is a coupling of π(x,⋅)\pi(x,\cdot)π(x,⋅) and π(y,⋅)\pi(y,\cdot)π(y,⋅), and E[ρ(X′(x,y,⋅),Y′(x,y,⋅))]≤e−cρ(x,y)E[\rho(X'(x,y,\cdot),Y'(x,y,\cdot))]\le e^{-c}\rho(x,y)E[ρ(X′(x,y,⋅),Y′(x,y,⋅))]≤e−cρ(x,y) whenever ψ(x)≤C\psi(x)\le Cψ(x)≤C and ψ(y)≤C\psi(y)\le Cψ(y)≤C.

Finally,

δ(C)=sup⁡{φ(x)+φ(y)ψ(x)+ψ(y):x,y∈S, ψ(x)>C or ψ(y)>C}∈[0,∞].\delta(C)=\sup\Big\{\frac{\varphi(x)+\varphi(y)}{\psi(x)+\psi(y)}:x,y\in S,\ \psi(x)>C\text{ or }\psi(y)>C\Big\}\in[0,\infty].δ(C)=sup{ψ(x)+ψ(y)φ(x)+φ(y)​:x,y∈S, ψ(x)>C or ψ(y)>C}∈[0,∞].

Formalization targets

Goal: Theorem 2.11

Under Assumption 2.3, for every n∈Nn\in\mathbb Nn∈N and all probability measures ν,η\nu,\etaν,η on (S,B(S))(S,\mathcal B(S))(S,B(S)),

Wρ(νπn,ηπn)≤e−cnWρ(ν,η)+βnλn−1(∫ψ dν+∫ψ dη)δ(C).(42)\mathcal W_\rho(\nu\pi^n,\eta\pi^n)\le e^{-cn}\mathcal W_\rho(\nu,\eta)+\beta^n\lambda^{n-1}\Big(\int\psi\,d\nu+\int\psi\,d\eta\Big)\delta(C).\tag{42}Wρ​(νπn,ηπn)≤e−cnWρ​(ν,η)+βnλn−1(∫ψdν+∫ψdη)δ(C).(42)

The constants are those of the paper and are not weakened. Each quantity may be infinite, and the bound is read in [0,∞][0,\infty][0,∞].

Milestones

  1. Lemma 6.1. If a measurable coupling contracts ρ\rhoρ by e−ce^{-c}e−c in one step from every pair in A×AA\times AA×A, then for every initial coupling γ\gammaγ there is a coupled Markov chain (Xn,Yn)(X_n,Y_n)(Xn​,Yn​) with (X0,Y0)∼γ(X_0,Y_0)\sim\gamma(X0​,Y0​)∼γ and both marginals Markov with kernel π\piπ. Along this chain, Mn=ec(n∧T)ρ(Xn∧T,Yn∧T)M_n=e^{c(n\wedge T)}\rho(X_{n\wedge T},Y_{n\wedge T})Mn​=ec(n∧T)ρ(Xn∧T​,Yn∧T​) is a non-negative supermartingale, where TTT is the exit time from A×AA\times AA×A.
  2. (134). ecnE[ρ(Xn,Yn);n≤T]≤E[Mn]≤∫ρ dγe^{cn}E[\rho(X_n,Y_n);n\le T]\le E[M_n]\le\int\rho\,d\gammaecnE[ρ(Xn​,Yn​);n≤T]≤E[Mn​]≤∫ρdγ.
  3. (135). E[ρ(Xn,Yn);n>T]≤βnE[ψ(XT)+ψ(YT);n>T] δ(C)E[\rho(X_n,Y_n);n>T]\le\beta^nE[\psi(X_T)+\psi(Y_T);n>T]\,\delta(C)E[ρ(Xn​,Yn​);n>T]≤βnE[ψ(XT​)+ψ(YT​);n>T]δ(C), through the intermediate bounds by φ\varphiφ.
  4. (136). E[ψ(XT)+ψ(YT);n>T]≤λn−1(∫ψ dν+∫ψ dη)E[\psi(X_T)+\psi(Y_T);n>T]\le\lambda^{n-1}\big(\int\psi\,d\nu+\int\psi\,d\eta\big)E[ψ(XT​)+ψ(YT​);n>T]≤λn−1(∫ψdν+∫ψdη).

Significance

The result. Theorem 2.11 separates two tasks that are usually entangled in convergence proofs for Markov chains on unbounded spaces. One is a contraction estimate that only has to hold on a sublevel set {ψ≤C}\{\psi\le C\}{ψ≤C}. The other is a pair of drift conditions that control excursions out of that set. The second term of (42) is made small by choosing CCC large, and the first by choosing nnn large. In the paper this gives W1\mathcal W^1W1 bounds to the invariant measure for adjusted numerical HMC (Theorem 2.12), whose contraction (Theorems 2.4 and 2.7) is only established on a ball. The theorem uses nothing about HMC and applies to any chain with a locally contractive coupling and the two Lyapunov conditions. Examples are other discretized diffusions and Metropolis-adjusted samplers.

Formalizing it. The result is proved in the paper. As far as is known, it has no machine-checked proof. A formalization requires constructing a Markovian coupling on a general measurable space and working with a generalized, [0,∞][0,\infty][0,∞]-valued supermartingale stopped at an exit time. It also needs the Markov property with respect to the joint filtration of a coupled pair. Both pieces are reusable in coupling arguments for Markov chains in general.

Difficulty

Contraction on {ψ≤C}2\{\psi\le C\}^2{ψ≤C}2 gives no control once either copy leaves that set, and the exit time TTT is random and may be infinite. The bound therefore has to be split at TTT. On {n≤T}\{n\le T\}{n≤T} the contraction accumulates, which requires optional stopping for a supermartingale that need not be integrable, because ∫ρ dγ\int\rho\,d\gamma∫ρdγ may be +∞+\infty+∞. On {n>T}\{n>T\}{n>T} the distance at time nnn has to be bounded by quantities at the random time TTT. This requires the Markov property of each copy with respect to the filtration of the pair: the event {T=k}\{T=k\}{T=k} depends on both copies. A Markov property of each copy in its own filtration does not suffice. Finally, ψ\psiψ at the exit time has to be controlled by its initial integral, which is a second stopped supermartingale built from (C1).

Formalization scope

  • (S,ρ)(S,\rho)(S,ρ) is a Lean MetricSpace with its Borel σ\sigmaσ-algebra, complete and separable; ρ\rhoρ is dist. π\piπ is a Markov kernel (Kernel S S with IsMarkovKernel), and νπn\nu\pi^nνπn is the bind of ν\nuν with the nnn-fold composition of π\piπ.
  • Every expectation of a non-negative quantity, every ∫ψ dν\int\psi\,d\nu∫ψdν, δ(C)\delta(C)δ(C) and Wρ\mathcal W_\rhoWρ​ is valued in [0,∞][0,\infty][0,∞] (lower Lebesgue integrals, ℝ≥0∞). No Bochner integral appears, so a non-integrable quantity can never be replaced by a junk 000. In particular, ∫ψ dν=∞\int\psi\,d\nu=\infty∫ψdν=∞ is allowed, as on the page.
  • Couplings are the published definition MongeKantorovichYao.transferencePlans.
  • (C3)'s probability space and coupling map are parameters of the theorem, which then holds for every such realization.
  • λn−1\lambda^{n-1}λn−1 is an integer power, so n=0n=0n=0 is included (and (42) is then trivially true).
  • Lemma 6.1's chain is the coordinate process on the path space (S×S)N(S\times S)^{\mathbb N}(S×S)N, which is determined up to its law. The supermartingale property is the generalized one, E[Mn+1;F]≤E[Mn;F]E[M_{n+1};F]\le E[M_n;F]E[Mn+1​;F]≤E[Mn​;F] for F∈FnF\in\mathcal F_nF∈Fn​. Mathlib's Supermartingale requires integrability, which the page does not assume. The exit time is N∪{∞}\mathbb N\cup\{\infty\}N∪{∞}-valued, and n∧T=nn\wedge T=nn∧T=n when the chain never leaves.
  • The marginal Markov property is stated with respect to the filtration of the pair. This is what the proof of (135) and (136) uses, and it implies the marginal Markov property in each copy's own filtration.
  • The proof on p. 43 applies Lemma 6.1 "with A={ψ>C}A=\{\psi>C\}A={ψ>C}". The set on which (C3) contracts and whose exit time is TTT is {ψ≤C}\{\psi\le C\}{ψ≤C}, and that set is used. The text before (135) says "{n<T}\{n<T\}{n<T}" where its displays use {n>T}\{n>T\}{n>T}, and the displays are formalized.
  • A formalization in which Wρ\mathcal W_\rhoWρ​ or δ(C)\delta(C)δ(C) is a real number obtained by truncating +∞+\infty+∞, or in which the measures need not be probability measures (so that the coupling set is empty and Wρ=∞\mathcal W_\rho=\inftyWρ​=∞), would make (42) vacuous and is excluded.

A complete development needs Ionescu-Tulcea's construction of a Markov chain on a general measurable space (ProbabilityTheory.Kernel.traj in Mathlib), the measurability of the coupling kernel (x,y)↦P∘(X′,Y′)(x,y,⋅)−1(x,y)\mapsto P\circ(X',Y')(x,y,\cdot)^{-1}(x,y)↦P∘(X′,Y′)(x,y,⋅)−1, and optional stopping for [0,∞][0,\infty][0,∞]-valued supermartingales stopped at an exit time. Contributions are welcome on the milestones individually. The optional-stopping and joint-Markov-property lemmas are reusable beyond this mission.

Selected references

  • N. Bou-Rabee, A. Eberle, R. Zimmer, Coupling and convergence for Hamiltonian Monte Carlo, Ann. Appl. Probab. 30(3), 2020. arXiv:1805.00452 (v2 is the version cited here).
  • A. Joulin, Y. Ollivier, Curvature, concentration and error estimates for Markov chain Monte Carlo, Ann. Probab. 38(6), 2010. doi:10.1214/10-AOP541
  • C. Villani, Optimal Transport: Old and New, Springer, 2009. doi:10.1007/978-3-540-71050-9
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Markov ChainNumerical AnalysisOptimal Transport+1·Captain: mikedeng1

Coupling and Convergence for Hamiltonian Monte Carlo 1: Exact HMC Contracts the Concave Kantorovich Distance W_ρ at Rate c = (1/10)·min(1, ½KT²(1+ℛ/T)e^{−ℛ/(2T)})·e^{−2ℛ/T}Research Paper

Why convergence bounds for Hamiltonian Monte Carlo matter

Hamiltonian Monte Carlo (HMC) is one of the most widely used Markov chain Monte Carlo methods for sampling from a probability density μ(dx)∝e−U(x) dx\mu(dx)\propto e^{-U(x)}\,dxμ(dx)∝e−U(x)dx on Rd\mathbb R^dRd. It is the default sampler of probabilistic programming systems such as Stan, and it is used throughout Bayesian statistics, molecular dynamics and machine learning. In practice the chain is run for a finite number of steps, and a user needs to know how many steps make its law close to μ\muμ. That requires a quantitative, dimension-explicit convergence bound.

Before the paper of Bou-Rabee, Eberle and Zimmer, such bounds were known essentially only when UUU is strongly convex everywhere: then two copies of the chain driven by the same random velocity contract deterministically (Mangoubi and Smith, arXiv:1708.07114). Bou-Rabee, Eberle and Zimmer (arXiv:1805.00452, Ann. Appl. Probab. 30(3), 2020) remove global convexity. They require UUU to be strongly convex only outside a ball, and they introduce a coupling of two HMC transitions under which a suitably concave distance contracts on average for every pair of starting points. This mission formalizes that contraction theorem for exact HMC, together with its consequence, exponential convergence in the L1L^1L1 Wasserstein distance.

Setting

Let U:Rd→RU:\mathbb R^d\to\mathbb RU:Rd→R be four times continuously differentiable with ∫e−U<∞\int e^{-U}<\infty∫e−U<∞. The Hamiltonian is H(x,v)=U(x)+12∣v∣2H(x,v)=U(x)+\tfrac12|v|^2H(x,v)=U(x)+21​∣v∣2, and the exact Hamiltonian flow (qt,pt)(q_t,p_t)(qt​,pt​) solves

ddtqt=pt,ddtpt=−∇U(qt),(q0(x,v),p0(x,v))=(x,v).\tfrac{d}{dt}q_t=p_t,\qquad \tfrac{d}{dt}p_t=-\nabla U(q_t),\qquad (q_0(x,v),p_0(x,v))=(x,v).dtd​qt​=pt​,dtd​pt​=−∇U(qt​),(q0​(x,v),p0​(x,v))=(x,v).

Fix a duration T>0T>0T>0. One step of exact HMC from xxx draws a fresh velocity ξ∼N(0,Id)\xi\sim N(0,I_d)ξ∼N(0,Id​) and moves to X′(x)=qT(x,ξ)X'(x)=q_T(x,\xi)X′(x)=qT​(x,ξ); its transition kernel is π(x,⋅)=law(qT(x,ξ))\pi(x,\cdot)=\mathrm{law}(q_T(x,\xi))π(x,⋅)=law(qT​(x,ξ)), and μ\muμ is invariant for π\piπ.

Assumption 2.1 asks that (A1) UUU has a local minimum at 000 with U(0)=0U(0)=0U(0)=0; (A2) the second, third and fourth derivatives of UUU are bounded, with L=sup⁡∥∇2U∥L=\sup\|\nabla^2U\|L=sup∥∇2U∥, M=sup⁡∥∇3U∥M=\sup\|\nabla^3U\|M=sup∥∇3U∥ and N=sup⁡∥∇4U∥N=\sup\|\nabla^4U\|N=sup∥∇4U∥; and (A3) there are R≥0\mathcal R\ge0R≥0 and K>0K>0K>0 such that

(x−y)⋅(∇U(x)−∇U(y))≥K∣x−y∣2whenever ∣x−y∣≥R.(x-y)\cdot(\nabla U(x)-\nabla U(y))\ge K|x-y|^2\quad\text{whenever }|x-y|\ge\mathcal R.(x−y)⋅(∇U(x)−∇U(y))≥K∣x−y∣2whenever ∣x−y∣≥R.

The coupling. For two starting points x,yx,yx,y with z=x−yz=x-yz=x−y, e=z/∣z∣e=z/|z|e=z/∣z∣, both copies use the same ξ\xiξ. If ∣x−y∣≥2R|x-y|\ge2\mathcal R∣x−y∣≥2R the second copy also uses ξ\xiξ (synchronous coupling). If ∣x−y∣<2R|x-y|<2\mathcal R∣x−y∣<2R it uses

η={ξ+γzif U~≤φ0,1(e⋅ξ+γ∣z∣)/φ0,1(e⋅ξ),ξ−2(e⋅ξ)eotherwise,\eta=\begin{cases}\xi+\gamma z&\text{if }\tilde{\mathcal U}\le\varphi_{0,1}(e\cdot\xi+\gamma|z|)/\varphi_{0,1}(e\cdot\xi),\\ \xi-2(e\cdot\xi)e&\text{otherwise,}\end{cases}η={ξ+γzξ−2(e⋅ξ)e​if U~≤φ0,1​(e⋅ξ+γ∣z∣)/φ0,1​(e⋅ξ),otherwise,​

with U~∼Unif(0,1)\tilde{\mathcal U}\sim\mathrm{Unif}(0,1)U~∼Unif(0,1) independent of ξ\xiξ and φ0,1\varphi_{0,1}φ0,1​ the standard normal density. This is a maximal coupling of N(0,Id)N(0,I_d)N(0,Id​) with its shift by γz\gamma zγz, completed by a reflection. The coupled positions are X′=qT(x,ξ)X'=q_T(x,\xi)X′=qT​(x,ξ) and Y′=qT(y,η)Y'=q_T(y,\eta)Y′=qT​(y,η), with R′(x,y)=∣X′−Y′∣R'(x,y)=|X'-Y'|R′(x,y)=∣X′−Y′∣.

The distance and the parameters. With γ=min⁡(T−1,R−1/4)\gamma=\min(T^{-1},\mathcal R^{-1}/4)γ=min(T−1,R−1/4), a=T−1a=T^{-1}a=T−1 and R1=52(R+T)R_1=\tfrac52(\mathcal R+T)R1​=25​(R+T), set

f(r)=∫0re−amin⁡(s,R1) ds,ρ(x,y)=f(∣x−y∣),f(r)=\int_0^r e^{-a\min(s,R_1)}\,ds,\qquad \rho(x,y)=f(|x-y|),f(r)=∫0r​e−amin(s,R1​)ds,ρ(x,y)=f(∣x−y∣),

and let Wρ(ν,η)=inf⁡γ∈C(ν,η)∫ρ dγ\mathcal W_\rho(\nu,\eta)=\inf_{\gamma\in C(\nu,\eta)}\int\rho\,d\gammaWρ​(ν,η)=infγ∈C(ν,η)​∫ρdγ be the Kantorovich distance over couplings C(ν,η)C(\nu,\eta)C(ν,η).

Formalization targets

Goal: Theorem 2.3

Under Assumption 2.1 and LT2≤min⁡(K/L,14,116Λ)LT^2\le\min(K/L,\tfrac14,\tfrac1{16\Lambda})LT2≤min(K/L,41​,16Λ1​) with Λ=16LR2\Lambda=16L\mathcal R^2Λ=16LR2, for all x,y∈Rdx,y\in\mathbb R^dx,y∈Rd,

E[f(R′(x,y))]≤(1−c) f(∣x−y∣),c=110min⁡(1,12KT2(1+RT)e−R/(2T))e−2R/T.E\bigl[f(R'(x,y))\bigr]\le(1-c)\,f(|x-y|),\qquad c=\frac1{10}\min\Bigl(1,\frac12KT^2\Bigl(1+\frac{\mathcal R}{T}\Bigr)e^{-\mathcal R/(2T)}\Bigr)e^{-2\mathcal R/T}.E[f(R′(x,y))]≤(1−c)f(∣x−y∣),c=101​min(1,21​KT2(1+TR​)e−R/(2T))e−2R/T.

This is the paper's main result for exact HMC, stated with its own constants.

Milestones (in the order of the proof)

  1. (112)–(116): the parameter inequalities γT≤1\gamma T\le1γT≤1, LT≤γ/4LT\le\gamma/4LT≤γ/4, γR≤14\gamma\mathcal R\le\tfrac14γR≤41​, aT≥1aT\ge1aT≥1, R1≥52(1+γT)RR_1\ge\tfrac52(1+\gamma T)\mathcal RR1​≥25​(1+γT)R.
  2. Lemma 3.4 (h=0h=0h=0): ∣qt(x,v)−qt(y,v)∣2≤(1−Kt2/2)∣x−y∣2|q_t(x,v)-q_t(y,v)|^2\le(1-Kt^2/2)|x-y|^2∣qt​(x,v)−qt​(y,v)∣2≤(1−Kt2/2)∣x−y∣2 for ∣x−y∣≥2R|x-y|\ge2\mathcal R∣x−y∣≥2R.
  3. Theorem 2.1: the synchronous coupling contracts far-apart points, R′2≤(1−12KT2)r2R'^2\le(1-\tfrac12KT^2)r^2R′2≤(1−21​KT2)r2.
  4. (119)–(120): inf⁡r>0rf′(r)/f(r)≥max⁡(1,aR1)e−aR1\inf_{r>0}rf'(r)/f(r)\ge\max(1,aR_1)e^{-aR_1}infr>0​rf′(r)/f(r)≥max(1,aR1​)e−aR1​, and the resulting bound on c1c_1c1​.
  5. Lemma 3.2 (h=0h=0h=0): first-variation bounds for the flow.
  6. Term I: on {η=ξ+γz}\{\eta=\xi+\gamma z\}{η=ξ+γz}, R′≤(1−34γT)rR'\le(1-\tfrac34\gamma T)rR′≤(1−43​γT)r.
  7. Lemma 3.7 (62): P[ξ−η≠−γz]≤∣γz∣/2πP[\xi-\eta\ne-\gamma z]\le|\gamma z|/\sqrt{2\pi}P[ξ−η=−γz]≤∣γz∣/2π​.
  8. (123): the truncated loss on the reflection event is at most (γT/2π) rf′(r)(\gamma T/\sqrt{2\pi})\,rf'(r)(γT/2π​)rf′(r).
  9. Term III: E[(R′−R1)+; ξ−η≠−γz]≤54γrTE[(R'-R_1)^+;\,\xi-\eta\ne-\gamma z]\le\tfrac54\gamma rTE[(R′−R1​)+;ξ−η=−γz]≤45​γrT.
  10. (127): 15γTmax⁡(1,2aR)e−2aR≥110e−2R/T\tfrac15\gamma T\max(1,2a\mathcal R)e^{-2a\mathcal R}\ge\tfrac1{10}e^{-2\mathcal R/T}51​γTmax(1,2aR)e−2aR≥101​e−2R/T.

Companions

The coupling property (η∼N(0,Id)\eta\sim N(0,I_d)η∼N(0,Id​), p. 9), Corollary 2.8 (Wρ(νπn,ηπn)≤e−cnWρ(ν,η)\mathcal W_\rho(\nu\pi^n,\eta\pi^n)\le e^{-cn}\mathcal W_\rho(\nu,\eta)Wρ​(νπn,ηπn)≤e−cnWρ​(ν,η), the W1\mathcal W^1W1 bound with factor M=e52(1+R/T)M=e^{\frac52(1+\mathcal R/T)}M=e25​(1+R/T), and the step count (41)), and the comparison (133), e−aR1∣x−y∣≤ρ(x,y)≤∣x−y∣e^{-aR_1}|x-y|\le\rho(x,y)\le|x-y|e−aR1​∣x−y∣≤ρ(x,y)≤∣x−y∣.

Significance

Theorem 2.3 gives a contraction rate for exact HMC that depends on ddd only through the constants LLL, KKK and R\mathcal RR of the potential, and that holds without global convexity. Through the coupling characterization of Wρ\mathcal W_\rhoWρ​ it yields Corollary 2.8, an explicit number of steps after which the law of the chain is within ϵ\epsilonϵ of μ\muμ in W1\mathcal W^1W1. The same coupling and concave-distance technique underlies the paper's results for numerical (velocity Verlet) HMC and later work on Langevin and HMC couplings.

The theorems are proved in the paper; none of them is machine-checked. Formalizing them requires the Hamiltonian ODE flow and its first-variation estimates, a Gaussian maximal/reflection coupling, and the transfer from one-step contraction to Kantorovich contraction of Markov kernels. Each of these is reusable well beyond HMC. A formal development also settles the constants. Three printed displays of the proof are not delivered by the printed argument, and Theorem 2.1 as printed is false, while the goal itself survives: see Formalization scope.

Difficulty

The obvious argument fails for nearby points. When ∣x−y∣<2R|x-y|<2\mathcal R∣x−y∣<2R, UUU may be non-convex between them, and the synchronous coupling can push the two trajectories apart. The coupling must therefore change the velocity of one copy, and doing so makes the contraction only hold on average, on the event η=ξ+γz\eta=\xi+\gamma zη=ξ+γz. On the complementary reflection event the distance can grow, and the growth must be paid for by the concavity of fff, through the truncation at R1R_1R1​ and the tail term. Balancing these terms, uniformly in xxx, yyy and ddd, is the heart of the proof. For far-apart points the difficulty is different: the contraction of Lemma 3.4 needs the trajectories to stay outside the non-convex region over the whole time interval, which is where the condition LT2<K/LLT^2<K/LLT2<K/L enters.

Formalization scope

  • Space and objects. Rd\mathbb R^dRd is EuclideanSpace ℝ (Fin d); ∇U\nabla U∇U is Mathlib's gradient, and ∇kU\nabla^kU∇kU is iteratedFDeriv. L,M,NL,M,NL,M,N are upper bounds on the derivative norms, which is equivalent for every statement here. The flow is pinned by a predicate on (q,p)(q,p)(q,p) (initial values and the ODE for all t∈Rt\in\mathbb Rt∈R); it is never a free function. Assumption 2.1 includes the standing hypotheses of §2.1: U∈C4U\in C^4U∈C4, ∫e−U<∞\int e^{-U}<\infty∫e−U<∞, and TTT deterministic.
  • Probability. The randomness of one step is (ξ,U~)(\xi,\tilde{\mathcal U})(ξ,U~) with law N(0,Id)⊗Unif(0,1)N(0,I_d)\otimes\mathrm{Unif}(0,1)N(0,Id​)⊗Unif(0,1). Expectations of nonnegative quantities are Lebesgue integrals in [0,∞][0,\infty][0,∞]. The signed expectation in (123) uses a Bochner integral together with an explicit integrability conclusion, so no bound can hold because a non-integrable integral is read as 000. Kantorovich distances take values in [0,∞][0,\infty][0,∞] over the published set of couplings MongeKantorovichYao.transferencePlans. The nnn-step kernel is the iterated composition πn+1=π∘πn\pi^{n+1}=\pi\circ\pi^nπn+1=π∘πn.
  • Conventions at R=0\mathcal R=0R=0. γ\gammaγ is T−1T^{-1}T−1 and LT2≤1/(16Λ)LT^2\le1/(16\Lambda)LT2≤1/(16Λ) is written 256L2R2T2≤1256L^2\mathcal R^2T^2\le1256L2R2T2≤1, so that no division by zero decides a constant.
  • Corrections. The strict condition (56) in Lemma 3.4 is written L2t2<KL^2t^2<KL2t2<K, which preserves its meaning at L=0L=0L=0. Theorem 2.1 is stated as its proof delivers it, R′2≤(1−12KT2)r2R'^2\le(1-\tfrac12KT^2)r^2R′2≤(1−21​KT2)r2. The printed R′≤(1−12KT2)rR'\le(1-\tfrac12KT^2)rR′≤(1−21​KT2)r fails for U(x)=12∣x∣2U(x)=\tfrac12|x|^2U(x)=21​∣x∣2, where R′=∣cos⁡T∣ rR'=|\cos T|\,rR′=∣cosT∣r. The displays (117), (122), the last inequality of (124), and (126) are not posed, because the printed argument does not deliver their constants. The goal's rate ccc of (32) is nevertheless unaffected: under the step condition and d≥1d\ge1d≥1, c=120KT2(1+R/T)e−5R/(2T)c=\tfrac1{20}KT^2(1+\mathcal R/T)e^{-5\mathcal R/(2T)}c=201​KT2(1+R/T)e−5R/(2T), which lies below both corrected rates c1c_1c1​ and c2c_2c2​.
  • Ruled out. The goal is not trivialized by a vacuous hypothesis: the hypotheses are met by U(x)=12∣x∣2U(x)=\tfrac12|x|^2U(x)=21​∣x∣2, L=K=1L=K=1L=K=1, R=0\mathcal R=0R=0, T=12T=\tfrac12T=21​. Nor is it trivialized by a junk value: fff, R′R'R′ and the integral are genuine, and the flow is the unique solution of the ODE.
  • Contributions welcome. Gronwall-type first-variation bounds for Lipschitz Hamiltonian flows, the Gaussian maximal/reflection coupling (Lemma 3.7 and the coupling property), and the general passage from a one-step average contraction to Wρ\mathcal W_\rhoWρ​ contraction of a Markov kernel.

Selected references

  • N. Bou-Rabee, A. Eberle, R. Zimmer, Coupling and convergence for Hamiltonian Monte Carlo, Ann. Appl. Probab. 30(3), 2020. arXiv:1805.00452, doi:10.1214/19-AAP1528
  • O. Mangoubi, A. Smith, Rapid mixing of Hamiltonian Monte Carlo on strongly log-concave distributions, 2017. arXiv:1708.07114
  • A. Eberle, Reflection couplings and contraction rates for diffusions, Probab. Theory Related Fields 166, 2016. arXiv:1305.1233
  • A. Eberle, A. Guillin, R. Zimmer, Couplings and quantitative contraction rates for Langevin dynamics, Ann. Probab. 47(4), 2019. arXiv:1703.01617
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Algorithmic Game TheoryEconomics·Captain: mikedeng1

Competitive Equilibrium with Indivisible Goods and Generic Budgets 3: Two Agents with Identical Additive Preferences and Generic Budgets Have a Competitive Equilibrium Giving Truncated SharesResearch Paper

Motivation

How should a set of indivisible items (courses, shifts, inherited objects) be divided among people who have different entitlements but no money to transfer? A classical answer for divisible goods is the competitive equilibrium from equal incomes (CEEI): give every agent a budget of artificial currency, find prices at which every agent can afford her favourite bundle and the market clears. The resulting allocation is Pareto optimal and fair. With indivisible items a CEEI can fail to exist already for one item and two agents with equal budgets: at any price, either both agents can afford the item or neither can.

Babaioff, Nisan and Talgam-Cohen (arXiv:1703.08150; Math. Oper. Res. 2021, doi:10.1287/moor.2020.1062) study this Fisher market with indivisible goods when budgets are generic: unequal budgets, with a measure-zero set of exceptional budget pairs excluded. Their main result is for two agents with almost equal budgets. This mission formalizes the companion result for two agents with identical additive preferences and arbitrary unequal budgets (Theorem 8.1 of the paper, its informal Theorem 1.4). With identical preferences the division problem is a discrete claims (bankruptcy) problem: one cake of fixed value is split between claimants with different entitlements b1,b2b_1, b_2b1​,b2​.

Timeline of the relevant results:

  • Budish (2011, doi:10.1086/664613): approximate CEEI with almost equal budgets for many agents, with an approximate market-clearing error.
  • Segal-Halevi (AAMAS 2018, arXiv:1705.04212), a follow-up to the preprint of this paper: for four agents with arbitrary budgets, non-existence of CE persists even with generic budgets.
  • Babaioff, Nisan and Talgam-Cohen (preprint 2017, journal 2021): exact CE for two additive agents with almost equal unequal budgets (Theorem 7.1), and for two agents with identical preferences and generic budgets (Theorem 8.1).

Setting

There are mmm indivisible items MMM and two agents. Agent iii has a valuation vi:2M→Rv_i : 2^M \to \mathbb Rvi​:2M→R that is additive, normalized (vi(M)=1v_i(M)=1vi​(M)=1), non-negative, monotone and strict (different bundles have different values), and a budget bi>0b_i > 0bi​>0, with b1+b2=1b_1 + b_2 = 1b1​+b2​=1. An allocation S=(S1,S2)\mathcal S = (\mathcal S_1, \mathcal S_2)S=(S1​,S2​) gives every item to exactly one agent. Item prices pj≥0p_j \ge 0pj​≥0 price a bundle at p(S)=∑j∈Spjp(S) = \sum_{j \in S} p_jp(S)=∑j∈S​pj​.

A bundle SSS is demanded by agent iii at prices ppp if p(S)≤bip(S) \le b_ip(S)≤bi​ and p(T)>bip(T) > b_ip(T)>bi​ for every bundle TTT with vi(T)>vi(S)v_i(T) > v_i(S)vi​(T)>vi​(S). A competitive equilibrium (CE) is a pair (S,p)(\mathcal S, p)(S,p) in which each Si\mathcal S_iSi​ is demanded by agent iii. An allocation is Pareto optimal (PO) if every other allocation is strictly worse for some agent. It is budget-proportional if vi(Si)≥biv_i(\mathcal S_i) \ge b_ivi​(Si​)≥bi​ for both agents, and anti-proportional if vi(Si)≤biv_i(\mathcal S_i) \le b_ivi​(Si​)≤bi​ for both, strictly for one.

The truncated share of agent iii is

bi−=max⁡{vi(Si′):S′ PO, vi(Si′)≤bi},b_i^- = \max\{ v_i(\mathcal S'_i) : \mathcal S' \text{ PO},\ v_i(\mathcal S'_i) \le b_i \},bi−​=max{vi​(Si′​):S′ PO, vi​(Si′​)≤bi​},

the best she can get in a PO allocation that gives her at most her budget share; an allocation gives her the truncated share if vi(Si)≥bi−v_i(\mathcal S_i) \ge b_i^-vi​(Si​)≥bi−​. The exceptional set RiR_iRi​ (Definition 6.2) consists of the budget pairs (bi,1−bi)(b_i, 1-b_i)(bi​,1−bi​) for which two PO allocations S(r),S(r+1)\mathcal S(r), \mathcal S(r+1)S(r),S(r+1), consecutive in agent iii's order of preference, satisfy bi/vi(S(r+1)i)=(1−bi)/(1−vi(S(r)i))b_i / v_i(\mathcal S(r+1)_i) = (1-b_i)/(1-v_i(\mathcal S(r)_i))bi​/vi​(S(r+1)i​)=(1−bi​)/(1−vi​(S(r)i​)). It is finite. The rectangle TiT_iTi​ (Definition 6.1) is a set of allocations between the truncated-share maximizers of the two agents.

In Lean all objects live in GenericBudgets.IdenticalPrefs: bundle, price, IsDemanded, IsCE, IsPO, IsStandardValuation, IsBudgetProportional, IsAntiProportional, GetsTruncatedShare, IsTruncMaximizer, InRectT, InR.

Formalization targets

Goal: Theorem 8.1 (p. 20)

If v1=v2v_1 = v_2v1​=v2​, b1>b2b_1 > b_2b1​>b2​, and (b1,b2)∉Ri(b_1,b_2) \notin R_i(b1​,b2​)∈/Ri​ for some agent iii, then

∃ (S,p) a CE with vj(Sj)≥bj− for j=1,2.\exists\, (\mathcal S, p) \text{ a CE with } v_j(\mathcal S_j) \ge b_j^- \text{ for } j = 1, 2.∃(S,p) a CE with vj​(Sj​)≥bj−​ for j=1,2.

Milestones

  1. Proposition 5.1 (p. 12): every budget-proportional, and every anti-proportional, PO allocation is supported in a CE.
  2. Lemma 6.3 (p. 15): no budget-proportional allocation, no PO anti-proportional allocation, (b1,b2)∉Ri(b_1,b_2) \notin R_i(b1​,b2​)∈/Ri​ and Ti=∅T_i = \emptysetTi​=∅ imply a CE with truncated shares.
  3. Constant-sum claim (p. 20): with identical preferences every allocation is PO and none is anti-proportional.
  4. Lemma 8.2 (p. 20): if every allocation is PO and (b1,b2)∉Ri(b_1,b_2) \notin R_i(b1​,b2​)∈/Ri​ for some iii, a CE exists; if moreover no PO allocation is anti-proportional, the same CE gives truncated shares.

Significance

Theorem 8.1 shows that the non-existence of CEEI for identical preferences is a knife-edge phenomenon: for every market with identical strict additive preferences, every unequal budget pair outside a finite set admits a CE, and the CE allocation is as close to budget-proportional as indivisibility allows. It gives a market-based solution to the indivisible claims problem with unequal entitlements, and its CE inherits Pareto optimality from the first welfare theorem (Theorem 2.4 of the paper).

The formalization targets three things on top of the paper. First, a machine-checked proof of the paper's main technical tool, Lemma 6.3, which also drives the paper's main Theorem 7.1 (mission 1 of this series), where it is applied to almost equal budgets instead of identical preferences. Second, precise definitions of the truncated share, the rectangle TiT_iTi​ and the exceptional set RiR_iRi​, whose informal versions leave conventions implicit (the maximization runs over PO allocations only; RiR_iRi​ is indexed by consecutive PO allocations). Third, verification of the proof chain Proposition 5.1 → Lemma 6.3 → Lemma 8.2 → Theorem 8.1. The statements compile, but none of these results has a machine-checked proof yet.

Difficulty

The reduction of Theorem 8.1 to Lemma 8.2 and the proof of Lemma 8.2 from Proposition 5.1 and Lemma 6.3 are short. The substance is in Lemma 6.3, which must exhibit prices supporting a PO allocation when no allocation gives both agents their budget shares. Demand is a condition over all 2m2^m2m bundles, so a candidate price vector has to be checked against every bundle each agent prefers, and the paper's construction breaks down on the exceptional budget pairs RiR_iRi​, which is why they are excluded; the argument is a case analysis over the finite Pareto frontier. The easy case, Proposition 5.1, covers only markets with a budget-proportional or anti-proportional PO allocation; with identical preferences and unequal budgets neither typically exists (no allocation is ever anti-proportional), so Lemma 6.3 cannot be avoided.

Formalization scope

Items are Fin m; agents are Fin 2, with indices 0,10, 10,1 for the paper's agents 1,21, 21,2, so b1>b2b_1 > b_2b1​>b2​ is b 1 < b 0. Valuations are functions Finset (Fin m) → ℝ bundled with the standing assumptions in IsStandardValuation; identical preferences are the hypothesis v 0 = v 1. An allocation is a map Fin m → Fin 2, so every item is allocated exactly once. Budgets are positive reals summing to 111. All quantities are real.

Committed conventions and disclosed restrictions:

  • Strictness is injectivity of each valuation on bundles. The paper allows one exception, identical items; that exception is dropped, so markets with identical items are not covered by these statements.
  • The budget-proportional share is written bi vi(M)b_i\,v_i(M)bi​vi​(M), which equals bib_ibi​ under normalization.
  • The truncated share is stated without a max: vi(Si)≥vi(Si′)v_i(\mathcal S_i) \ge v_i(\mathcal S'_i)vi​(Si​)≥vi​(Si′​) for every PO S′\mathcal S'S′ with vi(Si′)≤biv_i(\mathcal S'_i) \le b_ivi​(Si′​)≤bi​.
  • "(b1,b2)(b_1,b_2)(b1​,b2​) does not belong to RiR_iRi​ for some agent iii" is read as an existential over iii.
  • RiR_iRi​ is encoded with consecutive PO allocations and the cross-multiplied equation, equivalent to the page's quotient form.
  • The constant-sum sentence of p. 20 says "at most their truncated share"; the definition it paraphrases (anti-proportional, p. 12) uses the budget-proportional share, and that is what is stated.

Trivializing formalizations are ruled out: the demand condition quantifies over every bundle with strict inequality, allocations must assign every item, prices are non-negative, the truncated share is maximized over PO allocations only (not over all allocations), and the budget hypothesis excludes only the finite set RiR_iRi​ for one agent, never all unequal budgets.

Proposition 5.1 and Lemma 6.3 are posed with the same statement as in mission 1 of this series; a proof of either transfers verbatim. Contributions welcome: the finite-frontier infrastructure (existence and uniqueness of the truncated-share maximizer), Proposition 5.1 through budget-exhausting combination pricing, and Lemma 6.3.

Selected references

  • M. Babaioff, N. Nisan, I. Talgam-Cohen, Competitive Equilibrium with Indivisible Goods and Generic Budgets, arXiv:1703.08150v2, 2018; Mathematics of Operations Research 46(1), 2021. https://arxiv.org/abs/1703.08150, https://doi.org/10.1287/moor.2020.1062
  • E. Budish, The Combinatorial Assignment Problem: Approximate Competitive Equilibrium from Equal Incomes, Journal of Political Economy 119(6), 2011. https://doi.org/10.1086/664613
  • E. Segal-Halevi, Competitive Equilibrium for Almost All Incomes, Proceedings of the 17th International Conference on Autonomous Agents and Multi-Agent Systems (AAMAS), 2018, pp. 1267–1275. https://arxiv.org/abs/1705.04212
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Mathematical Physics·Captain: Lucas

Electroweak Interaction (Wikipedia) I: Tree-Level Gauge Boson MassesTextbook

Motivation

The electroweak interaction is the unified description of electromagnetism and the weak nuclear force in the Standard Model of particle physics. Glashow, Salam and Weinberg shared the 1979 Nobel Prize in Physics for this unification, and its central predictions — neutral weak currents (Gargamelle, 1973) and the massive W±W^\pmW± and Z0Z^0Z0 bosons (UA1/UA2, 1983) — have been confirmed experimentally. The algebraic core of the theory is short: an SU(2)×U(1)\mathrm{SU}(2)\times\mathrm{U}(1)SU(2)×U(1) gauge theory whose symmetry is broken by the vacuum value of a Higgs doublet, after which the neutral gauge fields are rotated by the weak mixing angle θW\theta_WθW​ into the photon and the Z0Z^0Z0, and the masses satisfy mZ=mW/cos⁡θWm_Z = m_W/\cos\theta_WmZ​=mW​/cosθW​.

This mission formalizes those tree-level algebraic facts as they are stated in the Wikipedia article Electroweak interaction (revision 1360331872), sections Formulation and Lagrangian.

Timeline (as recounted in the article). After the Wu experiment (1956) exposed parity violation, Glashow combined a chiral and an achiral symmetry and predicted a ZZZ boson; Salam and Ward (1964) proposed a massless photon and three massive gauge bosons with manually broken symmetry; Weinberg (1967) used spontaneous symmetry breaking (Englert–Brout, Higgs, Guralnik–Hagen–Kibble, 1964) and predicted rough WWW and ZZZ masses; 't Hooft (1971) proved that spontaneously broken gauge theories are renormalizable. Neutral currents were observed in 1973 and the WWW, ZZZ in 1983.

Setting

Fix the weak isospin coupling g>0g>0g>0 and the weak hypercharge coupling g′>0g'>0g′>0. The gauge fields at a spacetime point, for one Lorentz component, are real numbers W1,W2,W3W_1, W_2, W_3W1​,W2​,W3​ (weak isospin) and BBB (weak hypercharge).

  1. Weak mixing angle. θW=arctan⁡(g′/g)\theta_W = \arctan(g'/g)θW​=arctan(g′/g), the angle of the right triangle with legs ggg, g′g'g′ and hypotenuse g2+g′2\sqrt{g^2+g'^2}g2+g′2​ (the figure Weinberg's weak mixing angle in the article). The electromagnetic coupling is the altitude of that triangle, e=gg′/g2+g′2e = gg'/\sqrt{g^2+g'^2}e=gg′/g2+g′2​.
  2. Physical neutral fields. γ=cos⁡θ B+sin⁡θ W3\gamma = \cos\theta\,B + \sin\theta\,W_3γ=cosθB+sinθW3​ and Z0=−sin⁡θ B+cos⁡θ W3Z^0 = -\sin\theta\,B + \cos\theta\,W_3Z0=−sinθB+cosθW3​.
  3. Charged fields. W±=(W1∓iW2)/2W^\pm = (W_1 \mp i W_2)/\sqrt 2W±=(W1​∓iW2​)/2​.
  4. Higgs sector. The Higgs field is a complex doublet h∈C2h\in\mathbb C^2h∈C2 with ∣h∣2=∣h1∣2+∣h2∣2|h|^2 = |h_1|^2+|h_2|^2∣h∣2=∣h1​∣2+∣h2​∣2 and potential V(h)=λ (∣h∣2−v2/2)2V(h) = \lambda\,(|h|^2 - v^2/2)^2V(h)=λ(∣h∣2−v2/2)2. Its vacuum is h0=(0,v/2)h_0 = (0, v/\sqrt2)h0​=(0,v/2​).
  5. Covariant derivative. Dμ=∂μ−ig′2YBμ−ig2σjWμjD_\mu = \partial_\mu - i\tfrac{g'}{2} Y B_\mu - i \tfrac{g}{2}\sigma_j W^j_\muDμ​=∂μ​−i2g′​YBμ​−i2g​σj​Wμj​ with σj\sigma_jσj​ the Pauli matrices. On the constant vacuum the derivative term vanishes, so ∣Dμh0∣2=∣Mh0∣2|D_\mu h_0|^2 = |M h_0|^2∣Dμ​h0​∣2=∣Mh0​∣2 with M=g′2YB 1+g2(W1σ1+W2σ2+W3σ3)M = \tfrac{g'}{2}YB\,\mathbb 1 + \tfrac g2(W_1\sigma_1+W_2\sigma_2+W_3\sigma_3)M=2g′​YB1+2g​(W1​σ1​+W2​σ2​+W3​σ3​) and Y=1Y=1Y=1 for the Higgs.
  6. Charge. Q=T3+12YQ = T_3 + \tfrac12 YQ=T3​+21​Y.
  7. Masses. mW=gv/2m_W = gv/2mW​=gv/2 and mZ=g2+g′2 v/2m_Z = \sqrt{g^2+g'^2}\,v/2mZ​=g2+g′2​v/2.

Formalization targets

Goal: the gauge boson mass terms

For all real v,W1,W2,W3,Bv, W_1, W_2, W_3, Bv,W1​,W2​,W3​,B,

∣Mh0∣2=mW2 W+W−+12mZ2 (Z0)2,|M h_0|^2 = m_W^2\, W^+ W^- + \tfrac12 m_Z^2 \,(Z^0)^2 ,∣Mh0​∣2=mW2​W+W−+21​mZ2​(Z0)2,

which is the mass part mW2Wμ+W−μ+12mZ2ZμZμm_W^2 W^+_\mu W^{-\mu} + \tfrac12 m_Z^2 Z_\mu Z^\mumW2​Wμ+​W−μ+21​mZ2​Zμ​Zμ of LK\mathcal L_KLK​ in the article. The photon field γ\gammaγ does not appear: it stays massless.

Milestones

  1. The Weinberg triangle: cos⁡θW=g/g2+g′2\cos\theta_W = g/\sqrt{g^2+g'^2}cosθW​=g/g2+g′2​, sin⁡θW=g′/g2+g′2\sin\theta_W = g'/\sqrt{g^2+g'^2}sinθW​=g′/g2+g′2​.
  2. e=gsin⁡θW=g′cos⁡θWe = g\sin\theta_W = g'\cos\theta_We=gsinθW​=g′cosθW​.
  3. (γ,Z0)(\gamma, Z^0)(γ,Z0) is a rotation of (B,W3)(B, W_3)(B,W3​): it can be inverted and γ2+(Z0)2=B2+W32\gamma^2+(Z^0)^2 = B^2+W_3^2γ2+(Z0)2=B2+W32​.
  4. W−=W+‾W^- = \overline{W^+}W−=W+, W1=(W++W−)/2W_1 = (W^++W^-)/\sqrt2W1​=(W++W−)/2​, W2=i(W+−W−)/2W_2 = i(W^+-W^-)/\sqrt2W2​=i(W+−W−)/2​, W+W−=(W12+W22)/2W^+W^- = (W_1^2+W_2^2)/2W+W−=(W12​+W22​)/2.
  5. mZ=mW/cos⁡θWm_Z = m_W/\cos\theta_WmZ​=mW​/cosθW​.
  6. h0h_0h0​ minimizes the Higgs potential, and the zero set of VVV is the sphere ∣h∣2=v2/2|h|^2 = v^2/2∣h∣2=v2/2.
  7. Q=T3+12YQ = T_3 + \tfrac12 YQ=T3​+21​Y annihilates h0h_0h0​, and (for v≠0v\neq0v=0) it is the only combination aT3+b Y/2aT_3 + b\,Y/2aT3​+bY/2, up to scale, that does.
  8. The neutral-current coupling: gT3W3+g′Y2B=eQ γ+gcos⁡θW(T3−sin⁡2θW Q) Z0gT_3W_3 + g'\tfrac Y2 B = eQ\,\gamma + \frac{g}{\cos\theta_W}(T_3 - \sin^2\theta_W\,Q)\,Z^0gT3​W3​+g′2Y​B=eQγ+cosθW​g​(T3​−sin2θW​Q)Z0.

Significance

These identities are the content behind the article's statements that "the axes ... have been rotated by the angle θW\theta_WθW​", that mZ=mW/cos⁡θWm_Z = m_W/\cos\theta_WmZ​=mW​/cosθW​, that e=gsin⁡θW=g′cos⁡θWe = g\sin\theta_W = g'\cos\theta_We=gsinθW​=g′cosθW​, and that U(1)em\mathrm U(1)_{em}U(1)em​ is unbroken because it does not couple to the Higgs. The formal library produced here (Pauli matrices, the Higgs doublet, the mixing rotation, the mass formulas) can be reused by later missions on the full electroweak Lagrangian, on the Yukawa sector, or on the custodial relation ρ=mW2/(mZ2cos⁡2θW)=1\rho = m_W^2/(m_Z^2\cos^2\theta_W) = 1ρ=mW2​/(mZ2​cos2θW​)=1.

All statements are classical tree-level results. None is open; the work is to formalize them.

Difficulty

The mathematics is finite-dimensional linear algebra and trigonometry. The main pitfalls are conventions: the factor 12\tfrac1221​ in front of the Pauli matrices, the hypercharge normalization Q=T3+Y/2Q = T_3 + Y/2Q=T3​+Y/2 (so the Higgs has Y=1Y=1Y=1), and the sign conventions in the rotation matrix. The goal also requires handling complex doublets, 2\sqrt 22​ factors and the inverse trigonometric definition of θW\theta_WθW​ at the same time.

Formalization scope

All fields are real numbers at one spacetime point and for one Lorentz component; the Lorentz contraction and the kinetic (derivative) terms are not modeled. The Higgs doublet is a function Fin 2 → ℂ, and its squared norm is written out as ∣h1∣2+∣h2∣2|h_1|^2 + |h_2|^2∣h1​∣2+∣h2​∣2 (not the sup norm of the product type). The Pauli matrices are defined explicitly. The angle is θW=arctan⁡(g′/g)\theta_W = \arctan(g'/g)θW​=arctan(g′/g); with g>0g>0g>0 this agrees with the triangle. The standing convention g,g′>0g, g' > 0g,g′>0 is a hypothesis wherever θW\theta_WθW​ appears. The goal is stated as an equation in C\mathbb CC so that the product W+W−W^+W^-W+W− appears exactly as in LK\mathcal L_KLK​.

All declarations live in the namespace ElectroweakWiki.

Selected references

  • Wikipedia contributors, Electroweak interaction, revision 1360331872. https://en.wikipedia.org/w/index.php?title=Electroweak_interaction&oldid=1360331872
  • S. Weinberg, A Model of Leptons, Phys. Rev. Lett. 19 (1967) 1264. https://doi.org/10.1103/PhysRevLett.19.1264
  • D. J. Griffiths, Introduction to Elementary Particles, Wiley, 1987.
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Quantum GravityQuantum Information·Captain: Alien60

Oreshkov–Costa–Brukner 2012: Quantum Correlations with No Causal OrderResearch Paper

Motivation

In ordinary quantum mechanics, and in quantum field theory on a fixed spacetime, events happen in a definite causal order: an operation either precedes another, follows it, or the two are spacelike separated. Attempts to combine quantum theory with general relativity call this assumption into question. In general relativity the causal structure is dynamical, and a quantum theory of gravity may allow it to be indefinite. Oreshkov, Costa and Brukner (Nat. Commun. 3, 1092 (2012), arXiv:1105.4464) turned this question into a precise mathematical one. They assume that quantum mechanics holds locally in each laboratory and make no assumption about any global causal order. Within that framework they ask which correlations between two laboratories are possible. They find correlations that no definite causal order can produce: these correlations violate a causal inequality, which every causally ordered scenario satisfies.

Timeline.

  • 2005: Hardy proposes probabilistic theories with dynamic causal structure as a framework for quantum gravity (arXiv:gr-qc/0509120).
  • 2009: Chiribella, D'Ariano and Perinotti introduce quantum combs, which describe quantum networks with a fixed causal order (Phys. Rev. A 80, 022339). Chiribella, D'Ariano, Perinotti and Valiron introduce the quantum switch, a superposition of gate orders (arXiv:0912.0195, Phys. Rev. A 88, 022318 (2013)).
  • 2012: Oreshkov, Costa and Brukner define process matrices and the causal inequality psucc≤3/4p_{succ} \le 3/4psucc​≤3/4. They exhibit a four-qubit process matrix reaching psucc=(2+2)/4p_{succ} = (2+\sqrt2)/4psucc​=(2+2​)/4, and show that classical processes are always causally separable.
  • 2015–2016: Araújo et al. introduce witnesses of causal nonseparability (arXiv:1506.03776). Branciard et al. classify the simplest causal inequalities and their quantum violations (arXiv:1508.01704). Oreshkov and Giarmatzi extend causal separability to more parties (arXiv:1506.05449). Procopio et al. realize the quantum switch with photons (arXiv:1412.4006).

Setting

Alice's laboratory has an input system A1A_1A1​ and an output system A2A_2A2​, and Bob's has B1B_1B1​ and B2B_2B2​. All four are finite-dimensional, with dimensions dA1,dA2,dB1,dB2d_{A_1}, d_{A_2}, d_{B_1}, d_{B_2}dA1​​,dA2​​,dB1​​,dB2​​, and operators on A1A2B1B2A_1A_2B_1B_2A1​A2​B1​B2​ are complex matrices indexed by (a1×a2)×(b1×b2)(a_1\times a_2)\times(b_1\times b_2)(a1​×a2​)×(b1​×b2​).

A local operation of Alice is described by its Choi–Jamiołkowski (CJ) matrix MA1A2M^{A_1A_2}MA1​A2​. The operation is a completely positive trace-preserving (CPTP) map exactly when

MA1A2≥0,Tr⁡A2MA1A2=1A1.M^{A_1A_2} \ge 0, \qquad \operatorname{Tr}_{A_2} M^{A_1A_2} = \mathbb 1^{A_1}.MA1​A2​≥0,TrA2​​MA1​A2​=1A1​.

A process matrix is a matrix WA1A2B1B2W^{A_1A_2B_1B_2}WA1​A2​B1​B2​ satisfying

W≥0,Tr⁡[W (MA1A2⊗MB1B2)]=1  for all CJ matrices of CPTP mapsW \ge 0,\qquad \operatorname{Tr}\big[W\,(M^{A_1A_2}\otimes M^{B_1B_2})\big] = 1 \ \text{ for all CJ matrices of CPTP maps}W≥0,Tr[W(MA1​A2​⊗MB1​B2​)]=1  for all CJ matrices of CPTP maps

(Eqs. (4)–(5) of the source). The probability of a pair of local outcomes is P=Tr⁡[W(MA1A2⊗MB1B2)]P = \operatorname{Tr}[W(M^{A_1A_2}\otimes M^{B_1B_2})]P=Tr[W(MA1​A2​⊗MB1​B2​)] (Eq. (3)).

The task (Eq. (1)). Alice, Bob and a second bit for Bob receive independent uniform bits aaa, bbb and b′b'b′. Alice uses an instrument {MA(x∣a)}x\{M^A(x\mid a)\}_x{MA(x∣a)}x​ to produce a guess xxx, and Bob uses {MB(y∣b,b′)}y\{M^B(y\mid b,b')\}_y{MB(y∣b,b′)}y​ to produce a guess yyy. If b′=0b'=0b′=0 Bob must communicate bbb to Alice, and if b′=1b'=1b′=1 Alice must communicate aaa to Bob:

psucc=12[P(x=b∣b′=0)+P(y=a∣b′=1)].p_{succ} = \tfrac12\big[P(x=b\mid b'=0) + P(y=a\mid b'=1)\big].psucc​=21​[P(x=b∣b′=0)+P(y=a∣b′=1)].

Causal separability (Eq. (6)). A process matrix of the form 1A2⊗WA1B1B2\mathbb 1^{A_2}\otimes W^{A_1B_1B_2}1A2​⊗WA1​B1​B2​ allows no signalling from Alice to Bob, written A⪯̸BA\not\preceq BA⪯B. One of the form 1B2⊗WA1A2B1\mathbb 1^{B_2}\otimes W^{A_1A_2B_1}1B2​⊗WA1​A2​B1​ allows none from Bob to Alice. WWW is causally separable if W=q WB⪯̸A+(1−q) WA⪯̸BW = q\,W^{B\not\preceq A} + (1-q)\,W^{A\not\preceq B}W=qWB⪯A+(1−q)WA⪯B for some 0≤q≤10\le q\le 10≤q≤1.

Formalization targets

Goal: violation of the causal inequality

∃ W, {MA(x∣a)}, {MB(y∣b,b′)} on four qubits:W is a process matrix and psucc>34.\exists\, W,\ \{M^A(x\mid a)\},\ \{M^B(y\mid b,b')\} \text{ on four qubits}:\quad W \text{ is a process matrix and } p_{succ} > \tfrac34 .∃W, {MA(x∣a)}, {MB(y∣b,b′)} on four qubits:W is a process matrix and psucc​>43​.

The goal states only that a violation exists, with no hard-coded value. The specific value (2+2)/4(2+\sqrt2)/4(2+2​)/4 is a milestone.

Milestones (in source order)

  1. Eq. (2): every causally separable WWW satisfies psucc≤3/4p_{succ} \le 3/4psucc​≤3/4, for every choice of local instruments and in every finite dimension.
  2. Eq. (7): the four-qubit matrix
W=14[1+12(σzA2σzB1+σzA1σxB1σzB2)]W = \tfrac14\Big[\mathbb 1 + \tfrac{1}{\sqrt2}\big(\sigma_z^{A_2}\sigma_z^{B_1} + \sigma_z^{A_1}\sigma_x^{B_1}\sigma_z^{B_2}\big)\Big]W=41​[1+2​1​(σzA2​​σzB1​​+σzA1​​σxB1​​σzB2​​)]

is a process matrix. 3. Eq. (8): with the instruments of Eqs. (20)–(23), this WWW gives psucc=(2+2)/4p_{succ} = (2+\sqrt2)/4psucc​=(2+2​)/4, for every state ρB2\rho^{B_2}ρB2​ that Bob may prepare. 4. p. 5: the matrix of Eq. (7) is not causally separable. 5. Appendix F: every process matrix that is diagonal in a product basis (a classical process) is causally separable. 6. Appendix C, Fig. 3: for Hermitian WWW, the normalization condition (5) holds if and only if Tr⁡W=dA2dB2\operatorname{Tr}W = d_{A_2}d_{B_2}TrW=dA2​​dB2​​ and WWW has no Hilbert–Schmidt component of type A2A_2A2​, B2B_2B2​, A1A2A_1A_2A1​A2​, B1B2B_1B_2B1​B2​, A2B2A_2B_2A2​B2​, A1A2B2A_1A_2B_2A1​A2​B2​, A2B1B2A_2B_1B_2A2​B1​B2​ or A1A2B1B2A_1A_2B_1B_2A1​A2​B1​B2​. 7. Appendix E, Eq. (26): P(y∣a,b,b′=1)=12[1+(−1)y+a/2]P(y\mid a,b,b'=1) = \tfrac12\big[1 + (-1)^{y+a}/\sqrt2\big]P(y∣a,b,b′=1)=21​[1+(−1)y+a/2​], and P(x=b∣b′=0)=(2+2)/4P(x=b\mid b'=0) = (2+\sqrt2)/4P(x=b∣b′=0)=(2+2​)/4.

Significance

The result. Milestones 1 and 3 together show that quantum mechanics, applied locally in each laboratory, does not by itself imply a definite causal order. The causal inequality is a device-independent test of causal order, analogous to a Bell inequality for local realism. Milestone 5 shows that indefinite causal order disappears in the classical limit, and the source reads this as a hint that spacetime causal structure may emerge in a quantum-to-classical transition. The process-matrix framework has since become standard for indefinite causal order. Milestone 6 is the characterization that later work on witnesses and causal inequalities relies on.

Formalizing it. All seven milestones and the goal are proved in the source; none are open mathematics. This mission produces machine-checked versions in a common vocabulary: process matrices, CJ instruments, causal separability and Hilbert–Schmidt type analysis. That vocabulary can be reused for later results such as witnesses of causal nonseparability, multipartite causal separability and the quantum switch.

Status honesty. The formal statements are about matrices. Whether causal-inequality violations can occur in nature is not settled. Laboratory realizations of the quantum switch certify causal nonseparability with witnesses, not with a causal-inequality violation, and the source leaves open whether (2+2)/4(2+\sqrt2)/4(2+2​)/4 is the largest possible violation.

Difficulty

The violation itself (milestones 2, 3 and 7) is finite linear algebra on 16×1616\times1616×16 matrices, but the irrational entries 1/21/\sqrt21/2​ rule out a purely computational check. Positivity of WWW is the nontrivial part of milestone 2. The two Pauli strings in WWW anticommute, which fixes its spectrum, but this has to be turned into a positive-semidefiniteness proof.

Milestone 1 needs more than inspecting the definitions. The bound has to be shown for each no-signalling form separately and then carried through convex mixtures, with instruments of arbitrary dimension.

Milestone 4 is a non-existence statement over all decompositions. A direct search is hopeless; it follows from milestones 1 and 3.

Milestone 5 (Appendix F) is the deepest: it builds the two positive parts of the decomposition by an eigenvalue-shifting procedure.

Milestone 6 needs orthogonality computations with arbitrary Hilbert–Schmidt bases on four tensor factors.

Formalization scope

  • Representation. Finite index types, complex matrices, and Mathlib's Kronecker product ⊗ₖ with tensor order (A1×A2)×(B1×B2)(A_1\times A_2)\times(B_1\times B_2)(A1​×A2​)×(B1​×B2​). Local operations are represented directly by their CJ matrices, so the transpose in the source's CJ convention never enters the statements. Bits are Bool (false ↦ 0). Probabilities are real parts of traces, which are real whenever all inputs are positive semidefinite.
  • Definitions. These live in OCB2012_defs: partial trace ptrace₂, IsCPTP_CJ, IsProcessMatrix, prob, IsAliceInstrument, IsBobInstrument, pSucc, the no-signalling forms, IsCausallySeparable, the Pauli matrices, W7, the instruments ξ and η, the structure HSBasis and the predicate AllowedType. Density matrices come from the published PeresTerno.IsDensityMatrix.
  • Hilbert–Schmidt bases. Milestone 6 quantifies over every basis satisfying the source's conditions: σ0=1\sigma_0=\mathbb 1σ0​=1, Hermitian, traceless, and Tr⁡σμσν=d δμν\operatorname{Tr}\sigma_\mu\sigma_\nu = d\,\delta_{\mu\nu}Trσμ​σν​=dδμν​. Hermiticity matches the source's use of real coefficients.
  • Not trivial. Instruments range only over positive semidefinite CJ matrices whose outcome sum is CPTP. The goal, milestones 2–4 and milestone 7 are stated on qubits, so no hypothesis can be vacuous.
  • Out of scope. The source's derivation of Eq. (2) in Appendix A uses events in a partially ordered causal structure and a free-choice assumption, and it has no faithful matrix-level counterpart. Milestone 1 is the process-matrix form of the bound, which the source applies on p. 4. The closed-timelike-curve model of Appendix D is not formalized.
  • Contributions welcome. Reusable lemmas on partial traces of Kronecker products, positive semidefiniteness of Pauli-string combinations, and expansions in Hilbert–Schmidt bases.

Selected references

  • O. Oreshkov, F. Costa, Č. Brukner, Quantum correlations with no causal order, Nat. Commun. 3, 1092 (2012). doi:10.1038/ncomms2076, arXiv:1105.4464
  • L. Hardy, Probability theories with dynamic causal structure: a new framework for quantum gravity (2005). arXiv:gr-qc/0509120
  • G. Chiribella, G. M. D'Ariano, P. Perinotti, Theoretical framework for quantum networks, Phys. Rev. A 80, 022339 (2009). arXiv:0904.4483
  • G. Chiribella, G. M. D'Ariano, P. Perinotti, B. Valiron, Quantum computations without definite causal structure, Phys. Rev. A 88, 022318 (2013). arXiv:0912.0195
  • M. Araújo, C. Branciard, F. Costa, A. Feix, C. Giarmatzi, Č. Brukner, Witnessing causal nonseparability, New J. Phys. 17, 102001 (2015). arXiv:1506.03776
  • C. Branciard, M. Araújo, A. Feix, F. Costa, Č. Brukner, The simplest causal inequalities and their violation, New J. Phys. 18, 013008 (2016). arXiv:1508.01704
  • O. Oreshkov, C. Giarmatzi, Causal and causally separable processes, New J. Phys. 18, 093020 (2016). arXiv:1506.05449
  • L. M. Procopio et al., Experimental superposition of orders of quantum gates, Nat. Commun. 6, 7913 (2015). arXiv:1412.4006
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Number Theory·Captain: Yuxuan Xu

Irrationality of ζ(9)Open Problem

Motivation and history

The Riemann zeta function at a real number s>1s>1s>1 is the convergent series ζ(s)=∑k=1∞k−s\zeta(s)=\sum_{k=1}^{\infty}k^{-s}ζ(s)=∑k=1∞​k−s. Number theorists studying its special values distinguish between proving that a family contains irrational numbers and determining the arithmetic nature of one specified member. This mission asks for a proof that ζ(9)\zeta(9)ζ(9) is irrational. The target remains unproved in this development; the supporting results below do not close it.

Two landmarks explain the distinction:

  • 2000: Rivoal proved that infinitely many odd zeta values are irrational, through a dimension bound for their rational span. Rivoal's paper.
  • 2002; published 2004: Zudilin proved that at least one of ζ(5),ζ(7),ζ(9),ζ(11)\zeta(5),\zeta(7),\zeta(9),\zeta(11)ζ(5),ζ(7),ζ(9),ζ(11) is irrational. This disjunction does not identify ζ(9)\zeta(9)ζ(9). Zudilin's paper.
  • 2026, this development: explicit coefficient maps, weighted lattices, arithmetic estimates, and alternative constructions were assembled in research notes and source supplements. Separately, a saved 4 October audit recorded 51 supporting proofs as Accepted and public Proved. This is a dated supporting checkpoint, not an irrationality proof.

Setting

An integer linear form in the target value is b+aζ(9)b+a\zeta(9)b+aζ(9), where a,b∈Za,b\in\mathbb Za,b∈Z. It is useful for irrationality only when its actual value is nonzero and tends to zero along an infinite sequence. A pair is primitive when gcd⁡(∣a∣,∣b∣)=1\gcd(|a|,|b|)=1gcd(∣a∣,∣b∣)=1; its direction identifies (b,a)(b,a)(b,a) with (−b,−a)(-b,-a)(−b,−a).

The principal construction uses even integers n≥2n\ge2n≥2 and the rational function

Rn(t)=(n!)7∏i=1n(t−i)(t+n+i)∏j=0n(t+j)9.R_n(t)=(n!)^7 \frac{\prod_{i=1}^{n}(t-i)(t+n+i)} {\prod_{j=0}^{n}(t+j)^9}.Rn​(t)=(n!)7∏j=0n​(t+j)9∏i=1n​(t−i)(t+n+i)​.

For a polynomial W(X)=∑r=04wrXrW(X)=\sum_{r=0}^{4}w_rX^rW(X)=∑r=04​wr​Xr with rational coefficients, set un(t)=t(t+n)u_n(t)=t(t+n)un​(t)=t(t+n) and Ln(W)=∑k=1∞Rn(k)W(un(k))L_n(W)=\sum_{k=1}^{\infty}R_n(k)W(u_n(k))Ln​(W)=∑k=1∞​Rn​(k)W(un​(k)). Its actual partial fractions and harmonic sums determine rational coefficients in the exact identity

Ln(W)=Bn(W)+ρ3,n(W)ζ(3)+ρ5,n(W)ζ(5)+ρ7,n(W)ζ(7)+ρ9,n(W)ζ(9).L_n(W)=B_n(W)+\rho_{3,n}(W)\zeta(3)+\rho_{5,n}(W)\zeta(5) +\rho_{7,n}(W)\zeta(7)+\rho_{9,n}(W)\zeta(9).Ln​(W)=Bn​(W)+ρ3,n​(W)ζ(3)+ρ5,n​(W)ζ(5)+ρ7,n​(W)ζ(7)+ρ9,n​(W)ζ(9).

The coefficient map sends WWW to this ordered row of five rational coefficients. The matrix FnF_nFn​ has row rrr equal to the coefficient row of XrX^rXr, for 0≤r≤40\le r\le40≤r≤4. These are coefficients constructed from the actual rational function; their definition does not assume independence of odd zeta values. The map is bijective over Q\mathbb QQ for every even n≥2n\ge2n≥2 in the completed supporting theorem The actual five-dimensional rational coefficient map is bijective. This later theorem is separate from the dated source packages.

The integer-output lattice consists of the rational polynomial-coordinate rows

Ln={(b,0,0,0,a)Fn−1:a,b∈Z}.\mathcal L_n=\{(b,0,0,0,a)F_n^{-1}:a,b\in\mathbb Z\}.Ln​={(b,0,0,0,a)Fn−1​:a,b∈Z}.

Its weighted norm is the Euclidean norm after multiplying coordinates by (1,n2,n4,n6,n8)(1,n^2,n^4,n^6,n^8)(1,n2,n4,n6,n8). A shortest nonzero row has a primitive integer output; a fixed convention resolves ties. An integer output can have a rational polynomial preimage. Integer polynomial coefficients and their denominator cost require additional arithmetic statements.

Formalization targets

The stable goal is

ζ(9)∉Q.\boxed{\zeta(9)\notin\mathbb Q.}ζ(9)∈/Q.​

The goal imposes no chosen decay constant or prescribed construction. The coefficient-map route supplies supporting targets; a complete independent construction of nonzero integer linear forms tending to zero would also settle the goal.

The joint-margin condition J in the research notes asks for a fixed positive exponent margin on infinitely many even indices in the actual weighted-lattice and arithmetic diagnostics. It remains mathematically open. Under the written volume and transport results, it is an equivalent exit to the target and to failure of eventual fixation of the shortest primitive output direction. The stronger shape condition S is sufficient with the written volume estimate; it is not an additional necessary hurdle. Precise conditions and dependencies.

Significance

A complete proof would determine the arithmetic nature of one specified odd zeta value. The formal development also produces reusable links between rational-function coefficients, absolutely convergent series, polynomial inverse images, and primitive integer outputs.

Completed machine-checked supporting stages include harmonic-denominator clearing and stability, finite-prime arithmetic, the actual short-zero coefficient's signed lower bound and nonvanishing, and unconditional harmonic denominator rates using an actual prime-number-theorem dependency. The coefficient route has complete proofs of highest-pole identities, all nine local orders, full local-array injectivity, global partial fractions, reflection and cancellation, finite harmonic identities, absolute summability, and the exact infinite linear form. Its genuine aggregate map is bijective over rational quartics for even n≥2n\ge2n≥2, with a unique rational preimage of every rational target. The actual fifteen-coordinate connection system also has unique polynomial solutions for every n≥1n\ge1n≥1. The supporting results The actual inverse multiplier has its prescribed sum and absolute convergence and The five original connection systems have unique bounded rational solutions state these later conclusions with their exact domains.

The 7 October 2026 authenticated readback reconfirmed the 51 complete accepted supporting proofs and their public Proved statements. The irrationality goal remained Open. The three separately published explicit-matrix statements were also Open; local Matrix proofs and completed kernel-and-inverse results do not imply platform acceptance of those separate statements. These are statuses of existing supporting results, not a completion count for this new mission.

Public supplements provide independently rebuilt sources for nine complete proofs and for the later coefficient-sign and unconditional denominator-rate developments. Each package records its precise scope and standard foundational axioms. They do not contain a proof of the root goal. Nine-proof supplement, advanced source supplement, independent source-package review.

Difficulty

Small real values alone do not settle irrationality: an integer form may be exactly zero. Under a rationality assumption, the shortest primitive output can eventually follow the unique integer zero relation. The existing volume and approximation estimates do not exclude that behavior. Finite changes of direction, large matrix determinants, or a few certified small nonzero forms do not establish the required infinite assertion. Direction frontier and boundaries.

Alternative routes retain different gaps. Growing-dimensional positive Gram constructions have positive exponentially decreasing real errors but lack control of the full reduced denominators. A differentiated rational-sum construction isolates ζ(9)\zeta(9)ζ(9) but has polynomial endpoint leakage; its eightfold-zero repair removes that leakage and still needs eventual nonvanishing, the actual analytic rate, and primitive-content estimates. These are alternatives, not conditions that must all be solved. Alternative constructions and exact boundaries.

Formalization scope

The Lean goal applies Irrational to the real part of Mathlib's complex riemannZeta at 999. The coefficient construction fixes rational quartics, the output order (B,ρ3,ρ5,ρ7,ρ9)(B,\rho_3,\rho_5,\rho_7,\rho_9)(B,ρ3​,ρ5​,ρ7​,ρ9​), and even n≥2n\ge2n≥2 for the inverse and infinite identity. Connection results retain their own n≥1n\ge1n≥1 domain and regular-point hypotheses. Saturated integer kernels, positive common denominators, Smith factors, primitive normalization, weighted norms, and shortest nonzero vectors must use the actual objects in the notes. An arbitrary replacement map, zero witness, or hypothesis already asserting the required transport or infinite margin cannot discharge these targets.

Four principal formalization work packages remain:

  1. Parameter transport: complete the genuine five-output and infinite-sum transport. Proved polynomial connection systems and rational-function differences do not alone constitute this result; the proposed full output assembly is not yet a verified theorem.
  2. Integer normalization, heights, and content: prove the actual integral structures and denominator bounds. Rational bijectivity of FnF_nFn​ does not supply those arithmetic bounds.
  3. Uniform analytic estimates A: formalize the written moment asymptotics, infinite-tail bounds, and error estimates uniform in varying quartic coefficients. Elementary phase lemmas alone do not establish this package.
  4. Arithmetic volume estimates V: formalize the written prime budgets, Smith data, saturated-kernel geometry, and resulting volume asymptotics. The written volume proof does not establish J.

These four packages distinguish remaining Lean work from the separate missing mathematical input for J. Rational matrices, integer modules, formal power series, summability, asymptotic analysis, and geometry of numbers are reusable infrastructure. Faithful formalizations, independent audits, and new mathematical approaches are welcome. Written research record.

Selected references

  • T. Rivoal, La fonction zêta de Riemann prend une infinité de valeurs irrationnelles aux entiers impairs, C. R. Acad. Sci. Paris Sér. I Math. 331 (2000), 267–270. arXiv:math/0008051.
  • W. Zudilin, Arithmetic of linear forms involving odd zeta values, Journal de Théorie des Nombres de Bordeaux 16 (2004), 251–291; preprint 2002. arXiv:math/0206176.
  • Zeta(9) research notes, source, and verification records, research archive, 2 October 2026, with separately dated formal proof supplements. Public release.
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🏆Completed
Differential GeometryGeometrodynamicsMathematical Physics+2·Captain: Mazecto

Wheeler–DeWitt Equation: Superspace, Semiclassical Limit and Lattice Constraint AlgebraResearch Paper

Motivation

The Wheeler–DeWitt equation is the quantum version of the Hamiltonian constraint of general relativity. In the canonical formulation, a spacetime is described by the evolution of the metric habh_{ab}hab​ of a spatial slice, and Einstein's equations include a constraint: the Hamiltonian density vanishes at every point of space. Quantizing this constraint, as DeWitt did (Phys. Rev. 160, 1967), gives a second-order functional differential equation for a wavefunctional Ψ[h]\Psi[h]Ψ[h] with no external time parameter.

Three structural facts make the equation distinctive:

  • its kinetic term is built from an indefinite metric on the space of metrics, the DeWitt supermetric, so the equation is hyperbolic;
  • the timelike direction of that supermetric is the local volume, which serves as an intrinsic time;
  • in the limit ℏ→0\hbar\to0ℏ→0, a WKB ansatz turns the equation into the Einstein–Hamilton–Jacobi equation, recovering classical general relativity.

A fourth issue is not settled: consistency. In the continuum, the Poisson bracket of two Hamiltonian constraints is a combination of the momentum constraints, so imposing all constraints is consistent (Dirac's first-class condition). Any regularization of the quantum equation, a lattice for instance, must reproduce this. Generic lattice discretizations do not: the constraints become second class (Bander 1987; Dittrich 2008; Bahr–Dittrich 2009). Whether, and with which anomaly, the Hamiltonian-constraint commutators close as the lattice is refined was singled out as an open question by Loll (Living Rev. Rel. 1998, §2.12).

The first three facts are the standard entry points of quantum geometrodynamics, as reviewed by Kiefer (arXiv 0812.0295): Section 2 for the constraints and their quantization, eqs. (3)–(8), and Section 3 for the Hamilton–Jacobi equation, eq. (10), and the semiclassical approximation, eq. (11).

Setting

A spatial metric at a point is a symmetric positive-definite 3×33\times33×3 matrix h=(hab)h=(h_{ab})h=(hab​). Write h=det⁡h\sqrt h=\sqrt{\det h}h​=deth​. The DeWitt supermetric is

Gabcd(h)=hachbd+hadhbc−habhcd2h.G_{abcd}(h)=\frac{h_{ac}h_{bd}+h_{ad}h_{bc}-h_{ab}h_{cd}}{2\sqrt h}.Gabcd​(h)=2h​hac​hbd​+had​hbc​−hab​hcd​​.

It is a quadratic form G(p,p)=Gabcd pabpcdG(p,p)=G_{abcd}\,p^{ab}p^{cd}G(p,p)=Gabcd​pabpcd on symmetric momenta. Its inverse Gabcd=12h (hachbd+hadhbc−2habhcd)G^{abcd}=\tfrac12\sqrt h\,(h^{ac}h^{bd}+h^{ad}h^{bc}-2h^{ab}h^{cd})Gabcd=21​h​(hachbd+hadhbc−2habhcd) acts on velocities.

Space is represented by a finite set XXX of sites; this is a lattice regularization. A configuration assigns to each site xxx a matrix h(x)h(x)h(x). All nine entries are coordinates, so configuration space is R9∣X∣\mathbb{R}^{9|X|}R9∣X∣, and physical configurations are those that are symmetric and positive definite at every site. A wavefunction is a function Ψ\PsiΨ from configurations to C\mathbb{C}C. The functional derivative δ/δhab(x)\delta/\delta h_{ab}(x)δ/δhab​(x) is the partial derivative ∂ab(x)\partial_{ab}(x)∂ab​(x) with respect to the coordinate hab(x)h_{ab}(x)hab​(x), with the cell volume normalized to one.

The Wheeler–DeWitt operator at site xxx, with gravitational coupling κ\kappaκ, cosmological constant Λ\LambdaΛ, and a supplied potential R(h,x)R(h,x)R(h,x) playing the role of the spatial scalar curvature, is

H^xΨ=−2κℏ2 Gabcd(h(x)) ∂ab(x) ∂cd(x)Ψ−h(x)2κ (R−2Λ) Ψ.\widehat{\mathcal H}_x\Psi=-2\kappa\hbar^2\,G_{abcd}(h(x))\,\partial_{ab}(x)\,\partial_{cd}(x)\Psi-\frac{\sqrt{h(x)}}{2\kappa}\,(R-2\Lambda)\,\Psi .Hx​Ψ=−2κℏ2Gabcd​(h(x))∂ab​(x)∂cd​(x)Ψ−2κh(x)​​(R−2Λ)Ψ.

Write Vz(h)=−h(z)2κ(R(h,z)−2Λ)V_z(h)=-\tfrac{\sqrt{h(z)}}{2\kappa}(R(h,z)-2\Lambda)Vz​(h)=−2κh(z)​​(R(h,z)−2Λ) for the potential at site zzz. On the classical phase space of pairs (h,p)(h,p)(h,p), with pab(z)p^{ab}(z)pab(z) conjugate to hab(z)h_{ab}(z)hab​(z), the lattice constraints are

Hz(h,p)=2κ Gabcd(h(z)) pab(z) pcd(z)+Vz(h),H_z(h,p)=2\kappa\,G_{abcd}(h(z))\,p^{ab}(z)\,p^{cd}(z)+V_z(h),Hz​(h,p)=2κGabcd​(h(z))pab(z)pcd(z)+Vz​(h),

with the canonical Poisson bracket. They are first class if each bracket {Hx,Hy}\{H_x,H_y\}{Hx​,Hy​} vanishes wherever all constraints vanish.

The supermetric stands to the left of both derivatives (Kiefer, eq. (7), vacuum case; the coupling is κ=8πG\kappa=8\pi Gκ=8πG, so 2κ=16πG2\kappa=16\pi G2κ=16πG as in Kiefer's eq. (10)). The kinetic term involves only derivatives at the same site, as in the continuum; it is ultralocal. The potential may couple neighbouring sites.

Formalization targets

Milestones: geometry of the supermetric

  • Signature. G(p,p)>0G(p,p)>0G(p,p)>0 for every nonzero symmetric ppp with tr⁡(hp)=0\operatorname{tr}(hp)=0tr(hp)=0, and G(h−1,h−1)<0G(h^{-1},h^{-1})<0G(h−1,h−1)<0.
  • Inverse. GabcdGcdef pef=pabG^{abcd}G_{cdef}\,p^{ef}=p^{ab}GabcdGcdef​pef=pab for symmetric ppp.
  • Intrinsic time. With h=sh^h=s\hat hh=sh^, det⁡h^=1\det\hat h=1deth^=1 and τ=32/3 s3/4\tau=\sqrt{32/3}\,s^{3/4}τ=32/3​s3/4, the velocity form of the supermetric is −dτ2+332τ2tr⁡((h^−1dh^)2)-d\tau^2+\tfrac{3}{32}\tau^2\operatorname{tr}\big((\hat h^{-1}d\hat h)^2\big)−dτ2+323​τ2tr((h^−1dh^)2).

Milestone: the conformal sector

For Ψ=f(det⁡h(x0))\Psi=f(\sqrt{\det h(x_0)})Ψ=f(deth(x0​)​) with f∈C2f\in C^2f∈C2 and v=det⁡h(x0)v=\sqrt{\det h(x_0)}v=deth(x0​)​:

Gabcd ∂ab∂cdΨ=−38 (vf′′(v)+7f′(v)).G_{abcd}\,\partial_{ab}\partial_{cd}\Psi=-\tfrac38\,\big(vf''(v)+7f'(v)\big).Gabcd​∂ab​∂cd​Ψ=−83​(vf′′(v)+7f′(v)).

Milestone: the semiclassical limit

For every real C2C^2C2 function SSS and ℏ≠0\hbar\neq0ℏ=0:

e−iS/ℏ H^x eiS/ℏ=2κ Gabcd ∂abS ∂cdS−h2κ(R−2Λ)  −  iℏ 2κ Gabcd ∂ab∂cdS.e^{-iS/\hbar}\,\widehat{\mathcal H}_x\,e^{iS/\hbar}=2\kappa\,G_{abcd}\,\partial_{ab}S\,\partial_{cd}S-\frac{\sqrt h}{2\kappa}(R-2\Lambda)\;-\;i\hbar\,2\kappa\,G_{abcd}\,\partial_{ab}\partial_{cd}S .e−iS/ℏHx​eiS/ℏ=2κGabcd​∂ab​S∂cd​S−2κh​​(R−2Λ)−iℏ2κGabcd​∂ab​∂cd​S.

The ℏ\hbarℏ-independent part is the Einstein–Hamilton–Jacobi functional of Kiefer's eq. (10), Hamiltonian part, with SSS the eikonal of the WKB form (11) (amplitude C=1C=1C=1). This is the weakest statement exhibiting the classical limit, and it holds for every potential.

Milestone: the lattice commutator

For Ψ∈C4\Psi\in C^4Ψ∈C4 and sites x≠yx\neq yx=y:

[H^x,H^y]Ψ=−2κℏ2(Gabcd(h(x))(2 ∂abxVy ∂cdxΨ+∂abx∂cdxVy Ψ)−(x↔y)).[\widehat{\mathcal H}_x,\widehat{\mathcal H}_y]\Psi=-2\kappa\hbar^2\Big(G_{abcd}(h(x))\big(2\,\partial^{x}_{ab}V_y\,\partial^{x}_{cd}\Psi+\partial^{x}_{ab}\partial^{x}_{cd}V_y\,\Psi\big)-(x\leftrightarrow y)\Big).[Hx​,Hy​]Ψ=−2κℏ2(Gabcd​(h(x))(2∂abx​Vy​∂cdx​Ψ+∂abx​∂cdx​Vy​Ψ)−(x↔y)).

Milestone: the strong-coupling case

If every VzV_zVz​ depends only on h(z)h(z)h(z), then {Hx,Hy}=0\{H_x,H_y\}=0{Hx​,Hy​}=0 identically.

Goal: lattice constraints are second class

If the symmetric part of ∂Vy/∂hab(x)\partial V_y/\partial h_{ab}(x)∂Vy​/∂hab​(x) is nonzero at a physical hhh, for some x≠yx\neq yx=y, then there is a point of the constraint surface over hhh at which {Hx,Hy}≠0\{H_x,H_y\}\neq0{Hx​,Hy​}=0.

Every finite-difference curvature couples neighbouring sites, so the goal applies to every such discretization. It is the weakest statement that the discretized constraint algebra is inconsistent, and it holds uniformly in the discretization.

Stronger targets

  • The limit form ℏ→0\hbar\to0ℏ→0, as a Tendsto statement.
  • The same results with the Laplace–Beltrami ordering of the kinetic term on the six-dimensional fibre of symmetric matrices, and an explicit formula for the difference between the two orderings.
  • A potential realized as the scalar curvature of a smooth metric field on a coordinate patch, computed from Christoffel symbols, with its scaling law R[sh]=R[h]/sR[sh]=R[h]/sR[sh]=R[h]/s for constant s>0s>0s>0.
  • The momentum constraints (Kiefer, eq. (8)).
  • Open as far as the drafter could determine. Fix a cubic lattice of spacing ε\varepsilonε and a standard finite-difference scalar curvature. Determine the limit ε→0\varepsilon\to0ε→0 of the suitably rescaled commutator [H^x,H^y][\widehat{\mathcal H}_x,\widehat{\mathcal H}_y][Hx​,Hy​], and decide whether it reproduces the continuum Dirac algebra {H(x),H(y)}=(habHb(x)+habHb(y)) ∂aδ(x,y)\{H(x),H(y)\}=(h^{ab}H_b(x)+h^{ab}H_b(y))\,\partial_a\delta(x,y){H(x),H(y)}=(habHb​(x)+habHb​(y))∂a​δ(x,y) or leaves an anomaly. Give the anomaly explicitly if there is one. This is the metric-variable analogue of the question Loll raised.

Significance

The signature theorem is the mathematical content behind two physical facts: the hyperbolic character of the Wheeler–DeWitt equation, and the instability of the conformal mode (the "conformal factor problem" of Euclidean quantum gravity). DeWitt's cone form identifies the local volume as an intrinsic clock. On this rests the reading of the equation as a wave equation in superspace, with τ\tauτ as time. The conformal-sector reduction shows explicitly how the timelike direction appears in the operator, with the sign opposite to the traceless modes. The WKB identity is the precise sense in which the quantum constraint contains classical general relativity: its leading order is the Hamilton–Jacobi form of the Einstein constraint (Peres 1962; Kiefer, eq. (10)), and its next order is the one used in derivations of the Schrödinger equation from quantum gravity.

All of these are classical computations. The drafter knows of no machine-checked version. A formalization fixes conventions that the literature handles loosely:

  • the normalization of GabcdG_{abcd}Gabcd​;
  • the treatment of symmetric versus independent metric components;
  • the ordering of operators.

It does so with genuine derivatives in place of formal symbols.

The constraint-algebra part turns a phenomenon described qualitatively in the literature into a theorem with exact hypotheses. Lattice constraints are second class as soon as curvature couples sites, and the quantum commutator is given in closed form. It also isolates precisely what a consistent discretization would have to cancel. The continuum-limit target addresses an open question in canonical quantum gravity.

Difficulty

The supermetric statements are finite-dimensional, but none is a single computation. The signature requires a positivity argument for tr⁡((h1/2ph1/2)2)\operatorname{tr}\big((h^{1/2}ph^{1/2})^2\big)tr((h1/2ph1/2)2) on an hhh-traceless subspace. The cone form requires separating the trace part of a velocity in a non-orthonormal frame.

The analytic targets require second derivatives of compositions through the determinant and the matrix inverse. The derivative of det⁡\detdet at hhh in the direction of a single entry is det⁡h (h−1)ba\det h\,(h^{-1})_{ba}deth(h−1)ba​, and the derivative of h−1h^{-1}h−1 produces terms like h−1Eabh−1h^{-1}E_{ab}h^{-1}h−1Eab​h−1; a sign or index slip changes the constant 777. Treating the nine entries as independent coordinates, rather than the six symmetric ones, changes the numerical coefficients; the conventions below fix this.

For the constraint algebra, the quantum commutator involves up to fourth derivatives of Ψ\PsiΨ, which cancel only by the symmetry of mixed partials. The classical goal needs a point on the constraint surface where the bracket is nonzero. Each constraint fixes the value of an indefinite quadratic form in the momenta, and the bracket is linear in them, so the proof must use the Lorentzian signature to show that the bracket is not constant on that quadric.

A naive formalization that replaces ∂ab\partial_{ab}∂ab​ by an abstract linear map reduces every target to ring arithmetic, and is ruled out by the definitions.

Formalization scope

  • Definitions (module Def_WheelerDeWittSuperspace):
    • metric components as Fin 3 → Fin 3 → ℝ, so that configuration space X → Fin 3 → Fin 3 → ℝ with X a Fintype is a normed space;
    • matrices via Matrix.of;
    • ∂ab(x)\partial_{ab}(x)∂ab​(x) as fderiv ℝ Ψ h applied to the coordinate direction of hab(x)h_{ab}(x)hab​(x);
    • h\sqrt hh​ as Real.sqrt of the determinant;
    • the operator with the supermetric on the left.
  • Conventions:
    • all nine metric entries are independent coordinates, and statements that need symmetry assume it at the evaluation point (Matrix.PosDef includes symmetry);
    • lattice cell volume equal to 111;
    • vacuum (no matter term).
  • Not formalized; the potential is an interface: the potential RRR is supplied data on configurations and sites, and every target holds for all such RRR. The continuum limit of the lattice, a Hilbert-space domain for H^\widehat{\mathcal H}H, regularization of coincident derivatives in the continuum, and existence of solutions are outside the mission and must not be inferred from it.
  • Trivial cases to rule out:
    • the WKB milestone must hold for every C2C^2C2 phase SSS, not only for Ψ=0\Psi=0Ψ=0 or constant SSS;
    • the goal must exhibit a point on the full constraint surface, with every HzH_zHz​ vanishing, not merely a point where the bracket is nonzero;
    • the dependence hypothesis is on the symmetric part, because antisymmetric metric directions are invisible to GGG.
  • Phase-space convention: the bracket is the canonical one on all nine components per site. The symmetric reduction changes off-diagonal normalizations but not the first-class property.
  • Welcome contributions: the stronger targets, a matter field with its energy density, and minisuperspace reductions (e.g. homogeneous isotropic metrics h=a2δh=a^2\deltah=a2δ) derived from the operator here rather than postulated.

Selected references

  • B. S. DeWitt, Quantum Theory of Gravity. I. The Canonical Theory, Phys. Rev. 160 (1967), 1113–1148. https://doi.org/10.1103/PhysRev.160.1113
  • C. Kiefer, Quantum Geometrodynamics: whence, whither?, Gen. Relativ. Gravit. 41 (2009), 877–901. https://arxiv.org/abs/0812.0295
  • A. Peres, On Cauchy's problem in general relativity – II, Nuovo Cimento 26 (1962), 53–62. https://doi.org/10.1007/BF02754342
  • C. Kiefer, Quantum Gravity, 3rd ed., Oxford University Press (2012), Chapter 5. https://doi.org/10.1093/acprof:oso/9780199585205.001.0001
  • R. Loll, Discrete approaches to quantum gravity in four dimensions, Living Rev. Relativ. 1 (1998), 13, Section 2.12. https://arxiv.org/abs/gr-qc/9805049
  • R. Loll, On the diffeomorphism-commutators of lattice quantum gravity, Class. Quantum Grav. 15 (1998), 799–809. https://arxiv.org/abs/gr-qc/9708025
  • P. Renteln, Some results of SU(2) spinorial lattice gravity, Class. Quantum Grav. 7 (1990), 493–502.
  • M. Bander, Hamiltonian lattice gravity. Deformations of discrete manifolds, Phys. Rev. D 36 (1987), 2297. https://doi.org/10.1103/PhysRevD.36.2297
  • R. Gambini, J. Pullin, Canonical quantization of general relativity in discrete space-times, 2002. https://arxiv.org/abs/gr-qc/0206055
  • B. Dittrich, Diffeomorphism symmetry in quantum gravity models, 2008. https://arxiv.org/abs/0810.3594
  • B. Bahr, B. Dittrich, (Broken) Gauge symmetries and constraints in Regge calculus, 2009. https://arxiv.org/abs/0905.1670
  • C. J. Isham, Some quantum field theory aspects of the superspace quantization of general relativity, Proc. R. Soc. Lond. A 351 (1976), 209.
  • K. Pilati, Strong-coupling quantum gravity. I. Solution in a particular gauge, Phys. Rev. D 26 (1982), 2645. https://doi.org/10.1103/PhysRevD.26.2645
  • H. W. Hamber, R. M. Williams, Discrete Wheeler–DeWitt equation, 2011. https://arxiv.org/abs/1109.2530
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Differential GeometryMathematical Physics·Captain: Lucas

No-Hair Conjecture: Uniqueness of Stationary Kerr–Newman Black HolesOpen Problem

Motivation

General relativity predicts that a black hole, once it has settled down after collapse, retains almost no memory of the matter that formed it. The no-hair theorem, also called the black hole uniqueness theorem, states that all stationary black-hole solutions of the Einstein–Maxwell equations are completely characterized by three externally observable parameters: mass, angular momentum and electric charge; all other information ("hair") disappears behind the event horizon. The phrase "black holes have no hair" was popularized by John Archibald Wheeler. Its observational content is tested in gravitational-wave ringdown signals and in black-hole imaging.

Despite its name, there is no rigorous proof of the general statement: mathematicians refer to it as the no-hair conjecture.

Timeline.

  • 1967 — W. Israel proves uniqueness of the Schwarzschild metric among static vacuum black holes (Phys. Rev. 164, 1776).
  • 1968 — Israel extends this to static electrovacuum black holes, obtaining Reissner–Nordström (Commun. Math. Phys. 8, 245).
  • 1971 — B. Carter shows that an axisymmetric vacuum black hole has only two degrees of freedom (Phys. Rev. Lett. 26, 331); D. C. Robinson later completes uniqueness of Kerr.
  • 1970s — S. Hawking's rigidity theorem, combined with Carter and Robinson, yields uniqueness of Kerr in vacuum under the additional hypotheses of non-degenerate horizons and real analyticity of spacetime.
  • 2007 — extension to positive cosmological constant (Bhattacharya–Lahiri, arXiv:gr-qc/0702006).

Counterexamples are known in dimensions above four, for non-abelian Yang–Mills fields and for some non-minimally coupled scalar fields; this mission concerns only the four-dimensional Einstein–Maxwell theory with zero cosmological constant.

Setting

A spacetime is a smooth 4-manifold MMM with a Lorentzian metric ggg of signature (−,+,+,+)(-,+,+,+)(−,+,+,+), an electromagnetic field FFF (a 2-form) and a time orientation TTT. The pair (g,F)(g,F)(g,F) is electrovacuum if, in geometrized Gaussian units,

Gμν=2(FμαFνα−14gμνFαβFαβ),∇μFμν=0,dF=0.G_{\mu\nu}=2\Big(F_{\mu\alpha}F_\nu{}^\alpha-\tfrac14g_{\mu\nu}F_{\alpha\beta}F^{\alpha\beta}\Big),\qquad\nabla_\mu F^{\mu\nu}=0,\qquad dF=0 .Gμν​=2(Fμα​Fν​α−41​gμν​Fαβ​Fαβ),∇μ​Fμν=0,dF=0.

The spacetime is stationary if a one-parameter group φt\varphi_tφt​ of isometries preserves FFF, and it has a stationary asymptotically flat end MextM_{\rm ext}Mext​ if coordinates (t,x⃗)(t,\vec x)(t,x), ∣x⃗∣>R|\vec x|>R∣x∣>R, cover an open set on which φt\varphi_tφt​ is the time translation and gμν−ημν=O(1/∣x⃗∣)g_{\mu\nu}-\eta_{\mu\nu}=O(1/|\vec x|)gμν​−ημν​=O(1/∣x∣), ∂g=O(1/∣x⃗∣2)\partial g=O(1/|\vec x|^2)∂g=O(1/∣x∣2), F=O(1/∣x⃗∣2)F=O(1/|\vec x|^2)F=O(1/∣x∣2).

With I±I^\pmI± the chronological future and past, the domain of outer communications is ⟨⟨Mext⟩⟩=I+(Mext)∩I−(Mext)\langle\langle M_{\rm ext}\rangle\rangle=I^+(M_{\rm ext})\cap I^-(M_{\rm ext})⟨⟨Mext​⟩⟩=I+(Mext​)∩I−(Mext​), the black-hole region is M∖I−(Mext)M\setminus I^-(M_{\rm ext})M∖I−(Mext​) and the future event horizon is ∂I−(Mext)\partial I^-(M_{\rm ext})∂I−(Mext​).

The Kerr–Newman family, in Kerr–Schild coordinates, is gKN=η+f k⊗kg^{KN}=\eta+f\,k\otimes kgKN=η+fk⊗k with

f=r2(2mr−e2)r4+a2z2,k=(1,rx+ayr2+a2,ry−axr2+a2,zr),x2+y2r2+a2+z2r2=1,f=\frac{r^2(2mr-e^2)}{r^4+a^2z^2},\qquad k=\Big(1,\frac{rx+ay}{r^2+a^2},\frac{ry-ax}{r^2+a^2},\frac zr\Big),\qquad \frac{x^2+y^2}{r^2+a^2}+\frac{z^2}{r^2}=1,f=r4+a2z2r2(2mr−e2)​,k=(1,r2+a2rx+ay​,r2+a2ry−ax​,rz​),r2+a2x2+y2​+r2z2​=1,

with potential A=er3r4+a2z2kA=\frac{er^3}{r^4+a^2z^2}kA=r4+a2z2er3​k. For m>0m>0m>0, a2+e2≤m2a^2+e^2\le m^2a2+e2≤m2 its domain of outer communications is {r>r+}\{r>r_+\}{r>r+​}, r+=m+m2−a2−e2r_+=m+\sqrt{m^2-a^2-e^2}r+​=m+m2−a2−e2​.

Formalization targets

Goal: the no-hair conjecture

Under the standing hypotheses (smooth electrovacuum, stationary, asymptotically flat end, globally hyperbolic ⟨⟨Mext⟩⟩\langle\langle M_{\rm ext}\rangle\rangle⟨⟨Mext​⟩⟩, nonempty black-hole region, connected event horizon), there are m>0m>0m>0, aaa, eee with a2+e2≤m2a^2+e^2\le m^2a2+e2≤m2, an angle β\betaβ and a diffeomorphism Ψ\PsiΨ with

Ψ:{r>r+}→≅⟨⟨Mext⟩⟩,Ψ∗g=gm,a,eKN,Ψ∗F=cos⁡β FKN+sin⁡β ⋆FKN.\Psi:\{r>r_+\}\xrightarrow{\cong}\langle\langle M_{\rm ext}\rangle\rangle,\qquad\Psi^*g=g^{KN}_{m,a,e},\qquad\Psi^*F=\cos\beta\,F^{KN}+\sin\beta\,\star F^{KN}.Ψ:{r>r+​}≅​⟨⟨Mext​⟩⟩,Ψ∗g=gm,a,eKN​,Ψ∗F=cosβFKN+sinβ⋆FKN.

Milestones

  1. The Kerr–Newman metric solves the Einstein–Maxwell equations where r>0r>0r>0.
  2. Kerr–Newman black holes satisfy the standing hypotheses (the goal is not vacuous).
  3. Israel 1967: static vacuum ⇒\Rightarrow⇒ Schwarzschild (a=e=0a=e=0a=e=0).
  4. Israel 1968: static electrovacuum ⇒\Rightarrow⇒ Reissner–Nordström (a=0a=0a=0).
  5. Carter 1971 / Robinson: axisymmetric vacuum ⇒\Rightarrow⇒ Kerr (e=0e=0e=0).
  6. Hawking–Carter–Robinson: analytic vacuum with non-degenerate horizon ⇒\Rightarrow⇒ Kerr.
  7. Frame normalization: a Lorentz boost takes a timelike 4-momentum to rest, ΛP=(−P2,0,0,0)\Lambda P=(\sqrt{-P^2},0,0,0)ΛP=(−P2​,0,0,0).
  8. Frame normalization: a rotation aligns the spin, RJ=(0,0,∣J∣)RJ=(0,0,|J|)RJ=(0,0,∣J∣).

Significance

A proof of the goal would establish that the Kerr–Newman metrics exhaust the stationary, asymptotically flat electrovacuum black holes with connected horizon, which is the mathematical basis for treating astrophysical black holes as described by three numbers. It would also remove the analyticity and non-degeneracy hypotheses from the known vacuum results.

No machine-checked proof of any statement in this mission is known. Milestones 1, 7 and 8 are classical computations; milestones 3–6 are published theorems whose proofs rely on substantial Lorentzian geometry and elliptic PDE; the goal is open.

Difficulty

Uniqueness proofs reduce the problem to an elliptic boundary-value problem on the orbit space once enough symmetry is available. In the general stationary case the extra axial symmetry is not known to exist: Hawking's rigidity argument produces it only for analytic metrics, because it extends a Killing field off the horizon by analytic continuation. Without analyticity, unique continuation for the Killing equation across the horizon is the obstruction. Degenerate (extremal) horizons further break arguments that rely on a bifurcation surface.

Formalization scope

Spacetimes are Mathlib smooth manifolds modelled on EuclideanSpace ℝ (Fin 4); the metric and field are fields of continuous bilinear forms on tangent spaces, and curvature and field equations are imposed through components in every chart. Causal sets use C1C^1C1 curves parametrized by [0,1][0,1][0,1]. The Kerr–Newman comparison spacetime is the region {r>r+}\{r>r_+\}{r>r+​} of Kerr–Schild coordinate space with the explicit metric. Magnetic charge is accommodated by the duality angle β\betaβ.

The hypotheses are not vacuous: milestone 2 asserts that every Kerr–Newman black hole satisfies them. The connected-horizon hypothesis excludes the static multi-black-hole Majumdar–Papapetrou solutions, which would otherwise contradict the goal.

Needed infrastructure: Levi-Civita connection and curvature on manifolds, causal theory (global hyperbolicity, Cauchy surfaces), Killing fields and their flows, and the elliptic theory of harmonic maps used in uniqueness proofs. Contributions on any of these, and on milestones 1, 7 and 8, are welcome.

Selected references

  • Wikipedia, No-hair theorem, revision 1353599195, https://en.wikipedia.org/w/index.php?title=No-hair_theorem&oldid=1353599195
  • W. Israel, Event Horizons in Static Vacuum Space-Times, Phys. Rev. 164 (1967) 1776, https://doi.org/10.1103/PhysRev.164.1776
  • W. Israel, Event horizons in static electrovac space-times, Commun. Math. Phys. 8 (1968) 245, https://doi.org/10.1007/BF01645859
  • B. Carter, Axisymmetric Black Hole Has Only Two Degrees of Freedom, Phys. Rev. Lett. 26 (1971) 331, https://doi.org/10.1103/PhysRevLett.26.331
  • S. Bhattacharya, A. Lahiri, No hair theorems for positive Λ, Phys. Rev. Lett. 99 (2007) 201101, https://arxiv.org/abs/gr-qc/0702006
39 thms3 active usersReviewed
🏆Completed
CombinatoricsComplexity TheoryLinear Optimization+1·Captain: mikedeng1

Promise Constraint Satisfaction: Algebraic Structure and a Symmetric Boolean Dichotomy 2: The LP Algorithm Decides PCSPs with Majority or Alternating-Threshold Polymorphisms of All Odd AritiesResearch Paper

Motivation

A constraint satisfaction problem (CSP) asks whether variables can be assigned values so that every constraint of a given instance holds. Feder and Vardi conjectured, and Bulatov and Zhuk proved in 2017, that every CSP over a finite set of relations is either polynomial-time solvable or NP-complete, and that the answer is governed by the polymorphisms of the relations: the functions that map tuples of satisfying assignments, coordinate by coordinate, to a satisfying assignment.

A promise CSP (PCSP) relaxes the question. Each constraint comes as a pair of relations P⊆QP \subseteq QP⊆Q; the input is promised to be satisfiable with every constraint read as PPP, or unsatisfiable even with every constraint read as QQQ, and the task is to tell which. Approximate graph colouring ("is this 3-colourable graph 100-colourable?") and (2+ε)(2+\varepsilon)(2+ε)-SAT are of this kind. Austrin, Guruswami and Håstad (2017, doi:10.1137/15M1006507) showed that (2+ε)(2+\varepsilon)(2+ε)-SAT is NP-hard via polymorphisms; Brakensiek and Guruswami extended the polymorphism view to general Boolean PCSPs and proved a dichotomy for symmetric Boolean families (arXiv:1704.01937v2, SODA 2018, SIAM J. Comput. 2021). Later work by Barto, Bulín, Krokhin and Opršal (arXiv:1811.00970) built the general algebraic theory of PCSPs on this foundation.

This mission takes one ingredient of the dichotomy: the tractable side for two polymorphism families that have no counterpart among tractable CSPs, the Majority and the Alternating-Threshold functions. The paper solves both with the same linear programming test.

Setting

The domain is {0,1}\{0,1\}{0,1}. A finite family of promise relations is Γ={(PR,QR):R∈τ}\Gamma = \{(P_R, Q_R) : R \in \tau\}Γ={(PR​,QR​):R∈τ}, with τ\tauτ finite and PR⊆QR⊆{0,1}kRP_R \subseteq Q_R \subseteq \{0,1\}^{k_R}PR​⊆QR​⊆{0,1}kR​. An instance Ψ=(ΨP,ΨQ)\Psi = (\Psi_P, \Psi_Q)Ψ=(ΨP​,ΨQ​) has variables x1,…,xnx_1, \dots, x_nx1​,…,xn​ and clauses Rj(xj1,…,xjk)R_j(x_{j_1}, \dots, x_{j_k})Rj​(xj1​​,…,xjk​​); a variable may occur several times in a clause. ΨP\Psi_PΨP​ reads each clause with PRjP_{R_j}PRj​​, and ΨQ\Psi_QΨQ​ with QRjQ_{R_j}QRj​​. Since P⊆QP \subseteq QP⊆Q, satisfiability of ΨP\Psi_PΨP​ implies that of ΨQ\Psi_QΨQ​.

A function f:{0,1}L→{0,1}f : \{0,1\}^L \to \{0,1\}f:{0,1}L→{0,1} is a polymorphism of Γ\GammaΓ if for every RRR and all x(1),…,x(L)∈PRx^{(1)}, \dots, x^{(L)} \in P_Rx(1),…,x(L)∈PR​ the tuple (f(x1(1),…,x1(L)),…,f(xk(1),…,xk(L)))\big(f(x^{(1)}_1, \dots, x^{(L)}_1), \dots, f(x^{(1)}_k, \dots, x^{(L)}_k)\big)(f(x1(1)​,…,x1(L)​),…,f(xk(1)​,…,xk(L)​)) lies in QRQ_RQR​. For odd LLL,

MajL(x)=1  ⟺  ∑i=1Lxi>L2,ATL(x)=1  ⟺  ∑i=1L(−1)i−1xi>0.\mathrm{Maj}_L(x) = 1 \iff \sum_{i=1}^L x_i > \frac L2, \qquad \mathrm{AT}_L(x) = 1 \iff \sum_{i=1}^L (-1)^{i-1} x_i > 0 .MajL​(x)=1⟺i=1∑L​xi​>2L​,ATL​(x)=1⟺i=1∑L​(−1)i−1xi​>0.

The LP relaxation of Ψ\PsiΨ has one unknown vj∈[0,1]v_j \in [0,1]vj​∈[0,1] per variable, and for every clause Rj(xj1,…,xjk)R_j(x_{j_1}, \dots, x_{j_k})Rj​(xj1​​,…,xjk​​) of ΨP\Psi_PΨP​ it requires (vj1,…,vjk)(v_{j_1}, \dots, v_{j_k})(vj1​​,…,vjk​​) to lie in the convex hull of PRjP_{R_j}PRj​​. The §3.2 algorithm loops over the variables: it fixes vj=0v_j = 0vj​=0 and re-solves the LP, then, if that is infeasible, fixes vj=1v_j = 1vj​=1 and re-solves, and outputs "unsatisfiable" if both are infeasible. If every variable passes, it outputs "satisfiable". In Lean the answer is the predicate LPAlgAccepts 𝔸 X: the LP is feasible and, for each jjj, it has a solution with vj=0v_j = 0vj​=0 or one with vj=1v_j = 1vj​=1.

Formalization targets

Goal: correctness of the §3.2 algorithm

If MajL∈Pol(Γ)\mathrm{Maj}_L \in \mathrm{Pol}(\Gamma)MajL​∈Pol(Γ) for every odd LLL, or ATL∈Pol(Γ)\mathrm{AT}_L \in \mathrm{Pol}(\Gamma)ATL​∈Pol(Γ) for every odd LLL, then for every instance Ψ\PsiΨ

ΨP satisfiable  ⟹  LPAlgAccepts(Ψ)  ⟹  ΨQ satisfiable.\Psi_P \text{ satisfiable} \;\Longrightarrow\; \texttt{LPAlgAccepts}(\Psi) \;\Longrightarrow\; \Psi_Q \text{ satisfiable}.ΨP​ satisfiable⟹LPAlgAccepts(Ψ)⟹ΨQ​ satisfiable.

No symmetry of the relations is assumed.

Milestones, in the order of the proof (pp. 14–15)

  1. Completeness. If ΨP\Psi_PΨP​ is satisfiable, the algorithm accepts; no polymorphism is needed.
  2. Convexity. A convex combination of LP solutions is an LP solution.
  3. Case 1 claim. If M∈([0,1]∩Q)n×nM \in ([0,1]\cap\mathbb Q)^{n\times n}M∈([0,1]∩Q)n×n has Mii∈{0,1}M_{ii} \in \{0,1\}Mii​∈{0,1}, some rational probability vector vvv has (Mv)i≠1/2(Mv)_i \ne 1/2(Mv)i​=1/2 for all iii.
  4. Case 1 rounding. With MajL\mathrm{Maj}_LMajL​ for all odd LLL, an LP solution www with no coordinate 1/21/21/2 rounds to a satisfying assignment xi∗=⌊wi⌉x^*_i = \lfloor w_i \rceilxi∗​=⌊wi​⌉ of ΨQ\Psi_QΨQ​.
  5. Case 2 perturbation. For such MMM and any rational w^\hat ww^, some vvv has (Mv)i≠w^i(Mv)_i \ne \hat w_i(Mv)i​=w^i​ wherever w^i∉{0,1}\hat w_i \notin \{0,1\}w^i​∈/{0,1}.
  6. Case 2 rounding. With ATL\mathrm{AT}_LATL​ for all odd LLL, two LP solutions w,w^w, \hat ww,w^ that agree only where w^i∈{0,1}\hat w_i \in \{0,1\}w^i​∈{0,1} give the satisfying assignment xi∗=[wi>w^i or wi=w^i=1]x^*_i = [w_i > \hat w_i \text{ or } w_i = \hat w_i = 1]xi∗​=[wi​>w^i​ or wi​=w^i​=1] of ΨQ\Psi_QΨQ​.

Significance

The theorem shows that the Majority and Alternating-Threshold cases of Theorem 3.2 are tractable. Since Γ\GammaΓ is fixed, the LP has size linear in the instance, so linear programming decides PCSP(Γ)\mathrm{PCSP}(\Gamma)PCSP(Γ) in polynomial time. Unlike the Zero, One, AND, OR and Parity cases of §3.1, these families cannot be handled by sandwiching a tractable CSP between PPP and QQQ: footnote 12 of the paper observes that the closure of {MajL}\{\mathrm{Maj}_L\}{MajL​} or {ATL}\{\mathrm{AT}_L\}{ATL​} under identification of variables is not a clone. The tractable half of the paper's symmetric Boolean dichotomy (Theorem 2.16) depends on this result. Later work replaced this LP by the Basic LP and BLP+Affine relaxations (Brakensiek–Guruswami 2019, Barto et al. 2021).

The result is proved in the paper; to our knowledge it has no machine-checked proof. The formal content is a finite-dimensional rational convexity argument plus a counting argument on columns of polymorphism inputs. Related platform work: the published PCSPBLPAff.Symmetric.theorem_2 and theorem_3 concern the BLP+Affine algorithm with symmetric or block-symmetric polymorphisms. That is a different relaxation, and ATL\mathrm{AT}_LATL​ is not symmetric.

Difficulty

Completeness is immediate. Soundness is where the difficulty lies. The obvious approach, rounding an arbitrary LP solution, fails. For Majority, a coordinate equal to 1/21/21/2 has no nearest integer, and the LP may admit no solution without such coordinates unless one uses the per-variable solutions the algorithm found. For Alternating-Threshold, there is no fixed threshold at all, and a single LP solution gives no rule for rounding a fractional coordinate. Two further points need care. Getting from a fractional point back to a polymorphism application needs a polymorphism of an arity that depends on the denominators of the hull weights, so a single fixed arity does not suffice. In the Alternating-Threshold case, as printed, the paper pads the inputs with an arbitrary point of PPP, and that step fails at coordinates where both solutions equal 000 or 111; the padding point has to come from the support of the hull weights.

Formalization scope

The domain {0,1}\{0,1\}{0,1} is Bool. Γ\GammaΓ is a pair 𝔸 𝔹 : RelStruct τ ar Bool with [Fintype τ] and 𝔸.rel R ⊆ 𝔹.rel R, and instances, satisfiability and polymorphisms come from the published PCSPBLPAff_Symmetric_Setting. Coordinates are 0-based (Fin L), so the sign of ATL\mathrm{AT}_LATL​ is (−1)i(-1)^i(−1)i. The LP is stated over Q\mathbb QQ; an LP with rational data is feasible over R\mathbb RR exactly when it is feasible over Q\mathbb QQ. The hull condition uses PRP_RPR​, never QRQ_RQR​. The acceptance predicate also requires the LP itself to be feasible, which matters only for instances without variables. The hypothesis is a disjunction of two universal statements ("MajL\mathrm{Maj}_LMajL​ for all odd LLL, or ATL\mathrm{AT}_LATL​ for all odd LLL"), not "for every odd LLL, one of the two". A formalization that drops the hull constraint, replaces PPP by QQQ in the LP, or lets the acceptance predicate be satisfied without solving the LP would make the theorem trivial or different, and is ruled out by the definitions here.

Out of scope: polynomial running time and the printed conclusion "PCSP(Γ) is polynomial-time tractable" of Theorem 3.2; the polynomial-time solvability of linear programs; the Zero/One/AND/OR/Parity cases (Lemma 3.1, which invokes Schaefer's theorem); and the non-idempotent ("anti-") cases, which go through the reduction of Lemma 2.13(2). The Remark on p. 15 says the algorithm decides but does not find a solution. Only the decision is formalized.

Infrastructure needed: finite convex combinations over Q\mathbb QQ, a perturbation lemma for avoiding finitely many hyperplanes in the rational simplex, and counting identities for MajL\mathrm{Maj}_LMajL​ and ATL\mathrm{AT}_LATL​ on block inputs. The perturbation lemma and the counting identities are reusable beyond this mission. Proofs of any milestone, and alternative arguments (e.g. via the affine-hull algorithm in the Remark on p. 14), are welcome.

Selected references

  • J. Brakensiek, V. Guruswami, Promise Constraint Satisfaction: Algebraic Structure and a Symmetric Boolean Dichotomy, arXiv:1704.01937v2, 2021; SIAM J. Comput. 50(6), 2021. https://arxiv.org/abs/1704.01937v2
  • P. Austrin, V. Guruswami, J. Håstad, (2+ε)-Sat Is NP-Hard, SIAM J. Comput. 46(5), 2017. https://doi.org/10.1137/15M1006507
  • L. Barto, J. Bulín, A. Krokhin, J. Opršal, Algebraic Approach to Promise Constraint Satisfaction, J. ACM 68(4), 2021. https://arxiv.org/abs/1811.00970
  • J. Brakensiek, V. Guruswami, An Algorithmic Blend of LPs and Ring Equations for Promise CSPs, SODA 2019. https://arxiv.org/abs/1807.05194
  • T. J. Schaefer, The Complexity of Satisfiability Problems, STOC 1978. https://doi.org/10.1145/800133.804350
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Mathematical Physics·Captain: Lucas

Naculich 2020: Regge colour basis of the four-gluon amplitude and the all-loop coefficient B_ℓℓResearch Paper

Motivation

At high energies (s≫−ts\gg -ts≫−t, the Regge limit) scattering amplitudes of gauge theories simplify and organise into towers of logarithms log⁡∣s/t∣\log|s/t|log∣s/t∣. For the four-gluon amplitude of N=4\mathcal N=4N=4 super-Yang–Mills theory with gauge group SU(N)SU(N)SU(N), the colour structure is what makes the nonplanar (subleading in 1/N1/N1/N) amplitude hard to control. Naculich (2020) builds a basis of colour factors CikC_{ik}Cik​ adapted to the Regge limit at every loop order, writes the ℓ\ellℓ-loop amplitude in that basis, and uses one of its coefficients, Bℓℓ(ℓ)B^{(\ell)}_{\ell\ell}Bℓℓ(ℓ)​, to motivate a conjectured all-loop relation with the Regge limit of the N=8\mathcal N=8N=8 supergravity four-graviton amplitude. The physics conjecture itself is not a mathematical statement; what is exact and checkable is the colour algebra underlying it — finite-dimensional linear algebra over polynomials in NNN.

Setting

Trace basis. Four-gluon colour factors are expanded in six single and double traces c[1],…,c[6]c[1],\dots,c[6]c[1],…,c[6] of fundamental generators (eq. (2.1)). A colour vector is a column v=(v1,…,v6)v=(v_1,\dots,v_6)v=(v1​,…,v6​) of polynomials in NNN, with complex coefficients.

Colour operators. The ttt-channel Casimir Tt2\mathbf T_t^2Tt2​ and the crossing-odd combination Ts−u2=12(Ts2−Tu2)\mathbf T_{s-u}^2=\tfrac12(\mathbf T_s^2-\mathbf T_u^2)Ts−u2​=21​(Ts2​−Tu2​) act on colour vectors as the explicit 6×66\times66×6 matrices of eq. (4.15) (entries in Z[12][N]\mathbb Z[\tfrac12][N]Z[21​][N]). The tree-level ttt-channel colour factor is C00=c[1]−c[3]C_{00}=c[1]-c[3]C00​=c[1]−c[3]. Crossing (exchange of legs 2 and 3) is the permutation PPP: c[1]↔c[3]c[1]\leftrightarrow c[3]c[1]↔c[3], c[4]↔c[6]c[4]\leftrightarrow c[6]c[4]↔c[6].

Regge colour factors. With [A,B]=AB−BA[A,B]=AB-BA[A,B]=AB−BA,

Cii=(Ts−u2)iC00,Ci1=[Tt2,[Tt2,…,[Tt2,Ts−u2]⋯ ]]C00,Ci,i−1=[Ts−u2,…,[Ts−u2,[Tt2,Ts−u2]]⋯ ]C00,C_{ii}=(\mathbf T_{s-u}^2)^iC_{00},\qquad C_{i1}=[\mathbf T_t^2,[\mathbf T_t^2,\dots,[\mathbf T_t^2,\mathbf T_{s-u}^2]\cdots]]C_{00},\qquad C_{i,i-1}=[\mathbf T_{s-u}^2,\dots,[\mathbf T_{s-u}^2,[\mathbf T_t^2,\mathbf T_{s-u}^2]]\cdots]C_{00},Cii​=(Ts−u2​)iC00​,Ci1​=[Tt2​,[Tt2​,…,[Tt2​,Ts−u2​]⋯]]C00​,Ci,i−1​=[Ts−u2​,…,[Ts−u2​,[Tt2​,Ts−u2​]]⋯]C00​,

each with exactly iii operators. The admissible pairs are (0,0)(0,0)(0,0), (1,1)(1,1)(1,1), (2,1),(2,2)(2,1),(2,2)(2,1),(2,2) and (i,1),(i,i−1),(i,i)(i,1),(i,i-1),(i,i)(i,1),(i,i−1),(i,i) for i≥3i\ge3i≥3.

Extended trace basis. At ℓ\ellℓ loops, tλ+6k(ℓ)=Nℓ−2kc[λ]t^{(\ell)}_{\lambda+6k}=N^{\ell-2k}c[\lambda]tλ+6k(ℓ)​=Nℓ−2kc[λ] for λ=1,2,3\lambda=1,2,3λ=1,2,3 and Nℓ−2k−1c[λ]N^{\ell-2k-1}c[\lambda]Nℓ−2k−1c[λ] for λ=4,5,6\lambda=4,5,6λ=4,5,6, giving 3ℓ+33\ell+33ℓ+3 elements (eq. (2.3)). The colour-ordered amplitudes Aλ(ℓ)A^{(\ell)}_\lambdaAλ(ℓ)​ of an amplitude are its coordinates in this basis (eq. (2.4)).

Regge-basis amplitude. Eq. (4.24):

A(ℓ)=A1(0)a~ℓ∑i=0ℓ∑kBik(ℓ) Nℓ−iCik.\mathcal A^{(\ell)}=A_1^{(0)}\tilde a^\ell\sum_{i=0}^{\ell}\sum_{k}B^{(\ell)}_{ik}\,N^{\ell-i}C_{ik}.A(ℓ)=A1(0)​a~ℓi=0∑ℓ​k∑​Bik(ℓ)​Nℓ−iCik​.

Null vectors. Four vectors per loop order ℓ≥2\ell\ge2ℓ≥2 (eqs. (2.10), (2.12), extended by prepending zeros) encode the SU(N)SU(N)SU(N) group-theory relations among the Aλ(ℓ)A^{(\ell)}_\lambdaAλ(ℓ)​.

Formalization targets

Goal: the all-loop coefficient Bℓℓ(ℓ)B^{(\ell)}_{\ell\ell}Bℓℓ(ℓ)​ (eqs. (4.26)–(4.27))

For every even ℓ\ellℓ,

A1(0)a~ℓ Bℓℓ(ℓ)=12⋅3ℓ/2(A3ℓ+1(ℓ)−A3ℓ+3(ℓ)),A_1^{(0)}\tilde a^\ell\,B^{(\ell)}_{\ell\ell}=\frac{1}{2\cdot3^{\ell/2}}\Big(A^{(\ell)}_{3\ell+1}-A^{(\ell)}_{3\ell+3}\Big),A1(0)​a~ℓBℓℓ(ℓ)​=2⋅3ℓ/21​(A3ℓ+1(ℓ)​−A3ℓ+3(ℓ)​),

and for ℓ=1\ell=1ℓ=1, A1(0)a~ B11(1)=−(A1(1)+A3(1))A_1^{(0)}\tilde a\,B^{(1)}_{11}=-(A^{(1)}_1+A^{(1)}_3)A1(0)​a~B11(1)​=−(A1(1)​+A3(1)​). The paper obtains the even-ℓ\ellℓ formula by guessing from explicit results through ℓ=9\ell=9ℓ=9; a proof for all ℓ\ellℓ is not given there.

Milestones

  1. Tt2C00=NC00\mathbf T_t^2C_{00}=NC_{00}Tt2​C00​=NC00​ (eqs. (4.2), (4.7)).
  2. Crossing parity: PTt2P=Tt2P\mathbf T_t^2P=\mathbf T_t^2PTt2​P=Tt2​, PTs−u2P=−Ts−u2P\mathbf T_{s-u}^2P=-\mathbf T_{s-u}^2PTs−u2​P=−Ts−u2​, PC00=−C00PC_{00}=-C_{00}PC00​=−C00​ (eqs. (3.7), (4.7)).
  3. Signature: PCik=(−1)k+1CikPC_{ik}=(-1)^{k+1}C_{ik}PCik​=(−1)k+1Cik​ for every admissible (i,k)(i,k)(i,k) (Sec. 4.4).
  4. Nℓ−iCikN^{\ell-i}C_{ik}Nℓ−iCik​ expands in t1(ℓ),…,t3ℓ+3(ℓ)t^{(\ell)}_1,\dots,t^{(\ell)}_{3\ell+3}t1(ℓ)​,…,t3ℓ+3(ℓ)​ (eqs. (2.3), (4.24)).
  5. Explicit components through three loops (eqs. (4.16), (4.20)).
  6. Explicit coefficients Bik(2)B^{(2)}_{ik}Bik(2)​, Bik(3)B^{(3)}_{ik}Bik(3)​ (eqs. (4.18), (4.22)).
  7. The Regge colour factors satisfy the four null-vector constraints and have no t2(ℓ)t^{(\ell)}_2t2(ℓ)​ component, for all ℓ≥2\ell\ge2ℓ≥2.
  8. The Regge colour factors are linearly independent, and for ℓ≥2\ell\ge2ℓ≥2 span all constrained Regge-limit amplitudes (the "basis" claim of Sec. 4).

Significance

The result. Eq. (4.26) is the input to the paper's analysis of the infrared behaviour of Bℓℓ(ℓ)B^{(\ell)}_{\ell\ell}Bℓℓ(ℓ)​ (at most 1/ϵℓ1/\epsilon^\ell1/ϵℓ, manifest for even ℓ\ellℓ because only most-subleading-colour amplitudes appear), and hence to the conjectured all-orders relation between Bℓℓ(ℓ)B^{(\ell)}_{\ell\ell}Bℓℓ(ℓ)​ and the Regge limit of N=8\mathcal N=8N=8 supergravity (Sec. 6). An all-ℓ\ellℓ proof replaces an extrapolation from nine loop orders by a theorem.

Formalizing it. The low-loop tables (4.16), (4.20), (4.18), (4.22) are finite computations; the goal and milestones 3, 4, 7, 8 are statements for every loop order and need genuine arguments (induction on ℓ\ellℓ, structure of the operators on the extended basis).

Difficulty

The coefficient Bℓℓ(ℓ)B^{(\ell)}_{\ell\ell}Bℓℓ(ℓ)​ is defined through the whole (3ℓ−2)(3\ell-2)(3ℓ−2)-element basis: a formula for it must vanish on every other Nℓ−iCikN^{\ell-i}C_{ik}Nℓ−iCik​, including the nested commutators Ci1C_{i1}Ci1​ and Ci,i−1C_{i,i-1}Ci,i−1​ whose components grow in complexity with iii. Checking the formula loop order by loop order does not give a proof; one needs to control how Tt2\mathbf T_t^2Tt2​ and Ts−u2\mathbf T_{s-u}^2Ts−u2​ act on the two most-subleading slots of the extended basis uniformly in ℓ\ellℓ.

Formalization scope

  • Colour vectors are Fin 6 → ℂ[X], with NNN the polynomial variable X; operators are Matrix (Fin 6) (Fin 6) ℂ[X] acting by Matrix.mulVec. Coefficients BikB_{ik}Bik​ and the prefactor κ=A1(0)a~ℓ\kappa=A_1^{(0)}\tilde a^\ellκ=A1(0)​a~ℓ are arbitrary complex numbers; BBB is a function ℕ × ℕ → ℂ of which only the admissible pairs matter.
  • Extended-basis indices λ\lambdaλ are 1-based natural numbers, 1≤λ≤3ℓ+31\le\lambda\le3\ell+31≤λ≤3ℓ+3; the coordinate function returns 000 outside this range. The colour-ordered amplitudes are defined as the coordinates of κ∑BikNℓ−iCik\kappa\sum B_{ik}N^{\ell-i}C_{ik}κ∑Bik​Nℓ−iCik​, so the goal says: whatever the coefficients, the stated combination of coordinates returns κBℓℓ\kappa B_{\ell\ell}κBℓℓ​. This is equivalent to the paper's reading for amplitudes lying in the span of the Regge basis (milestone 8).
  • The odd-ℓ\ellℓ formula (4.28) for ℓ>1\ell>1ℓ>1 is not included. It agrees with the model at ℓ=3\ell=3ℓ=3 (it is the B33B_{33}B33​ line of eq. (4.22)), but an exploratory exact-rational computation (not machine-checked) found that at ℓ=5\ell=5ℓ=5 no linear combination of the six amplitudes A3ℓ−8,A3ℓ−6,A3ℓ−5,A3ℓ−3,A3ℓ−2,A3ℓA_{3\ell-8},A_{3\ell-6},A_{3\ell-5},A_{3\ell-3},A_{3\ell-2},A_{3\ell}A3ℓ−8​,A3ℓ−6​,A3ℓ−5​,A3ℓ−3​,A3ℓ−2​,A3ℓ​ reproduces B55(5)B^{(5)}_{55}B55(5)​ in this model. Including it would risk a false milestone.
  • Local checks of the statements used Lean v4.28.0 with Mathlib; only standard Mathlib API (polynomials, matrices, LinearIndependent, finite sums) is used.
  • Welcome contributions: lemmas describing Tt2\mathbf T_t^2Tt2​ and Ts−u2\mathbf T_{s-u}^2Ts−u2​ as operators on extended-basis coordinates (shift of NNN-degree), and general tools for iterated commutators.

Selected references

  • S. G. Naculich, All-loop-orders relation between Regge limits of N=4\mathcal N=4N=4 SYM and N=8\mathcal N=8N=8 supergravity four-point amplitudes, arXiv:2012.00030 (2020), https://arxiv.org/abs/2012.00030.
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Mathematical Physics·Captain: Lucas

Gubser-Klebanov-Polyakov 1998: dimensions of operators dual to massive string statesResearch Paper

Motivation

In 1997 Maldacena conjectured that N=4\mathcal N=4N=4 super-Yang–Mills theory with gauge group U(N)U(N)U(N) is equivalent to type IIB string theory on AdS5×S5\mathrm{AdS}_5\times S^5AdS5​×S5 (hep-th/9711200). The paper of Gubser, Klebanov and Polyakov (hep-th/9802109), together with Witten's paper of the same year (hep-th/9802150), turned the conjecture into a computational rule: the generating functional of connected gauge theory correlators equals the minimum of the supergravity action subject to boundary conditions at the edge of anti-de Sitter space. The concrete outputs of the paper are two-point functions and operator dimensions, read off from the small-momentum, non-analytic behaviour of solutions of a radial ordinary differential equation.

The mathematical core is classical analysis of modified Bessel functions: which solution is regular in the throat, how KνK_\nuKν​ splits into I±νI_{\pm\nu}I±ν​, and what the leading non-analytic term of a logarithmic derivative is as the momentum tends to zero. The physical headline, Eq. (46), is that operators dual to massive string states at level nnn acquire dimensions growing like 2(n gYM2N)1/22(n\,g_{YM}\sqrt{2N})^{1/2}2(ngYM​2N​)1/2 at large 't Hooft coupling.

Setting

Let R>0R>0R>0 be the AdS radius and z>0z>0z>0 the radial coordinate, with the boundary at z=Rz=Rz=R and the horizon at z=∞z=\inftyz=∞. For a bulk field ϕ(x,z)=eik⋅xf~k(z)\phi(x,z)=e^{ik\cdot x}\tilde f_k(z)ϕ(x,z)=eik⋅xf~​k​(z) with Euclidean momentum k>0k>0k>0, the radial equation is

(Dk,μf)(z)  =  z3 ∂z ⁣(z−3∂zf)−k2f−μz2 f  =  0,(\mathcal D_{k,\mu}f)(z)\;=\;z^3\,\partial_z\!\left(z^{-3}\partial_z f\right)-k^2 f-\frac{\mu}{z^2}\,f\;=\;0,(Dk,μ​f)(z)=z3∂z​(z−3∂z​f)−k2f−z2μ​f=0,

with μ=0\mu=0μ=0 for the massless s-wave (Eq. (20)), μ=l(l+4)\mu=l(l+4)μ=l(l+4) for the lll-th partial wave (Eq. (34)), and μ=(mR)2\mu=(mR)^2μ=(mR)2 for a scalar string state of mass mmm (Eq. (40)).

The modified Bessel functions are defined for x>0x>0x>0 and real ν\nuν by

Kν(x)=∫0∞e−xcosh⁡tcosh⁡(νt) dt,Iν(x)=∑j≥0(x/2)2j+νj! Γ(j+ν+1).K_\nu(x)=\int_0^\infty e^{-x\cosh t}\cosh(\nu t)\,dt,\qquad I_\nu(x)=\sum_{j\ge0}\frac{(x/2)^{2j+\nu}}{j!\,\Gamma(j+\nu+1)}.Kν​(x)=∫0∞​e−xcoshtcosh(νt)dt,Iν​(x)=j≥0∑​j!Γ(j+ν+1)(x/2)2j+ν​.

The normalised radial profile is f~k(z)=z2Kν(kz)/(R2Kν(kR))\tilde f_k(z)=z^2K_\nu(kz)/(R^2K_\nu(kR))f~​k​(z)=z2Kν​(kz)/(R2Kν​(kR)), the flux factor is F(k)=[z−3∂zlog⁡f~k(z)]z=R\mathcal F(k)=\big[z^{-3}\partial_z\log\tilde f_k(z)\big]_{z=R}F(k)=[z−3∂z​logf~​k​(z)]z=R​, and the two-point function is ⟨O(k)O(q)⟩=(2π)4δ4(k+q) N216π2F(k)\langle O(k)O(q)\rangle=(2\pi)^4\delta^4(k+q)\,\tfrac{N^2}{16\pi^2}\mathcal F(k)⟨O(k)O(q)⟩=(2π)4δ4(k+q)16π2N2​F(k) (Eq. (26)). For a level-nnn string state m2=4n/α′m^2=4n/\alpha'm2=4n/α′, R4=2NgYM2α′2R^4=2Ng_{YM}^2\alpha'^2R4=2NgYM2​α′2, the Bessel order is ν=4+(mR)2\nu=\sqrt{4+(mR)^2}ν=4+(mR)2​ (Eq. (41)) and the dimension of the dual operator is Δ=2+ν\Delta=2+\nuΔ=2+ν (Eq. (45)).

Formalization targets

Goal (Eqs. (41)–(46))

For n≥1n\ge1n≥1, N,gYM,α′,m,R>0N,g_{YM},\alpha',m,R>0N,gYM​,α′,m,R>0 with m2=4n/α′m^2=4n/\alpha'm2=4n/α′, R4=2NgYM2α′2R^4=2Ng_{YM}^2\alpha'^2R4=2NgYM2​α′2 and ν=4+(mR)2∉Z\nu=\sqrt{4+(mR)^2}\notin\mathbb Zν=4+(mR)2​∈/Z: there is a function AAA real-analytic at 000 with

N216π2F(k)=A(k2)−N28π2Γ(1−ν)Γ(ν)(kR2)2νR−4+o(k2ν)(k→0+),\frac{N^2}{16\pi^2}\mathcal F(k)=A(k^2)-\frac{N^2}{8\pi^2}\frac{\Gamma(1-\nu)}{\Gamma(\nu)}\Big(\frac{kR}{2}\Big)^{2\nu}R^{-4}+o(k^{2\nu})\quad(k\to0^+),16π2N2​F(k)=A(k2)−8π2N2​Γ(ν)Γ(1−ν)​(2kR​)2νR−4+o(k2ν)(k→0+),

Δ=2+ν=2+4+4n gYM2N\Delta=2+\nu=2+\sqrt{4+4n\,g_{YM}\sqrt{2N}}Δ=2+ν=2+4+4ngYM​2N​​, and Δ/(2(n g2N)1/2)→1\Delta\big/\big(2(n\,g\sqrt{2N})^{1/2}\big)\to1Δ/(2(ng2N​)1/2)→1 as g→∞g\to\inftyg→∞.

Milestones

Solutions of the radial equation (Eqs. (22), (35), (39)–(41)), regularity selecting KνK_\nuKν​ (text after (23)), the connection formula Kν=π2sin⁡πν(I−ν−Iν)K_\nu=\frac{\pi}{2\sin\pi\nu}(I_{-\nu}-I_\nu)Kν​=2sinπνπ​(I−ν​−Iν​) (Eq. (42)), the flux factor for integer order (Eqs. (36)–(37)) and non-integer order (Eqs. (43)–(44)), the relation (mR)2=4ngYM2N(mR)^2=4ng_{YM}\sqrt{2N}(mR)2=4ngYM​2N​ (Eq. (41)) and the asymptotics (45)–(46).

Significance

The computation is the prototype of the AdS/CFT dictionary between bulk masses and boundary dimensions, Δ(Δ−4)=(mR)2\Delta(\Delta-4)=(mR)^2Δ(Δ−4)=(mR)2 in five bulk dimensions. The massless case reproduces the non-renormalisation of dimensions of operators dual to supergravity fields; the massive case is the first prediction that unprotected operators acquire dimensions growing without bound at strong coupling.

The mathematical statements are classical, but their formalisation needs modified Bessel functions of real order, their connection formula, and asymptotic expansions near 000 with logarithmic terms — material not currently present in Mathlib as far as the drafter checked. None of the statements below has a machine-checked proof yet.

Corrections to the source. Numerical exploration by the drafter (not machine-checked) indicates that the sign of the logarithmic coefficient printed in Eqs. (36)–(37) is reversed (the standard expansion has (−1)n+1log⁡(x/2) In(x)(-1)^{n+1}\log(x/2)\,I_n(x)(−1)n+1log(x/2)In​(x) in Kn(x)K_n(x)Kn​(x)), and that Eq. (27) is inconsistent with Eq. (37) at l=0l=0l=0: the correct leading term for l=0l=0l=0 is −14k4log⁡(kR)=−18k4log⁡(k2R2)-\tfrac14k^4\log(kR)=-\tfrac18k^4\log(k^2R^2)−41​k4log(kR)=−81​k4log(k2R2). The partial-wave milestone is stated with the corrected coefficient. Eq. (44) (non-integer order), which carries the paper's main prediction, agrees with the standard expansions.

Difficulty

The flux factor is a logarithmic derivative of KνK_\nuKν​ evaluated at the boundary. The leading term of KνK_\nuKν​ near 000 is a pure power, which contributes only an analytic part; the physical information sits in a subleading term of relative size k2νk^{2\nu}k2ν (or k2l+4log⁡kk^{2l+4}\log kk2l+4logk for integer order). Extracting it requires the full series structure of KνK_\nuKν​ near 000, not only its leading asymptotics, together with control of the remainder uniformly enough to pass through a logarithm and a derivative.

Formalization scope

All functions are real-valued; KνK_\nuKν​ is defined by its integral representation and IνI_\nuIν​ by its power series, both used only for x>0x>0x>0. The convention 1/Γ(pole)=01/\Gamma(\text{pole})=01/Γ(pole)=0 is realised by Lean's 1/0=01/0=01/0=0. "An analytic function of k2k^2k2 plus a term plus o(⋅)o(\cdot)o(⋅)" is encoded as: there exists AAA with AnalyticAt ℝ A 0 such that the difference is little-ooo of the given power as k→0+k\to0^+k→0+. Because 2ν2\nu2ν is not an even integer when ν∉Z\nu\notin\mathbb Zν∈/Z (and because of the logarithm in the integer case), the coefficient of the leading non-analytic term is uniquely determined, so the statements are not vacuous. The physics steps (the identification of generating functionals, Eq. (12), and the Fourier transform to position space) are not formalised: the two-point function is defined through the flux factor, Eq. (26). Welcome contributions: general facts about KνK_\nuKν​ and IνI_\nuIν​ (differential equation, positivity, asymptotics, series near 000), reusable beyond this mission.

Selected references

  • S.S. Gubser, I.R. Klebanov, A.M. Polyakov, Gauge theory correlators from non-critical string theory, Phys. Lett. B 428 (1998) 105–114. https://arxiv.org/abs/hep-th/9802109
  • J. Maldacena, The large N limit of superconformal field theories and supergravity, Adv. Theor. Math. Phys. 2 (1998) 231. https://arxiv.org/abs/hep-th/9711200
  • E. Witten, Anti de Sitter space and holography, Adv. Theor. Math. Phys. 2 (1998) 253. https://arxiv.org/abs/hep-th/9802150
  • NIST Digital Library of Mathematical Functions, Chapter 10 (Bessel functions). https://dlmf.nist.gov/10
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AnalysisMathematical Physics·Captain: Lucas

Witten 1998: Anti de Sitter Space and Holography — the massive scalar boundary-value problemResearch Paper

Motivation

In February 1998 Witten's paper Anti de Sitter Space and Holography made precise Maldacena's proposal that large-NNN conformal field theories in ddd dimensions are described by gravity on (d+1)(d+1)(d+1)-dimensional anti de Sitter space AdSd+1\mathrm{AdS}_{d+1}AdSd+1​. The dictionary it proposes identifies boundary values of bulk fields with sources of boundary operators, and reads correlation functions off the dependence of the bulk action on those boundary values. Its most quoted quantitative consequence is the mass–dimension relation: a scalar of mass mmm on AdSd+1\mathrm{AdS}_{d+1}AdSd+1​ corresponds to a boundary operator of conformal dimension

Δ=12(d+d2+4m2),Δ(Δ−d)=m2.\Delta=\tfrac12\big(d+\sqrt{d^2+4m^2}\big),\qquad \Delta(\Delta-d)=m^2 .Δ=21​(d+d2+4m2​),Δ(Δ−d)=m2.

Behind this physics statement sits a piece of classical analysis on hyperbolic space: the Dirichlet-type problem for the operator Δg−m2\Delta_g-m^2Δg​−m2 with prescribed boundary asymptotics, solved by an explicit Poisson-type integral (Section 2 of the paper, eqs. (2.15)–(2.44)). This mission formalizes that analytic core.

Timeline. Maldacena 1997 (hep-th/9711200) conjectured the correspondence; Gubser–Klebanov–Polyakov (hep-th/9802109) and Witten (hep-th/9802150, both February 1998) proposed the precise dictionary; the Euclidean black-hole thermodynamics used in Section 3 goes back to Hawking–Page 1983.

Setting

Euclidean AdSd+1\mathrm{AdS}_{d+1}AdSd+1​ is modelled as the upper half space {(x0,x):x0>0, x∈Rd}\{(x_0,x): x_0>0,\ x\in\mathbb R^d\}{(x0​,x):x0​>0, x∈Rd} with the hyperbolic metric

ds2=1x02(dx02+∑i=1ddxi2)(eq. (2.15)).ds^2=\frac{1}{x_0^2}\Big(dx_0^2+\sum_{i=1}^d dx_i^2\Big)\qquad\text{(eq. (2.15))}.ds2=x02​1​(dx02​+i=1∑d​dxi2​)(eq. (2.15)).

Its Laplace–Beltrami operator is

Δgu=x0d+1∂0(x01−d∂0u)+x02∑j=1d∂j2u=x02(∂02u+∑j∂j2u)−(d−1)x0 ∂0u.\Delta_g u=x_0^{d+1}\partial_0\big(x_0^{1-d}\partial_0 u\big)+x_0^2\sum_{j=1}^d\partial_j^2u = x_0^2\Big(\partial_0^2u+\sum_j\partial_j^2u\Big)-(d-1)x_0\,\partial_0u .Δg​u=x0d+1​∂0​(x01−d​∂0​u)+x02​j=1∑d​∂j2​u=x02​(∂02​u+j∑​∂j2​u)−(d−1)x0​∂0​u.

A massive scalar of squared mass m2∈Rm^2\in\mathbb Rm2∈R solves Δgu=m2u\Delta_g u=m^2uΔg​u=m2u (eqs. (2.34), (2.37)). The conformal dimension is Δ=12(d+d2+4m2)\Delta=\tfrac12(d+\sqrt{d^2+4m^2})Δ=21​(d+d2+4m2​) (eq. (2.44)), the bulk-to-boundary kernel is

KΔ(x0,x)=x0Δ(x02+∣x∣2)Δ(eqs. (2.19), (2.38)),K_\Delta(x_0,x)=\frac{x_0^{\Delta}}{(x_0^2+|x|^2)^{\Delta}}\qquad\text{(eqs. (2.19), (2.38))},KΔ​(x0​,x)=(x02​+∣x∣2)Δx0Δ​​(eqs. (2.19), (2.38)),

and the Poisson-type integral of a boundary datum φ0\varphi_0φ0​ is ∫RdKΔ(x0,x−x′) φ0(x′) dx′\int_{\mathbb R^d}K_\Delta(x_0,x-x')\,\varphi_0(x')\,dx'∫Rd​KΔ​(x0​,x−x′)φ0​(x′)dx′ (eqs. (2.20), (2.41)).

Formalization targets

Goal (eq. (2.41) with (2.43)–(2.44))

For m2>−d2/4m^2>-d^2/4m2>−d2/4 there is a constant c>0c>0c>0 such that for every bounded continuous φ0\varphi_0φ0​ on Rd\mathbb R^dRd,

φ(x0,x)=c∫Rdx0Δ(x02+∣x−x′∣2)Δ φ0(x′) dx′\varphi(x_0,x)=c\int_{\mathbb R^d}\frac{x_0^{\Delta}}{(x_0^2+|x-x'|^2)^{\Delta}}\,\varphi_0(x')\,dx'φ(x0​,x)=c∫Rd​(x02​+∣x−x′∣2)Δx0Δ​​φ0​(x′)dx′

is a C2C^2C2 solution of Δgφ=m2φ\Delta_g\varphi=m^2\varphiΔg​φ=m2φ on the upper half space and x0Δ−d φ(x0,x)→φ0(x)x_0^{\Delta-d}\,\varphi(x_0,x)\to\varphi_0(x)x0Δ−d​φ(x0​,x)→φ0​(x) as x0→0+x_0\to0^+x0​→0+, i.e. φ∼x0d−Δφ0\varphi\sim x_0^{d-\Delta}\varphi_0φ∼x0d−Δ​φ0​ at the boundary (eq. (2.36) with f=x0f=x_0f=x0​).

Milestones

  1. x0Δx_0^{\Delta}x0Δ​ solves the massive equation when Δ(Δ−d)=m2\Delta(\Delta-d)=m^2Δ(Δ−d)=m2 (eqs. (2.16)–(2.17), (2.37)).
  2. The inverted kernel KΔK_\DeltaKΔ​ solves it too (eqs. (2.18)–(2.19), (2.38)).
  3. Scaling: ∫x02Δ−d(x02+∣x∣2)−Δdx\int x_0^{2\Delta-d}(x_0^2+|x|^2)^{-\Delta}dx∫x02Δ−d​(x02​+∣x∣2)−Δdx is independent of x0x_0x0​ (eq. (2.40)).
  4. Approximate identity: these kernels tend to a multiple of δ(x)\delta(x)δ(x) (eq. (2.39)).
  5. The massless case Δ=d\Delta=dΔ=d with φ→φ0\varphi\to\varphi_0φ→φ0​ (eq. (2.20)).
  6. Δ=12(d+d2+4m2)\Delta=\tfrac12(d+\sqrt{d^2+4m^2})Δ=21​(d+d2+4m2​) is the larger root of Δ(Δ−d)=m2\Delta(\Delta-d)=m^2Δ(Δ−d)=m2 (eqs. (2.43)–(2.44)).
  7. The gauge-field profile x0d−2x_0^{d-2}x0d−2​ solves the reduced Maxwell equation (eqs. (2.24)–(2.25)).
  8. Hawking–Page, d=3d=3d=3: β(r+)=12πr+/(1+3r+2)\beta(r_+)=12\pi r_+/(1+3r_+^2)β(r+​)=12πr+​/(1+3r+2​) has a maximum and I(r+)=πr+2(1−r+2)/(1+3r+2)I(r_+)=\pi r_+^2(1-r_+^2)/(1+3r_+^2)I(r+​)=πr+2​(1−r+2​)/(1+3r+2​) is negative for large r+r_+r+​ (eqs. (3.15)–(3.16)).

Significance

The goal is the analytic statement underlying the mass–dimension relation Δ(Δ−d)=m2\Delta(\Delta-d)=m^2Δ(Δ−d)=m2 of the AdS/CFT dictionary: it shows that the boundary datum φ0\varphi_0φ0​ of a massive field is naturally a density of weight d−Δd-\Deltad−Δ, which is how the paper identifies the dimension of the dual operator. The same kernel is the starting point for the two-point function (2.42). The result is classical mathematics (scattering theory on hyperbolic space), proved informally in the paper; this mission produces a machine-checked version together with reusable infrastructure for the hyperbolic Laplacian in half-space coordinates.

Difficulty

The pointwise identities (milestones 1, 2, 6, 7, 8) are calculus. The substance is analytic: differentiating the Poisson-type integral twice under the integral sign with only boundedness of φ0\varphi_0φ0​, and proving the approximate-identity limit with the right normalisation; the scaling integral requires Δ>d/2\Delta>d/2Δ>d/2, and the endpoint m2=−d2/4m^2=-d^2/4m2=−d2/4 (where Δ=d/2\Delta=d/2Δ=d/2 and the kernel is not integrable) must be excluded.

Formalization scope

Points are pairs (x0,x)∈R×EuclideanSpace R (Fin d)(x_0,x)\in\mathbb R\times\mathrm{EuclideanSpace}\ \mathbb R\ (\mathrm{Fin}\ d)(x0​,x)∈R×EuclideanSpace R (Fin d); partial derivatives are one-variable derivs, so the solution predicate also demands C2C^2C2 regularity on {x0>0}\{x_0>0\}{x0​>0}, which rules out junk values of deriv. Real powers are Real.rpow; integrals are Bochner integrals for Lebesgue measure. Boundary data are bounded continuous functions. All declarations live in the namespace WittenAdSHolography, with the shared definitions in one definition file.

Selected references

  • E. Witten, Anti de Sitter Space and Holography, Adv. Theor. Math. Phys. 2 (1998) 253–291. https://arxiv.org/abs/hep-th/9802150
  • J. Maldacena, The Large N Limit of Superconformal Field Theories and Supergravity, Adv. Theor. Math. Phys. 2 (1998) 231–252. https://arxiv.org/abs/hep-th/9711200
  • S. S. Gubser, I. R. Klebanov, A. M. Polyakov, Gauge Theory Correlators from Non-Critical String Theory, Phys. Lett. B 428 (1998) 105–114. https://arxiv.org/abs/hep-th/9802109
  • S. W. Hawking, D. N. Page, Thermodynamics of Black Holes in Anti-de Sitter Space, Commun. Math. Phys. 87 (1983) 577–588. https://doi.org/10.1007/BF01208266
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