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Actuarial ScienceProbability·Captain: WillR

Actuarial Mathematics LVII: Finite Tail-Loss Measures, Stop-Loss and Conditional Value-at-Risk Threshold FunctionalTextbook

Motivation

Insurers price retention layers and assess high-loss capital needs using distributions of losses rather than only expected claim frequency. The Rockafellar and Uryasev paper introduces an auxiliary loss-threshold objective for conditional value-at-risk (CVaR). Its central mathematical construction uses expected positive-part loss in excess of a threshold. The existing core relationship is established in published research; this mission develops an original exact finite-scenario Lean formalisation and its necessary boundary lemmas.

The published reference identifies the actuarial basis for this work. Finite source-specific formalisation in Lean remains open, while the motivating mathematical identities and technical conventions have been established in the literature. No compiler check or numerical example is an accepted proof.

Setting

A finite lattice has loss outcomes 0 through n with nonnegative scenario weights p(k); it represents a genuine probability distribution only when their total mass equals one. The scenario-weighted excess above deductible t is SL_n(t)=sum p(k) max(k-t,0), which is an expected excess under unit total probability mass. For a conventional confidence alpha in the interval from zero to one, excluding one, the tail fraction 1-alpha is positive and the Rockafellar-Uryasev objective equals F_alpha(t)=t+SL_n(t)/(1-alpha). The lower cumulative weight includes outcomes less than or equal to an integer threshold, while upper mass includes only strictly larger losses. Both parts partition the original finite weight. The Lean identities hold more generally for nonnegative weights without asserting that unnormalised weights define a probability distribution or that a fixed threshold minimises the CVaR objective.

Formalization targets

All declarations below are original derived actuarial formal results. The supporting milestone order builds an intentional mathematical chain to a single root theorem.

Finite scenario probabilities, losses and positive-part payouts

This block contributes 11 theorem targets and 4 definitions. The model distinguishes direct source identities from hypotheses used to extend them to a general cashflow or life-contingent valuation system.

Representative theorem `ActuarialValuation.tailExcess_antitone_threshold`:

t≤u⇒(x−u)+≤(x−t)+t\le u\Rightarrow(x-u)_+\le(x-t)_+t≤u⇒(x−u)+​≤(x−t)+​

Increasing retention cannot increase payment for any insured loss.

Finite stop-loss and Rockafellar-Uryasev threshold objective

This block contributes 11 theorem targets and 4 definitions. The model distinguishes direct source identities from hypotheses used to extend them to a general cashflow or life-contingent valuation system.

Representative theorem `ActuarialValuation.tailScaledExcess_nonneg`:

SL≥0,τ>0⇒K≥0SL\ge0,\tau>0\Rightarrow K\ge0SL≥0,τ>0⇒K≥0

Nonnegative expected excess and positive tail mass make a valid nonnegative scaling.

Discrete cumulative tails, thresholds and monetary shifts

This block contributes 10 theorem targets and 4 definitions. The model distinguishes direct source identities from hypotheses used to extend them to a general cashflow or life-contingent valuation system.

Representative theorem `ActuarialValuation.tailTailRisk_fundamental`:

SL(t)≥0,  Fα(t)≥t,  FαX+s(t+s)=FαX(t)+sSL(t)\ge0,\;F_\alpha(t)\ge t,\;F_\alpha^{X+s}(t+s)=F_\alpha^X(t)+sSL(t)≥0,Fα​(t)≥t,FαX+s​(t+s)=FαX​(t)+s

The root joins tail-stop-loss nonnegativity, a valid finite CVaR objective, monetary translation equivalence and the complete lower/upper finite loss partition.

Capstone theorem

The main target is `ActuarialValuation.tailTailRisk_fundamental`. The root joins tail-stop-loss nonnegativity, a valid finite CVaR objective, monetary translation equivalence and the complete lower/upper finite loss partition.

SL(t)≥0,  Fα(t)≥t,  FαX+s(t+s)=FαX(t)+sSL(t)\ge0,\;F_\alpha(t)\ge t,\;F_\alpha^{X+s}(t+s)=F_\alpha^X(t)+sSL(t)≥0,Fα​(t)≥t,FαX+s​(t+s)=FαX​(t)+s

Significance

A scenario version of the original threshold-objective formula is suitable for rigorous deterministic actuarial software tests. Exact stop-loss monotonicity and positive-part partition results are reusable in reinsurance, capital modelling and future optimisation research. The root proves meaningful financial invariants: nonnegative ceded loss, a lower bound on the objective, and translation equivariance. It does not claim the objective at an arbitrary threshold equals optimised CVaR: that requires minimising over all thresholds.

Difficulty

The confidence parameter alpha must remain below one, otherwise dividing by 1-alpha is meaningless and positivity assertions fail. An insurance loss scenario at the deductible does not generate ceded payout. Discrete distributions may have atoms at a quantile: the conditional tail mean needs partial quantile mass, not a careless conditional expectation over all values greater than or equal to VaR. The auxiliary objective is defined for all real thresholds, whereas finite lower/upper tails at integer thresholds have disjoint endpoints. Zero-weight degenerate examples cannot establish the universal finite-scenario results.

The Rockafellar-Uryasev expression represents an auxiliary objective at each fixed threshold, with the conditional value-at-risk corresponding to its minimum across thresholds. This proposal does not assume that any arbitrary deductible minimises the objective. It distinguishes a discrete lattice distribution from a continuous loss density and preserves the mass at the chosen deductible in the lower tail. Taking a retention greater than every possible loss yields zero ceded premium but does not prove a zero capital risk measure. Translation equivariance follows from shifting the distribution of losses and the monetary threshold together, so the excess layer itself remains unchanged.

Formalization scope

This is finite-scenario algebraic formal verification of a classic CVaR optimisation building block, not a continuous-distribution conditional expectation theorem or an assertion of existence/uniqueness of the minimising quantile. No distributional normalisation is inferred from truncated mass. The meaningful root relates insurance payouts, risk objective and monetary translation across arbitrary finite nonnegative-weight scenarios, preserving explicit denominator restrictions. This supports independent future research on convexity, optimum threshold and subadditive coherent measures.

These are original derived finite/analytic Actuarial formalisation targets rather than reproductions of a numbered textbook theorem. Exact Lean binder declarations are authoritative. The complete source uses targeted Mathlib imports and no local Lean compilation. All proof bodies remain genuinely open and do not constitute accepted results. Assumptions about negative rates, survival, policyholder independence, discounting and benefit timing must be preserved exactly.

Selected references

  • R. Tyrrell Rockafellar and Stanislav Uryasev, Optimization of Conditional Value-at-Risk (1999 preprint; Journal of Risk 2000), Equation (4), p. 5. https://sites.math.washington.edu/~rtr/papers/rtr179-CVaR1.pdf
  • Rockafellar and Uryasev, Optimization of Conditional Value-at-Risk (2000), Journal of Risk 2, pp. 21–42. https://econpapers.repec.org/RePEc:rsk:journ4:2161159
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Actuarial ScienceProbability·Captain: WillR

Actuarial Mathematics LIV: Compound Poisson Aggregate Claims and Panjer RecursionTextbook

Motivation

Actuarial collective risk models represent total insured losses as a random sum of claim amounts. Panjer's 1981 recursive method provides a tractable recurrence for aggregate probabilities when claim number frequencies belong to a specified recursive family. This mission uses the compound Poisson special case and formalises the positive integer severity setting, its unique recursive aggregate law and finite premium and stop-loss valuations.

Finite actuarial valuation follows published literature, including the principal source. Definitions of finite event counts, valuation factors and cashflow conventions must be treated as precise mathematical inputs. Established actuarial formulae motivate the work; the resulting Lean statements are newly proposed, open proof obligations. The formal verification of these identities is distinct from the existing published mathematical development. No numerical tests or private declaration compilation constitute accepted proofs.

Setting

For intensity lambda at least zero, individual claims take strictly positive integer sizes with nonnegative severity weights f(j) and f(0)=0. The Poisson zero-claims probability is exp(-lambda). The aggregate loss lattice masses g(k) satisfy, for positive k, kg(k)=lambdasum from j=1 to k of j*f(j)*g(k-j). A finite probability prefix through n gives G(n), and 1-G(n) denotes its modelled tail complement. Finite expected aggregate loss and stop-loss premiums use sums over outcomes 0 through n.

Formalization targets

All declarations below are original derived actuarial formal results. The supporting milestone order builds an intentional mathematical chain to a single root theorem.

Finite claim-size severity and convolution

This block contributes 11 theorem targets and 4 definitions. The model distinguishes direct source identities from hypotheses used to extend them to a general cashflow or life-contingent valuation system.

Representative theorem `ActuarialValuation.panjerWeightedSeverity_nonneg`:

fk≥0⇒kfk≥0f_k\ge0\Rightarrow kf_k\ge0fk​≥0⇒kfk​≥0

Nonnegative severity weights yield nonnegative weighted claims.

Compound Poisson Panjer recurrence

This block contributes 12 theorem targets and 4 definitions. The model distinguishes direct source identities from hypotheses used to extend them to a general cashflow or life-contingent valuation system.

Representative theorem `ActuarialValuation.panjerRecurrence_nonneg`:

λ,f≥0⇒gk≥0\lambda,f\ge0\Rightarrow g_k\ge0λ,f≥0⇒gk​≥0

The uniquely generated compound Poisson aggregate coefficients are nonnegative for nonnegative severity probabilities.

Finite aggregate loss reserve and stop-loss valuation

This block contributes 12 theorem targets and 4 definitions. The model distinguishes direct source identities from hypotheses used to extend them to a general cashflow or life-contingent valuation system.

Representative theorem `ActuarialValuation.panjerAggregateClaims_fundamental`:

g=h,  gk≥0,  Gn+Tn=1,  SLn(d)≥0,  λμn≥0g=h,\;g_k\ge0,\;G_n+T_n=1,\;SL_n(d)\ge0,\;\lambda\mu_n\ge0g=h,gk​≥0,Gn​+Tn​=1,SLn​(d)≥0,λμn​≥0

The compound aggregate-claims capstone combines genuine uniqueness of forward Panjer probabilities, nonnegative aggregate coefficients, and finite claim-payment cost controls.

Capstone theorem

The main target is `ActuarialValuation.panjerAggregateClaims_fundamental`. The compound aggregate-claims capstone combines genuine uniqueness of forward Panjer probabilities, nonnegative aggregate coefficients, and finite claim-payment cost controls.

g=h,  gk≥0,  Gn+Tn=1,  SLn(d)≥0,  λμn≥0g=h,\;g_k\ge0,\;G_n+T_n=1,\;SL_n(d)\ge0,\;\lambda\mu_n\ge0g=h,gk​≥0,Gn​+Tn​=1,SLn​(d)≥0,λμn​≥0

Significance

The core mathematical target proves that the forward recurrence with initial mass exp(-lambda) uniquely fixes all aggregate coefficients, and nonnegative intensity and severities imply all generated probabilities are nonnegative. It reconciles finite cumulative mass, a tail complement, expected aggregate costs and a ceded stop-loss value in one theorem. The recursion is independent of the earlier negative-binomial frequency moment mission and leaves full normalisation to separate infinite-series proofs.

The importance of the formal result is the availability of reusable, source-explicit lemmas for actuarial software audit and subsequent independent mathematical work, as described in the published literature. It goes beyond an elementary reformulation of a single definition: the capstone simultaneously connects different construction stages with monetary or probability reconciliation and precise boundary hypotheses. A vacuous zero-data specialisation cannot establish these relationships across arbitrary finite schedules.

Difficulty

The Panjer recurrence requires positive severity weights indexed by j at least one: allowing mass at zero without changing the denominator and initial atom would make its stated form incorrect. For each target k only lower aggregate coefficients occur, permitting ordinary induction. Natural index subtraction is safe within the finite sum. Intensity positivity, exp(-lambda), natural-to-real index coercions and finite sums need careful attention. This mission deliberately does not claim that a truncated mass automatically sums to one or that a sequence satisfying the recurrence is normalised without additional assumptions.

The recurrence's fundamental mathematical content is the coefficient-by-coefficient relationship: the coefficient at aggregate loss k depends only on previously calculated coefficients for aggregate losses strictly below k. This well-founded structure supports a strong induction proof of uniqueness and a separate positivity induction. The initial mass exp(-lambda) applies only when each individual claim has strictly positive loss. A severity law admitting zero-sized claims would require a corrected initial atom and a denominator involving zero-severity mass. A finite prefix of recursive probabilities is not, by itself, an exhaustive law. Further work can add total normalisation and full expectation formulas.

Formalization scope

The model is the lattice compound Poisson special case, not the full (a,b,0) family. It distinguishes algebraic consistency of a recursively specified sequence from measure-theoretic construction of an independent compound random sum. Stop-loss results are finite truncation values and do not by themselves control omitted large losses. All theorems are original derived proof obligations.

These are original derived finite/analytic Actuarial formalisation targets rather than reproductions of a numbered textbook theorem. Exact Lean binder declarations are authoritative. The complete source uses targeted Mathlib imports and no local Lean compilation. All proof bodies remain genuinely open and do not constitute accepted results. Assumptions about negative rates, survival, policyholder independence, discounting and benefit timing must be preserved exactly.

Selected references

  • H. H. Panjer, Recursive Evaluation of a Family of Compound Distributions, ASTIN Bulletin 12 (1981), pp. 22–26. https://www.casact.org/sites/default/files/database/astin_vol12no1_22.pdf
  • Sundt and Jewell, Further Results on Recursive Evaluation of Compound Distributions, ASTIN Bulletin 12 (1981), pp. 27–39. https://www.casact.org/sites/default/files/database/astin_vol12no1_27.pdf
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Actuarial ScienceProbability·Captain: WillR

Actuarial Mathematics LV: Kaplan-Meier Survival Estimation and Greenwood VarianceTextbook

Motivation

Insurance mortality investigations must estimate survival probabilities from observed death times when some policyholders leave the observation period alive or are otherwise censored. Kaplan-Meier product-limit estimation accounts for changing risk sets without misclassifying censoring as mortality. Greenwood's formula provides the standard plug-in variance. This mission formalises a finite death-event calculation, risk-set conservation, survival probability bounds, and variance bookkeeping.

Finite actuarial valuation follows published literature, including the principal source. Definitions of finite event counts, valuation factors and cashflow conventions must be treated as precise mathematical inputs. Established actuarial formulae motivate the work; the resulting Lean statements are newly proposed, open proof obligations. The formal verification of these identities is distinct from the existing published mathematical development. No numerical tests or private declaration compilation constitute accepted proofs.

Setting

At event index t, the observed risk set r_t is positive immediately before deaths d_t and censoring exits c_t. Deaths and censors are disjoint exits, so the next risk set is r_t-d_t-c_t under a closed cohort. The estimated event-time mortality fraction is d_t/r_t, and Kaplan-Meier survival through n events is the product of 1-d_t/r_t. The complement gives cumulative failure. With 0<=d_t<r_t, the Greenwood term is d_t/[r_t(r_t-d_t)] and the plug-in variance equals squared Kaplan-Meier survival times the accumulated terms. Restricted expected lifetime is a finite sum of discrete event-time survival values.

Formalization targets

All declarations below are original derived actuarial formal results. The supporting milestone order builds an intentional mathematical chain to a single root theorem.

Observed risk sets and interval exits

This block contributes 11 theorem targets and 4 definitions. The model distinguishes direct source identities from hypotheses used to extend them to a general cashflow or life-contingent valuation system.

Representative theorem `ActuarialValuation.kmRiskExit_reconciliation`:

d/r+c/r=(d+c)/rd/r+c/r=(d+c)/rd/r+c/r=(d+c)/r

Death and censoring hazards sum to the total observed exit fraction, without equating censoring to mortality.

Kaplan-Meier product-limit survival

This block contributes 11 theorem targets and 4 definitions. The model distinguishes direct source identities from hypotheses used to extend them to a general cashflow or life-contingent valuation system.

Representative theorem `ActuarialValuation.kmSurvivalStep_exact`:

Sn+1=SnpnS_{n+1}=S_np_nSn+1​=Sn​pn​

An actuarial one-step survival update reproduces the exact finite product-limit estimate.

Greenwood uncertainty and finite restricted survival

This block contributes 12 theorem targets and 4 definitions. The model distinguishes direct source identities from hypotheses used to extend them to a general cashflow or life-contingent valuation system.

Representative theorem `ActuarialValuation.kmSurvivalGreenwood_fundamental`:

0≤Sn+1≤Sn,  Sn+1+Fn+1=1,  Vn+1≥0,  RMSTn+1≥00\le S_{n+1}\le S_n,\;S_{n+1}+F_{n+1}=1,\;V_{n+1}\ge0,\;RMST_{n+1}\ge00≤Sn+1​≤Sn​,Sn+1​+Fn+1​=1,Vn+1​≥0,RMSTn+1​≥0

The survival-estimation capstone proves the complete finite product-limit probability bounds, failure partition, nonnegative Greenwood plug-in variance and nonnegative restricted expected lifetime under strict risk-set conditions.

Capstone theorem

The main target is `ActuarialValuation.kmSurvivalGreenwood_fundamental`. The survival-estimation capstone proves the complete finite product-limit probability bounds, failure partition, nonnegative Greenwood plug-in variance and nonnegative restricted expected lifetime under strict risk-set conditions.

0≤Sn+1≤Sn,  Sn+1+Fn+1=1,  Vn+1≥0,  RMSTn+1≥00\le S_{n+1}\le S_n,\;S_{n+1}+F_{n+1}=1,\;V_{n+1}\ge0,\;RMST_{n+1}\ge00≤Sn+1​≤Sn​,Sn+1​+Fn+1​=1,Vn+1​≥0,RMSTn+1​≥0

Significance

The capstone formally guarantees nonnegative and nonincreasing estimated survival, a complementary failure estimate, a nonnegative Greenwood plug-in variance and a nonnegative finite restricted survival integral under actual risk-set constraints. These are foundational actuarial quality-control properties and provide reusable results for experience investigations. Censoring changes future exposures but never directly counts as a death.

The importance of the formal result is the availability of reusable, source-explicit lemmas for actuarial software audit and subsequent independent mathematical work, as described in the published literature. It goes beyond an elementary reformulation of a single definition: the capstone simultaneously connects different construction stages with monetary or probability reconciliation and precise boundary hypotheses. A vacuous zero-data specialisation cannot establish these relationships across arbitrary finite schedules.

Difficulty

The denominator must be the individuals under observation immediately before the death time. Event times with r_t=0 cannot identify a mortality fraction. The Greenwood variance denominator requires r_t>d_t, so a complete mortality exhaustion creates a boundary where the usual finite formula is undefined. Event-time product-limit survival does not imply unbiasedness under informative censoring; external independent/non-informative censoring assumptions are needed for statistical interpretations. A finite restricted sum is not an unrestricted life expectancy.

The survival estimator is indexed by actual ordered death-event intervals. People censored without dying should remain at risk up to the censoring time and leave the risk set before later events. At a death time the product decreases by a factor determined by deaths divided by lives currently exposed. At an interval containing no death the factor is one. The standard Greenwood approximation is only defined when positive risk remains after each included set of deaths. At complete exhaustion the finite variance expression must not divide by zero, and the usual delta-method approximation should not be silently extrapolated. Results are deterministic algebra conditional on observed counts, not a theorem of statistical consistency.

Formalization scope

The formal model is a finite discrete event-time product-limit calculation, not an asymptotic proof of the Kaplan-Meier central limit theorem. Greenwood's plug-in formula is defined explicitly; the proof obligations concern its algebra, positivity and consistency under stated boundaries, not an estimator-unbiasedness claim. Definitions and milestones are original derived Lean results based on published survival-method principles.

These are original derived finite/analytic Actuarial formalisation targets rather than reproductions of a numbered textbook theorem. Exact Lean binder declarations are authoritative. The complete source uses targeted Mathlib imports and no local Lean compilation. All proof bodies remain genuinely open and do not constitute accepted results. Assumptions about negative rates, survival, policyholder independence, discounting and benefit timing must be preserved exactly.

Selected references

  • Society of Actuaries, Mortality Differences by Handedness, Transactions of the Society of Actuaries 45 (1993), p. 267, on product-limit estimation and Greenwood variance. https://www.soa.org/globalassets/assets/library/research/transactions-of-society-of-actuaries/1990-95/1993/january/tsa93v459.pdf
  • Kaplan and Meier, Nonparametric Estimation from Incomplete Observations (1958), Journal of the American Statistical Association 53, pp. 457–481. https://doi.org/10.1080/01621459.1958.10501452
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Actuarial ScienceProbability·Captain: WillR

Actuarial Mathematics LIII: Chain-Ladder Claims Development and Bornhuetter-Ferguson ReservesTextbook

Motivation

Paid claims triangles are essential to general insurance reserving. A volume-weighted chain-ladder link factor projects mature cohorts and less developed cohorts to a common ultimate basis, while the Bornhuetter-Ferguson approach apportions expected remaining development to an externally selected prior ultimate. This research mission formalises their finite algebra and reconciliation without asserting stochastic unbiasedness or any distributional variance result.

Finite actuarial valuation follows published literature, including the principal source. Definitions of finite event counts, valuation factors and cashflow conventions must be treated as precise mathematical inputs. Established actuarial formulae motivate the work; the resulting Lean statements are newly proposed, open proof obligations. The formal verification of these identities is distinct from the existing published mathematical development. No numerical tests or private declaration compilation constitute accepted proofs.

Setting

For origin cohort i and development period j, C(i,j) denotes cumulative paid claims and C(i,j+1)-C(i,j) the incremental payment. A selected rectangular subset with m fully observed adjacent development points gives volume-weighted factor f_j=Sum_i C(i,j+1)/Sum_i C(i,j), defined when denominator nonzero. The remaining development factor F is the finite product of selected nonnegative age-to-age factors. Latest cumulative paid claims C yield chain-ladder ultimate CF and reserve C(F-1). With a priori ultimate E, the Bornhuetter-Ferguson unpaid reserve is E(1-1/F), and ultimate is C plus this reserve.

Formalization targets

All declarations below are original derived actuarial formal results. The supporting milestone order builds an intentional mathematical chain to a single root theorem.

Cumulative triangles and selected development factors

This block contributes 11 theorem targets and 4 definitions. The model distinguishes direct source identities from hypotheses used to extend them to a general cashflow or life-contingent valuation system.

Representative theorem `ActuarialValuation.clVolumeFactor_nonneg`:

Nj≥0,Dj>0⇒fj≥0N_j\ge0,D_j>0\Rightarrow f_j\ge0Nj​≥0,Dj​>0⇒fj​≥0

Nonnegative claims and positive exposure make the factor nonnegative.

Development to ultimate and outstanding reserve

This block contributes 11 theorem targets and 4 definitions. The model distinguishes direct source identities from hypotheses used to extend them to a general cashflow or life-contingent valuation system.

Representative theorem `ActuarialValuation.clUltimate_reserve_balance`:

C+R=UC+R=UC+R=U

The ultimate estimate is reconciled exactly to paid claims and outstanding reserve.

Prior expected ultimate and Bornhuetter-Ferguson reconciliation

This block contributes 14 theorem targets and 4 definitions. The model distinguishes direct source identities from hypotheses used to extend them to a general cashflow or life-contingent valuation system.

Representative theorem `ActuarialValuation.clClaimsDevelopment_fundamental`:

fD=N,  C+RCL=UCL,  UBF=wUCL+(1−w)E,  RCL,RBF≥0fD=N,\;C+R_{CL}=U_{CL},\;U_{BF}=wU_{CL}+(1-w)E,\;R_{CL},R_{BF}\ge0fD=N,C+RCL​=UCL​,UBF​=wUCL​+(1−w)E,RCL​,RBF​≥0

The substantive capstone reconciles a volume-selected development factor, chain-ladder valuation, and prior-informed Bornhuetter-Ferguson valuation under economically meaningful positivity assumptions.

Capstone theorem

The main target is `ActuarialValuation.clClaimsDevelopment_fundamental`. The substantive capstone reconciles a volume-selected development factor, chain-ladder valuation, and prior-informed Bornhuetter-Ferguson valuation under economically meaningful positivity assumptions.

fD=N,  C+RCL=UCL,  UBF=wUCL+(1−w)E,  RCL,RBF≥0fD=N,\;C+R_{CL}=U_{CL},\;U_{BF}=wU_{CL}+(1-w)E,\;R_{CL},R_{BF}\ge0fD=N,C+RCL​=UCL​,UBF​=wUCL​+(1−w)E,RCL​,RBF​≥0

Significance

The main formal result reconciles numerator and denominator on the same observed cohorts, the paid-plus-reserve valuation identity, and the exact BF weighted-average identity. It distinguishes development-based estimation from prior-informed estimation. These results establish algebraic control checks for finite claims triangles and reserve reconciliation, while reserving model predictive uncertainty for subsequent work.

The importance of the formal result is the availability of reusable, source-explicit lemmas for actuarial software audit and subsequent independent mathematical work, as described in the published literature. It goes beyond an elementary reformulation of a single definition: the capstone simultaneously connects different construction stages with monetary or probability reconciliation and precise boundary hypotheses. A vacuous zero-data specialisation cannot establish these relationships across arbitrary finite schedules.

Difficulty

Carefully distinguish incremental and cumulative claims, the latest paid amount and ultimate, and an age-to-age factor from the full age-to-ultimate product. The volume-weighted ratio must use identical origin-cohort exposure in numerator and denominator. A zero denominator does not identify a meaningful observed development factor. The BF interpretation requires strictly positive F, and nonnegative future emergence requires F at least one. Deterministic algebra is not an assertion of unbiased predictive reserves without statistical assumptions.

An age-to-age ratio represents an explicitly selected rectangular cohort of observed cumulative values. It is not interchangeable with the arithmetic average of individual ratios, nor with an extrapolated tail factor after the final observed maturity. Where paid and incurred development patterns differ, separate sets of factors must be selected. In the Bornhuetter-Ferguson setting the chosen external expectation must correspond to the same basis as the observed cumulative paid claims: mixing paid claims and reported case estimates invalidates the interpretation. The final theorem therefore tests linked monetary identities rather than asserting an objective optimal reserve.

Formalization scope

The task is finite deterministic paid-claims reserving in a single currency and valuation date, with nonnegative selected cumulative development under hypotheses of each theorem. It formalises no future-tail extrapolation or reserve variability, and no stochastic independence or Mack conditional unbiasedness. Every theorem is an original derived Lean goal requiring an accepted proof.

These are original derived finite/analytic Actuarial formalisation targets rather than reproductions of a numbered textbook theorem. Exact Lean binder declarations are authoritative. The complete source uses targeted Mathlib imports and no local Lean compilation. All proof bodies remain genuinely open and do not constitute accepted results. Assumptions about negative rates, survival, policyholder independence, discounting and benefit timing must be preserved exactly.

Selected references

  • Klaus D. Schmidt, Methods and Models of Loss Reserving Based on Run-Off Triangles, CAS Forum (2006), especially section 4.3 and p. 283. https://www.casact.org/sites/default/files/database/forum_06fforum_273.pdf
  • Schmidt and Zocher, The Bornhuetter-Ferguson Principle, Casualty Actuarial Society (2008). https://www.casact.org/sites/default/files/2021-07/Bornhuetter-Ferguson-Schmidt-Zocher.pdf
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Actuarial ScienceProbability·Captain: WillR

Actuarial Mathematics LII: Commutation Functions and Assurance-Annuity Present Value IdentityTextbook

Motivation

Actuarial valuation of these claims follows published actuarial mathematics (https://www.actuaries.org.uk/system/files/documents/pdf/0042-0071.pdf). Actuarial commutation functions provide a classical exact connection between life-table survival and financial discounting. The Institute of Actuaries' International Actuarial Notation (1969–1971) records the discounted survivor and death columns and their accumulated insurance and annuity values. Dickson, Hardy and Waters' Actuarial Mathematics for Life Contingent Risks (2009), Chapter 5, explains valuation relationships between assurance and annuity payments. The objective is a connected proof of the finite-horizon assurance, annuity-due and pure endowment identity, rather than a cataloguing of conventional symbols.

Setting

Existing known actuarial results from the reference sources motivate these new original-derived theorem obligations. The actuarial formulae in published literature provide the mathematical background, while the proposed Lean theorem declarations are original derived results and remain unproved. A genuine nonzero mortality, service or insurance cashflow model is required rather than a vacuous zero-value special case. Accepted results will support more advanced actuarial valuation tasks.

An integer-age life table l(x) gives survivors at age x and decreases over the covered term. An annual discount factor v is strictly positive. The commutation functions are D_x=v^x l_x and C_x=v^(x+1)(l_x−l_(x+1)), where the second discounts a death claim payable at the end of the year. The finite sums N_(x:n)=sum_(k<n)D_(x+k) and M_(x:n)=sum_(k<n)C_(x+k) measure the temporary annuity-due and term assurance numerators. Terminal survival is D_(x+n), and the financial effective discount rate is d=1−v. Dividing the numerator sums by D_x gives the corresponding conditional actuarial present values, when D_x is nonzero.

Formalization targets

All declarations below are original derived actuarial formal results. The supporting milestone order builds an intentional mathematical chain to a single root theorem.

Discounted life table functions

This block contributes 10 theorem targets and 4 definitions. The model distinguishes direct source identities from hypotheses used to extend them to a general cashflow or life-contingent valuation system.

Representative theorem ActuarialValuation.commLocalDeathIdentity:

Cx+(1−v)Dx=Dx−Dx+1C_x+(1-v)D_x=D_x-D_{x+1}Cx​+(1−v)Dx​=Dx​−Dx+1​

One-year death and annuity-discount value telescope to the discounted decrement.

Finite commutation functions

This block contributes 11 theorem targets and 4 definitions. The model distinguishes direct source identities from hypotheses used to extend them to a general cashflow or life-contingent valuation system.

Representative theorem ActuarialValuation.commGrossReconciliation_identity:

Mx:n+dNx:n+Dx+n=DxM_{x:n}+dN_{x:n}+D_{x+n}=D_xMx:n​+dNx:n​+Dx+n​=Dx​

The full insurance-annuity-survival decomposition follows by telescoping annual differences.

Assurance and annuity monetary values

This block contributes 12 theorem targets and 4 definitions. The model distinguishes direct source identities from hypotheses used to extend them to a general cashflow or life-contingent valuation system.

Representative theorem ActuarialValuation.commAssuranceAnnuity_fundamental:

M+dN+Dx+n=Dx,A+da¨+E=1M+dN+D_{x+n}=D_x,\quad A+d\ddot a+E=1M+dN+Dx+n​=Dx​,A+da¨+E=1

The capstone establishes both raw and conditional actuarial valuation identities and nonnegativity of term assurance and pure endowment for a valid life table.

Capstone theorem

The main target is ActuarialValuation.commAssuranceAnnuity_fundamental. The capstone establishes both raw and conditional actuarial valuation identities and nonnegativity of term assurance and pure endowment for a valid life table.

M+dN+Dx+n=Dx,A+da¨+E=1M+dN+D_{x+n}=D_x,\quad A+d\ddot a+E=1M+dN+Dx+n​=Dx​,A+da¨+E=1

Significance

The resulting formal identities will be reusable by future downstream pensions and insurance valuation missions. Formal actuarial modelling of these obligations follows the published valuation literature (https://www.actuaries.org.uk/system/files/documents/pdf/0042-0071.pdf). The one-year identity C_x+(1−v)D_x=D_x−D_(x+1) telescopes over successive payment years. The resulting finite equation M_(x:n)+dN_(x:n)+D_(x+n)=D_x reconciles three disjoint financially timed payment streams. Dividing by D_x yields A_(x:n)+d a_due_(x:n)+E_(x:n)=1, connecting term assurance, annuity due and survival to term expiration. This provides a powerful actuarial valuation consistency check: omitting a terminal survival payment or discounting deaths at the beginning rather than end of the year breaks the identity.

Difficulty

The annual life-table decrement l_x−l_(x+1) must not be confused with the financial discount d=1−v. The annuity-due includes the initial survivor payment at age x whereas the insurance claim is payable at the end of the death year. Each exponent and half-open finite sum endpoint must be exact. The main telescope holds without assumptions on real survivor counts, but financial probability interpretation requires nonnegative remaining lives and a nonincreasing table, plus positive valuation-age survivors. The conditional ratios require a nonzero D_x. A general theorem must not assume the result by defining the numerator balance identically equal to D_x.

Formalization scope

The model is a finite integer-age life table and a common annual interest basis with unit annuity payments, year-end unit death claims and a unit pure endowment at the terminal payment date. It makes no independence assumption about additional lives and introduces no continuous-time death benefits. The capstone proves the raw commutation identity, the actuarial present value identity and nonnegativity of its insurance and terminal survival components. All declarations are original Lean formalisation targets and should remain open until genuine accepted remote proofs exist.

These are original derived finite/analytic Actuarial formalisation targets rather than reproductions of a numbered textbook theorem. Exact Lean binder declarations are authoritative. The complete source uses targeted Mathlib imports and no local Lean compilation. All proof bodies remain genuinely open and do not constitute accepted results. Assumptions about negative rates, survival, policyholder independence, discounting and benefit timing must be preserved exactly.

Selected references

  • Institute of Actuaries, International Actuarial Notation and Commutation Functions (1969–1971). https://www.actuaries.org.uk/system/files/documents/pdf/0042-0071.pdf
  • David C. M. Dickson, Mary R. Hardy and Howard R. Waters, Actuarial Mathematics for Life Contingent Risks: Annuities (2009). https://www.cambridge.org/core/books/abs/actuarial-mathematics-for-life-contingent-risks/annuities/6E4AF10872F5D04E3437447F025ECA97
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Actuarial ScienceProbability·Captain: WillR

Actuarial Mathematics LI: Life Insurance Reserve Differences, Paid-Up Benefits and Policy AlterationsTextbook

Motivation

Actuarial valuation of these claims follows published actuarial mathematics (https://onlinelibrary.wiley.com/doi/10.1002/9781119971528.ch6). Life insurance policy alterations require a mathematically coherent link between reserves, remaining premium payments, reduced paid-up cover and cash surrender settlements. In Fundamentals of Actuarial Mathematics, S. David Promislow develops the premium difference and paid-up formulae in Chapter 6, Section 6.8 (2010/2015). Dickson, Hardy and Waters cover policy values and alterations within life-contingent reserve theory. The proposal creates a connected sequence of algebraic valuation results for these choices, without treating a surrender value as if it were always the prospective reserve.

Setting

Existing known actuarial results from the reference sources motivate these new original-derived theorem obligations. The actuarial formulae in published literature provide the mathematical background, while the proposed Lean theorem declarations are original derived results and remain unproved. A genuine nonzero mortality, service or insurance cashflow model is required rather than a vacuous zero-value special case. Accepted results will support more advanced actuarial valuation tasks.

At the policy alteration date, B denotes the complete present value of remaining insured benefits and a denotes the value of future unit premium payments. A level premium P leaves prospective policy reserve V=B−Pa. An equivalent newly repriced premium Ps=B/a is meaningful for nonzero a. A reserve-equivalent paid-up benefit amount b is V/Aunit for an explicitly positive unit insurance present value Aunit. A proportionally scaled paid-up policy uses z=V/B under nonzero B. Cash surrender value is the simplified payment SV=V−c, with a separate nonnegative surrender deduction c not exceeding V when positive surrender cash is required. All values are compared at the same time and on one consistent actuarial valuation basis.

Formalization targets

All declarations below are original derived actuarial formal results. The supporting milestone order builds an intentional mathematical chain to a single root theorem.

Prospective reserve and premium difference

This block contributes 11 theorem targets and 4 definitions. The model distinguishes direct source identities from hypotheses used to extend them to a general cashflow or life-contingent valuation system.

Representative theorem ActuarialValuation.alterationRevisedReserve_delta:

V(P2)−V(P1)=(P1−P2)aV(P_2)-V(P_1)=(P_1-P_2)aV(P2​)−V(P1​)=(P1​−P2​)a

Change in future premiums shifts the actuarial reserve by the monetised payment difference.

Paid-up insurance and equivalent cover

This block contributes 10 theorem targets and 4 definitions. The model distinguishes direct source identities from hypotheses used to extend them to a general cashflow or life-contingent valuation system.

Representative theorem ActuarialValuation.alterationPaidUpScaledValue_add:

PV(f+g)=PV(f)+PV(g)PV(f+g)=PV(f)+PV(g)PV(f+g)=PV(f)+PV(g)

Paid-up proportional benefit values are additive over cover portions.

Surrender deductions and policy value comparisons

This block contributes 9 theorem targets and 3 definitions. The model distinguishes direct source identities from hypotheses used to extend them to a general cashflow or life-contingent valuation system.

Representative theorem ActuarialValuation.alterationReservePaidUpSurrender_fundamental:

V=(Ps−P)a=bPUAunit,0≤SV≤VV=(P_s-P)a=b_{\rm PU}A_{\rm unit},\quad0\le SV\le VV=(Ps​−P)a=bPU​Aunit​,0≤SV≤V

Main policy alteration theorem reconciles prospective reserve, repriced premium difference and reserve-equivalent paid-up cover while bounding surrender cash by the reserve.

Capstone theorem

The main target is ActuarialValuation.alterationReservePaidUpSurrender_fundamental. Main policy alteration theorem reconciles prospective reserve, repriced premium difference and reserve-equivalent paid-up cover while bounding surrender cash by the reserve.

V=(Ps−P)a=bPUAunit,0≤SV≤VV=(P_s-P)a=b_{\rm PU}A_{\rm unit},\quad0\le SV\le VV=(Ps​−P)a=bPU​Aunit​,0≤SV≤V

Significance

Formal actuarial modelling of these obligations follows the published valuation literature (https://onlinelibrary.wiley.com/doi/10.1002/9781119971528.ch6). The premium difference theorem identifies reserve as the present value of the deficiency of original premiums relative to the equivalent premium currently required for remaining benefits. Paid-up insurance conversion substitutes a benefit without future premiums whose expected present value equals the original reserve. A surrender amount can differ from reserve when contractual charges apply. These three concepts reconcile actuarially while remaining different legal and financial benefit forms. The final theorem combines premium-difference equivalence, paid-up monetary equivalence, and the inequality between surrender value and reserve under explicit reserve and deduction constraints.

Difficulty

Divisions in reprice and paid-up formulae require nonzero insurance and premium annuity denominators, unlike Lean's totalised real division. A prospective reserve can be negative if future premiums exceed remaining insurance values, so nonnegative paid-up cover and cash surrender cannot be claimed without additional assumptions. An actual policy might use tax, expenses, guaranteed surrender values, bonus distributions or other legal terms not represented by a simple deduction. The model distinguishes a change in premium value from a change in benefit value, and the capstone cannot be established through a degenerate zero-cover simplification.

Formalization scope

The mathematical scope is a finite real-valued prospective valuation model supplied with consistent actuarial present-value factors. Benefit discounting, mortality basis and benefit dates are represented by B, a and Aunit rather than silently re-derived. Paid-up and surrender transformations are idealised actuarial alternatives and are not universal contractual entitlements. Asset share is a separate retrospective concept and is not asserted equal to prospective reserve without further matching assumptions. Every theorem remains an original derived obligation, suitable for subsequent extensions with expense-adjusted reserves and policyholder nonforfeiture terms.

These are original derived finite/analytic Actuarial formalisation targets rather than reproductions of a numbered textbook theorem. Exact Lean binder declarations are authoritative. The complete source uses targeted Mathlib imports and no local Lean compilation. All proof bodies remain genuinely open and do not constitute accepted results. Assumptions about negative rates, survival, policyholder independence, discounting and benefit timing must be preserved exactly.

Selected references

  • S. David Promislow, Fundamentals of Actuarial Mathematics (2010), Chapter 6. https://onlinelibrary.wiley.com/doi/10.1002/9781119971528.ch6
  • David C. M. Dickson, Mary R. Hardy and Howard R. Waters, Actuarial Mathematics for Life Contingent Risks (2009). https://www.cambridge.org/core/books/actuarial-mathematics-for-life-contingent-risks/51C0B04099D4DE1D1DDEF9551024133B/listing
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Actuarial ScienceProbability·Captain: WillR

Actuarial Mathematics L: Projected Unit Pension Cost, Accrued Liability and Funding AmortisationTextbook

Motivation

Actuarial valuation of these claims follows published actuarial mathematics (https://www.actuary.org/sites/default/files/pdf/pension/fundamentals_0704.pdf). Projected unit credit funding is a standard actuarial cost method that allocates pension retirement benefits to completed and future years of service. The American Academy of Actuaries describes actuarial accrued liability and normal cost under this method in its Fundamentals of Pension Accounting and Funding (2004). The Institute of Actuaries' GN26 Pension Fund Terminology (2006) likewise describes projected unit cost, standard contribution rates and amortisation. This formal research mission unites the benefit attribution and funding calculations in a single theorem graph; it goes beyond the separate salary-linked CARE/DC terminal equivalence already treated in the preceding mission.

Setting

The actuarial formulae in published literature provide the mathematical background, while the proposed Lean theorem declarations are original derived results and remain unproved. A genuine nonzero mortality, service or insurance cashflow model is required rather than a vacuous zero-value special case. Accepted results will support more advanced actuarial valuation tasks.

A finite salary-linked accrued annual pension is expressed as a sum of projected retirement benefit units b(t). Completed service years occupy the half-open index range zero through n−1, and m future years occupy n through n+m−1. An actuarial retirement factor f is a survival probability times an appropriate discount and pension annuity package. The accrued liability is AL=f sum of completed service units, and projected future normal costs equal f times the future-service units. Assets A are measured at the same valuation date. An unfunded liability UL=AL−A is financed by a constant contribution rate c applied to a strictly positive present value F of pensionable payroll, and S=A+cF−AL is the resulting simplified funding surplus.

Formalization targets

All declarations below are original derived actuarial formal results. The supporting milestone order builds an intentional mathematical chain to a single root theorem.

Projected service and accrued benefits

This block contributes 10 theorem targets and 4 definitions. The model distinguishes direct source identities from hypotheses used to extend them to a general cashflow or life-contingent valuation system.

Representative theorem ActuarialValuation.pucTotalBenefit_zero:

B0,0=0B_{0,0}=0B0,0​=0

An empty past and future service ledger has zero pension.

Actuarial liability and normal cost

This block contributes 11 theorem targets and 5 definitions. The model distinguishes direct source identities from hypotheses used to extend them to a general cashflow or life-contingent valuation system.

Representative theorem ActuarialValuation.pucProjectedBenefitPV_add_future:

PVFBm+1=PVFBm+NCn+mPVFB_{m+1}=PVFB_m+NC_{n+m}PVFBm+1​=PVFBm​+NCn+m​

Projected PV of benefits increases by the normal cost of the added service year.

Funding shortfall and contribution amortisation

This block contributes 11 theorem targets and 3 definitions. The model distinguishes direct source identities from hypotheses used to extend them to a general cashflow or life-contingent valuation system.

Representative theorem ActuarialValuation.pucPensionFunding_fundamental:

PVFB=AL+PVFNC,c∗F=UL,c≥c∗⇒S(c)≥0PVFB=AL+PVFNC,\quad c^*F=UL,\quad c\ge c^*\Rightarrow S(c)\ge0PVFB=AL+PVFNC,c∗F=UL,c≥c∗⇒S(c)≥0

The pension funding capstone unites projected-unit service attribution with the exact amortisation contribution threshold and surplus monotonicity.

Capstone theorem

The main target is ActuarialValuation.pucPensionFunding_fundamental. The pension funding capstone unites projected-unit service attribution with the exact amortisation contribution threshold and surplus monotonicity.

PVFB=AL+PVFNC,c∗F=UL,c≥c∗⇒S(c)≥0PVFB=AL+PVFNC,\quad c^*F=UL,\quad c\ge c^*\Rightarrow S(c)\ge0PVFB=AL+PVFNC,c∗F=UL,c≥c∗⇒S(c)≥0

Significance

Formal actuarial modelling of these obligations follows the published valuation literature (https://www.actuary.org/sites/default/files/pdf/pension/fundamentals_0704.pdf). A sound pension valuation must reconcile the projected retirement benefit with both its accrued-service obligation and the cost of further service. The formal capstone proves that PVFB=AL+PVFNC under the same projected benefit assumptions. It additionally derives the unique amortisation percentage c*=UL/F required to extinguish a nonnegative valuation-date deficit and proves that every larger contribution percentage produces nonnegative surplus. This establishes a financial and actuarial accounting invariant across valuation and funding. It can support later analyses of demographic experience, recovery periods, employer contributions and aggregate scheme funding, but does not automatically impose any scheme-specific contribution rule.

Difficulty

The benefit units represent projected retirement benefits, not past salary amounts at historical ages. Past and future service must be disjoint and exhaustion of the projection horizon must be exact. The pension factor uses the same assumed retirement date, survival and payment schedule throughout each monetary reconciliation; changes in that basis are outside the elementary attribution equation. Zero service and zero accrued liability are meaningful. A nonzero payroll base is necessary to define the funding rate, and positive payroll PV is essential to monotonicity. Deficits and surpluses are financially different: the chosen capstone assumes a nonnegative unfunded deficit rather than assuming the same payment solves an overfunded scheme under all regulations.

Formalization scope

The formal results treat an individual or coherently aggregated finite service schedule under one actuarial pension valuation basis and a simplified fixed-rate contribution financing model. They do not assert that the selected funding contribution must be paid by law or accounting standards, nor do they value ancillary expenses, deferred pension increases or new entrants automatically. The main theorem combines independently defined actuarial benefit allocation, pension liability and funding surplus. Existing pension funding textbooks provide the conceptual derivations, while every proposed Lean statement is an original finite formalisation requiring a real proof.

These are original derived finite/analytic Actuarial formalisation targets rather than reproductions of a numbered textbook theorem. Exact Lean binder declarations are authoritative. The complete source uses targeted Mathlib imports and no local Lean compilation. All proof bodies remain genuinely open and do not constitute accepted results. Assumptions about negative rates, survival, policyholder independence, discounting and benefit timing must be preserved exactly.

Selected references

  • American Academy of Actuaries, Fundamentals of Pension Accounting and Funding (2004). https://www.actuary.org/sites/default/files/pdf/pension/fundamentals_0704.pdf
  • Institute of Actuaries, GN26 Pension Fund Terminology (2006). https://www.actuaries.org.uk/system/files/documents/pdf/gn26v2-1.pdf
  • International Monetary Fund, Conducting Stress Tests of Defined Benefit Pension Plans (2014). https://www.elibrary.imf.org/display/book/9781484368589/ch012.xml
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Actuarial ScienceProbability·Captain: WillR

Actuarial Mathematics XCIX: Life-Table Notation, Survival Laws and Commutation FunctionsTextbook

Motivation

A life table summarises the survival of a cohort as ages advance, as developed in Promislow's life-table treatment. It provides an essential common language for life assurance, retirement pensions, annuities and reserves. A credible mathematical foundation must make precise when cohort counts define conditional probabilities, how death counts exhaust an assumed closed population, and why commutation-function ratios give the same values as discounted contractual payments. The classical notation is widely understood by actuaries but can conceal assumptions at terminal ages, when there are no remaining lives, and at fractional-year payment times. This formalisation specifies those assumptions so that later results can safely reuse them.

Setting

Consider an integer-age cohort with a finite terminal age, nonnegative numbers alive and nonincreasing numbers alive at successive ages. At the terminal age the remaining cohort is zero. Annual deaths are the change in cohort size over each year. Conditional survival starts only from an age with positive numbers alive. The model also has a strictly positive annual discount factor; when the corresponding effective interest rate is nonnegative, that factor is at most one. A due annuity pays on the integer anniversaries at which the insured life is alive. An annual death assurance pays at the end of the year of death. All financial amounts in the principal identities are per unit benefit, valued at the attained age of the insured life.

Formalization targets

Cohort probabilities and lifetime laws

The opening group establishes that successive survivor and decrement counts conserve population mass. Multi-year survival, conditional and deferred mortality must be derived from original counts and remain coherent under time shifts. A zero survivor count is an explicit boundary of the probability model. Curtate lifetime moments are obtained from the annual death distribution and its tail probabilities. Continuous survival and hazard relationships form an additional interface requiring a genuine measurable lifetime law. They cannot be inferred from the table's integer-age observations without an interpolation assumption.

Select and fractional-age assumptions

The next group distinguishes age at selection from time since selection and attained age. Ultimate mortality applies only after the selection period. Within a year, uniform distribution of deaths, constant force and Balducci interpolation share the annual survival endpoints but generally disagree between those endpoints. Each conditional fractional formula needs the corresponding survival denominator to be positive. These are alternative models, so the choice of interpolation must remain explicit.

Commutation columns and benefit timing

The commutation columns are defined from the same original survivor counts and a fixed annual discount factor. Discounted survivors and year-end deaths create the first-order columns. Their finite forward sums create the second-order columns, and sums of those forward sums create the increasing-benefit columns. In particular, for survivors the discounted payments begin at the valuation anniversary, whereas for deaths the benefit is payable on the next anniversary. The finite terminal convention is essential for the last year's assurance payment and the last available annuity instalment.

Principal finite-cohort capstone

The principal goal is the finite-cohort valuation reconciliation. Starting independently from annual numbers alive and numbers dying, it shows that total deaths exhaust the living cohort, actual survival-contingent payments agree with the annuity commutation ratio, actual annual death payments agree with the assurance commutation ratio, and the commutation sums satisfy their backward recursions. It also establishes the capital identity expressing unit present value as annual death assurance plus the discount loss on an annuity due. No commutation recurrence or present-value equivalence is assumed as an input.

At a valid attained age, the annuity and assurance are independently valued from the original cohort:

a¨x=NxDx,Ax=MxDx,Ax+(1−v)a¨x=1.\ddot a_x=\frac{N_x}{D_x},\qquad A_x=\frac{M_x}{D_x},\qquad A_x+(1-v)\ddot a_x=1.a¨x​=Dx​Nx​​,Ax​=Dx​Mx​​,Ax​+(1−v)a¨x​=1.

Significance

As in the classical actuarial notation, the resulting interfaces separate cohort mass from conditional probability and separate mortality from the economic discounting basis. This allows a later actuarial mission to combine them only where the required regularity and positivity assumptions are available. The commutation functions supply a transparent independent valuation route alongside direct finite cashflow sums. Their ratios remain useful as a reference calculation even when production models value very large pension populations by member-level cashflow projection. Higher-order commutation functions are also the natural algebraic representation of benefits that increase by one unit at each subsequent anniversary.

This foundation is reusable across future mortality and valuation missions. A foundational namespace is particularly important where related existing missions already use different local definitions. The present work provides a compatibility design and a proposed canonical public vocabulary. Publishing an older equivalent definition does not automatically establish a safe imported interface: exact source, revision, visibility, and declaration signatures must match. The programme therefore retains existing mission objects and develops explicit crosswalks, rather than silently replacing earlier results.

Difficulty

The mathematical difficulty centres on conditioning, index shifts and independent routes to the same financial result. At an age with no survivors, a formal programming language may return a totalised value for division by zero even though no conditional mortality probability exists. A common off-by-one error values a death at the beginning of its year or includes a due annuity payment after the terminal age. Another error confuses discounting to time zero with discounting to the current valuation age. Select mortality requires careful handling of attained age at the exact selection-duration boundary. Continuous lifetime hazard and moment formulas additionally need probability, measurability and integrability assumptions that finite cohort counts alone cannot supply.

The double-sum commutation identities require a finite discrete summation argument and must use published survivor and assurance conventions consistently. The goal compares separate original definitions of payment cashflows, the population exit distribution, and commutation columns under one valid finite life table. The capstone is nonvacuous: a positive starting cohort and positive discount factor exclude empty-cohort substitutions and make its conditional cashflows meaningful. Its assumptions impose cohort validity and positive discounting; they do not contain the desired present-value identities as hypotheses.

Formalization scope

The initial formalisation supplies a canonical finite discrete cohort and annual cashflow basis. The continuous-law, hazard, select and fractional-age results are separately specified mathematical interfaces and are admitted into the formal theorem inventory only when remote declaration checks establish valid Lean signatures. For nonnegative effective interest the annual discount is in the interval from zero excluded to one included. More general deterministic term structures and stochastic discount factors require separate cashflow definitions. Joint-life and competing-decrement extensions must identify any independence or mutually exclusive decrement assumptions explicitly.

No assertion is made about mortality being stationary across calendar years or about the validity of a specific mortality table for a real population. The terminal-age assumption imposes certain death before the finite horizon. It is unsuitable without modification for a lifetime distribution with unbounded support. A lifetime with an atom at an integer boundary requires separate weak and strict survival events; interpreting a one-year death count as the hazard at the death instant is unjustified without further assumptions. Open formal statements remain proof obligations, and passing a declaration check would establish only well-formed Lean, not the mathematical truth of the intended result.

The finite-cohort valuation targets also include independently defined one-year and multi-year mortality probabilities, temporary and deferred annuities, term and endowment assurances, pure endowments, annuities in arrears and increasing finite-term cashflows. The expanded candidate graph has 26 definitions and 48 open theorem obligations in a coherent reconciliation programme. New results require independently derived cashflow-to-commutation identities.

Related proposals LII (commutation functions and finite-term benefits) and LXII (fractional-duration valuation) are in review, not public importable dependencies. Existing published life-table theorems in XLV must be reused where signatures match. The fractional-age and continuous-law interfaces require separate hypotheses. All research targets remain provisional until their exact published-name overlap checks, authoritative declaration elaboration and dependency links are validated. No private diagnostic is counted as a proved theorem.

The increasing-insurance commutation column requires the relative-duration or absolute-age convention to be declared explicitly. Annual UDD includes certain year-end death, but constant-force and Balducci interpolation require annual death probability strictly below one.

Selected references

  • S. David Promislow (2015), Fundamentals of Actuarial Mathematics, third edition, Wiley, Chapters 2–5, 7, 9 and 13–14. https://www.wiley.com/en-us/Fundamentals+of+Actuarial+Mathematics%2C+3rd+Edition-p-9781118782521
  • David C. M. Dickson, Mary R. Hardy and Howard R. Waters (2020), Actuarial Mathematics for Life Contingent Risks, third edition, Cambridge University Press, Chapters 2–5. https://doi.org/10.1017/9781108784184
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Mathematical Physics·Captain: Lucas

Onsager Reciprocal Relations: Symmetry of Kinetic CoefficientsTextbook

Motivation

Near thermodynamic equilibrium, flows of extensive quantities (heat, matter, charge) depend linearly on the thermodynamic forces (gradients of the conjugate intensive variables). Some of the coefficients in these linear laws describe cross effects: a temperature gradient driving an electric current (Seebeck effect), a voltage driving a heat flow (Peltier effect), a temperature gradient driving diffusion (Soret effect) and its converse (Dufour effect). In 1931 Lars Onsager showed that, as a consequence of the time-reversibility of microscopic dynamics, the matrix of these coefficients is symmetric (Onsager 1931). These reciprocal relations were confirmed experimentally across many classes of irreversible processes (Miller 1960), and Onsager received the 1968 Nobel Prize in Chemistry for them.

This mission formalizes the abstract, finite-dimensional version of Onsager's principle as presented by Landau and Lifshitz (Statistical Physics, Part 1, 1975) and reproduced in the Wikipedia article Onsager reciprocal relations, sections "Abstract formulation" and "Proof".

Setting

Let x=(x1,…,xn)∈Rnx=(x_1,\dots,x_n)\in\mathbb R^nx=(x1​,…,xn​)∈Rn be the fluctuations of nnn thermodynamic quantities from their equilibrium values. For small fluctuations the entropy is quadratic, and Boltzmann's formula gives the Gaussian fluctuation distribution

w(x)=A~ e−12βikxixk,w(x)=\tilde A\,e^{-\frac12\beta_{ik}x_ix_k},w(x)=A~e−21​βik​xi​xk​,

where β\betaβ is a positive definite symmetric real n×nn\times nn×n matrix and summation over repeated indices is understood. Write ⟨f⟩\langle f\rangle⟨f⟩ for the average of f(x)f(x)f(x) with respect to www.

The thermodynamic conjugate quantities are Xi=βikxkX_i=\beta_{ik}x_kXi​=βik​xk​. In the quasi-stationary regime the fluctuations relax according to x˙i=−λikxk\dot x_i=-\lambda_{ik}x_kx˙i​=−λik​xk​ for a real matrix λ\lambdaλ, so that x˙i=−γikXk\dot x_i=-\gamma_{ik}X_kx˙i​=−γik​Xk​ with the kinetic coefficients

γik=λil (β−1)lk.\gamma_{ik}=\lambda_{il}\,(\beta^{-1})_{lk}.γik​=λil​(β−1)lk​.

The mean value at time ttt of a fluctuation which takes the value xxx at t=0t=0t=0 is ξ(t)=e−tλx\xi(t)=e^{-t\lambda}xξ(t)=e−tλx, and Ξ(t)=βξ(t)\Xi(t)=\beta\xi(t)Ξ(t)=βξ(t). The time correlation is ⟨xi(t)xk(0)⟩=⟨ξi(t)xk⟩\langle x_i(t)x_k(0)\rangle=\langle\xi_i(t)x_k\rangle⟨xi​(t)xk​(0)⟩=⟨ξi​(t)xk​⟩.

Formalization targets

Goal: Onsager's principle

If fluctuations are symmetric under time reversal,

⟨ξi(t) xk⟩=⟨xi ξk(t)⟩(t≥0, 1≤i,k≤n),\langle \xi_i(t)\,x_k\rangle=\langle x_i\,\xi_k(t)\rangle\qquad(t\ge0,\ 1\le i,k\le n),⟨ξi​(t)xk​⟩=⟨xi​ξk​(t)⟩(t≥0, 1≤i,k≤n),

then the kinetic coefficients are symmetric:

γik=γki.\gamma_{ik}=\gamma_{ki}.γik​=γki​.

Milestones (in the order of the source's argument)

  1. x˙i=−λikxk=−γikXk\dot x_i=-\lambda_{ik}x_k=-\gamma_{ik}X_kx˙i​=−λik​xk​=−γik​Xk​ (definition of kinetic coefficients).
  2. ξ(0)=x\xi(0)=xξ(0)=x and ξ˙i(t)=−γikΞk(t)\dot\xi_i(t)=-\gamma_{ik}\Xi_k(t)ξ˙​i​(t)=−γik​Ξk​(t).
  3. ddt⟨ξi(t)xk⟩=−γil⟨Ξl(t)xk⟩\frac{d}{dt}\langle\xi_i(t)x_k\rangle=-\gamma_{il}\langle\Xi_l(t)x_k\rangledtd​⟨ξi​(t)xk​⟩=−γil​⟨Ξl​(t)xk​⟩.
  4. ⟨Xixk⟩=δik\langle X_ix_k\rangle=\delta_{ik}⟨Xi​xk​⟩=δik​.
  5. Under time-reversal symmetry, γil⟨Xlxk⟩=γkl⟨Xlxi⟩\gamma_{il}\langle X_lx_k\rangle=\gamma_{kl}\langle X_lx_i\rangleγil​⟨Xl​xk​⟩=γkl​⟨Xl​xi​⟩.

Significance

The symmetry γik=γki\gamma_{ik}=\gamma_{ki}γik​=γki​ is the mathematical content of the reciprocal relations: it reduces the number of independent transport coefficients from n2n^2n2 to n(n+1)/2n(n+1)/2n(n+1)/2 and yields the equality of measurable cross-coefficients such as the Peltier and Seebeck coefficients. Together with the positive semi-definiteness of the coefficient matrix (from non-negative entropy production), it is the basic structural input of linear irreversible thermodynamics.

The result is classical and its proof is standard in physics textbooks; this mission produces a machine-checked version of the finite-dimensional argument, including the Gaussian moment identity ⟨Xixk⟩=δik\langle X_ix_k\rangle=\delta_{ik}⟨Xi​xk​⟩=δik​ and the differentiation of the time-correlation function under the integral sign. No machine-checked formalization of this statement is known to the proposer.

Difficulty

The algebraic core is short, but the formal argument needs analytic input that the textbook treats as routine: Gaussian integrals over Rn\mathbb R^nRn for a general positive definite β\betaβ (integrability of polynomial moments against e−12xTβxe^{-\frac12x^{\mathsf T}\beta x}e−21​xTβx and the value of the second moments), differentiation of a parameter-dependent integral involving a matrix exponential, and the passage from an identity valid for t≥0t\ge0t≥0 to an identity between derivatives at the boundary point t=0t=0t=0, where only a one-sided derivative is available from the hypothesis.

Formalization scope

Vectors are functions Fin n → ℝ with Lebesgue measure; matrices are Matrix (Fin n) (Fin n) ℝ, and β.PosDef (which includes symmetry) is assumed in every theorem. The average ⟨f⟩\langle f\rangle⟨f⟩ is the ratio ∫f w dx/∫w dx\int f\,w\,dx/\int w\,dx∫fwdx/∫wdx of Bochner integrals, so the normalizing constant A~\tilde AA~ cancels. The mean relaxation is the matrix exponential ξ(t)=e−tλx\xi(t)=e^{-t\lambda}xξ(t)=e−tλx. The time-reversal hypothesis is assumed only for t≥0t\ge0t≥0. The entropy SSS and Boltzmann's constant are not modelled; β\betaβ is the primitive datum, as in the source's statement of the principle. The hypothesis is non-vacuous (e.g. λ=β\lambda=\betaλ=β satisfies it), and the conclusion concerns γ=λβ−1\gamma=\lambda\beta^{-1}γ=λβ−1, not λ\lambdaλ.

All definitions are collected in Definitions.Def_OnsagerReciprocal_basic (namespace OnsagerReciprocal). Reusable Gaussian-moment lemmas for positive definite quadratic forms are welcome contributions.

Selected references

  • L. Onsager, Reciprocal Relations in Irreversible Processes. I, Physical Review 37 (1931) 405–426. doi:10.1103/physrev.37.405
  • D. G. Miller, Thermodynamics of Irreversible Processes. The Experimental Verification of the Onsager Reciprocal Relations, Chemical Reviews 60 (1960) 15–37. doi:10.1021/cr60203a003
  • L. D. Landau, E. M. Lifshitz, Statistical Physics, Part 1, Butterworth-Heinemann (1975).
  • Wikipedia, Onsager reciprocal relations, oldid 1355014688.
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Differential GeometryMathematical Physics·Captain: Lucas

Einstein–Grossmann 1913 (Entwurf): energy-momentum conservation for matter and gravitational fieldResearch Paper

Motivation

In 1913 Albert Einstein and the mathematician Marcel Grossmann published the Entwurf ("outline") of a generalized theory of relativity and a theory of gravitation. It is the first theory in which the gravitational field is described by the ten components gμνg_{\mu\nu}gμν​ of a space-time metric, ds2=∑μνgμν dxμdxνds^2=\sum_{\mu\nu}g_{\mu\nu}\,dx_\mu dx_\nuds2=∑μν​gμν​dxμ​dxν​, and in which Ricci and Levi-Civita's absolute differential calculus (Grossmann's mathematical part) is brought into physics. Its gravitational field equations were superseded by the generally covariant field equations of November 1915, but the framework of the Entwurf — metric as gravitational potential, the energy-momentum law of matter in a gravitational field, a stress-energy expression for the gravitational field itself — carried over to general relativity.

The physical part (Part I, by Einstein) derives the field equations from one requirement: the energy-momentum law must hold for matter and gravitational field together. The derivation runs through an explicit differential identity, eq. (12), whose rewritten form (12a) yields the field equations (18) and the total conservation law (19). This mission formalizes that chain of statements.

Timeline.

  • 1912: Einstein's theory of the static gravitational field, with a single scalar potential c(x)c(x)c(x) (Ann. d. Physik 38).
  • 1913: Einstein–Grossmann, Entwurf: metric tensor gμνg_{\mu\nu}gμν​, energy-momentum law (10), field equations (18), conservation law (19).
  • 1915: Einstein, Die Feldgleichungen der Gravitation (Sitzungsber. Preuss. Akad. Wiss.): generally covariant field equations replace (18).

Setting

All objects live in one coordinate chart, x=(x1,x2,x3,x4)∈R4x=(x_1,x_2,x_3,x_4)\in\mathbb R^4x=(x1​,x2​,x3​,x4​)∈R4, with x4x_4x4​ the time coordinate. The fundamental tensor gμν(x)g_{\mu\nu}(x)gμν​(x) is a symmetric 4×44\times44×4 matrix field with negative determinant g=det⁡(gμν)g=\det(g_{\mu\nu})g=det(gμν​); γμν\gamma_{\mu\nu}γμν​ is the reciprocal (contravariant) tensor, the inverse matrix, and −g\sqrt{-g}−g​ is the density factor. All sums run over 1,…,41,\dots,41,…,4.

A material process is described by its contravariant stress-energy tensor Θμν\Theta_{\mu\nu}Θμν​ (for incoherent dust, Θμν=ϱ0dxμdsdxνds\Theta_{\mu\nu}=\varrho_0\frac{dx_\mu}{ds}\frac{dx_\nu}{ds}Θμν​=ϱ0​dsdxμ​​dsdxν​​). Its energy-momentum law in the gravitational field is eq. (10):

∑μν∂∂xν(−g gσμΘμν)−12∑μν−g ∂gμν∂xσΘμν=0(σ=1,2,3,4).\sum_{\mu\nu}\frac{\partial}{\partial x_\nu}\big(\sqrt{-g}\,g_{\sigma\mu}\Theta_{\mu\nu}\big)-\tfrac12\sum_{\mu\nu}\sqrt{-g}\,\frac{\partial g_{\mu\nu}}{\partial x_\sigma}\Theta_{\mu\nu}=0\qquad(\sigma=1,2,3,4).μν∑​∂xν​∂​(−g​gσμ​Θμν​)−21​μν∑​−g​∂xσ​∂gμν​​Θμν​=0(σ=1,2,3,4).

The second sum is the momentum (for σ=4\sigma=4σ=4, the energy) transferred per unit volume from the gravitational field to matter.

The gravitational field carries its own stress-energy tensor ϑμν\vartheta_{\mu\nu}ϑμν​, eq. (13):

−2κ ϑμν=∑αβτρ(γαμγβν∂gτρ∂xα∂γτρ∂xβ−12γμνγαβ∂gτρ∂xα∂γτρ∂xβ),-2\kappa\,\vartheta_{\mu\nu}=\sum_{\alpha\beta\tau\rho}\Big(\gamma_{\alpha\mu}\gamma_{\beta\nu}\frac{\partial g_{\tau\rho}}{\partial x_\alpha}\frac{\partial\gamma_{\tau\rho}}{\partial x_\beta}-\tfrac12\gamma_{\mu\nu}\gamma_{\alpha\beta}\frac{\partial g_{\tau\rho}}{\partial x_\alpha}\frac{\partial\gamma_{\tau\rho}}{\partial x_\beta}\Big),−2κϑμν​=αβτρ∑​(γαμ​γβν​∂xα​∂gτρ​​∂xβ​∂γτρ​​−21​γμν​γαβ​∂xα​∂gτρ​​∂xβ​∂γτρ​​),

and the field equations involve the second-order operator of eq. (15),

Δμν(γ)=∑αβ1−g∂∂xα(γαβ−g ∂γμν∂xβ)−∑αβτργαβgτρ∂γμτ∂xα∂γνρ∂xβ.\Delta_{\mu\nu}(\gamma)=\sum_{\alpha\beta}\frac{1}{\sqrt{-g}}\frac{\partial}{\partial x_\alpha}\Big(\gamma_{\alpha\beta}\sqrt{-g}\,\frac{\partial\gamma_{\mu\nu}}{\partial x_\beta}\Big)-\sum_{\alpha\beta\tau\rho}\gamma_{\alpha\beta}g_{\tau\rho}\frac{\partial\gamma_{\mu\tau}}{\partial x_\alpha}\frac{\partial\gamma_{\nu\rho}}{\partial x_\beta}.Δμν​(γ)=αβ∑​−g​1​∂xα​∂​(γαβ​−g​∂xβ​∂γμν​​)−αβτρ∑​γαβ​gτρ​∂xα​∂γμτ​​∂xβ​∂γνρ​​.

The Entwurf field equations (18) read Δμν(γ)=κ(Θμν+ϑμν)\Delta_{\mu\nu}(\gamma)=\kappa(\Theta_{\mu\nu}+\vartheta_{\mu\nu})Δμν​(γ)=κ(Θμν​+ϑμν​), with κ\kappaκ a constant. Lowering indices with ggg gives the covariant objects Tμν=∑gμαgνβΘαβT_{\mu\nu}=\sum g_{\mu\alpha}g_{\nu\beta}\Theta_{\alpha\beta}Tμν​=∑gμα​gνβ​Θαβ​, tμνt_{\mu\nu}tμν​ (eq. (14)) and the operator Dμν(g)D_{\mu\nu}(g)Dμν​(g) (eq. (16)).

Formalization targets

Goal: eq. (19)

If the energy-momentum law (10) and the field equations (18) hold, then for σ=1,2,3,4\sigma=1,2,3,4σ=1,2,3,4

∑μν∂∂xν{−g gσμ(Θμν+ϑμν)}=0.\sum_{\mu\nu}\frac{\partial}{\partial x_\nu}\Big\{\sqrt{-g}\,g_{\sigma\mu}(\Theta_{\mu\nu}+\vartheta_{\mu\nu})\Big\}=0.μν∑​∂xν​∂​{−g​gσμ​(Θμν​+ϑμν​)}=0.

Milestones

  1. The electrostatic model identity of p. 14, which illustrates the method.
  2. Identity (12a): ∑μν∂∂xν{−g gσμκϑμν}=12∑μν−g ∂gμν∂xσ{−Δμν(γ)+κϑμν}\sum_{\mu\nu}\frac{\partial}{\partial x_\nu}\{\sqrt{-g}\,g_{\sigma\mu}\kappa\vartheta_{\mu\nu}\}=\tfrac12\sum_{\mu\nu}\sqrt{-g}\,\frac{\partial g_{\mu\nu}}{\partial x_\sigma}\{-\Delta_{\mu\nu}(\gamma)+\kappa\vartheta_{\mu\nu}\}∑μν​∂xν​∂​{−g​gσμ​κϑμν​}=21​∑μν​−g​∂xσ​∂gμν​​{−Δμν​(γ)+κϑμν​}, for every metric.
  3. Identity (12b), the covariant counterpart, with tμνt_{\mu\nu}tμν​ and Dμν(g)D_{\mu\nu}(g)Dμν​(g).
  4. Eq. (10) ⇔\Leftrightarrow⇔ eq. (20), the covariant energy-momentum law.
  5. Eq. (18) ⇒\Rightarrow⇒ eq. (21), −Dμν(g)=κ(tμν+Tμν)-D_{\mu\nu}(g)=\kappa(t_{\mu\nu}+T_{\mu\nu})−Dμν​(g)=κ(tμν​+Tμν​).
  6. Eq. (22), the covariant conservation law for matter plus field.

Significance

The result itself. Eq. (19) is the property Einstein required of any relativistic theory of gravitation: the energy of the gravitational field acts as a source in the same way as every other form of energy, and matter together with field obeys conservation laws of divergence form. Identity (12a) is what makes this work for the Entwurf operator Δμν(γ)\Delta_{\mu\nu}(\gamma)Δμν​(γ); together with the matter law (10), the field equations (18) and the gravitational stress-energy ϑμν\vartheta_{\mu\nu}ϑμν​ are fixed by it.

Formalizing it. These statements are proved in the source by explicit computation, and the steps (12) → (12a) and the covariant forms (20)–(22) are given without the intermediate algebra. A machine-checked development provides the full index computations: derivatives of γμν\gamma_{\mu\nu}γμν​ and −g\sqrt{-g}−g​ in terms of those of gμνg_{\mu\nu}gμν​, the contractions in (12a) and (12b), and the lowering identities linking Δμν(γ)\Delta_{\mu\nu}(\gamma)Δμν​(γ) to Dμν(g)D_{\mu\nu}(g)Dμν​(g) and ϑμν\vartheta_{\mu\nu}ϑμν​ to tμνt_{\mu\nu}tμν​. A search of the platform library found no existing formalization of these statements.

Difficulty

There is no conceptual obstacle, but the identities are long. Identity (12a) involves second derivatives of γμν\gamma_{\mu\nu}γμν​, the derivative of −g\sqrt{-g}−g​, and contractions over up to six indices. The source gives only the final form of (12) and says the identity is obtained "nach dem angedeuteten Verfahren"; the intermediate algebra, and the analytic facts behind it (differentiability of matrix inversion and of −det⁡g\sqrt{-\det g}−detg​ under the standing assumptions), are not written out. A naive expansion of all sums produces thousands of terms.

Formalization scope

  • Space-time is R4\mathbb R^4R4 as one global chart, with points x:Fin 4→Rx:\mathrm{Fin}\,4\to\mathbb Rx:Fin4→R; two-index fields are matrix-valued functions. Partial derivatives are Fréchet derivatives along coordinate directions.
  • Standing assumptions on the metric: entries C2C^2C2, symmetric, det⁡g<0\det g<0detg<0 everywhere. No signature condition beyond the sign of the determinant; γ\gammaγ is the matrix inverse, −g\sqrt{-g}−g​ the real square root of −det⁡g-\det g−detg.
  • κ≠0\kappa\neq0κ=0 is assumed wherever ϑμν\vartheta_{\mu\nu}ϑμν​ or tμνt_{\mu\nu}tμν​ (defined with the factor 1/(2κ)1/(2\kappa)1/(2κ)) appears. Matter tensors are assumed C1C^1C1, and symmetric where the source's manipulation needs it (eq. (20)).
  • In eq. (14) the sum over α,β\alpha,\betaα,β is taken only in the term containing them, following the paper's convention. The printed eq. (22) has an inconsistent index placement; milestone 6 uses the placement of (20) and (12b).
  • The goal must not be trivialized: the field equations and the matter law are hypotheses about the same Θμν\Theta_{\mu\nu}Θμν​, and the hypotheses are satisfiable (e.g. constant metric, Θ=0\Theta=0Θ=0) but not degenerate in general.
  • Reusable infrastructure: derivative formulas for the inverse and determinant of a CkC^kCk matrix field, coordinate tensor calculus on R4\mathbb R^4R4. Contributions of these as separate lemmas are welcome.

Selected references

  • A. Einstein and M. Grossmann, Entwurf einer verallgemeinerten Relativitätstheorie und einer Theorie der Gravitation, B. G. Teubner, Leipzig und Berlin, 1913; reprinted in Zeitschrift für Mathematik und Physik 62 (1914). The source of all statements of this mission (Part I, §§4–5, pp. 10–17).
  • A. Einstein, Die Feldgleichungen der Gravitation, Sitzungsberichte der Preußischen Akademie der Wissenschaften, 1915, pp. 844–847.
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Mathematical Physics·Captain: Lucas

First Law of Thermodynamics (Wikipedia) I: Internal Energy as a State Function from Adiabatic WorkTextbook

Motivation

The first law of thermodynamics is the form the law of conservation of energy takes for thermodynamic processes. For a closed system (no transfer of matter) it is usually written, in the sign convention of Clausius, as

ΔU=Q−W,\Delta U = Q - W,ΔU=Q−W,

where QQQ is the heat supplied to the system, WWW is the work done by the system on its surroundings, and UUU is the internal energy. Heat and work describe a process and depend on the path; the internal energy is a property of the state, and its change depends only on the initial and final states.

The Wikipedia article First law of thermodynamics (revision oldid=1366986255) describes two ways of reaching this statement. In the original "thermodynamic approach" (Clausius 1850, Rankine), heat, defined by calorimetry, and work are primitive notions. In the "mechanical approach" (Bryan 1907, Carathéodory 1909, Born 1921), only adiabatic work is primitive. The law then asserts that adiabatic work is independent of the path, and that this work defines a state function UUU, fixed up to an additive constant. Heat becomes a derived quantity, the residual Q=ΔU+WQ = \Delta U + WQ=ΔU+W. This mission formalizes the logical core of the mechanical approach.

Setting

A closed system has a set σ\sigmaσ of states. A process ppp has an initial state pstartp_{\mathrm{start}}pstart​, a final state pfinishp_{\mathrm{finish}}pfinish​, a net work W(p)∈RW(p)\in\mathbb RW(p)∈R done by the system on its surroundings, and a label recording whether it is adiabatic (carried out inside an adiabatic enclosure, so that energy is transferred only as work). A set P\mathcal PP of processes stands for the processes that can actually be carried out. It is assumed to satisfy:

  1. Composition: if p,q∈Pp,q\in\mathcal Pp,q∈P and pfinish=qstartp_{\mathrm{finish}}=q_{\mathrm{start}}pfinish​=qstart​, then the composite "first ppp, then qqq" lies in P\mathcal PP. Its work is W(p)+W(q)W(p)+W(q)W(p)+W(q), and it is adiabatic exactly when both stages are.
  2. Null processes: for every state AAA, leaving the system in state AAA (with no work and no exchange) is in P\mathcal PP.
  3. Path independence of adiabatic work: any two adiabatic processes in P\mathcal PP with the same initial and final states involve the same work.
  4. Adiabatic accessibility: there is a reference state OOO such that every state AAA is reached from OOO, or reaches OOO, by some adiabatic process in P\mathcal PP.

A function U:σ→RU:\sigma\to\mathbb RU:σ→R is an internal energy for P\mathcal PP if U(pfinish)−U(pstart)=−W(p)U(p_{\mathrm{finish}})-U(p_{\mathrm{start}})=-W(p)U(pfinish​)−U(pstart​)=−W(p) for every adiabatic p∈Pp\in\mathcal Pp∈P. For a given UUU, the heat supplied in a process is the residual

QU(p)=U(pfinish)−U(pstart)+W(p).Q_U(p)=U(p_{\mathrm{finish}})-U(p_{\mathrm{start}})+W(p).QU​(p)=U(pfinish​)−U(pstart​)+W(p).

Formalization targets

Goal: existence and uniqueness of internal energy

Under assumptions 1 to 4,

∃ U internal energy for P,andU,U′ internal energies  ⟹  ∃c∈R ∀A, U′(A)=U(A)+c.\exists\,U \text{ internal energy for } \mathcal P,\qquad\text{and}\qquad U,U' \text{ internal energies} \implies \exists c\in\mathbb R\ \forall A,\ U'(A)=U(A)+c.∃U internal energy for P,andU,U′ internal energies⟹∃c∈R ∀A, U′(A)=U(A)+c.

This is the article's statement: "For all adiabatic processes between two specified states of a closed system of any nature, the net work done is the same regardless the details of the process, and determines a state function called internal energy, UUU", together with its remark that the internal energy "is defined only up to an arbitrary additive constant of integration".

Milestones

  1. Formula (1) and the chain through the reference state. If quasi-static adiabatic work WA→BW_{A\to B}WA→B​ satisfies WA→O=−WO→AW_{A\to O}=-W_{O\to A}WA→O​=−WO→A​ and WA→B=WA→O+WO→BW_{A\to B}=W_{A\to O}+W_{O\to B}WA→B​=WA→O​+WO→B​, and U(A)=U(O)−WO→AU(A)=U(O)-W_{O\to A}U(A)=U(O)−WO→A​, then −WA→B=U(B)−U(A)-W_{A\to B}=U(B)-U(A)−WA→B​=U(B)−U(A).
  2. Shifting an internal energy by a constant gives an internal energy.
  3. Under adiabatic accessibility, two internal energies differ by a constant.
  4. Under assumptions 1 to 4, an internal energy exists (normalized by U(O)=0U(O)=0U(O)=0).
  5. The Clausius form ΔU=Q−W\Delta U=Q-WΔU=Q−W holds for the residual heat.
  6. Adiabatic processes involve no heat.
  7. In an adynamic process (no work), Q=ΔUQ=\Delta UQ=ΔU.
  8. Heat does not depend on the additive constant in UUU.
  9. In a cyclic process, the net work done equals the net heat taken in.
  10. No adiabatic cyclic process produces net work (no perpetual motion machine of the first kind).

Significance

The goal makes precise the step in the mechanical approach where internal energy is defined from adiabatic work instead of being postulated. It shows which properties of the set of realizable processes are needed for the definition to make sense. Once UUU exists, the familiar consequences follow at once: the Clausius equation for every process, the heat-free character of adiabatic processes, Q=ΔUQ=\Delta UQ=ΔU for adynamic processes, the equality of work and heat over a cycle, and the impossibility of perpetual motion of the first kind. Milestones 5 to 10 record these.

The mathematics is elementary and the results are classical. The value of the formalization is that it states exactly the hypotheses under which "path-independent adiabatic work defines a state function" holds. The article itself notes the gaps: experimental evidence for independence from the order of stages is thin (Bailyn), and Münster observes that one cannot always go adiabatically in both directions between two states. Assumption 4 therefore asks only for one direction.

Difficulty

The only non-routine step is existence when accessibility holds in just one direction per state. One defines U(A)=−W(O→A)U(A)=-W(O\to A)U(A)=−W(O→A) or U(A)=W(A→O)U(A)=W(A\to O)U(A)=W(A→O), depending on which link exists. Showing that this choice is consistent, and that it gives ΔU=−W\Delta U=-WΔU=−W for an arbitrary adiabatic process A→BA\to BA→B, requires splitting into four cases according to how AAA and BBB are linked to OOO. In some of these cases the composite process is an adiabatic cycle, which must be compared with a null process. Without null processes, or without closure under composition, the naive definition is not well-defined.

Formalization scope

  • States form an arbitrary type σ\sigmaσ. Work is real-valued and is work done by the system (Clausius convention), so that ΔU=−W\Delta U=-WΔU=−W for adiabatic processes and ΔU=Q−W\Delta U=Q-WΔU=Q−W in general.
  • "Adiabatic" is a primitive label on processes, as adiabatic walls are primitive in the mechanical approach. Heat is not primitive: it is defined as the residual QU(p)=ΔU+WQ_U(p)=\Delta U+WQU​(p)=ΔU+W.
  • The physically realizable processes form a set P\mathcal PP. All hypotheses are stated about P\mathcal PP, never about every conceivable process.
  • The goal is not vacuous: assumptions 1 to 4 can all hold at once (for example, states R\mathbb RR, with adiabatic work from aaa to bbb equal to a−ba-ba−b).
  • Open systems, matter transfer, the extensivity statement U0=U1+U2U_0=U_1+U_2U0​=U1​+U2​, and the differential form dU=δQ−δWdU=\delta Q-\delta WdU=δQ−δW are out of scope for this first mission.

Selected references

  • Wikipedia, First law of thermodynamics, revision oldid=1366986255. https://en.wikipedia.org/w/index.php?title=First_law_of_thermodynamics&oldid=1366986255
  • C. Carathéodory, Untersuchungen über die Grundlagen der Thermodynamik, Mathematische Annalen 67 (1909), 355–386. https://ui.adsabs.harvard.edu/abs/1909MatAn..67..355C
  • M. Born, Kritische Betrachtungen zur traditionellen Darstellung der Thermodynamik, Physikalische Zeitschrift 22 (1921), 218–224.
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Partial Differential EquationsProbabilityStochastic Systems·Captain: Lucas

Black–Scholes Model: Pricing Formula, PDE and GreeksTextbook

Motivation

The Black–Scholes model (Black and Scholes, 1973; Merton, 1973) is the reference model for pricing European options. Its closed-form price, the Black–Scholes formula, is quoted daily by options markets, its partial derivatives (the Greeks) are the standard risk measures that trading desks limit and hedge, and the Black–Scholes equation is the prototype of the parabolic pricing PDEs that are solved numerically when no closed form exists. Merton and Scholes received the 1997 Nobel Memorial Prize in Economic Sciences for this work.

Timeline. Bachelier (1900) first applied Brownian motion to option pricing. In the 1960s Sprenkle, Boness, Samuelson and Merton refined the theory. Black and Scholes found the risk-neutral hedging argument in 1968 and published the formula in The Pricing of Options and Corporate Liabilities (Journal of Political Economy, 1973); Merton's paper of the same year extended the mathematical framework and coined the name.

Setting

Fix a strike K>0K>0K>0, an expiry TTT, a constant risk-free rate r∈Rr\in\mathbb Rr∈R and a constant volatility σ>0\sigma>0σ>0. At time t<Tt<Tt<T the time to maturity is τ=T−t>0\tau=T-t>0τ=T−t>0 and the spot price of the (non-dividend-paying) stock is S>0S>0S>0. Let

N(x)=12π∫−∞xe−z2/2 dz,N′(x)=12πe−x2/2N(x)=\frac1{\sqrt{2\pi}}\int_{-\infty}^x e^{-z^2/2}\,dz,\qquad N'(x)=\frac1{\sqrt{2\pi}}e^{-x^2/2}N(x)=2π​1​∫−∞x​e−z2/2dz,N′(x)=2π​1​e−x2/2

be the standard normal distribution and density functions, and set

d+=1στ[ln⁡SK+(r+σ22)τ],d−=d+−στ.d_+=\frac{1}{\sigma\sqrt{\tau}}\Big[\ln\frac SK+\Big(r+\frac{\sigma^2}2\Big)\tau\Big],\qquad d_-=d_+-\sigma\sqrt\tau .d+​=στ​1​[lnKS​+(r+2σ2​)τ],d−​=d+​−στ​.

The Black–Scholes call and put prices are

C(S,t)=N(d+)S−N(d−)Ke−rτ,P(S,t)=N(−d−)Ke−rτ−N(−d+)S.C(S,t)=N(d_+)S-N(d_-)Ke^{-r\tau},\qquad P(S,t)=N(-d_-)Ke^{-r\tau}-N(-d_+)S .C(S,t)=N(d+​)S−N(d−​)Ke−rτ,P(S,t)=N(−d−​)Ke−rτ−N(−d+​)S.

In the alternative (Black '76) parametrisation one uses the discount factor D=e−rτD=e^{-r\tau}D=e−rτ and the forward price F=erτSF=e^{r\tau}SF=erτS, with d±=1στ[ln⁡FK±12σ2τ]d_\pm=\frac1{\sigma\sqrt\tau}\big[\ln\frac FK\pm\frac12\sigma^2\tau\big]d±​=στ​1​[lnKF​±21​σ2τ], and C=D[N(d+)F−N(d−)K]C=D[N(d_+)F-N(d_-)K]C=D[N(d+​)F−N(d−​)K]. Under the risk-neutral measure the terminal price is ST=Sexp⁡((r−12σ2)τ+στ Z)S_T=S\exp\big((r-\tfrac12\sigma^2)\tau+\sigma\sqrt\tau\,Z\big)ST​=Sexp((r−21​σ2)τ+στ​Z) with ZZZ standard normal.

Formalization targets

Goal: the formula solves the Black–Scholes equation

On the domain {S>0, t<T}\{S>0,\ t<T\}{S>0, t<T} the call price CCC is C∞C^\inftyC∞ and satisfies

∂C∂t+12σ2S2∂2C∂S2+rS∂C∂S−rC=0,\frac{\partial C}{\partial t}+\frac12\sigma^2S^2\frac{\partial^2C}{\partial S^2}+rS\frac{\partial C}{\partial S}-rC=0,∂t∂C​+21​σ2S2∂S2∂2C​+rS∂S∂C​−rC=0,

together with the boundary and terminal conditions C(S,t)→0C(S,t)\to0C(S,t)→0 as S→0+S\to0^+S→0+, C(S,t)−(S−Ke−r(T−t))→0C(S,t)-(S-Ke^{-r(T-t)})\to0C(S,t)−(S−Ke−r(T−t))→0 as S→∞S\to\inftyS→∞, and C(S,t)→max⁡{S−K,0}C(S,t)\to\max\{S-K,0\}C(S,t)→max{S−K,0} as t→T−t\to T^-t→T−.

Milestones

  1. The density N′N'N′ is the derivative of NNN.
  2. The alternative (forward) formulation of the call and put prices.
  3. Put–call parity, P=Ke−rτ−S+CP=Ke^{-r\tau}-S+CP=Ke−rτ−S+C, and its forward form C−P=D(F−K)C-P=D(F-K)C−P=D(F−K).
  4. The Greeks table: Delta, Gamma, Vega, Theta and Rho for calls and puts.
  5. Risk-neutral pricing: C=e−rτ E[max⁡(ST−K,0)]C=e^{-r\tau}\,\mathbb E[\max(S_T-K,0)]C=e−rτE[max(ST​−K,0)].
  6. Binary options: cash-or-nothing values e−rτN(±d−)e^{-r\tau}N(\pm d_-)e−rτN(±d−​) and asset-or-nothing values SN(±d+)SN(\pm d_+)SN(±d+​).

Significance

The result. The goal is the statement that ties the model's two faces together: the closed-form price is a classical solution of the pricing PDE with the payoff as terminal datum. The Greeks are what hedging strategies are built from (delta hedging is the core of the model's replication argument), put–call parity is the basic no-arbitrage relation, and the risk-neutral and binary-option identities are the probabilistic reading of the two terms in the formula.

Formalizing it. All results here are classical and proved in textbooks (e.g. Hull, Options, Futures, and Other Derivatives). The work is formalization: building a reusable, machine-checked library for the normal distribution function, the Black–Scholes price and its sensitivities, and Gaussian expectations of log-normal payoffs, on top of Mathlib's real analysis and its Gaussian measure gaussianReal.

Difficulty

Each identity is elementary on paper, but the calculus is long: every Greek requires differentiating N∘d±N\circ d_\pmN∘d±​ through a logarithm, a square root and a quotient, and the simplifications rest on the identity SN′(d+)=Ke−rτN′(d−)SN'(d_+)=Ke^{-r\tau}N'(d_-)SN′(d+​)=Ke−rτN′(d−​). The limits in the goal need Gaussian tail estimates (e.g. SN(−d+)→0SN(-d_+)\to0SN(−d+​)→0 as S→∞S\to\inftyS→∞, where SSS grows while N(−d+)N(-d_+)N(−d+​) decays). The risk-neutral identities require computing Gaussian integrals over half-lines with an exponential weight, i.e. a change of variables shifting the mean of the normal distribution.

Formalization scope

All objects are real-valued and deterministic: NNN is defined by the integral formula above (a Lebesgue integral over (−∞,x](-\infty,x](−∞,x]), N′N'N′ by its closed form, and prices by the formulas, as functions of (S,t)(S,t)(S,t) with parameters (K,r,σ,T)(K,r,\sigma,T)(K,r,σ,T). Partial derivatives are stated with HasDerivAt (genuine differentiability plus the value), except in the goal's PDE, where deriv is used together with an explicit C∞C^\inftyC∞ clause on the open domain. Each theorem carries the standing assumptions K>0K>0K>0, σ>0\sigma>0σ>0, S>0S>0S>0, t<Tt<Tt<T where they are needed; the parity identities hold without them and are stated unconditionally. At S=0S=0S=0 and t=Tt=Tt=T the formula is undefined in the source, so the boundary and terminal conditions are stated as one-sided limits rather than values. Risk-neutral expectations are integrals against the standard Gaussian gaussianReal 0 1 of an explicit log-normal terminal price; no stochastic calculus (Itô integrals, SDEs, Girsanov, Feynman–Kac) is required or formalized. The dividend-paying extensions, American options and the perpetual put are out of scope; binary options are formalized for the non-dividend case q=0q=0q=0.

Contributions of reusable lemmas (derivative of NNN, symmetry N(x)+N(−x)=1N(x)+N(-x)=1N(x)+N(−x)=1, limits of NNN at ±∞\pm\infty±∞, Gaussian half-line integrals) are welcome.

Selected references

  • F. Black, M. Scholes, The Pricing of Options and Corporate Liabilities, Journal of Political Economy 81(3), 1973. https://doi.org/10.1086/260062
  • R. C. Merton, Theory of Rational Option Pricing, Bell Journal of Economics and Management Science 4(1), 1973. https://doi.org/10.2307/3003143
  • J. C. Hull, Options, Futures, and Other Derivatives, Pearson.
  • Wikipedia, Black–Scholes model. https://en.wikipedia.org/wiki/Black%E2%80%93Scholes_model
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Number Theory·Captain: Lucas

Dirichlet's Unit Theorem and the RegulatorTextbook

Motivation

The units of a ring of algebraic integers control much of the arithmetic of a number field. They decide when two generators of the same principal ideal differ, they enter the analytic class number formula through the regulator, and for real quadratic fields they are the solutions of Pell's equation x2−dy2=±1x^2 - dy^2 = \pm 1x2−dy2=±1. Dirichlet's unit theorem (Dirichlet, 1846) determines the structure of this unit group completely: it is finitely generated, and its rank is computed from the way the field embeds into R\mathbb RR and C\mathbb CC. With the finiteness of the class group, it is one of the two basic finiteness theorems of algebraic number theory and appears in every introductory text on the subject.

This mission follows the account of the theorem, the regulator and its standard examples given in the Wikipedia article Dirichlet's unit theorem (https://en.wikipedia.org/wiki/Dirichlet%27s_unit_theorem).

Setting

A number field KKK is a field containing Q\mathbb QQ with finite dimension n=[K:Q]n = [K:\mathbb Q]n=[K:Q] as a Q\mathbb QQ-vector space. Its ring of integers OK\mathcal O_KOK​ consists of the elements of KKK that are roots of monic polynomials with integer coefficients, and its unit group OK×\mathcal O_K^\timesOK×​ is the group of invertible elements of OK\mathcal O_KOK​.

The field KKK has exactly nnn field embeddings σ:K→C\sigma : K \to \mathbb Cσ:K→C. Let r1r_1r1​ be the number of embeddings with image in R\mathbb RR, and r2r_2r2​ the number of pairs of complex-conjugate non-real embeddings, so that n=r1+2r2n = r_1 + 2r_2n=r1​+2r2​. Equivalently, r1r_1r1​ and r2r_2r2​ count the real and complex infinite places www of KKK, i.e. the absolute values ∣x∣w=∣σ(x)∣|x|_w = |\sigma(x)|∣x∣w​=∣σ(x)∣. Write Nw=1N_w = 1Nw​=1 for a real place and Nw=2N_w = 2Nw​=2 for a complex place.

The rank of an abelian group is the largest number of elements that are independent over Z\mathbb ZZ. For OK×\mathcal O_K^\timesOK×​ this is the largest number of multiplicatively independent units. Units of finite order are exactly the roots of unity in KKK.

Put r=r1+r2−1r = r_1 + r_2 - 1r=r1​+r2​−1. If u1,…,uru_1, \dots, u_ru1​,…,ur​ generate OK×\mathcal O_K^\timesOK×​ modulo roots of unity, the r×(r+1)r \times (r+1)r×(r+1) matrix (Nwlog⁡∣ui∣w)\big(N_w \log |u_i|_w\big)(Nw​log∣ui​∣w​) has every row summing to 000. The absolute value RRR of the determinant of the square matrix left after deleting any one column is the regulator of KKK.

Formalization targets

Goal: Dirichlet's unit theorem

OK× is finitely generated and rank⁡OK×=r1+r2−1.\mathcal O_K^\times \text{ is finitely generated and } \operatorname{rank}\mathcal O_K^\times = r_1 + r_2 - 1.OK×​ is finitely generated and rankOK×​=r1​+r2​−1.

Milestones

  1. The signature identity n=r1+2r2n = r_1 + 2r_2n=r1​+2r2​. If K/QK/\mathbb QK/Q is Galois, then r1=0r_1 = 0r1​=0 or r2=0r_2 = 0r2​=0.
  2. Two other ways to compute (r1,r2)(r_1, r_2)(r1​,r2​): real and non-real roots of the minimal polynomial of a primitive element, and R⊗QK≅Rr1×Cr2\mathbb R \otimes_{\mathbb Q} K \cong \mathbb R^{r_1} \times \mathbb C^{r_2}R⊗Q​K≅Rr1​×Cr2​.
  3. Quadratic fields have unit rank 111 when real and 000 when imaginary. The rank is positive except for Q\mathbb QQ and imaginary quadratic fields.
  4. Torsion: the torsion units are the roots of unity and form a finite cyclic group. When KKK has a real embedding they are ±1\pm 1±1.
  5. Rank equality in a proper extension L/KL/KL/K holds exactly when KKK is totally real and L/KL/KL/K is a totally complex quadratic extension.
  6. The unit theorem for an arbitrary order O⊆OK\mathcal O \subseteq \mathcal O_KO⊆OK​.
  7. The logarithmic picture: ∑wNwlog⁡∣u∣w=0\sum_w N_w \log |u|_w = 0∑w​Nw​log∣u∣w​=0 for every unit, and the vectors (Nwlog⁡∣u∣w)w\big(N_w \log |u|_w\big)_w(Nw​log∣u∣w​)w​ form a lattice in the hyperplane of coordinate sum 000.
  8. The regulator does not depend on the generators or on the deleted column, and it is positive.
  9. Examples: Reg⁡=1\operatorname{Reg} = 1Reg=1 for Q\mathbb QQ and imaginary quadratic fields. Reg⁡(Q(5))=log⁡1+52\operatorname{Reg}(\mathbb Q(\sqrt5)) = \log\frac{1+\sqrt5}{2}Reg(Q(5​))=log21+5​​. For the cyclic cubic field defined by x3+x2−2x−1x^3 + x^2 - 2x - 1x3+x2−2x−1, the fundamental units are α2+α−1\alpha^2 + \alpha - 1α2+α−1 and 2−α22 - \alpha^22−α2, and Reg⁡≈0.5255\operatorname{Reg} \approx 0.5255Reg≈0.5255.

Significance

The result itself. The unit theorem gives OK×≅μ(K)×Zr1+r2−1\mathcal O_K^\times \cong \mu(K) \times \mathbb Z^{r_1 + r_2 - 1}OK×​≅μ(K)×Zr1​+r2​−1. This is the input for the analytic class number formula, where the regulator appears next to the class number. It also yields the finiteness of solutions of norm-form and SSS-unit problems and the structure of solutions of Pell's equation. It is the model for Hasse and Chevalley's SSS-unit theorem and for Leopoldt's conjecture on ppp-adic regulators.

Formalizing it. The theorem itself is classical and has already been formalized: Mathlib contains the unit group's rank, a system of fundamental units and a regulator in its NumberField.Units development. This mission adds the surrounding statements of the source article as explicit, independently checkable targets. These are the alternative descriptions of the signature, the rank in quadratic fields and in extensions, the unit theorem for non-maximal orders, the well-definedness of the regulator in the generator-free form given in the article, and the worked examples. The examples involve explicit numerical regulator values that are not in the library.

Difficulty

The upper bound on the rank follows by showing that the logarithmic image of the units is discrete. The hard part is the lower bound: one must produce r1+r2−1r_1 + r_2 - 1r1​+r2​−1 independent units. This requires constructing units of prescribed size at the infinite places. The obvious approach of writing down units explicitly does not work in general. The standard route uses Minkowski's geometry of numbers. The examples carry their own difficulty: showing that given units are fundamental and pinning a regulator to four decimal places takes certified bounds, not just exhibiting units. The statement for orders requires passing between O×\mathcal O^\timesO× and OK×\mathcal O_K^\timesOK×​ through a finite-index argument.

Formalization scope

Statements are in Lean 4 over Mathlib, in the namespace DirichletUnitTheorem. They use Mathlib's notions directly: NumberField, 𝓞 K, InfinitePlace, nrRealPlaces/nrComplexPlaces for r1r_1r1​/r2r_2r2​, InfinitePlace.mult for NwN_wNw​, IsTotallyReal/IsTotallyComplex for real/imaginary quadratic fields, and NumberField.Units.regulator for the regulator in the example milestones. The rank is Module.rank ℤ of the additive version of the unit group. This is a cardinal, so finite generation and the rank are stated separately. An order is a subring of OK\mathcal O_KOK​ of finite additive index. Approximate numerical values from the source are encoded as open intervals.

Units of finite order are written with IsOfFinOrder, so no statement depends on a particular torsion API. The goal is not trivialized by the truncated subtraction in r1+r2−1r_1 + r_2 - 1r1​+r2​−1, because r1+r2≥1r_1 + r_2 \ge 1r1​+r2​≥1 always holds.

Welcome contributions include proofs that bridge to the existing Mathlib development, certified numerical bounds for regulators, and the order and extension statements, which are reusable beyond this mission.

Selected references

  • Wikipedia contributors, Dirichlet's unit theorem, Wikipedia. https://en.wikipedia.org/wiki/Dirichlet%27s_unit_theorem
  • J. Neukirch, Algebraic Number Theory, Grundlehren 322, Springer, 1999, Chapter I §7. https://doi.org/10.1007/978-3-662-03983-0
  • H. Cohen, A Course in Computational Algebraic Number Theory, GTM 138, Springer, 1993, Table B.4. https://doi.org/10.1007/978-3-662-02945-9
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Economics·Captain: Lucas

Supply and Demand I: Comparative Statics of Market EquilibriumTextbook

Motivation

Supply and demand is the basic model of price determination in a perfectly competitive market: holding everything else fixed, the price of a good adjusts until the quantity buyers want equals the quantity sellers offer. The model is the standard first chapter of microeconomics, it underlies partial-equilibrium policy analysis (taxes, subsidies, price controls), and it is applied to labour markets (with the wage as the price) and money markets (with the interest rate as the price). See the Wikipedia article, which is the source of this mission.

Timeline. Demand curves were first drawn by Cournot (1838); supply curves were added by Fleeming Jenkin (1870), who also drew the first comparative-statics diagrams of a curve shift; Marshall's Principles of Economics (1890) popularised the "Marshallian cross". Qualitative versions of the comparative-statics law are much older: Ibn Taymiyyah (14th century) wrote that "if desire for goods increases while its availability decreases, its price rises".

Setting

Prices and quantities are real numbers. A supply curve is a function S:R→RS:\mathbb R\to\mathbb RS:R→R giving the quantity supplied at each price, and a demand curve is a function D:R→RD:\mathbb R\to\mathbb RD:R→R giving the quantity demanded. A set I⊆RI\subseteq\mathbb RI⊆R of admissible prices is fixed (for example all reals, or the positive reals). Supply is upward-sloping: SSS is strictly increasing on III. Demand is downward-sloping (the law of demand): DDD is strictly decreasing on III.

A pair (p,q)(p,q)(p,q) is a market equilibrium of (S,D)(S,D)(S,D), written IsEquilibrium(S,D,p,q)\mathrm{IsEquilibrium}(S,D,p,q)IsEquilibrium(S,D,p,q), when

D(p)=qandS(p)=q,D(p)=q \quad\text{and}\quad S(p)=q,D(p)=qandS(p)=q,

i.e. the market clears at price ppp with quantity qqq transacted.

An increase in demand (a right shift of the demand curve) from D1D_1D1​ to D2D_2D2​ means D1(p)<D2(p)D_1(p)<D_2(p)D1​(p)<D2​(p) for every admissible price ppp; an increase in supply from S1S_1S1​ to S2S_2S2​ means S1(p)<S2(p)S_1(p)<S_2(p)S1​(p)<S2​(p) for every admissible price.

The market curve of finitely many individual curves fif_ifi​, i∈si\in si∈s, is their horizontal sum p↦∑i∈sfi(p)p\mapsto\sum_{i\in s}f_i(p)p↦∑i∈s​fi​(p). The point elasticity of a curve QQQ at PPP is Q′(P) P/Q(P)Q'(P)\,P/Q(P)Q′(P)P/Q(P). The article's example curves are Q(P)=3P−6Q(P)=3P-6Q(P)=3P−6 and Q(P)=5P0.5Q(P)=5P^{0.5}Q(P)=5P0.5 (supply) and Q(P)=32−2PQ(P)=32-2PQ(P)=32−2P and Q(P)=3P−2Q(P)=3P^{-2}Q(P)=3P−2 (demand).

Formalization targets

Goal: comparative statics of a curve shift

For upward-sloping supply and downward-sloping demand on III, with equilibria at admissible prices:

  1. if demand increases from D1D_1D1​ to D2D_2D2​ (supply SSS fixed), equilibria (p1,q1)(p_1,q_1)(p1​,q1​) of (S,D1)(S,D_1)(S,D1​) and (p2,q2)(p_2,q_2)(p2​,q2​) of (S,D2)(S,D_2)(S,D2​) satisfy
p1<p2andq1<q2;p_1<p_2\quad\text{and}\quad q_1<q_2;p1​<p2​andq1​<q2​;
  1. if supply increases from S1S_1S1​ to S2S_2S2​ (demand DDD fixed), equilibria (p1,q1)(p_1,q_1)(p1​,q1​) of (S1,D)(S_1,D)(S1​,D) and (p2,q2)(p_2,q_2)(p2​,q2​) of (S2,D)(S_2,D)(S2​,D) satisfy
p2<p1andq1<q2.p_2<p_1\quad\text{and}\quad q_1<q_2.p2​<p1​andq1​<q2​.

The corresponding statements for decreases (left shifts) are the same statements with the indices 1,21,21,2 exchanged.

Milestones

  • uniqueness of the equilibrium for strictly monotone curves;
  • the demand-shift and supply-shift laws separately;
  • the Ibn Taymiyyah law for simultaneous shifts: demand up and supply down raises the price, and demand down and supply up lowers it;
  • horizontal aggregation preserves the slope of supply and demand curves;
  • the article's example curves have the stated slopes, the isoelastic curves have the stated log-linear forms, and their point elasticities are the constants 0.50.50.5 and −2-2−2.

Significance

The comparative-statics laws are the qualitative predictions that make the supply-and-demand model usable: they say in which direction price and quantity move after a change in a non-price determinant (tastes, incomes, input costs, technology). The simultaneous-shift law is the precise form of the qualitative statement quoted above, and it also records what the model does not predict (the direction of the quantity change is left open).

These results are classical and elementary. The point of this mission is a clean, reusable formal vocabulary for partial-equilibrium market models (equilibrium, curve shifts, market curves, elasticity) on which later missions about taxes, surplus, and elasticity can build.

Difficulty

The mathematics is elementary; the care is in the modelling. Two traps: assuming the equilibria exist and lie in the admissible price set is necessary (the article's linear supply curve is negative for P<2P<2P<2, and the isoelastic curves are only meaningful for P>0P>0P>0); and the law of demand or of supply cannot be dropped, since for an upward-sloping demand curve (Veblen or Giffen goods, discussed in the article) the comparative-statics conclusions can fail.

Formalization scope

All curves are total functions R→R\mathbb R\to\mathbb RR→R; slope assumptions are imposed only on the admissible set III, an arbitrary set of reals, and every equilibrium price is assumed to lie in III. Strict monotonicity is used for both supply and demand, as in the article's figures and its law of demand. Existence of an equilibrium is not asserted; the statements are about given equilibria. Real powers P0.5P^{0.5}P0.5 and P−2P^{-2}P−2 are Mathlib's Real.rpow, and statements about them are restricted to P>0P>0P>0. The point elasticity uses Mathlib's deriv.

The definitions live in a single definition file, SupplyDemand_Model, in the namespace SupplyDemand, shared by all statements.

Selected references

  • Wikipedia contributors, "Supply and demand", revision 1378800284, https://en.wikipedia.org/w/index.php?title=Supply_and_demand&oldid=1378800284
  • A. A. Cournot, Recherches sur les principes mathématiques de la théorie des richesses, 1838.
  • F. Jenkin, "The Graphical Representation of the Laws of Supply and Demand, and their Application to Labour", in Recess Studies, 1870, https://books.google.com/books?id=NC5BAAAAIAAJ
  • A. Marshall, Principles of Economics, Macmillan, 1890.
  • T. M. Humphrey, "Marshallian Cross Diagrams and their Uses before Alfred Marshall", Economic Review (Federal Reserve Bank of Richmond), Mar/Apr 1992, 3–23.
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Economics·Captain: Lucas

Comparative Advantage I: Gains from Trade in the Ricardian ModelTextbook

Motivation

Comparative advantage is the principle that two parties can both gain from trade even when one of them is more productive at producing every good. It is usually credited to David Ricardo's On the Principles of Political Economy and Taxation (1817), with earlier formulations in an anonymous 1814 pamphlet and in Robert Torrens' Essay on the External Corn Trade (1815). It is widely described as one of the most powerful yet counter-intuitive insights in economics, and it underlies the standard argument that trade patterns are driven by relative, not absolute, productivity.

A short timeline of the two-country, two-good theory:

  • 1776 — Adam Smith, The Wealth of Nations: trade based on absolute advantage.
  • 1814–1815 — anonymous pamphlet Considerations on the Importation of Foreign Corn; Torrens, Essay on the External Corn Trade: first formulations of comparative advantage.
  • 1817 — Ricardo's England/Portugal example with cloth and wine.
  • 1833 — William Whewell publishes the first mathematical Ricardian model.
  • 1930 — Gottfried Haberler restates comparative advantage in terms of opportunity costs and production possibility curves.

Setting

The Ricardian model has two countries, Home and Foreign, and two goods, cloth and wine. Labour is the only factor of production; it moves freely between sectors inside a country but not between countries. Home has a labour force L>0L>0L>0; producing one unit of cloth takes aLC>0a_{LC}>0aLC​>0 units of labour and one unit of wine takes aLW>0a_{LW}>0aLW​>0. Foreign's data are written with a prime: L′L'L′, aLC′a'_{LC}aLC′​, aLW′a'_{LW}aLW′​.

Home has a comparative advantage in cloth when its opportunity cost of cloth in terms of wine is lower than Foreign's:

aLCaLW<aLC′aLW′,\frac{a_{LC}}{a_{LW}}<\frac{a'_{LC}}{a'_{LW}},aLW​aLC​​<aLW′​aLC′​​,

which is the same as saying that Home is relatively more productive in cloth, aLC/aLC′<aLW/aLW′a_{LC}/a'_{LC}<a_{LW}/a'_{LW}aLC​/aLC′​<aLW​/aLW′​. Nothing is assumed about absolute productivity.

In autarky a country can produce and consume any bundle (QC,QW)≥0(Q_C,Q_W)\ge 0(QC​,QW​)≥0 with aLCQC+aLWQW≤La_{LC}Q_C+a_{LW}Q_W\le LaLC​QC​+aLW​QW​≤L. Under free trade both goods sell at world prices PC,PW>0P_C,P_W>0PC​,PW​>0; the wage in the cloth sector is PC/aLCP_C/a_{LC}PC​/aLC​ and in the wine sector PW/aLWP_W/a_{LW}PW​/aLW​, and workers move to the sector with the higher wage. A country that produces only cloth and trades at the world relative price PC/PWP_C/P_WPC​/PW​ can consume any bundle with aLCQC+aLC(PW/PC)QW≤La_{LC}Q_C+a_{LC}(P_W/P_C)Q_W\le LaLC​QC​+aLC​(PW​/PC​)QW​≤L; a country that produces only wine can consume any bundle with aLW(PC/PW)QC+aLWQW≤La_{LW}(P_C/P_W)Q_C+a_{LW}Q_W\le LaLW​(PC​/PW​)QC​+aLW​QW​≤L.

Formalization targets

Goal: gains from trade

If Home has a comparative advantage in cloth and the world relative price lies between the two autarky prices,

aLCaLW≤PCPW≤aLC′aLW′,\frac{a_{LC}}{a_{LW}}\le\frac{P_C}{P_W}\le\frac{a'_{LC}}{a'_{LW}},aLW​aLC​​≤PW​PC​​≤aLW′​aLC′​​,

then Home's autarky set is contained in its consumption set when it specializes in cloth, and Foreign's autarky set is contained in its consumption set when it specializes in wine. When the corresponding inequality is strict, the inclusion is strict: the country can consume bundles it could not produce itself.

Milestones

  1. The two forms of the comparative-advantage assumption are equivalent.
  2. The five-case description of world relative supply: who specializes in what at each relative price.
  3. As long as relative demand is finite, the equilibrium relative price lies between the two autarky prices.
  4. The autarky production possibility frontier QC=L/aLC−(aLW/aLC)QWQ_C=L/a_{LC}-(a_{LW}/a_{LC})Q_WQC​=L/aLC​−(aLW​/aLC​)QW​.
  5. The free-trade consumption possibility frontier QC=L/aLC−(PW/PC)QWQ_C=L/a_{LC}-(P_W/P_C)Q_WQC​=L/aLC​−(PW​/PC​)QW​ lies on or above the autarky frontier.
  6. Terms of trade: specializing in a good leaves a country no worse off exactly when the world price lies on the right side of its own opportunity cost.
  7. Ricardo's numerical example: absolute and comparative advantage, the gain in world output from specialization, and terms of trade between 5/65/65/6 and 9/89/89/8 units of wine per unit of cloth.

Significance

The result is the textbook form of the classical argument for specialization and trade: the gain does not depend on either country being absolutely more productive, only on a difference in relative labour costs. The price-bound milestone says where world prices can settle, and the terms-of-trade milestone says that both countries gain exactly at prices between their opportunity costs. Ricardo's numbers make the general statements concrete.

These are classical results with elementary proofs. The value of the mission is a reusable, precisely stated Ricardian model — definitions of countries, autarky sets, trade consumption sets and competitive outputs — on which later missions in this series (many goods, many countries, the Dornbusch–Fischer–Samuelson continuum, Haberler's production possibility curves) can build.

Difficulty

There is no deep obstacle; the work is in stating the model faithfully. The obvious shortcut is to compare autarky and trade only at the two corner bundles, or to drop the wage-based description of who produces what and simply assume each country specializes. The milestones instead derive specialization from the wage comparison, so the five-case relative-supply statement has to cover the boundary prices where workers are indifferent and output is not unique.

Formalization scope

All quantities are real numbers. A country is a structure carrying LLL, aLCa_{LC}aLC​, aLWa_{LW}aLW​ and proofs that all three are positive, so no unit labour requirement can be zero. Prices PC,PWP_C,P_WPC​,PW​ are explicit arguments with positivity hypotheses wherever they are divided by. Bundles are pairs (QC,QW)∈R2(Q_C,Q_W)\in\mathbb R^2(QC​,QW​)∈R2. A competitive output is a bundle with full employment (aLCQC+aLWQW=La_{LC}Q_C+a_{LW}Q_W=LaLC​QC​+aLW​QW​=L, QC,QW≥0Q_C,Q_W\ge 0QC​,QW​≥0) in which a sector produces only if its wage is at least the other sector's wage. Relative demand is not modelled as a function; the price bound is stated for any competitive outputs whose world cloth and world wine supplies are both strictly positive (finite, nonzero relative supply, as market clearing with a finite positive relative demand requires). The comparative-advantage hypothesis is kept in the goal as the section's standing assumption, although the price-bound hypotheses imply its non-strict form.

Contributions welcome: proofs of the milestones and the goal, and follow-up missions extending the model to many goods or many countries.

Selected references

  • Wikipedia contributors, Comparative advantage, Wikipedia (PDF export supplied with the proposal). https://en.wikipedia.org/wiki/Comparative_advantage
  • D. Ricardo, On the Principles of Political Economy and Taxation, John Murray, London, 1817. https://www.econlib.org/library/Ricardo/ricP.html
  • P. Krugman, M. Obstfeld, M. Melitz, International Economics: Theory and Policy, Pearson (chapter on the Ricardian model).
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ProbabilityStatistics·Captain: Lucas

Zipf's Law: the Zipf Distribution, its Infinite Extension and Related LawsTextbook

Motivation

Zipf's law is the empirical observation that when a set of measured values is sorted in decreasing order, the value of the nnn-th entry is often approximately inversely proportional to nnn. Its best-known instance is word frequency in natural language: in the Brown Corpus the most frequent word, "the", accounts for nearly 7%7\%7% of all word occurrences, the second, "of", for slightly over 3.5%3.5\%3.5%, and so on. The same rank–size relation has been reported for city populations (Auerbach 1913), firm sizes (Axtell 2001), and many other data sets; it is named after the linguist George Kingsley Zipf (1932, 1935, 1949) and remains a central concept of quantitative linguistics (Piantadosi 2014).

In mathematical statistics the law is formalized as the Zipf distribution, a family of discrete probability distributions whose rank–frequency relation is an inverse power law, together with its relatives: the zeta distribution (Lotka's law), the Zipf–Mandelbrot law and the Yule–Simon distribution. Several generative explanations — random typing (Miller 1957, Li 1992) and preferential attachment — produce power laws by provable mechanisms.

Timeline of the results formalized here:

  • 1913–1932 — Auerbach (city sizes), Estoup (1916), Dewey (1923), Condon (1928) and Zipf (1932) observe the inverse rank–frequency relation.
  • 1957 — Miller: a power law emerges in randomly generated texts (doi:10.2307/1419346).
  • 1992 — Li: in random texts with equiprobable letters, word frequency follows Zipf's macro-trend (doi:10.1109/18.165464).

Setting

For a real exponent sss and an integer N≥1N \ge 1N≥1, the generalized harmonic number is

HN,s=∑k=1N1ks,HN=HN,1.H_{N,s} = \sum_{k=1}^{N}\frac{1}{k^s}, \qquad H_N = H_{N,1}.HN,s​=k=1∑N​ks1​,HN​=HN,1​.

The Zipf distribution on NNN elements with exponent sss assigns to the element of rank k∈{1,…,N}k \in\{1,\dots,N\}k∈{1,…,N} the probability

f(k;N,s)=1HN,s 1ks.f(k;N,s) = \frac{1}{H_{N,s}}\,\frac{1}{k^{s}} .f(k;N,s)=HN,s​1​ks1​.

The classical Zipf law is s=1s=1s=1. The source lists the parameter range s≥0s\ge0s≥0, N∈{1,2,3,… }N\in\{1,2,3,\dots\}N∈{1,2,3,…}.

The Riemann zeta function is ζ(s)=∑k≥1k−s\zeta(s)=\sum_{k\ge1}k^{-s}ζ(s)=∑k≥1​k−s for s>1s>1s>1. The Hurwitz zeta function is ζ(s,a)=∑n≥0(n+a)−s\zeta(s,a)=\sum_{n\ge0}(n+a)^{-s}ζ(s,a)=∑n≥0​(n+a)−s. The Zipf–Mandelbrot law on ranks k=1,2,…k=1,2,\dotsk=1,2,… with shift qqq and exponent sss is f(k;q,s)=1C1(k+q)sf(k;q,s)=\frac{1}{C}\frac{1}{(k+q)^s}f(k;q,s)=C1​(k+q)s1​ with C=ζ(s,q+1)C=\zeta(s,q+1)C=ζ(s,q+1). The Yule–Simon distribution with parameter ρ>0\rho>0ρ>0 is f(k;ρ)=ρ B(k,ρ+1)=ρ Γ(k)Γ(ρ+1)/Γ(k+ρ+1)f(k;\rho)=\rho\,B(k,\rho+1)=\rho\,\Gamma(k)\Gamma(\rho+1)/\Gamma(k+\rho+1)f(k;ρ)=ρB(k,ρ+1)=ρΓ(k)Γ(ρ+1)/Γ(k+ρ+1), k=1,2,…k = 1, 2, \dotsk=1,2,….

Formalization targets

Goal — the infinite-item extension

For s≥0s \ge 0s≥0:

∑k≥11ks<∞  ⟺  s>1;s>1  ⟹  HN,s→N→∞ζ(s);s≤1  ⟹  HN,s→N→∞∞.\sum_{k\ge1}\frac1{k^s}<\infty \iff s>1;\qquad s>1 \implies H_{N,s}\xrightarrow[N\to\infty]{}\zeta(s);\qquad s\le1 \implies H_{N,s}\xrightarrow[N\to\infty]{}\infty .k≥1∑​ks1​<∞⟺s>1;s>1⟹HN,s​N→∞​ζ(s);s≤1⟹HN,s​N→∞​∞.

That is, the generalized Zipf distribution extends to infinitely many items exactly when s>1s>1s>1, in which case the normalizing constant becomes Riemann's zeta function.

Milestones

  1. Normalization: ∑k=1Nf(k;N,s)=1\sum_{k=1}^N f(k;N,s)=1∑k=1N​f(k;N,s)=1.
  2. CDF: ∑k=1nf(k;N,s)=Hn,s/HN,s\sum_{k=1}^n f(k;N,s)=H_{n,s}/H_{N,s}∑k=1n​f(k;N,s)=Hn,s​/HN,s​ for n≤Nn\le Nn≤N.
  3. Mean: ∑kk f(k;N,s)=HN,s−1/HN,s\sum_{k} k\,f(k;N,s)=H_{N,s-1}/H_{N,s}∑k​kf(k;N,s)=HN,s−1​/HN,s​.
  4. Variance: HN,s−2HN,s−HN,s−12HN,s2\frac{H_{N,s-2}}{H_{N,s}}-\frac{H_{N,s-1}^2}{H_{N,s}^2}HN,s​HN,s−2​​−HN,s2​HN,s−12​​.
  5. Entropy: sHN,s∑k=1Nln⁡kks+ln⁡HN,s\frac{s}{H_{N,s}}\sum_{k=1}^N\frac{\ln k}{k^s}+\ln H_{N,s}HN,s​s​∑k=1N​kslnk​+lnHN,s​.
  6. Mode: rank 111 is a most probable element (for s≥0s \ge 0s≥0).
  7. Ratio: f(1;N,s)/f(n;N,s)=nsf(1;N,s)/f(n;N,s)=n^sf(1;N,s)/f(n;N,s)=ns — "the most common word occurs about nnn times the nnn-th most common one" when s=1s = 1s=1.
  8. Log–log linearity: ln⁡f(k;N,s)=−sln⁡k−ln⁡HN,s\ln f(k;N,s) = -s\ln k-\ln H_{N,s}lnf(k;N,s)=−slnk−lnHN,s​, an affine function of ln⁡k\ln klnk with slope −s-s−s.
  9. Zipf–Mandelbrot: with C=ζ(s,q+1)C=\zeta(s,q+1)C=ζ(s,q+1) the law is a probability distribution (s>1s>1s>1, q≥0q\ge0q≥0).
  10. Yule–Simon tail: f(k;ρ)∼C/kρ+1f(k;\rho)\sim C/k^{\rho+1}f(k;ρ)∼C/kρ+1 for some constant C>0C>0C>0.
  11. Random typing (Li): word probability is bounded above and below by a power of the rank.
  12. Benford connection: the leading digits of a Zipf (s=1s=1s=1) random rank follow Benford's law as N→∞N\to\inftyN→∞.

Significance

The goal pins down exactly when "Zipf's law with infinitely many items" makes sense, and identifies the resulting distribution (the zeta distribution) with Riemann's zeta function. The milestones are the infobox facts that statisticians use when fitting Zipf models (CDF, mean, variance, entropy, mode), the log–log diagnostic used to test data against the law, two of the related laws the source lists (Zipf–Mandelbrot, Yule–Simon), one of the generative explanations (random typing), and the stated link to Benford's law.

The results are classical; the work is formalizing them. Most milestones are finite algebra about HN,sH_{N,s}HN,s​; the goal, the Yule–Simon tail, the random-typing bound and the Benford connection need analysis.

Difficulty

The finite identities are routine once the support conventions are fixed. The analytic content is concentrated in four places. The goal needs the ppp-series test and the identification of the limit with Mathlib's complex riemannZeta, which is defined by analytic continuation rather than by the series. The Yule–Simon tail needs the asymptotics Γ(k)/Γ(k+a)∼k−a\Gamma(k)/\Gamma(k+a)\sim k^{-a}Γ(k)/Γ(k+a)∼k−a. The random-typing bound requires controlling the rank of a word through the number of strictly shorter words, uniformly over every rank order compatible with the probabilities. The Benford connection requires comparing the harmonic sums over each block of integers with a fixed leading digit with ln⁡(1+1/d)\ln(1+1/d)ln(1+1/d), with an error that is negligible against HN∼ln⁡NH_N\sim\ln NHN​∼lnN.

Formalization scope

  • HN,sH_{N,s}HN,s​ uses a real exponent (Real.rpow); H0,s=0H_{0,s}=0H0,s​=0.
  • zipfPMF N s k is defined for every natural kkk and is 000 outside the support {1,…,N}\{1,\dots,N\}{1,…,N}. Statements that need a nonempty support assume N≥1N\ge1N≥1.
  • The goal states convergence to the complex number riemannZeta s of the real partial sums viewed as complex numbers, and divergence as Tendsto … atTop atTop. The source's parameter range s≥0s\ge0s≥0 is kept as a hypothesis.
  • The Hurwitz zeta function is defined by its series (value 000 when the series diverges); the Zipf–Mandelbrot law is the infinite-item version on ranks k≥1k\ge1k≥1, with q≥0q\ge0q≥0.
  • The Yule–Simon distribution is defined through the Gamma function; the tail statement asserts existence of a positive constant, matching the source's "[constant]".
  • Random typing is formalized in Li's equiprobable model: m≥2m\ge2m≥2 letters each typed with probability q>0q>0q>0, a space with probability 1−mq>01-mq>01−mq>0, and a word www has probability q∣w∣(1−mq)q^{|w|}(1-mq)q∣w∣(1−mq). "Sorted by rank" means any bijection eee from N\mathbb NN onto the nonempty words along which the probability is non-increasing; the conclusion is a two-sided power-law bound with exponent log⁡m(1/q)\log_m(1/q)logm​(1/q).
  • The Benford connection uses the leading decimal digit of the rank kkk, with kkk drawn from the Zipf distribution with s=1s=1s=1.
  • Not formalized: the empirical claims (word, city, income data), the atlas-model result, Belevitch's Taylor-series argument, the parabolic fractal distribution and the Pareto exchange of variables; their statements in the source are not precise enough to formalize faithfully.

Selected references

  • G. K. Zipf, Human Behavior and the Principle of Least Effort, Addison-Wesley, 1949. https://archive.org/details/in.ernet.dli.2015.90211
  • E. U. Condon, Statistics of vocabulary, Science 67 (1928), 300. https://doi.org/10.1126/science.67.1733.300
  • G. A. Miller, Some effects of intermittent silence, American Journal of Psychology 70 (1957), 311–314. https://doi.org/10.2307/1419346
  • W. Li, Random texts exhibit Zipf's-law-like word frequency distribution, IEEE Trans. Inform. Theory 38 (1992), 1842–1845. https://doi.org/10.1109/18.165464
  • B. Conrad, M. Mitzenmacher, Power laws for monkeys typing randomly: the case of unequal probabilities, IEEE Trans. Inform. Theory 50 (2004), 1403–1414. https://doi.org/10.1109/TIT.2004.830752
  • R. L. Axtell, Zipf distribution of U.S. firm sizes, Science 293 (2001), 1818–1820. https://doi.org/10.1126/science.1062081
  • M. E. J. Newman, Power laws, Pareto distributions and Zipf's law, Contemporary Physics 46 (2005), 323–351. https://arxiv.org/abs/cond-mat/0412004
  • S. T. Piantadosi, Zipf's word frequency law in natural language: a critical review and future directions, Psychon. Bull. Rev. 21 (2014), 1112–1130. https://doi.org/10.3758/s13423-014-0585-6
  • Wikipedia, Zipf's law. https://en.wikipedia.org/wiki/Zipf%27s_law
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Number TheoryProbability·Captain: Lucas

Benford's Law: Leading Digits of Powers, Fibonacci Numbers and FactorialsTextbook

Motivation

Benford's law (also the Newcomb–Benford law, or first-digit law) is the observation that in many real-life collections of numbers the leading significant digit is small far more often than a uniform guess would suggest: the digit 111 leads about 30.1%30.1\%30.1% of the time and the digit 999 less than 5%5\%5% of the time. Simon Newcomb noticed in 1881 that the early pages of logarithm tables were more worn than the later ones and proposed that digit ddd leads with probability log⁡10(d+1)−log⁡10d\log_{10}(d+1)-\log_{10} dlog10​(d+1)−log10​d (Newcomb 1881); Frank Benford rediscovered the law in 1938 and tested it on 20,229 observations from 20 domains (Benford 1938). The law is used today as a screening statistic in forensic accounting, election forensics and the detection of fabricated scientific data.

Beyond empirical data, many classical integer sequences satisfy the law exactly, in the asymptotic sense: the powers of 222, the powers of any integer kkk with log⁡10k\log_{10} klog10​k irrational, the Fibonacci numbers and the factorials. These are theorems, and they are the core of this mission.

Timeline of the mathematical results formalized here:

  • 1881 — Newcomb states the first-digit law (doi:10.2307/2369148).
  • 1938 — Benford's empirical study (JSTOR 984802).
  • 1961 — Pinkham: a scale-invariant first-digit law must be logarithmic (doi:10.1214/aoms/1177704862).
  • 1967, 1981 — Duncan and Washington: the Fibonacci numbers are Benford (doi:10.1080/00150517.1967.12431312, doi:10.1080/00150517.1981.12430109).
  • 1976 — Raimi's survey "The first digit problem" (doi:10.2307/2319349).
  • 1995 — Hill: base invariance and a statistical derivation; the distribution of digits beyond the first (doi:10.1214/ss/1177009869, doi:10.1080/00029890.1995.11990578).

Setting

Fix an integer base b≥2b \ge 2b≥2. Every real x≠0x \neq 0x=0 can be written uniquely as ∣x∣=m⋅be|x| = m \cdot b^{e}∣x∣=m⋅be with significand m∈[1,b)m \in [1, b)m∈[1,b) and e∈Ze \in \mathbb{Z}e∈Z. The leading digit of xxx is Db(x)=⌊m⌋∈{1,…,b−1}D_b(x) = \lfloor m \rfloor \in \{1,\dots,b-1\}Db​(x)=⌊m⌋∈{1,…,b−1}. Equivalently, with {t}=t−⌊t⌋\{t\} = t - \lfloor t \rfloor{t}=t−⌊t⌋ the fractional part,

Db(x)=⌊b{log⁡b∣x∣}⌋.D_b(x) = \left\lfloor b^{\{\log_b |x|\}} \right\rfloor .Db​(x)=⌊b{logb​∣x∣}⌋.

More generally, the integer formed by the first kkk significant digits is ⌊b{log⁡b∣x∣}+k−1⌋\lfloor b^{\{\log_b|x|\} + k - 1}\rfloor⌊b{logb​∣x∣}+k−1⌋, and the nnn-th significant digit is that integer for k=nk=nk=n reduced modulo bbb.

The Benford probabilities are

Pb(d)=log⁡b(d+1)−log⁡bd=log⁡b ⁣(1+1d),d=1,…,b−1.P_b(d) = \log_b(d+1) - \log_b d = \log_b\!\left(1 + \frac1d\right), \qquad d = 1, \dots, b-1 .Pb​(d)=logb​(d+1)−logb​d=logb​(1+d1​),d=1,…,b−1.

A real sequence (an)n≥0(a_n)_{n \ge 0}(an​)n≥0​ satisfies Benford's law in base bbb if for every digit d∈{1,…,b−1}d \in \{1,\dots,b-1\}d∈{1,…,b−1}

lim⁡N→∞#{0≤n<N:Db(an)=d}N=Pb(d).\lim_{N\to\infty} \frac{\#\{0 \le n < N : D_b(a_n) = d\}}{N} = P_b(d).N→∞lim​N#{0≤n<N:Db​(an​)=d}​=Pb​(d).

A positive random variable XXX satisfies the strong form of the law if {log⁡bX}\{\log_b X\}{logb​X} is uniformly distributed on [0,1)[0,1)[0,1).

Formalization targets

Goal — powers of kkk (Note 3 of the source)

For every natural number kkk such that log⁡10k\log_{10} klog10​k is irrational, the sequence k1,k2,k3,…k^1, k^2, k^3, \dotsk1,k2,k3,… satisfies Benford's law in base 101010:

lim⁡N→∞#{1≤n≤N:D10(kn)=d}N=log⁡10 ⁣(1+1d)(d=1,…,9).\lim_{N\to\infty}\frac{\#\{1\le n\le N : D_{10}(k^n)=d\}}{N}=\log_{10}\!\left(1+\frac1d\right)\quad (d=1,\dots,9).N→∞lim​N#{1≤n≤N:D10​(kn)=d}​=log10​(1+d1​)(d=1,…,9).

Milestones

  1. The Benford probabilities in base bbb sum to 111.
  2. Db(x)=dD_b(x) = dDb​(x)=d if and only if log⁡bd≤{log⁡bx}<log⁡b(d+1)\log_b d \le \{\log_b x\} < \log_b (d+1)logb​d≤{logb​x}<logb​(d+1).
  3. Strong form ⇒\Rightarrow⇒ first-digit law, in every base b≥2b \ge 2b≥2.
  4. In base 222 every nonzero number has leading digit 111.
  5. The powers of 222 satisfy Benford's law.
  6. The Fibonacci numbers satisfy Benford's law.
  7. The factorials satisfy Benford's law.
  8. Exponential growth or decay CertC e^{rt}Cert (r≠0r\ne 0r=0) spends an asymptotic fraction log⁡10(1+1/d)\log_{10}(1+1/d)log10​(1+1/d) of its time with leading digit ddd.
  9. A scale-invariant first-digit distribution is the Benford distribution.
  10. Under the strong form, the first kkk digits form the integer nnn with probability log⁡10(1+1/n)\log_{10}(1+1/n)log10​(1+1/n).
  11. Under the strong form, the nnn-th digit (n≥2n \ge 2n≥2) equals ddd with probability ∑k=10n−210n−1−1log⁡10 ⁣(1+110k+d)\sum_{k=10^{n-2}}^{10^{n-1}-1}\log_{10}\!\left(1+\frac{1}{10k+d}\right)∑k=10n−210n−1−1​log10​(1+10k+d1​).
  12. That nnn-th-digit probability tends to 1/101/101/10.
  13. The Benford first-digit distribution has mean 3.4403.4403.440 and variance 6.0576.0576.057 (to three decimals).
  14. The reciprocals 1/n1/n1/n and the square roots n\sqrt nn​ of the natural numbers do not satisfy Benford's law.

Significance

The goal is the cleanest instance of the mechanism behind Benford's law: a sequence obeys the law exactly when the fractional parts of its base-101010 logarithms are equidistributed modulo 111, and for knk^nkn those fractional parts are the multiples nlog⁡10kn\log_{10}knlog10​k reduced modulo 111. The milestones cover the rest of the mathematical content of the article: the definition and normalization of the law, the derivation from a log-uniform significand, the generalization to several leading digits and to the nnn-th digit, scale invariance, the continuous-time exponential case, and the negative results for 1/n1/n1/n and n\sqrt nn​.

All of these results are classical and proved in the literature cited above; the work here is formalizing the known proofs. Related entries already on the platform (a leading-digit / fractional-part characterization and an equidistribution-based Benford criterion, stated with different definitions) may be reusable by solvers.

Difficulty

The goal and milestones 5–7 reduce to equidistribution of a sequence modulo 111. For knk^nkn and Fibonacci numbers this is Weyl's equidistribution theorem for irrational rotations (Fibonacci additionally needs Binet's formula and an error term that vanishes). Factorials are harder: log⁡10n!\log_{10} n!log10​n! is not a linear sequence, and the classical proof combines Stirling's formula with an equidistribution criterion for sequences whose differences vary slowly. The scale-invariance theorem requires a Fourier-analytic argument on the circle R/Z\mathbb{R}/\mathbb{Z}R/Z. The negative results require showing that a counting ratio oscillates, which needs explicit lower and upper estimates along two subsequences.

Formalization scope

  • Digits are defined through real logarithms: Db(x)=⌊b{log⁡bx}⌋D_b(x) = \lfloor b^{\{\log_b x\}} \rfloorDb​(x)=⌊b{logb​x}⌋. Lean's Real.logb takes log⁡b∣x∣\log_b|x|logb​∣x∣, so negative numbers get the leading digit of their absolute value, and the junk value Db(0)=1D_b(0) = 1Db​(0)=1 occurs. Every statement either restricts to positive (or nonzero) inputs or only uses positive sequences.
  • Sequences are indexed from n=0n=0n=0; "the sequence k1,k2,…k^1, k^2, \dotsk1,k2,…" is encoded as an=kn+1a_n = k^{n+1}an​=kn+1, the Fibonacci numbers as Fn+1F_{n+1}Fn+1​ and the factorials as (n+1)!(n+1)!(n+1)!.
  • The asymptotic frequency is a natural density over {0,…,N−1}\{0,\dots,N-1\}{0,…,N−1}; "satisfies Benford's law" requires convergence for every digit 1≤d<b1\le d<b1≤d<b.
  • The strong form is encoded as: XXX measurable, X>0X>0X>0 almost surely, and the pushforward of the probability measure under ω↦{log⁡bX(ω)}\omega \mapsto \{\log_b X(\omega)\}ω↦{logb​X(ω)} equals Lebesgue measure restricted to [0,1)[0,1)[0,1) (this forces the underlying measure to have total mass 111).
  • Moments are stated to three decimals, matching the source's rounding: ∣mean−3.440∣<0.0005|\mathrm{mean} - 3.440| < 0.0005∣mean−3.440∣<0.0005 and ∣variance−6.057∣<0.0005|\mathrm{variance} - 6.057| < 0.0005∣variance−6.057∣<0.0005.
  • Not formalized: the empirical claims (tables, applications, statistical tests), Hill's 1995 theorem on random mixtures of distributions, and the Krieger–Kafri entropy explanation; their statements in the source are not precise enough to formalize faithfully.

Reusable infrastructure: leading-digit and significand API, equidistribution of nαn\alphanα modulo 111 (Weyl), Benford criteria via equidistribution. Contributions toward a general "equidistributed {log⁡10an}\{\log_{10} a_n\}{log10​an​} ⇒\Rightarrow⇒ Benford" lemma are welcome.

Selected references

  • S. Newcomb, Note on the frequency of use of the different digits in natural numbers, American Journal of Mathematics 4 (1881), 39–40. https://doi.org/10.2307/2369148
  • F. Benford, The law of anomalous numbers, Proc. Amer. Philos. Soc. 78 (1938), 551–572. https://www.jstor.org/stable/984802
  • R. S. Pinkham, On the distribution of first significant digits, Ann. Math. Statist. 32 (1961), 1223–1230. https://doi.org/10.1214/aoms/1177704862
  • R. L. Duncan, An application of uniform distribution to the Fibonacci numbers, Fibonacci Quarterly 5 (1967), 137–140. https://doi.org/10.1080/00150517.1967.12431312
  • L. C. Washington, Benford's law for Fibonacci and Lucas numbers, Fibonacci Quarterly 19 (1981), 175–177. https://doi.org/10.1080/00150517.1981.12430109
  • R. A. Raimi, The first digit problem, American Mathematical Monthly 83 (1976), 521–538. https://doi.org/10.2307/2319349
  • T. P. Hill, A statistical derivation of the significant-digit law, Statistical Science 10 (1995), 354–363. https://doi.org/10.1214/ss/1177009869
  • T. P. Hill, The significant-digit phenomenon, American Mathematical Monthly 102 (1995), 322–327. https://doi.org/10.1080/00029890.1995.11990578
  • A. Berger, T. P. Hill, The mathematics of Benford's law: a primer, Stat. Methods Appl. 30 (2021), 779–795. https://arxiv.org/abs/1909.07527
  • Wikipedia, Benford's law. https://en.wikipedia.org/wiki/Benford%27s_law
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Mathematical PhysicsQuantum Gravity·Captain: Lucas

Non-renormalizability of gravity from black-hole entropy (Shomer 2007)Research Paper

Motivation

Why is general relativity not a renormalizable quantum field theory? The textbook answer is perturbative: Newton's constant has negative mass dimension, so the gravitational coupling is irrelevant and loop divergences cannot be absorbed into finitely many counterterms. That argument can in principle be evaded (Weinberg's asymptotic safety). Shomer's note (arXiv:0709.3555), following Banks and Aharony–Banks, gives a non-perturbative, thermodynamic argument instead: the very-high-energy spectrum of any renormalizable ddd-dimensional QFT is that of a ddd-dimensional conformal field theory (CFT), whereas the high-energy spectrum of gravity is dominated by black holes, whose Bekenstein–Hawking entropy grows with energy in a way no CFT can match.

Setting

  • CFT side (Sec. IV, Eqs. 29–30). For a ddd-dimensional CFT on Rtime×Sd−1\mathbb R_{\text{time}}\times S^{d-1}Rtime​×Sd−1 (sphere radius RRR) at temperature TTT, dimensional analysis and extensivity give S=a (RT)d−1S=a\,(RT)^{d-1}S=a(RT)d−1 and E=b Rd−1TdE=b\,R^{d-1}T^{d}E=bRd−1Td with constants a,b>0a,b>0a,b>0. Eliminating TTT gives the entropy as a function of energy, SCFT(E)=a (R (E/(bRd−1))1/d)d−1∼E(d−1)/dS_{\rm CFT}(E)=a\,\bigl(R\,(E/(bR^{d-1}))^{1/d}\bigr)^{d-1}\sim E^{(d-1)/d}SCFT​(E)=a(R(E/(bRd−1))1/d)d−1∼E(d−1)/d.
  • Flat gravity (Sec. V.1, Eqs. 31–32). The ddd-dimensional Schwarzschild metric has f(r)=1−ωd−2GNM/rd−3f(r)=1-\omega_{d-2}G_N M/r^{d-3}f(r)=1−ωd−2​GN​M/rd−3 with ωn=16π/(n Vol(Sn))\omega_n=16\pi/(n\,\mathrm{Vol}(S^n))ωn​=16π/(nVol(Sn)). The horizon rHr_HrH​ is the zero of fff, and the Bekenstein–Hawking entropy is S=A/(4GN)S=A/(4G_N)S=A/(4GN​) with A=Vol(Sd−2) rHd−2A=\mathrm{Vol}(S^{d-2})\,r_H^{d-2}A=Vol(Sd−2)rHd−2​, giving S∼M(d−2)/(d−3)S\sim M^{(d-2)/(d-3)}S∼M(d−2)/(d−3).
  • AdS gravity (Sec. V.2, Eqs. 33–34). With f(r)=1−ωd−2GNM/rd−3+r2/RAdS2f(r)=1-\omega_{d-2}G_NM/r^{d-3}+r^2/R_{\rm AdS}^2f(r)=1−ωd−2​GN​M/rd−3+r2/RAdS2​ the horizon is the largest zero of fff and S∼M(d−2)/(d−1)S\sim M^{(d-2)/(d-1)}S∼M(d−2)/(d−1) — the CFT law of one dimension lower (a shadow of AdS/CFT).

Formalization targets

Goal — black-hole entropy is not CFT entropy (flat space, Sec. V.1)

For every spacetime dimension d≥4d\ge 4d≥4, every GN>0G_N>0GN​>0 and every CFT datum a,b,R>0a,b,R>0a,b,R>0,

SBH(E) is not Θ(SCFT(E))as E→∞.S_{\rm BH}(E)\ \text{is not}\ \Theta\bigl(S_{\rm CFT}(E)\bigr)\quad\text{as }E\to\infty .SBH​(E) is not Θ(SCFT​(E))as E→∞.

Here Θ\ThetaΘ means bounded above and below by positive multiples of each other for all large EEE; this is how the paper's "∼\sim∼" is read.

Milestones

Eq. (29) (the elimination of TTT), Eq. (30), Eq. (32) exactly, footnote 26 (exponent comparison), Eq. (34) asymptotically, the AdS mismatch with a ddd-dimensional CFT, and the AdS match with a (d−1)(d-1)(d−1)-dimensional CFT.

Significance

The goal is the precise mathematical content of the paper's one-line argument: once the black-hole entropy formula and the CFT scaling law are fixed, their large-energy growth exponents (d−2)/(d−3)>1>(d−1)/d(d-2)/(d-3)>1>(d-1)/d(d−2)/(d−3)>1>(d−1)/d are incompatible. The physics inputs (that a renormalizable QFT flows to a CFT in the UV, that black holes dominate the gravitational density of states, the Bekenstein–Hawking formula) are modelling assumptions, encoded as definitions; the mission formalizes the asymptotic analysis that turns them into a contradiction, not the physics itself.

Difficulty

Mathematically elementary but fiddly: the horizon radius is defined implicitly as the largest positive zero of fff, so one must solve f(rH)=0f(r_H)=0f(rH​)=0 (exactly in flat space, asymptotically in AdS, where rHd−3(1+rH2/RAdS2)=ωd−2GNMr_H^{d-3}(1+r_H^2/R_{\rm AdS}^2)=\omega_{d-2}G_NMrHd−3​(1+rH2​/RAdS2​)=ωd−2​GN​M), handle real powers, and compare asymptotic classes with distinct exponents.

Formalization scope

All statements live in namespace GravityNonRenorm and import one definition file. The unit-sphere volume is the closed form Vol(Sn)=2π(n+1)/2/Γ((n+1)/2)\mathrm{Vol}(S^n)=2\pi^{(n+1)/2}/\Gamma((n+1)/2)Vol(Sn)=2π(n+1)/2/Γ((n+1)/2). Horizon radii are sSup of the set of positive zeros of fff (junk value 000 when that set is empty, e.g. for M≤0M\le 0M≤0); all claims are asymptotic as E→∞E\to\inftyE→∞ or assume M>0M>0M>0, so the junk value is never used. Dimensions are natural numbers; d≥4d\ge 4d≥4 for flat-space statements, d≥3d\ge3d≥3 for AdS, d≥2d\ge2d≥2 for CFT statements.

Selected references

  • A. Shomer, A pedagogical explanation for the non-renormalizability of gravity, arXiv:0709.3555 (2007). https://arxiv.org/abs/0709.3555
  • O. Aharony and T. Banks, Note on the quantum mechanics of M theory, JHEP 9903:016 (1999), arXiv:hep-th/9812237.
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Mathematical PhysicsPartial Differential Equations·Captain: Lucas

Fick's Laws of Diffusion: Fundamental Solution and Classical SolutionsTextbook

Motivation

Fick's laws of diffusion, posited by Adolf Fick in 1855, are the basic constitutive and evolution laws for the transport of mass by diffusion. The first law states that the diffusive flux is proportional to minus the concentration gradient, J=−D ∂xφJ=-D\,\partial_x\varphiJ=−D∂x​φ; the second law is the resulting evolution equation for the concentration,

∂φ∂t=D ∂2φ∂x2.\frac{\partial\varphi}{\partial t}=D\,\frac{\partial^2\varphi}{\partial x^2}.∂t∂φ​=D∂x2∂2φ​.

They are the standard model for diffusion in solids, liquids and gases (in the absence of bulk flow), and are used to model transport in foods, neurons, biopolymers, pharmaceuticals, porous soils, nuclear materials and semiconductor doping. Mathematically, the second law is the heat equation with the thermal diffusivity replaced by the diffusion coefficient D>0D>0D>0.

This mission formalizes the mathematical content of the Wikipedia article Fick's laws of diffusion: the derivation of the second law from the first, the steady state, the fundamental solution, the error-function solutions for a constant source, and the mean-squared-displacement law.

Setting

A concentration is a real function φ(x,t)\varphi(x,t)φ(x,t) of position xxx and time ttt; a flux is a real function J(x,t)J(x,t)J(x,t). The diffusion coefficient is a constant D>0D>0D>0. For t>0t>0t>0 the diffusion kernel is

φD(x,t)=14πDtexp⁡(−x24Dt),\varphi_D(x,t)=\frac{1}{\sqrt{4\pi Dt}}\exp\Big(-\frac{x^2}{4Dt}\Big),φD​(x,t)=4πDt​1​exp(−4Dtx2​),

and in nnn space dimensions

φD(n)(x,t)=(4πDt)−n/2exp⁡(−∥x∥24Dt),x∈Rn.\varphi^{(n)}_D(x,t)=(4\pi Dt)^{-n/2}\exp\Big(-\frac{\|x\|^2}{4Dt}\Big),\qquad x\in\mathbb R^n.φD(n)​(x,t)=(4πDt)−n/2exp(−4Dt∥x∥2​),x∈Rn.

The complementary error function is erfc⁡(u)=2π∫u∞e−s2 ds\operatorname{erfc}(u)=\frac{2}{\sqrt\pi}\int_u^\infty e^{-s^2}\,dserfc(u)=π​2​∫u∞​e−s2ds.

Formalization targets

Goal: the fundamental solution

For D>0D>0D>0, φD\varphi_DφD​ solves ∂tφ=D∂x2φ\partial_t\varphi=D\partial_x^2\varphi∂t​φ=D∂x2​φ for t>0t>0t>0, has ∫RφD(x,t) dx=1\int_{\mathbb R}\varphi_D(x,t)\,dx=1∫R​φD​(x,t)dx=1 for every t>0t>0t>0, and satisfies

lim⁡t→0+∫RφD(x−y,t)f(y) dy=f(x)\lim_{t\to0^+}\int_{\mathbb R}\varphi_D(x-y,t)f(y)\,dy=f(x)t→0+lim​∫R​φD​(x−y,t)f(y)dy=f(x)

for every bounded continuous fff and every xxx.

Milestones

  1. Fick's second law follows from Fick's first law and mass conservation ∂tφ+∂xJ=0\partial_t\varphi+\partial_xJ=0∂t​φ+∂x​J=0 (constant DDD).
  2. A C2C^2C2 steady state in one dimension is linear: c(x)=ax+bc(x)=ax+bc(x)=ax+b.
  3. The three components of the goal, separately (PDE, unit mass, initial point source).
  4. n(x,t)=n0erfc⁡(x/(2Dt))n(x,t)=n_0\operatorname{erfc}\big(x/(2\sqrt{Dt})\big)n(x,t)=n0​erfc(x/(2Dt​)) solves the second law with n(0,t)=n0n(0,t)=n_0n(0,t)=n0​ and n(x,0+)=0n(x,0^+)=0n(x,0+)=0 for x>0x>0x>0.
  5. n(x,t)=n02erfc⁡(x/(2Dt))n(x,t)=\frac{n_0}{2}\operatorname{erfc}\big(x/(2\sqrt{Dt})\big)n(x,t)=2n0​​erfc(x/(2Dt​)) solves the second law with initial profile n0n_0n0​ on x<0x<0x<0 and 000 on x>0x>0x>0.
  6. Mean squared displacement in Rn\mathbb R^nRn: ∫∥x∥2φD(n)(x,t) dx=2nDt\int\|x\|^2\varphi^{(n)}_D(x,t)\,dx=2nDt∫∥x∥2φD(n)​(x,t)dx=2nDt.

Significance

The fundamental solution is what makes the second law usable: the solution of the one-dimensional diffusion problem with bounded continuous initial data is the convolution of the data with φD\varphi_DφD​, and the erfc profiles and diffusion length 2Dt2\sqrt{Dt}2Dt​ quoted throughout applications are derived from it. The mean-squared-displacement law 2nDt2nDt2nDt connects the macroscopic diffusion coefficient to the microscopic Brownian motion of particles.

All statements are classical and proved in the literature; the task here is to formalize them. Mathlib provides the Gaussian integral but has no error function and no development of the one-dimensional diffusion equation, so the mission also produces reusable infrastructure (erfc and its derivative and limits, Gaussian moments in Rn\mathbb R^nRn, the approximate-identity property).

Difficulty

The individual computations are routine on paper; the formal difficulty lies in rigor that the article leaves implicit: differentiating the kernel in both variables only on t>0t>0t>0, justifying limits of parameter-dependent integrals as t→0+t\to0^+t→0+ (dominated convergence for the point-source property), computing the second moment of an nnn-dimensional Gaussian on Euclidean space, and building erfc from scratch, including its derivative −2πe−u2-\frac{2}{\sqrt\pi}e^{-u^2}−π​2​e−u2 and its limits at ±∞\pm\infty±∞.

Formalization scope

All objects are real-valued; derivatives are Mathlib's deriv (which is 000 at non-differentiable points), integrals are Lebesgue integrals, and limits as t→0+t\to0^+t→0+ use the right-neighbourhood filter. Every statement about the kernel or erfc profiles assumes D>0D>0D>0 and evaluates the PDE only at t>0t>0t>0, so junk values of square root and division never matter. The steady-state milestone assumes C2C^2C2 regularity, without which deriv would admit non-smooth "solutions" such as ∣x∣|x|∣x∣. Rn\mathbb R^nRn is EuclideanSpace ℝ (Fin n). Physical parts of the article (Stokes–Einstein relation, Maxwell–Stefan, sorption kinetics, approximations) are out of scope.

Selected references

  • Wikipedia contributors, Fick's laws of diffusion. https://en.wikipedia.org/wiki/Fick%27s_laws_of_diffusion
  • A. Fick, Ueber Diffusion, Annalen der Physik 170 (1855) 59–86. https://doi.org/10.1002/andp.18551700105
  • J. Crank, The Mathematics of Diffusion, 2nd ed., Oxford University Press, 1975.
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Economics·Captain: Lucas

Okun's Law: Growth-Rate Form from the Gap VersionTextbook

Motivation

Okun's law is an empirically observed relationship between unemployment and losses in a country's production, named after Arthur M. Okun, who proposed it in 1962 (Okun 1962). It appears in two standard forms. The gap version relates the output gap to the unemployment gap; the difference (or growth-rate) version relates year-to-year changes in output to year-to-year changes in unemployment. Macroeconomics textbooks (Abel & Bernanke 2005) present the gap version and then derive the difference version from it by a short chain of algebraic manipulations followed by two approximations. The empirical validity of the law is disputed and is not the subject of this mission; the subject is the internal mathematics of the derivation.

Setting

Time is discrete: years are indexed by t∈Nt \in \mathbb Nt∈N. All quantities are real-valued time series:

  • YtY_tYt​ — actual output,
  • Y‾t\overline Y_tYt​ — potential GDP (full-employment output),
  • utu_tut​ — the actual unemployment rate,
  • u‾t\overline u_tut​ — the natural rate of unemployment,
  • ccc — the Okun coefficient, a real constant relating changes in unemployment to changes in output.

For a series xxx write Δxt=xt+1−xt\Delta x_t = x_{t+1} - x_tΔxt​=xt+1​−xt​ for its annual change and Δxt/xt\Delta x_t / x_tΔxt​/xt​ for its growth rate from year ttt to year t+1t+1t+1. The gap version of Okun's law in year ttt is

Y‾t−YtY‾t=c (ut−u‾t).\frac{\overline Y_t - Y_t}{\overline Y_t} = c\,(u_t - \overline u_t).Yt​Yt​−Yt​​=c(ut​−ut​).

Formalization targets

Goal — the growth-rate form with its exact remainder

The source's final formula is ΔYY≈k−c Δu\dfrac{\Delta Y}{Y} \approx k - c\,\Delta uYΔY​≈k−cΔu, where kkk is the growth rate of full-employment output. The goal states the derivation exactly: if the gap version holds in years ttt and t+1t+1t+1 (with positive YtY_tYt​, Y‾t\overline Y_tYt​, Y‾t+1\overline Y_{t+1}Yt+1​), the natural rate does not change (Δu‾t=0\Delta \overline u_t = 0Δut​=0) and potential output grows at rate kkk (ΔY‾t/Y‾t=k\Delta\overline Y_t/\overline Y_t = kΔYt​/Yt​=k), then

ΔYtYt=k−c Δut−c Δut(Y‾t+ΔY‾tYt−1).\frac{\Delta Y_t}{Y_t} = k - c\,\Delta u_t - c\,\Delta u_t\left(\frac{\overline Y_t + \Delta \overline Y_t}{Y_t} - 1\right).Yt​ΔYt​​=k−cΔut​−cΔut​(Yt​Yt​+ΔYt​​−1).

The last term is precisely the error made by the source's approximation Y‾+ΔY‾Y≈1\frac{\overline Y + \Delta\overline Y}{Y} \approx 1YY+ΔY​≈1.

Milestones — the steps of the derivation

  1. The gap version is equivalent to YtY‾t−1=c(u‾t−ut)\frac{Y_t}{\overline Y_t} - 1 = c(\overline u_t - u_t)Yt​Yt​​−1=c(ut​−ut​).
  2. Taking annual differences: Δ ⁣(YY‾)t=Yt+ΔYtY‾t+ΔY‾t−YtY‾t=c(Δu‾t−Δut)\Delta\!\left(\frac{Y}{\overline Y}\right)_t = \frac{Y_t + \Delta Y_t}{\overline Y_t + \Delta \overline Y_t} - \frac{Y_t}{\overline Y_t} = c(\Delta\overline u_t - \Delta u_t)Δ(YY​)t​=Yt​+ΔYt​Yt​+ΔYt​​−Yt​Yt​​=c(Δut​−Δut​).
  3. Common denominator: Y‾t ΔYt−Yt ΔY‾tY‾t(Y‾t+ΔY‾t)=c(Δu‾t−Δut)\frac{\overline Y_t\,\Delta Y_t - Y_t\,\Delta\overline Y_t}{\overline Y_t(\overline Y_t + \Delta\overline Y_t)} = c(\Delta\overline u_t - \Delta u_t)Yt​(Yt​+ΔYt​)Yt​ΔYt​−Yt​ΔYt​​=c(Δut​−Δut​).
  4. Exact growth identity: ΔYtYt−ΔY‾tY‾t=c(Δu‾t−Δut)⋅Y‾t+ΔY‾tYt\frac{\Delta Y_t}{Y_t} - \frac{\Delta \overline Y_t}{\overline Y_t} = c(\Delta\overline u_t - \Delta u_t)\cdot\frac{\overline Y_t + \Delta\overline Y_t}{Y_t}Yt​ΔYt​​−Yt​ΔYt​​=c(Δut​−Δut​)⋅Yt​Yt​+ΔYt​​.

Significance

The derivation is the textbook justification for using the difference form, which is the version actually estimated by regression. Making every step exact shows exactly which hypotheses (positivity of output, the gap law in two consecutive years with the same coefficient, a constant natural rate) and which approximation (the factor (Y‾+ΔY‾)/Y≈1(\overline Y+\Delta\overline Y)/Y \approx 1(Y+ΔY)/Y≈1) the difference form rests on, and gives the size of the neglected term. The result is elementary and known; what the mission adds is a machine-checked, approximation-free account of the derivation.

Difficulty

The algebra is elementary. The care required is in bookkeeping: the source uses "≈\approx≈" in two places and silently assumes all denominators are nonzero. A faithful statement must replace each "≈\approx≈" either by an explicit hypothesis or by an explicit remainder term, and must state the positivity assumptions that make the divisions meaningful.

Formalization scope

Series are functions N→R\mathbb N \to \mathbb RN→R; Δxt=xt+1−xt\Delta x_t = x_{t+1} - x_tΔxt​=xt+1​−xt​; the growth rate is Δxt/xt\Delta x_t / x_tΔxt​/xt​ (Lean's real division returns 000 when dividing by 000, so positivity hypotheses on YtY_tYt​, Y‾t\overline Y_tYt​, Y‾t+1\overline Y_{t+1}Yt+1​ are stated explicitly wherever a division by them occurs). The gap law is a predicate on one year ttt with a fixed coefficient ccc; all statements use the gap law in exactly the two years ttt and t+1t+1t+1 with the same ccc. The source's approximations Δu‾≈0\Delta\overline u \approx 0Δu≈0 and ΔY‾/Y‾≈k\Delta\overline Y/\overline Y \approx kΔY/Y≈k are taken as exact hypotheses, and the approximation (Y‾+ΔY‾)/Y≈1(\overline Y + \Delta \overline Y)/Y \approx 1(Y+ΔY)/Y≈1 is replaced by an explicit remainder term, so the goal is an exact identity rather than a vague approximation. The shared definitions live in one definition file (OkunsLaw_defs).

Selected references

  • A. M. Okun, Potential GNP: Its Measurement and Significance, Proceedings of the Business and Economic Statistics Section, American Statistical Association, 1962. https://cowles.yale.edu/node/142137
  • A. B. Abel and B. S. Bernanke, Macroeconomics, 5th ed., Pearson/Addison Wesley, 2005. ISBN 0-321-16212-9.
  • Wikipedia, Okun's law, revision 1341356066 — sections "Mathematical statements" and "Derivation of the growth rate form". https://en.wikipedia.org/w/index.php?title=Okun%27s_law&oldid=1341356066
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Economics·Captain: Lucas

Gresham's Law I: Bad Money Drives Out GoodTextbook

Motivation

Gresham's law is the monetary principle usually summarised as "bad money drives out good": when two kinds of coin circulate side by side and the law obliges everyone to accept both at the same face value, the coin whose metal is worth more tends to vanish from circulation, while the debased coin stays in use. The principle was named in 1857–58 by Henry Dunning Macleod after Sir Thomas Gresham, who explained to Elizabeth I in 1558 why the English coinage had deteriorated after the Great Debasements of Henry VIII and Edward VI. It appears much earlier in Aristophanes' The Frogs (405 BC), in Nicole Oresme's treatise on money (c. 1350–1357), in a 1472 Venetian report ("the bad money will chase out the good"), and in Copernicus' Monetae cudendae ratio (1519/1528), whence the alternative name Gresham–Copernicus law. The source of this mission is the Wikipedia article.

Modern instances quoted by the article include the disappearance of 90% silver U.S. half dollars after the Coinage Act of 1965, the 2007 U.S. ban on melting one- and five-cent coins, and Britain's drift to a de facto gold standard after Isaac Newton fixed the guinea at 21 shillings in 1717. The article also records the reverse phenomenon, Thiers' law (named by Peter Bernholz): without effective legal tender laws, good money drives out bad money once the bad money becomes nearly worthless.

Setting

A coin is described by two real numbers: its face value fff, the nominal value at which legal tender law requires it to be accepted, and its melt value mmm, the market value of the metal it contains (its intrinsic or commodity value). "Good money" has a melt value close to its face value; "bad money" has a melt value considerably below its face value while being accepted at the same face value.

A holder owns a finite wallet sss of coins, indexed by a type ι\iotaι, with face values fif_ifi​ and melt values mim_imi​. Legal tender at equal value means that all coins of the wallet carry the same face value. Because creditors must accept coins at face value, a set P⊆sP\subseteq sP⊆s is a legal payment of a debt ddd when ∑i∈Pfi=d\sum_{i\in P} f_i=d∑i∈P​fi​=d. The holder "prefers to save the intrinsically more valuable money": a legal payment PPP is optimal when no other legal payment QQQ of the same debt leaves the holder with more intrinsic value, i.e.

∑i∈s∖Qmi  ≤  ∑i∈s∖Pmi.\sum_{i\in s\setminus Q} m_i\;\le\;\sum_{i\in s\setminus P} m_i .i∈s∖Q∑​mi​≤i∈s∖P∑​mi​.

Without legal tender law, a seller values coins only by their metal, and accepts at market value a set PPP of coins for a price ppp exactly when ∑i∈Pmi≥p\sum_{i\in P} m_i\ge p∑i∈P​mi​≥p.

For the 1717 episode, the home legal rate is rrr shillings per guinea and abroad the gold of one guinea costs the silver of mmm shillings. One arbitrage round turns NNN shillings into the gold of N/mN/mN/m guineas abroad, which is coined at home and exchanged back at the legal rate for Nm r\tfrac{N}{m}\,rmN​r shillings.

Formalization targets

Goal: bad money is spent first

If the wallet is split into good coins and bad coins, every bad coin has strictly smaller melt value than every good coin, and all coins carry the same face value, then in any optimal payment PPP

(P∩good≠∅)  ⟹  bad⊆P:\bigl(P\cap\text{good}\neq\varnothing\bigr)\;\Longrightarrow\;\text{bad}\subseteq P:(P∩good=∅)⟹bad⊆P:

a good coin is handed over only once every bad coin has been handed over. Equivalently, as long as the holder retains a bad coin, no good coin circulates.

Milestones

  1. The sixpence example — paying with a single coin, the optimal choice is a coin of minimal melt value (the most debased coin), and conversely.
  2. Exchange characterization — with equal positive face values, a legal payment is optimal iff every paid coin has melt value at most that of every retained coin.
  3. Thiers' law — without legal tender, if the bad coins are nearly worthless (total melt value of all bad coins below the price), every accepted payment contains a good coin.
  4. Newton's guinea — if gold is overvalued at home (0<m<r0<m<r0<m<r), one arbitrage round is strictly profitable, and repeated rounds grow without bound.

Significance

The goal is the decision-theoretic core of the article's "Theory" section: legal tender laws act as a price control fixing the exchange ratio of coins with different intrinsic content, and a holder who keeps the more valuable coins therefore pays with the less valuable ones. The milestones isolate the article's worked example (sixpences and pennies), the exact optimality condition behind it, the reverse regime (Thiers' law, and Mundell's reformulation "bad money drives out good if they exchange for the same price"), and the bimetallic arbitrage that drained silver from Britain after 1717.

The statements are elementary; the value of the mission is a precise, checked account of which hypotheses carry the law — equal face value enforced by law, and a strict ranking of intrinsic values — so that the informal statement becomes an exact theorem with its conditions visible.

Difficulty

The obvious argument is a single swap: exchange a paid good coin for a retained bad coin. The swap keeps the payment legal only because all coins carry the same face value; with unequal face values it changes the amount paid and the argument fails. The exchange characterization also needs positive face values: with zero face values every subset is a payment of 000, and the condition "paid coins are no more valuable than retained ones" no longer implies optimality.

Formalization scope

Face and melt values are real numbers; wallets are finite sets (Finset) of indices, so distinct coins with identical values are distinct elements. Payments must match the debt exactly (no change is modelled inside a single payment; the shopkeeper giving change is another payer facing the same problem). Optimality compares retained intrinsic value among legal payments of the same debt from the same wallet. The arbitrage round ignores transport and minting costs. Melting, hoarding and export are not modelled as separate actions; the formal content is the payment choice, the market-value acceptance rule, and the arbitrage round.

The goal is not vacuous: optimal payments exist for every attainable debt (the wallet is finite), and the hypotheses are satisfiable, e.g. by one good and one bad coin of face value 111 and melt values 111 and 12\tfrac1221​.

All declarations live in the namespace GreshamLaw, in one definition file GreshamLaw_Model.

Selected references

  • Wikipedia, Gresham's law. https://en.wikipedia.org/wiki/Gresham%27s_law
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Economics·Captain: Lucas

Say's Law I: No General Glut in a Barter EconomyTextbook

Motivation

Say's law, or the law of markets, is the classical claim that production is the source of demand. Jean-Baptiste Say wrote in his Treatise on Political Economy (1803) that "a product is no sooner created, than it, from that instant, affords a market for other products to the full extent of its own value". The doctrine was restated by James Mill ("the production of commodities creates ... a market for the commodities produced") and David Ricardo ("demand depends only on supply"), and it was a key element of the framework of macroeconomics from the mid-19th century until the 1930s.

Its best-known consequence is that a general glut — a widespread excess of supply over demand for all goods at once — cannot occur: if one good remains unsold, some other good must be in short supply. This claim was disputed from the start. Thomas Malthus reported evidence of general gluts; John Stuart Mill argued that during a general glut there is excess demand for money, and rescued the no-glut principle by counting money as one of the commodities. During the Great Depression, Keynes argued that Say's law is simply not true, and Keynesian, post-Keynesian and Marxian critics locate its failure in the hoarding of money. Krugman called it "at best, a useless tautology when individuals have the option of accumulating money rather than purchasing real goods and services".

The debate turns on an accounting fact that is easy to state and easy to misstate: what exactly follows from budget constraints alone, and what changes when money can be held rather than spent. This mission pins that down formally.

Setting

Fix a finite set ι\iotaι of agents and a finite set GGG of goods. A price vector is p∈RGp\in\mathbb R^Gp∈RG. Agent iii brings the bundle si∈RGs_i\in\mathbb R^Gsi​∈RG to market (his supply) and plans to buy the bundle di∈RGd_i\in\mathbb R^Gdi​∈RG (his demand). The market value of a bundle xxx is

⟨p,x⟩=∑g∈Gpgxg,\langle p,x\rangle=\sum_{g\in G}p_g x_g,⟨p,x⟩=g∈G∑​pg​xg​,

and the aggregate excess demand for good ggg is zg=∑i∈ι(di,g−si,g)z_g=\sum_{i\in\iota}(d_{i,g}-s_{i,g})zg​=∑i∈ι​(di,g​−si,g​).

  • Say's budget principle ("products are paid for with products"): every agent spends the whole proceeds of his sales on other products, ⟨p,di⟩=⟨p,si⟩\langle p,d_i\rangle=\langle p,s_i\rangle⟨p,di​⟩=⟨p,si​⟩.
  • A general glut is a situation with zg<0z_g<0zg​<0 for every good ggg.
  • In a monetary economy, agent iii holds money mim_imi​ initially and plans to hold mi′m'_imi′​, subject to ⟨p,di⟩+mi′=⟨p,si⟩+mi\langle p,d_i\rangle+m'_i=\langle p,s_i\rangle+m_i⟨p,di​⟩+mi′​=⟨p,si​⟩+mi​. The aggregate excess demand for money is ∑i(mi′−mi)\sum_i(m'_i-m_i)∑i​(mi′​−mi​); it is positive when agents in aggregate hoard.

Formalization targets

Goal — no general glut

With at least one good, strictly positive prices and Say's budget principle,

¬(∀g∈G, zg<0).\neg\big(\forall g\in G,\ z_g<0\big).¬(∀g∈G, zg​<0).

Milestones

  1. Say's identity: ∑i⟨p,di⟩=∑i⟨p,si⟩\sum_i\langle p,d_i\rangle=\sum_i\langle p,s_i\rangle∑i​⟨p,di​⟩=∑i​⟨p,si​⟩ under Say's budget principle.
  2. Glut balanced by shortage: with positive prices, if zg0<0z_{g_0}<0zg0​​<0 then zg>0z_g>0zg​>0 for some g≠g0g\neq g_0g=g0​.
  3. Monetary budget identity: ⟨p,z⟩+∑i(mi′−mi)=0\langle p,z\rangle+\sum_i(m'_i-m_i)=0⟨p,z⟩+∑i​(mi′​−mi​)=0 under the monetary budget constraints.
  4. Mill's version with money as a commodity: with positive prices and at least one good, a general glut of goods and a non-positive excess demand for money cannot occur together.
  5. Hoarding permits a general glut: with at least one agent, for any prices, supplies and initial money, some demands and planned money holdings satisfy every budget constraint and produce a general glut.

Significance

The goal and milestones 1–2 isolate the content of Say's law as the article's "modern way of expressing" it: in a pure barter setting the budget constraints alone force gluts and shortages to cancel in value. Milestones 3–5 make the classical and Keynesian objections precise: once money can be held, the same constraints identify a general glut with an excess demand for money (Mill), and they no longer exclude a general glut (Keynes, Krugman, Marx's C–M–C critique). Together they separate what is an accounting identity from what is a behavioural assumption (no hoarding), which is the point at issue in the historical debate. The results are classical; the contribution here is a machine-checked, assumption-explicit statement of each.

Difficulty

The mathematics is elementary; the difficulty is entirely in stating the claims faithfully. The informal phrase "supply creates its own demand" is ambiguous between an identity about values and a claim about quantities of each good, and it silently requires positive prices and a nonempty set of goods — without them "every good is in excess supply" can hold vacuously or with no value consequence. The monetary results must keep money out of the set of goods, so that "an excess of all other commodities" means what Mill meant.

Formalization scope

Goods and agents are finite types; quantities, prices and money balances are real numbers with no sign restriction (supplies and demands may be read as gross amounts or as net trades). Positivity of prices and nonemptiness of the set of goods (or agents) are explicit hypotheses exactly where they are needed. Prices are taken as given; no utility maximisation, equilibrium existence, price adjustment or dynamics is modelled, so statements about full employment, persistence of depressions or the speed of price adjustment are out of scope. The definition file SaysLaw_Model is shared by every statement.

Selected references

  • Wikipedia, Say's law. https://en.wikipedia.org/wiki/Say%27s_law
  • J.-B. Say, A Treatise on Political Economy, 1803.
  • J. S. Mill, Principles of Political Economy, 1848.
  • J. M. Keynes, The General Theory of Employment, Interest and Money, 1936, ch. 2.
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AnalysisMathematical Physics·Captain: Lucas

BCS Theory: the universal gap ratio Δ(0) = (π/e^γ) k_B T_cTextbook

Motivation

The BCS theory of Bardeen, Cooper and Schrieffer (1957) is the microscopic theory of conventional superconductivity in metals; its authors received the 1972 Nobel Prize in Physics. Its most quoted quantitative predictions are universal numbers: in the weak-coupling limit the zero-temperature energy gap and the transition temperature are related by Δ(0)=(π/eγ) kBTc≈1.764 kBTc\Delta(0) = (\pi/e^{\gamma})\,k_BT_c \approx 1.764\,k_BT_cΔ(0)=(π/eγ)kB​Tc​≈1.764kB​Tc​, the gap closes as Δ(T)/Δ(0)≈1.741−T/Tc\Delta(T)/\Delta(0)\approx 1.74\sqrt{1-T/T_c}Δ(T)/Δ(0)≈1.741−T/Tc​​, and the specific heat jumps by (Ces−Cen)/Cen≈1.43(C_{es}-C_{en})/C_{en}\approx 1.43(Ces​−Cen​)/Cen​≈1.43 at TcT_cTc​. These numbers are what experiments compare against, and they follow from a single scalar integral equation, the BCS gap equation. This mission formalizes that mathematical core, following the section Erfolge der BCS-Theorie of the German Wikipedia article BCS-Theorie.

Timeline (as summarized in the source):

  • 1950 — isotope effect observed (Lock et al.; Maxwell; Serin et al.): TcT_cTc​ depends on the ionic mass MMM.
  • 1956 — Cooper shows that an arbitrarily weak attraction binds two electrons above a filled Fermi sea.
  • 1957 — Bardeen, Cooper and Schrieffer publish Theory of Superconductivity, including the gap equation and its consequences.

Setting

Fix the Boltzmann constant kB>0k_B>0kB​>0, the Debye energy ℏωD>0\hbar\omega_D>0ℏωD​>0 (called hbarOmegaD in Lean) and the dimensionless coupling λ=V0 Z(EF)>0\lambda = V_0\,Z(E_F)>0λ=V0​Z(EF​)>0 (called coupling), where V0V_0V0​ is the attractive pairing potential and Z(EF)Z(E_F)Z(EF​) is half the electronic density of states at the Fermi energy. With the quasiparticle energy E(η,Δ)=η2+Δ2E(\eta,\Delta)=\sqrt{\eta^2+\Delta^2}E(η,Δ)=η2+Δ2​ define

I0(ℏωD,Δ)=∫0ℏωDdηη2+Δ2,I(kB,ℏωD,Δ,T)=∫0ℏωDdηη2+Δ2tanh⁡η2+Δ22kBT.I_0(\hbar\omega_D,\Delta)=\int_0^{\hbar\omega_D}\frac{d\eta}{\sqrt{\eta^2+\Delta^2}},\qquad I(k_B,\hbar\omega_D,\Delta,T)=\int_0^{\hbar\omega_D}\frac{d\eta}{\sqrt{\eta^2+\Delta^2}}\tanh\frac{\sqrt{\eta^2+\Delta^2}}{2k_BT}.I0​(ℏωD​,Δ)=∫0ℏωD​​η2+Δ2​dη​,I(kB​,ℏωD​,Δ,T)=∫0ℏωD​​η2+Δ2​dη​tanh2kB​Tη2+Δ2​​.

The zero-temperature gap Δ(0)\Delta(0)Δ(0) is the positive solution of 1/λ=I0(ℏωD,Δ)1/\lambda = I_0(\hbar\omega_D,\Delta)1/λ=I0​(ℏωD​,Δ); the critical temperature TcT_cTc​ is the positive solution of 1/λ=I(kB,ℏωD,0,T)1/\lambda = I(k_B,\hbar\omega_D,0,T)1/λ=I(kB​,ℏωD​,0,T); and for 0<T<Tc0<T<T_c0<T<Tc​ the gap Δ(T)\Delta(T)Δ(T) is the positive solution of 1/λ=I(kB,ℏωD,Δ,T)1/\lambda = I(k_B,\hbar\omega_D,\Delta,T)1/λ=I(kB​,ℏωD​,Δ,T). The Fermi–Dirac function is f(E,T)=1/(eE/kBT+1)f(E,T) = 1/(e^{E/k_BT}+1)f(E,T)=1/(eE/kB​T+1), and 1−2f(E,T)=tanh⁡(E/2kBT)1-2f(E,T) = \tanh(E/2k_BT)1−2f(E,T)=tanh(E/2kB​T).

Formalization targets

Goal: the universal gap ratio

lim⁡λ→0+Δ(0)kBTc=πeγ=1.764…\lim_{\lambda\to0^+}\frac{\Delta(0)}{k_BT_c}=\frac{\pi}{e^{\gamma}}=1.764\ldotsλ→0+lim​kB​Tc​Δ(0)​=eγπ​=1.764…

with γ\gammaγ the Euler–Mascheroni constant. The source writes Δ(T=0)=2ℏωDe−1/V0Z(EF)=πeγkBTc\Delta(T=0)=2\hbar\omega_D e^{-1/V_0Z(E_F)}=\frac{\pi}{e^\gamma}k_BT_cΔ(T=0)=2ℏωD​e−1/V0​Z(EF​)=eγπ​kB​Tc​; both equalities are weak-coupling asymptotics, so the goal is stated as a limit λ→0+\lambda\to0^+λ→0+ at fixed kBk_BkB​, ℏωD\hbar\omega_DℏωD​.

Milestones

  1. I0(ℏωD,Δ)=arsinh⁡(ℏωD/Δ)I_0(\hbar\omega_D,\Delta) = \operatorname{arsinh}(\hbar\omega_D/\Delta)I0​(ℏωD​,Δ)=arsinh(ℏωD​/Δ).
  2. Δ(0)=ℏωD/sinh⁡(1/λ)\Delta(0)=\hbar\omega_D/\sinh(1/\lambda)Δ(0)=ℏωD​/sinh(1/λ), the unique positive solution of the T=0T=0T=0 gap equation.
  3. Δ(0)∼2ℏωDe−1/λ\Delta(0)\sim 2\hbar\omega_D e^{-1/\lambda}Δ(0)∼2ℏωD​e−1/λ as λ→0+\lambda\to0^+λ→0+.
  4. The Fermi–Dirac and tanh⁡\tanhtanh forms of the finite-temperature gap equation agree.
  5. The TcT_cTc​ equation has exactly one positive solution.
  6. kBTc∼2eγπℏωDe−1/λk_BT_c\sim\frac{2e^\gamma}{\pi}\hbar\omega_D e^{-1/\lambda}kB​Tc​∼π2eγ​ℏωD​e−1/λ (the source's 1,141{,}141,14).
  7. Isotope effect: with ℏωD=C/M\hbar\omega_D = C/\sqrt MℏωD​=C/M​, Tc∝M−1/2T_c\propto M^{-1/2}Tc​∝M−1/2.
  8. Δ(T)\Delta(T)Δ(T) exists uniquely for 0<T<Tc0<T<T_c0<T<Tc​, and the gap equation has no positive solution for T≥TcT\ge T_cT≥Tc​.
  9. Near TcT_cTc​: Δ(T)2/(1−T/Tc)\Delta(T)^2/(1-T/T_c)Δ(T)2/(1−T/Tc​) has a limit L(λ)L(\lambda)L(λ) as T→Tc−T\to T_c^-T→Tc−​, and L(λ)/Δ(0)2→8e2γ/(7ζ(3))=1.73672L(\lambda)/\Delta(0)^2\to 8e^{2\gamma}/(7\zeta(3)) = 1.7367^2L(λ)/Δ(0)2→8e2γ/(7ζ(3))=1.73672 as λ→0+\lambda\to0^+λ→0+.
  10. Specific-heat jump: the left derivative D(λ)D(\lambda)D(λ) of Δ(T)2\Delta(T)^2Δ(T)2 at TcT_cTc​ exists, and −D(λ)/(2π23kB2Tc)→12/(7ζ(3))=1.426…-D(\lambda)/(\tfrac{2\pi^2}{3}k_B^2T_c)\to 12/(7\zeta(3)) = 1.426\ldots−D(λ)/(32π2​kB2​Tc​)→12/(7ζ(3))=1.426….

Significance

The universal ratios are the standard quantitative test that separates weak-coupling (BCS-like) superconductors from strong-coupling ones; deviations from 1.7641.7641.764 and 1.431.431.43 are used to diagnose strong electron–phonon coupling. Mathematically, each statement is an assertion about a parameter-dependent integral equation and its asymptotics as λ→0+\lambda\to0^+λ→0+, with the Euler–Mascheroni constant and ζ(3)\zeta(3)ζ(3) arising from the asymptotics of ∫0Xtanh⁡(x)/x dx\int_0^X\tanh(x)/x\,dx∫0X​tanh(x)/xdx and from a Sommerfeld-type expansion near TcT_cTc​. These results are classical in the physics literature; the mission aims at a machine-checked derivation of the textbook constants from the gap equation, together with reusable lemmas on monotone parameter-dependent integrals.

Difficulty

The T=0T=0T=0 statements reduce to an explicit antiderivative. The finite-temperature statements do not: TcT_cTc​ and Δ(T)\Delta(T)Δ(T) are defined only implicitly, so the asymptotics require a uniform expansion ∫0Xtanh⁡(x)/x dx=log⁡X+log⁡(4eγ/π)+o(1)\int_0^X\tanh(x)/x\,dx=\log X+\log(4e^\gamma/\pi)+o(1)∫0X​tanh(x)/xdx=logX+log(4eγ/π)+o(1). The near-TcT_cTc​ and specific-heat statements additionally concern the behaviour of Δ(T)2\Delta(T)^2Δ(T)2 at the boundary point TcT_cTc​, where Δ\DeltaΔ itself is not differentiable, and the evaluation of the resulting coefficient in the limit ℏωD/kBTc→∞\hbar\omega_D/k_BT_c\to\inftyℏωD​/kB​Tc​→∞.

Formalization scope

  • All quantities are real numbers. Δ(0)\Delta(0)Δ(0), TcT_cTc​ and Δ(T)\Delta(T)Δ(T) are defined as real suprema (sSup) of the corresponding positive solution sets, so they equal 000 when no positive solution exists; existence and uniqueness are separate milestones. In particular Δ(T)=0\Delta(T)=0Δ(T)=0 for T≥TcT\ge T_cT≥Tc​.
  • The zero-temperature gap is a separate definition: at T=0T=0T=0 the finite-temperature integrand is not used.
  • The coupling enters only through λ=V0Z(EF)\lambda = V_0Z(E_F)λ=V0​Z(EF​); asymptotic claims are limits λ→0+\lambda\to0^+λ→0+ at fixed kB,ℏωD>0k_B,\hbar\omega_D>0kB​,ℏωD​>0, with the exact constants 2eγ/π2e^\gamma/\pi2eγ/π, 8e2γ/(7ζ(3))8e^{2\gamma}/(7\zeta(3))8e2γ/(7ζ(3)) and 12/(7ζ(3))12/(7\zeta(3))12/(7ζ(3)) in place of the rounded 1,141{,}141,14, 1,7421{,}74^21,742 and 1,431{,}431,43. ζ(3)\zeta(3)ζ(3) is written as the real part of riemannZeta 3.
  • The specific heat is not modeled thermodynamically; the jump milestone formalizes the source's closed-form expression in terms of −dΔ2/dT-d\Delta^2/dT−dΔ2/dT at TcT_cTc​.
  • Needed infrastructure: monotonicity and continuity of parameter-dependent interval integrals, the integral identity for arsinh⁡\operatorname{arsinh}arsinh, asymptotics of ∫0Xtanh⁡x/x dx\int_0^X\tanh x/x\,dx∫0X​tanhx/xdx, and Mathlib's Euler–Mascheroni constant and ζ(3)\zeta(3)ζ(3).

Selected references

  • J. Bardeen, L. N. Cooper, J. R. Schrieffer, Theory of Superconductivity, Phys. Rev. 108, 1175 (1957). https://doi.org/10.1103/PhysRev.108.1175
  • L. N. Cooper, Bound Electron Pairs in a Degenerate Fermi Gas, Phys. Rev. 104, 1189 (1956). https://doi.org/10.1103/PhysRev.104.1189
  • Wikipedia (de), BCS-Theorie, section Erfolge der BCS-Theorie (source used for all statements). https://de.wikipedia.org/wiki/BCS-Theorie
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Dynamical SystemsLinear algebra·Captain: Lucas

Dynamic Stochastic General Equilibrium I: The Taylor Principle and DeterminacyTextbook

Motivation

Dynamic stochastic general equilibrium (DSGE) models are the standard framework used by central banks and fiscal authorities for policy analysis and forecasting (Wikipedia overview). The models used for monetary-policy analysis are built from three interrelated blocks — demand, supply and a monetary-policy rule — that jointly determine output, inflation and the nominal interest rate. The canonical small-scale instance is the three-equation New Keynesian model (Woodford 2003; Galí 2008; Clarida, Galí and Gertler 1999).

A basic question about such a model is whether it pins down a unique equilibrium path at all. If many bounded paths solve the model, the model makes no definite prediction and expectations can become self-fulfilling. The answer for the three-equation model is the Taylor principle: the interest-rate rule must respond to inflation strongly enough.

Timeline. Blanchard and Kahn (1980) gave the eigenvalue-counting criterion for existence and uniqueness of bounded solutions of linear rational-expectations models. Kydland and Prescott (1982) started the real-business-cycle/DSGE programme. Rotemberg and Woodford (1997) introduced the New Keynesian DSGE framework. Bullard and Mitra (2002) derived the explicit determinacy condition κ(ϕπ−1)+(1−β)ϕy>0\kappa(\phi_\pi - 1) + (1-\beta)\phi_y > 0κ(ϕπ​−1)+(1−β)ϕy​>0 for the model with a contemporaneous Taylor rule, presented in textbook form by Galí (2008, Ch. 3).

Setting

Time is discrete, t=0,1,2,…t = 0, 1, 2, \dotst=0,1,2,…. All variables are deviations from the zero-inflation steady state: yty_tyt​ is the output gap, πt\pi_tπt​ inflation, and iti_tit​ the nominal interest rate. The parameters are σ>0\sigma > 0σ>0 (inverse elasticity of intertemporal substitution), β∈(0,1)\beta \in (0,1)β∈(0,1) (discount factor), κ>0\kappa > 0κ>0 (slope of the Phillips curve), and the policy coefficients ϕπ,ϕy≥0\phi_\pi, \phi_y \ge 0ϕπ​,ϕy​≥0.

A triple of real sequences (y,π,i)(y, \pi, i)(y,π,i) is an equilibrium if for every ttt

yt=yt+1−1σ(it−πt+1)(demand: dynamic IS curve)πt=βπt+1+κyt(supply: New Keynesian Phillips curve)it=ϕππt+ϕyyt(monetary policy: Taylor rule).\begin{aligned} y_t &= y_{t+1} - \tfrac{1}{\sigma}(i_t - \pi_{t+1}) && \text{(demand: dynamic IS curve)}\\ \pi_t &= \beta \pi_{t+1} + \kappa y_t && \text{(supply: New Keynesian Phillips curve)}\\ i_t &= \phi_\pi \pi_t + \phi_y y_t && \text{(monetary policy: Taylor rule).} \end{aligned}yt​πt​it​​=yt+1​−σ1​(it​−πt+1​)=βπt+1​+κyt​=ϕπ​πt​+ϕy​yt​​​(demand: dynamic IS curve)(supply: New Keynesian Phillips curve)(monetary policy: Taylor rule).​

The demand equation is the log-linearised consumption Euler equation, which equates marginal utility of consumption today with discounted marginal utility tomorrow. The model is determinate if the zero path is its only equilibrium in which yyy, π\piπ and iii all stay bounded.

Formalization targets

Goal: the Taylor principle

For σ>0\sigma > 0σ>0, 0<β<10 < \beta < 10<β<1, κ>0\kappa > 0κ>0, ϕπ,ϕy≥0\phi_\pi, \phi_y \ge 0ϕπ​,ϕy​≥0:

the model is determinate  ⟺  κ(ϕπ−1)+(1−β)ϕy>0.\text{the model is determinate} \iff \kappa(\phi_\pi - 1) + (1 - \beta)\phi_y > 0 .the model is determinate⟺κ(ϕπ​−1)+(1−β)ϕy​>0.

Milestones

  1. Consumption Euler equation. At an interior optimum of the two-period consumption–saving problem, u′(c0)=β(1+r)u′(c1)u'(c_0) = \beta(1+r)u'(c_1)u′(c0​)=β(1+r)u′(c1​).
  2. State-space form. For σ,β≠0\sigma, \beta \ne 0σ,β=0, the model is equivalent to (yt+1,πt+1)⊤=M(yt,πt)⊤(y_{t+1}, \pi_{t+1})^\top = M(y_t, \pi_t)^\top(yt+1​,πt+1​)⊤=M(yt​,πt​)⊤ together with the Taylor rule, for an explicit 2×22\times22×2 matrix MMM.
  3. Equilibria are parametrised by initial conditions. Each (y0,π0)(y_0, \pi_0)(y0​,π0​) determines exactly one equilibrium.
  4. Schur–Cohn test. For real TTT and D>0D > 0D>0, both roots of z2−Tz+Dz^2 - Tz + Dz2−Tz+D have modulus >1> 1>1 iff D>1D > 1D>1 and ∣T∣<1+D|T| < 1 + D∣T∣<1+D.
  5. Blanchard–Kahn lemma. For a real square matrix MMM, the only bounded solution of xt+1=Mxtx_{t+1} = Mx_txt+1​=Mxt​ is zero iff every complex eigenvalue of MMM has modulus >1> 1>1.

Significance

The result itself. The Taylor principle is the standard criterion for whether an interest-rate rule yields a well-defined equilibrium in New Keynesian models, and it is the first property checked when a policy rule is proposed. The determinacy region it describes is the starting point for the analysis of optimal policy and of learnability (Bullard and Mitra 2002).

Formalizing it. The result is classical and proved on paper. This mission formalizes the known argument. The mission produces a reusable Lean definition of the basic New Keynesian model, a general lemma on bounded orbits of linear recursions (which applies to any linear rational-expectations model with only forward-looking variables), and a formal Schur–Cohn criterion for real quadratics.

Difficulty

The economic content is elementary, but the obvious argument skips the hardest step. Textbook treatments state "determinacy holds iff both eigenvalues lie outside the unit circle" without proof, and the equivalence between "no nonzero bounded solution" and an eigenvalue condition has to be established for real sequences while the eigenvalues may be complex. In particular the converse direction needs a real bounded solution built from a complex eigenvector, and the boundary case of eigenvalues on the unit circle must come out on the non-determinate side. The parameter translation also has to handle complex-conjugate eigenvalues, not only real ones.

Formalization scope

  • Sequences are functions N→R\mathbb N \to \mathbb RN→R; the model is the deterministic (shock-free) version, so there are no expectation operators. Stochastic shocks do not change the determinacy condition, but that extension is outside the scope of this mission.
  • "Bounded" means a single real bound for all ttt; determinacy requires yyy, π\piπ and iii to be bounded. Boundedness of iii follows from that of yyy and π\piπ, so this adds no restriction.
  • Division is Lean's total division; every statement that divides by σ\sigmaσ or β\betaβ assumes they are nonzero (or positive).
  • Eigenvalues are complex roots of the characteristic polynomial of the complexified matrix.
  • The goal is not trivial: the zero path is always an equilibrium, determinacy is a genuine uniqueness claim, and the parameter hypotheses are satisfiable (e.g. σ=1\sigma = 1σ=1, β=0.99\beta = 0.99β=0.99, κ=0.1\kappa = 0.1κ=0.1, ϕπ=1.5\phi_\pi = 1.5ϕπ​=1.5, ϕy=0.5\phi_y = 0.5ϕy​=0.5).
  • All declarations live in the namespace DSGE. Contributions of general linear-recursion and polynomial-root lemmas are welcome.

Selected references

  • Wikipedia, Dynamic stochastic general equilibrium. https://en.wikipedia.org/wiki/Dynamic_stochastic_general_equilibrium
  • O. J. Blanchard and C. M. Kahn, The Solution of Linear Difference Models under Rational Expectations, Econometrica 48(5), 1980. https://doi.org/10.2307/1912186
  • F. E. Kydland and E. C. Prescott, Time to Build and Aggregate Fluctuations, Econometrica 50(6), 1982. https://doi.org/10.2307/1913386
  • R. Clarida, J. Galí and M. Gertler, The Science of Monetary Policy: A New Keynesian Perspective, Journal of Economic Literature 37(4), 1999. https://doi.org/10.1257/jel.37.4.1661
  • J. Bullard and K. Mitra, Learning about Monetary Policy Rules, Journal of Monetary Economics 49(6), 2002. https://doi.org/10.1016/S0304-3932(02)00144-7
  • M. Woodford, Interest and Prices: Foundations of a Theory of Monetary Policy, Princeton University Press, 2003.
  • J. Galí, Monetary Policy, Inflation, and the Business Cycle, Princeton University Press, 2008 (Chapter 3).
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AnalysisMathematical Physics·Captain: Lucas

Titius–Bode Law I: The −25%/+50% Coverage Band of Doubling Distance RulesTextbook

Motivation

The Titius–Bode law is an empirical rule, published in the eighteenth century by J. D. Titius and J. E. Bode, for the semi-major axes of the planets: in units in which the Earth's semi-major axis is 101010, the planets lie near 4+x4+x4+x with x=0,3,6,12,24,48,96,…x = 0, 3, 6, 12, 24, 48, 96, \dotsx=0,3,6,12,24,48,96,…. It anticipated the positions of Uranus (1781) and Ceres (1801), failed for Neptune (1846), and has since become a standard example of how a numerical pattern can fit data without a physical mechanism. Dermott's law (S. F. Dermott, 1968) is the analogous power law T(n)=T(0) CnT(n) = T(0)\,C^nT(n)=T(0)Cn for the orbital periods of the major satellites of Jupiter, Saturn and Uranus.

Much of the debate about such rules is quantitative rather than physical. The Wikipedia article on the law records, in a footnote to its data table, the observation that because consecutive predicted distances roughly double, an arbitrary planet may be found within −25%-25\%−25% to +50%+50\%+50% of one of the predicted positions. In other words, the agreement of any single body with the rule at that level carries no information. This mission formalizes that observation and the elementary arithmetic of the law as stated in the source.

Timeline (as recorded in the source). Gregory (1702, 1715) and Wolff (1723–24) give the sequence 4,7,10,16,52,1004, 7, 10, 16, 52, 1004,7,10,16,52,100; Titius (1766) and Bode (1772) publish the rule; Uranus (1781) and Ceres (1801) fit it; Neptune (1846) does not; Blagg (1913) and Richardson (1945) replace the ratio 222 by about 1.731.731.73; Dermott (1968) proposes the period law for satellite systems; Nieto (1970, 1972) reviews the subject.

Setting

For a formal exponent n∈{−∞,0,1,2,… }n \in \{-\infty, 0, 1, 2, \dots\}n∈{−∞,0,1,2,…} put 2−∞=02^{-\infty} = 02−∞=0. The Titius–Bode distance in astronomical units is

a(n)=0.4+0.3⋅2n,n=−∞,0,1,2,…,a(n) = 0.4 + 0.3 \cdot 2^{n}, \qquad n = -\infty, 0, 1, 2, \dots,a(n)=0.4+0.3⋅2n,n=−∞,0,1,2,…,

so a(−∞)=0.4a(-\infty) = 0.4a(−∞)=0.4, a(0)=0.7a(0) = 0.7a(0)=0.7, a(1)=1.0a(1) = 1.0a(1)=1.0, a(2)=1.6,…a(2) = 1.6, \dotsa(2)=1.6,…. The same numbers appear in three other guises in the source: the original form 4+x4 + x4+x (Earth =10=10=10), the form 4+3⋅2n4 + 3 \cdot 2^n4+3⋅2n (Earth =10=10=10), and the canonical form an=0.4+0.3⋅2na_n = 0.4 + 0.3 \cdot 2^nan​=0.4+0.3⋅2n for n=0,1,2,…n = 0, 1, 2, \dotsn=0,1,2,…. The relative deviation of an observed value ddd from a predicted value ppp is (d−p)/p(d - p)/p(d−p)/p, which the source reports as a percentage.

Dermott's law models the period of the nnn-th satellite as T(n)=T(0) CnT(n) = T(0)\,C^nT(n)=T(0)Cn. Kepler's third law makes the semi-major axis proportional to the 2/32/32/3 power of the period, a=K T2/3a = K\,T^{2/3}a=KT2/3.

Formalization targets

Goal: the coverage band

∀d≥0.3:∃ n∈{−∞,0,1,2,… },−14  ≤  d−a(n)a(n)  ≤  12.\forall d \ge 0.3:\quad \exists\, n \in \{-\infty,0,1,2,\dots\},\qquad -\tfrac14 \;\le\; \frac{d - a(n)}{a(n)} \;\le\; \tfrac12 .∀d≥0.3:∃n∈{−∞,0,1,2,…},−41​≤a(n)d−a(n)​≤21​.

Every distance of at least 0.30.30.3 au lies within −25%-25\%−25% to +50%+50\%+50% of some Titius–Bode position. The lower limit 0.3=34⋅0.40.3 = \tfrac34 \cdot 0.40.3=43​⋅0.4 is exactly where the statement begins to hold: below it no predicted position is close enough. The source says "an arbitrary planet"; the formal statement makes the range explicit.

Supporting milestones

  1. The four representations of the rule (original, Earth =10=10=10, au, canonical) agree.
  2. The recursion an+1=2an−0.4a_{n+1} = 2a_n - 0.4an+1​=2an​−0.4 holds for the canonical form; started from a0=0.55a_0 = 0.55a0​=0.55, as printed in the source, it produces the canonical sequence shifted by one index.
  3. The predicted distances in the data table: 0.4,0.7,1.0,1.6,2.8,5.2,10.0,19.6,38.80.4, 0.7, 1.0, 1.6, 2.8, 5.2, 10.0, 19.6, 38.80.4,0.7,1.0,1.6,2.8,5.2,10.0,19.6,38.8 au, and 77.277.277.2 au for the next term.
  4. Consecutive predicted distances less than double, with ratio tending to 222.
  5. The abstract principle behind the goal: for any unbounded sequence with pk+1≤2pkp_{k+1} \le 2p_kpk+1​≤2pk​, every d≥34p0d \ge \tfrac34 p_0d≥43​p0​ lies within −25%-25\%−25% to +50%+50\%+50% of some pkp_kpk​.
  6. The 2:32{:}32:3 resonance figures: semi-major axes of bodies with periods in ratio 2:32{:}32:3 differ by −23.69%-23.69\%−23.69% and +31.04%+31.04\%+31.04% relative to one another.
  7. Dermott's law gives geometric spacing of periods (ratio CCC) and, through Kepler's third law, of semi-major axes (ratio C2/3C^{2/3}C2/3).

Significance

The goal makes precise why a fit of a single body to the Titius–Bode rule within tens of percent is weak evidence: the predicted positions are spaced so that the whole half-line [0.3,∞)[0.3, \infty)[0.3,∞) is covered by such bands. The resonance milestone gives the corresponding figures for a 2:32{:}32:3 period commensurability, and the Dermott milestone connects period power laws to Titius–Bode-type distance laws, as the source asserts.

All results are elementary and none is open. The value of the mission is a checked, unambiguous record of the arithmetic claims in the source, including one place where the source's formulas disagree: the "recursive form" with a0=0.55a_0 = 0.55a0​=0.55 does not reproduce the canonical form index-for-index but is shifted by one (milestone 2). No machine-checked version of these statements is known to exist on the platform.

Difficulty

There is no deep obstacle. The covering argument needs care in two places: the first step of the rule (0.4→0.70.4 \to 0.70.4→0.7) is not a doubling, and the generic doubling lemma must locate the first term that exceeds ddd without assuming monotonicity. The resonance milestone requires certified numerical bounds on the irrational numbers (2/3)2/3(2/3)^{2/3}(2/3)2/3 and (3/2)2/3(3/2)^{2/3}(3/2)2/3 that are tight enough to fix the second decimal place of a percentage.

Formalization scope

Distances, periods and deviations are real numbers. The exponent set {−∞,0,1,2,… }\{-\infty, 0, 1, 2, \dots\}{−∞,0,1,2,…} is encoded as the natural numbers with a bottom element adjoined, and 2−∞2^{-\infty}2−∞ is defined to be 000. The relative deviation is the plain quotient (d−p)/p(d-p)/p(d−p)/p; every statement only evaluates it at positive ppp. Percent figures from the source (−23.69%-23.69\%−23.69%, +31.04%+31.04\%+31.04%) are stated as "within 0.0050.0050.005 percentage points", i.e. correct to the two decimals printed. Kepler's law enters only as the hypothesis a=K T2/3a = K\,T^{2/3}a=KT2/3 with K>0K > 0K>0; no orbital mechanics is formalized. The doubling lemma is stated for an arbitrary real sequence and is reusable for any Titius–Bode-type rule.

Trivializing encodings are ruled out: the goal is not stated for an empty or bounded range of ddd, the predicted set is the full image of the rule, and the deviation band is the one printed in the source.

Selected references

  • Wikipedia, Titius–Bode law, revision 1372822920. https://en.wikipedia.org/w/index.php?title=Titius%E2%80%93Bode_law&oldid=1372822920
  • Wikipedia, Dermott's law, revision 1315813288. https://en.wikipedia.org/w/index.php?title=Dermott%27s_law&oldid=1315813288
  • M. M. Nieto, Conclusions about the Titius–Bode Law of Planetary Distances, Astronomy and Astrophysics 8 (1970), 105–111.
  • S. F. Dermott, On the origin of commensurabilities in the solar system – II: The orbital period relation, MNRAS 141 (1968), 363–376. https://doi.org/10.1093/mnras/141.3.363
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