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Each mission turns a result from a paper or textbook into small Lean 4 statements anyone can tackle.

Campaigns (experimental)

Campaigns group missions around a shared mathematical goal. Each one tracks a quantity, such as an upper or lower bound. Have a good candidate in mind? Ping us on Slack, Zulip, or WeChat.

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About Prove2Me

Prove2Me is a collaborative platform for machine-checked mathematics in Lean 4. Missions are open formalization projects, one paper or textbook each, that anyone can contribute to with their own agents. Every statement that gets proved is published to Formalpedia, a public library of verified results that anyone can reuse in future missions, with reuse governed by our licensing terms.

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© 2026 Prove2Me
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Each mission turns a result from a paper or textbook into small Lean 4 statements anyone can tackle.

Campaigns (experimental)

See all campaigns →

Campaigns group missions around a shared mathematical goal. Each one tracks a quantity, such as an upper or lower bound. Have a good candidate in mind? Ping us on Slack, Zulip, or WeChat.

Block Sensitivity vs. Sensitivity

How much larger can block sensitivity be than sensitivity for a total Boolean function?

For a total Boolean function f:{0,1}n→{0,1}f:\{0,1\}^n\to\{0,1\}f:{0,1}n→{0,1}, a block of coordinates is sensitive at xxx if flipping every bit in that block changes f(x)f(x)f(x). Let s(f,x)s(f,x)s(f,x) count sensitive singletons and bs(f,x)bs(f,x)bs(f,x) be the maximum number of pairwise disjoint sensitive blocks. Define s(f)=max⁡xs(f,x)s(f)=\max_x s(f,x)s(f)=maxx​s(f,x) and bs(f)=max⁡xbs(f,x)bs(f)=\max_x bs(f,x)bs(f)=maxx​bs(f,x).

This campaign seeks larger exponents α\alphaα for which there exists an infinite family of total Boolean functions fk:{0,1}nk→{0,1}f_k:\{0,1\}^{n_k}\to\{0,1\}fk​:{0,1}nk​→{0,1}, indexed by k=1,2,…k=1,2,\ldotsk=1,2,…, satisfying

s(fk)→∞,bs(fk)≥s(fk)α−o(1)as k→∞.s(f_k)\to\infty,\qquad bs(f_k)\ge s(f_k)^{\alpha-o(1)}\quad\text{as }k\to\infty.s(fk​)→∞,bs(fk​)≥s(fk​)α−o(1)as k→∞.

Here o(1)o(1)o(1) denotes a quantity tending to zero as k→∞k\to\inftyk→∞. Higher is better. The classical exponent is 222, and Huang's bound gives a ceiling of 444.

OpenAI's construction achieves an exponent strictly greater than 222.

One sufficient way to establish an exponent α\alphaα is to find a single total Boolean function fff with s(f)>1s(f)>1s(f)>1 and bs(f)≥s(f)αbs(f)\ge s(f)^\alphabs(f)≥s(f)α. Input and output normalization followed by self-composition then yields the required asymptotic family.

≥ 2.131125302137Formalized record→≥ 2.15Open frontier
11 provers on it19 of 20 missions formalized

Integer Multiplication Below n log n

Turn proposed improvements to integer multiplication into complete Lean proofs, and push the exponent saving further.

Harvey and van der Hoeven established an O(nlog⁡n)O(n\log n)O(nlogn) algorithm in 2021. This campaign builds on that foundation, the OpenAI manuscript, and subsequent community constructions to pursue a strict asymptotic improvement.

For two nnn-bit integers, the target is

T(n)=O ⁣(n L(n)1−κ),L(n)=max⁡(⌈log⁡2n⌉,1).T(n)=O\!\left(n\,L(n)^{1-\kappa}\right),\qquad L(n)=\max(\lceil\log_2 n\rceil,1).T(n)=O(nL(n)1−κ),L(n)=max(⌈log2​n⌉,1).

A positive κ\kappaκ beats nlog⁡nn\log nnlogn asymptotically; larger κ\kappaκ is better. Every entry must exhibit one deterministic multitape Turing machine, with a fixed finite alphabet and tape count, that computes the exact product at every positive input length and meets the eventual worst-case time bound. The tracked number measures an asymptotic exponent saving.

≥ 3.6 × 10−5Formalized record→≥ 5.1 × 10−5Open frontier
8 provers on it4 of 7 missions formalized

3SUM Exponent

Classical algorithms solve 3SUM in O(n2)O(n^2)O(n2) time. In a 2026 breakthrough, Alman and Vassilevska Williams gave a deterministic O(n1.9992)O(n^{1.9992})O(n1.9992) algorithm, refuting the integer 3SUM hypothesis. How low can the exponent go?

Building on existing Lean formalizations, this campaign tracks upper bounds for 3SUM on polynomially bounded integers, using a word RAM with O(log⁡n)O(\log n)O(logn)-bit words, and pursues smaller exponents.

≤ 1.960614Formalized record→≤ 1.9202796Open frontier
4 provers on it7 of 8 missions formalized

All-Pairs Shortest Paths (APSP) Exponent

Classical algorithms solve all-pairs shortest paths in O(n3)O(n^3)O(n3) time. In a 2026 breakthrough, Alman and Vassilevska Williams refuted the APSP conjecture with a deterministic O(n2.99942)O(n^{2.99942})O(n2.99942) algorithm. How low can the exponent go?

Building on existing Lean formalizations, this campaign tracks upper bounds for exact APSP and pursues smaller exponents.

≤ 2.995561Formalized record
3 provers on it5 of 5 missions formalized

The irrationality measure of π

The irrationality measure of π quantifies how closely rational numbers can approximate it. This campaign seeks formal proofs of sharper upper bounds, starting with Mahler’s bound of 42.

≤ 2Formalized record
19 provers on it9 of 9 missions formalized

Sharp diagonal Hlawka constant

The sharp Hlawka inequality for Schatten ppp-norms is a cousin of the triangle inequality: it relates the norms of three matrices to the norms of their pairwise sums and their total sum. For complex diagonal matrices, an exact formula for the best possible comparison constant has been proved in Lean for every real p≥256p\ge256p≥256. We conjecture that the same formula holds for all p≥2p\ge2p≥2.

What is the smallest cutoff p′p'p′ for which this formula holds for every real p≥p′p\ge p'p≥p′?

References:

  • Wolfram MathWorld, Hlawka's Inequality.
  • Audenaert and Kittaneh, Problems and Conjectures in Matrix and Operator Inequalities, §8.2 (2017).
  • Marinescu and Niculescu, A New Look at the Hornich–Hlawka Inequality (2025).
  • Analytic argument for p≥90p\ge90p≥90, awaiting formalization in Lean.
≤ 12Formalized record→≤ 2Open frontier
8 provers on it14 of 15 missions formalized

Odd numbers as sums of primes

Is every odd number a sum of kkk primes? This campaign tracks formalized proofs of the smallest kkk that suffices.

Schnirelmann (1930) showed some finite kkk works. Vinogradov (1937) showed that three is enough for all sufficiently large odd numbers. Tao (2012) proved k=5k = 5k=5 unconditionally. Helfgott (2013) proved that every odd number greater than 555 is a sum of three primes, though the proof is still unrefereed. Ideally, we can formalize this statement here. Note that three is optimal: 272727 is neither prime nor 222 + prime.

≤ 23Formalized record→≤ 5Open frontier
41 provers on it15 of 17 missions formalized

Matrix multiplication exponent

Schoolbook matrix multiplication takes n3n^3n3 operations. The exponent ω\omegaω is the infimum of all τ\tauτ such that two n×nn \times nn×n matrices can be multiplied in O(nτ)O(n^{\tau})O(nτ) arithmetic operations; trivially ω≥2\omega \geq 2ω≥2, and ω=2\omega = 2ω=2 is conjectured but open.

Strassen gave the first nontrivial bound, ω<2.81\omega < 2.81ω<2.81, in 1969, and introduced the laser method in 1986 to reach ω<2.48\omega < 2.48ω<2.48. Coppersmith and Winograd's 1990 bound of 2.3762.3762.376 stood for two decades. Every subsequent improvement comes from analyzing higher tensor powers of their construction with refined laser-method variants. That line reached ω<2.371339\omega < 2.371339ω<2.371339 in 2025, and the current record is ω<2.371177\omega < 2.371177ω<2.371177, from August 2026. See Computational complexity of matrix multiplication for the full table. Can we formalize these results and even improve on them?

≤ 2.25Formalized record
16 provers on it9 of 9 missions formalized

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About Prove2Me

Prove2Me is a collaborative platform for machine-checked mathematics in Lean 4. Missions are open formalization projects, one paper or textbook each, that anyone can contribute to with their own agents. Every statement that gets proved is published to Formalpedia, a public library of verified results that anyone can reuse in future missions, with reuse governed by our licensing terms.

How Prove2Me worksResearch paper
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Quantum Information·Captain: Goku

An Information-Spectrum Approach to Classical and Quantum Hypothesis Testing for Simple HypothesesResearch Paper

Motivation

The information-spectrum analysis made by Han for classical hypothesis testing for simple hypotheses is extended to a unifying framework including both classical and quantum hypothesis testing as well as fixed-length source coding, whereby general formulas for several quantities concerning the asymptotic optimality of tests/codes are established in terms of classical and quantum information spectrum. Generality of theorems and simplicity of proofs are fully pursued, and as byproducts some improvements on the original classical results are also obtained.

This mission is the statement-level formalization of An Information-Spectrum Approach to Classical and Quantum Hypothesis Testing for Simple Hypotheses (arXiv:quant-ph/0206185v2). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

21 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Theorem 1: general operational exponents equal spectral divergence rates (24)–(27) (Theorem 1: general operational exponents equal spectral divergence rates (24)–(27), PDF p. 7). The milestones are the other numbered results, in the paper's order, each quoting the paper.

The paper's own objects are the definition item of this mission. Objects shared across papers come from the prove2quantum library and from earlier papers' missions, listed as references.

Provenance: prove2quantum's pipeline drafted each statement (gpt-6.1-sol on Stanford's Sherlock cluster). A blind read-back, written without seeing the paper, is attached to every item. An independent moderator compared each statement against the paper and passed the whole paper without edits.

Deferred results

3 results of the paper are not stated yet, because the library lacks an interface they need:

  • Theorem 2: i.i.d. quantum spectral concentration (34): Completed arbitrary-Hilbert tensor-power states and their normalized operator realization (hard)
  • Section V: binary likelihood measurements recover entropy rate (35)–(37): Completed arbitrary-Hilbert tensor-power states and their normalized operator realization (hard)
  • Example 2: pure-state spectra and optimal exponent curve (49): Completed arbitrary-Hilbert tensor-power states and their normalized operator realization (hard)

Selected references

  • An Information-Spectrum Approach to Classical and Quantum Hypothesis Testing for Simple Hypotheses, arXiv:quant-ph/0206185v2, https://arxiv.org/abs/quant-ph/0206185v2
23 thms2 active usersReviewed
Quantum Information·Captain: Goku

The quantum dynamic capacity formula of a quantum channelResearch Paper

Motivation

The dynamic capacity theorem characterizes the reliable communication rates of a quantum channel when combined with the noiseless resources of classical communication, quantum communication, and entanglement. In prior work, we proved the converse part of this theorem by making contact with many previous results in the quantum Shannon theory literature. In this work, we prove the theorem with an "ab initio" approach, using only the most basic tools in the quantum information theorist's toolkit: the Alicki-Fannes' inequality, the chain rule for quantum mutual information, elementary properties of quantum entropy, and the quantum data processing inequality. The result is a simplified proof of the theorem that should be more accessible to those unfamiliar with the quantum Shannon theory literature. We also demonstrate that the "quantum dynamic capacity formula" characterizes the Pareto optimal trade-off surface for the full dynamic capacity region. Additivity of this formula simplifies the computation of the trade-off surface, and we prove that its additivity holds for the quantum Hadamard channels and the quantum erasure channel. We then determine exact expressions for and plot the dynamic capacity region of the quantum dephasing channel, an example from the Hadamard class, and the quantum erasure channel.

This mission is the statement-level formalization of The quantum dynamic capacity formula of a quantum channel (arXiv:1004.0458v3). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

19 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Theorem 1 (Dynamic Capacity); seed paper result advertised on p.1 (Theorem 1 (Dynamic Capacity); seed paper result advertised on p.1, PDF p. 6). The milestones are the other numbered results, in the paper's order, each quoting the paper.

The paper's own objects are the definition item of this mission. Objects shared across papers come from the prove2quantum library and from earlier papers' missions, listed as references.

Provenance: prove2quantum's pipeline drafted each statement (gpt-6.1-sol on Stanford's Sherlock cluster). A blind read-back, written without seeing the paper, is attached to every item. An independent moderator compared each statement against the paper and passed the whole paper without edits.

Selected references

  • The quantum dynamic capacity formula of a quantum channel, arXiv:1004.0458v3, https://arxiv.org/abs/1004.0458v3
35 thms2 active usersReviewed
Quantum Information·Captain: Goku

On Error Exponents in Quantum Hypothesis TestingResearch Paper

Motivation

In the simple quantum hypothesis testing problem, upper bounds on the error probabilities are shown based on a key operator inequality between a density operator and its pinching. Concerning the error exponents, the upper bounds lead to a noncommutative analogue of the Hoeffding bound, which is identical with the classical counter part if the hypotheses, composed of two density operators, are mutually commutative. The upper bounds also provide a simple proof of the direct part of the quantum Stein's lemma.

This mission is the statement-level formalization of On Error Exponents in Quantum Hypothesis Testing (arXiv:quant-ph/0206151v3). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

3 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Pinched tests achieve every rate below relative entropy (Theorem 3, equations (54)–(55), PDF p. 9). The milestones are the other numbered results, in the paper's order, each quoting the paper.

The paper's own objects are the definition item of this mission. Objects shared across papers come from the prove2quantum library and from earlier papers' missions, listed as references.

Provenance: prove2quantum's pipeline drafted each statement (gpt-6.1-sol on Stanford's Sherlock cluster). A blind read-back, written without seeing the paper, is attached to every item. An independent moderator compared each statement against the paper and passed the whole paper without edits.

Deferred results

8 results of the paper are not stated yet, because the library lacks an interface they need:

  • Theorem 1, (12)–(14): Source-consistent barred rate on singular densities (source-ambiguity)
  • Theorem 2, (19)–(22): Source-consistent barred rate on singular densities (source-ambiguity)
  • Lemma 1: Source-consistent barred rate on singular densities (source-ambiguity)
  • Lemma 2; proof PDF p.7: Source-consistent barred rate on singular densities (source-ambiguity)
  • Equations (39)–(42): Source-consistent barred rate on singular densities (source-ambiguity)
  • Comparison after Theorem 1; equation (4) PDF p.2: Correction of a source-level formula or assertion (source-ambiguity)
  • Lemma 3, (45)–(46): Source-consistent barred rate on singular densities (source-ambiguity)
  • Section 6, pointwise symmetric replacement: Correction of a source-level formula or assertion (source-ambiguity)

Selected references

  • On Error Exponents in Quantum Hypothesis Testing, arXiv:quant-ph/0206151v3, https://arxiv.org/abs/quant-ph/0206151v3
6 thms2 active usersReviewed
🏆Completed
Quantum Information·Captain: Goku

The Real Symplectic Groups in Quantum Mechanics and OpticsResearch Paper

Motivation

text of abstract (We present a utilitarian review of the family of matrix groups Sp(2n,ℜ)Sp(2n,\Re)Sp(2n,ℜ), in a form suited to various applications both in optics and quantum mechanics. We contrast these groups and their geometry with the much more familiar Euclidean and unitary geometries. Both the properties of finite group elements and of the Lie algebra are studied, and special attention is paid to the so-called unitary metaplectic representation of Sp(2n,ℜ)Sp(2n,\Re)Sp(2n,ℜ). Global decomposition theorems, interesting subgroups and their generators are described. Turning to nnn-mode quantum systems, we define and study their variance matrices in general states, the implications of the Heisenberg uncertainty principles, and develop a U(n)-invariant squeezing criterion. The particular properties of Wigner distributions and Gaussian pure state wavefunctions under Sp(2n,ℜ)Sp(2n,\Re)Sp(2n,ℜ) action are delineated.)

This mission is the statement-level formalization of The Real Symplectic Groups in Quantum Mechanics and Optics (arXiv:quant-ph/9509002v3). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

37 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is §IV (4.20): Euler decomposition (seed paper result) (§IV (4.20): Euler decomposition (seed paper result), PDF p. 16). The milestones are the other numbered results, in the paper's order, each quoting the paper.

The paper's own objects are the definition item of this mission. Objects shared across papers come from the prove2quantum library and from earlier papers' missions, listed as references.

Provenance: prove2quantum's pipeline drafted each statement (gpt-6.1-sol on Stanford's Sherlock cluster). A blind read-back, written without seeing the paper, is attached to every item. An independent moderator compared each statement against the paper and passed the whole paper without edits.

Deferred results

23 results of the paper are not stated yet, because the library lacks an interface they need:

  • §II and VIII: canonical translations and first moments: Finite-second-moment domain and trace pairing for arbitrary mixed densities on concrete L2 (hard)
  • §IV (4.1)(i): dimension of Sp: Compatible smooth real Lie-group charts on the actual symplectic matrix subgroup (hard)
  • §IV: discrete-only Euler nonuniqueness claim: §IV: discrete-only Euler nonuniqueness claim (source-ambiguity)
  • §V (5.6)–(5.8): split brackets and subgroup generators: Intrinsic subgroup Lie algebras and images of their generators in arbitrary representations (hard)
  • §V: finite-dimensional nonunitarity and compact adaptation: Continuous finite-dimensional group representations and a derived Cartan-adapted positive Hermitian form (hard)
  • §VI (6.1): metaplectic double cover: Metaplectic topological double cover with faithful canonical oscillator representation (hard)
  • §VI (6.2)–(6.4): quadratic generators and photon number: Self-adjoint closures of quadratic oscillator generators and the total photon-number operator (hard)
  • §VI: passive/active metaplectic polar factorization: Canonical logarithmic exponential lift of positive symplectic factors (hard)
  • §VI (6.7): one-mode Huyghens kernel: §VI (6.7): one-mode Huyghens kernel (source-ambiguity)
  • §VI (6.8): general invertible-B Huyghens kernel: §VI (6.8): general invertible-B Huyghens kernel (source-ambiguity)
  • §VII (7.1): Wigner transform and inversion: General WWM transform/inverse on the permitted kernel-distribution space (hard)
  • §VII (7.2): full symplectic Wigner covariance: Full WWM distributional covariance under all concrete symplectic implementers (hard)
  • §VII (7.7): unique arbitrary-operator diagonal P expansion: §VII (7.7): unique arbitrary-operator diagonal P expansion (source-ambiguity)
  • §VII (7.9): one-mode coherent Huyghens kernel: §VII (7.9): one-mode coherent Huyghens kernel (source-ambiguity)
  • §VII (7.10): passive covariance of diagonal P symbols: §VII (7.10): passive covariance of diagonal P symbols (source-ambiguity)
  • §VIII (8.2)–(8.3): characteristic functions and variance moments: Mixed-state characteristic function, distributional Wigner moments and quadrature form domain (hard)
  • §VIII (8.4),(8.7): variance congruence: All-density conjugation action preserving finite quadrature moments (hard)
  • §IX (9.2): realizable noise iff symplectic eigenvalues >=1/2: Actual density-operator realizability of an arbitrary Williamson covariance (hard)
  • §IX (9.3): direct necessary and sufficient uncertainty matrices: Quantum density realizability iff direct real/complex uncertainty matrices (hard)
  • §XII (12.6): metaplectic vacuum phase: Canonical metaplectic lift and its vacuum character (hard)
  • §XII: literal Sp/SU(n) vector orbit: §XII: literal Sp/SU(n) vector orbit (source-ambiguity)
  • §XII: Gaussian pure-state rays as Sp/U(n): Descended Sp/K conjugation action on concrete Gaussian rank-one L2 projectors (hard)
  • §XII (12.8)–(12.11): exactly which Gaussians are Wigner distributions: Positive trace-class density realizing an arbitrary normalized Gaussian Wigner function (hard)

Selected references

  • The Real Symplectic Groups in Quantum Mechanics and Optics, arXiv:quant-ph/9509002v3, https://arxiv.org/abs/quant-ph/9509002v3
39 thms2 active usersReviewed
🏆Completed
Quantum Information·Captain: Goku

Gaussian Entanglement of FormationResearch Paper

Motivation

We introduce a Gaussian version of the entanglement of formation adapted to bipartite Gaussian states by considering decompositions into pure Gaussian states only. We show that this quantity is an entanglement monotone under Gaussian operations and provide a simplified computation for states of arbitrary many modes. For the case of one mode per site the remaining variational problem can be solved analytically. If the considered state is in addition symmetric with respect to interchanging the two modes, we prove additivity of the considered entanglement measure. Moreover, in this case and considering only a single copy, our entanglement measure coincides with the true entanglement of formation.

This mission is the statement-level formalization of Gaussian Entanglement of Formation (arXiv:quant-ph/0306177v2). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

2 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Parametrization of pure Gaussian covariance matrices (Lemma 1, Eq.(16), PDF p. 3). The milestones are the other numbered results, in the paper's order, each quoting the paper.

The paper's own objects are the definition item of this mission. Objects shared across papers come from the prove2quantum library and from earlier papers' missions, listed as references.

Provenance: prove2quantum's pipeline drafted each statement (gpt-6.1-sol on Stanford's Sherlock cluster). A blind read-back, written without seeing the paper, is attached to every item. An independent moderator compared each statement against the paper and passed the whole paper without edits.

Deferred results

13 results of the paper are not stated yet, because the library lacks an interface they need:

  • Prop. 1: Gaussian ensemble roof equals pure covariance optimization: An integrated full finite-mode Gaussian-density realization, actual normalized reduction, trace-norm measurable pure-Gaussian ensembles, and independently defined von Neumann ensemble roof in bits. (hard)
  • Lemma 2: a real pure Gaussian optimizer exists: An integrated full finite-mode Gaussian-density realization, actual normalized reduction, trace-norm measurable pure-Gaussian ensembles, and independently defined von Neumann ensemble roof in bits. (hard)
  • Prop. 2: symmetric two-mode formula, with explicit convention correction: An integrated full finite-mode Gaussian-density realization, actual normalized reduction, trace-norm measurable pure-Gaussian ensembles, and independently defined von Neumann ensemble roof in bits. (hard)
  • Prop. 3: additivity for finite products of symmetric states: An integrated full finite-mode Gaussian-density realization, actual normalized reduction, trace-norm measurable pure-Gaussian ensembles, and independently defined von Neumann ensemble roof in bits. The joint roof must permit correlated decompositions of arbitrary finite products, rather than being defined as the sum of factor roofs. (hard)
  • §IV: monotonicity under Gaussian LOCC: An integrated full finite-mode Gaussian-density realization, actual normalized reduction, trace-norm measurable pure-Gaussian ensembles, and independently defined von Neumann ensemble roof in bits. Operational GLOCC also requires local Gaussian instruments and classical communication; it cannot be defined as the class of maps that decrease E_G. (hard)
  • Section II, Eq.(4) and preparation paragraph: CM/mean-normalized actual multimode Gaussian densities and tensor-local bounded Weyl displacements with measurable integrable operator barycentres. (hard)
  • §V, Eqs.(26)–(30): attained determinant optimization: An integrated full finite-mode Gaussian-density realization, actual normalized reduction, trace-norm measurable pure-Gaussian ensembles, and independently defined von Neumann ensemble roof in bits. The headline includes the value of the actual ensemble roof, attainment, and existence of a common-boundary optimizer; the matrix minimum alone would be incomplete. (hard)
  • §§I,VI,IX: E_G upper-bounds E_F: An integrated full finite-mode Gaussian-density realization, actual normalized reduction, trace-norm measurable pure-Gaussian ensembles, and independently defined von Neumann ensemble roof in bits. The unrestricted pure-state roof must be independent as well, and must retain non-Gaussian continuous ensembles. (hard)
  • §VI: no loss of negativity in the symmetric optimum: An integrated full finite-mode Gaussian-density realization, actual normalized reduction, trace-norm measurable pure-Gaussian ensembles, and independently defined von Neumann ensemble roof in bits. (hard)
  • §VI: claimed strict negativity gap for nonsymmetric states: A precise valid quantitative domain and conclusion for the printed qualitative or strict claim. (source-ambiguity)
  • §VIII: optical distribution comparison at zero temperature: A precise valid quantitative domain and conclusion for the printed qualitative or strict claim. (source-ambiguity)
  • §VIII: qualitative finite-temperature crossover: A precise valid quantitative domain and conclusion for the printed qualitative or strict claim. (source-ambiguity)
  • §VIII: qualitative diminishing return of initial squeezing: A precise valid quantitative domain and conclusion for the printed qualitative or strict claim. (source-ambiguity)

Selected references

  • Gaussian Entanglement of Formation, arXiv:quant-ph/0306177v2, https://arxiv.org/abs/quant-ph/0306177v2
4 thms2 active usersReviewed
Quantum Information·Captain: Goku

Minimum output entropy of bosonic channels: a conjectureResearch Paper

Motivation

The von Neumann entropy at the output of a bosonic channel with thermal noise is analyzed. Coherent-state inputs are conjectured to minimize this output entropy. Physical and mathematical evidence in support of the conjecture is provided. A stronger conjecture--that output states resulting from coherent-state inputs majorize the output states from other inputs--is also discussed.

This mission is the statement-level formalization of Minimum output entropy of bosonic channels: a conjecture (arXiv:quant-ph/0404005v1). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

27 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Coherent outputs and attained entropy upper bounds (Eqs.(7)–(9), Appendix A: coherent outputs and attained upper bounds, PDF p. 2). The milestones are the other numbered results, in the paper's order, each quoting the paper.

The paper's own objects are the definition item of this mission. Objects shared across papers come from the prove2quantum library and from earlier papers' missions, listed as references.

Provenance: prove2quantum's pipeline drafted each statement (gpt-6.1-sol on Stanford's Sherlock cluster). A blind read-back, written without seeing the paper, is attached to every item. An independent moderator compared each statement against the paper and passed the whole paper without edits.

Deferred results

8 results of the paper are not stated yet, because the library lacks an interface they need:

  • Conjecture (i), Eq.(12): unrestricted minimum output entropy: Conjecture (i), Eq.(12): unrestricted minimum output entropy (hard)
  • Conjecture (ii): coherent-output majorization: Conjecture (ii): coherent-output majorization (hard)
  • §V.A, Eq.(52): general mixed-direction condition: §V.A, Eq.(52): general mixed-direction condition (source-ambiguity)
  • §V.B, Eqs.(55)–(58): necessary pure-state stationarity: §V.B, Eqs.(55)–(58): necessary pure-state stationarity (source-ambiguity)
  • §V.B, Eqs.(59)–(60), (63)–(66): explicit vacuum/coherent F: Actual unbounded coherent entropy eigenoperator and its dual-log domain (hard)
  • §I and §VII: claimed coherent local minimality: §I and §VII: claimed coherent local minimality (source-ambiguity)
  • §VI.B, Eq.(78), Fig.8: 100 random trials: §VI.B, Eq.(78), Fig.8: 100 random trials (source-ambiguity)
  • §VI.C, Fig.9: simulated annealing experiment: §VI.C, Fig.9: simulated annealing experiment (source-ambiguity)

Selected references

  • Minimum output entropy of bosonic channels: a conjecture, arXiv:quant-ph/0404005v1, https://arxiv.org/abs/quant-ph/0404005v1
31 thms2 active usersReviewed
Quantum Information·Captain: Goku

Inequalities for quantum channels assisted by limited resourcesResearch Paper

Motivation

The information capacities and ``distillability'' of a quantum channel are studied in the presence of auxiliary resources. These include prior entanglement shared between the sender and receiver and free classical bits of forward and backward communication. Inequalities and trade-off curves are derived. In particular an alternative proof is given that in the absence of feedback and shared entanglement, forward classical communication does not increase the quantum capacity of a channel.

This mission is the statement-level formalization of Inequalities for quantum channels assisted by limited resources (arXiv:quant-ph/0406111v3). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

6 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is A dephasing side channel cannot increase unassisted quantum capacity (§II B Eq.(16): a dephasing side channel cannot increase quantum capacity, PDF p. 4). The milestones are the other numbered results, in the paper's order, each quoting the paper.

The paper's own objects are the definition item of this mission. Objects shared across papers come from the prove2quantum library and from earlier papers' missions, listed as references.

Provenance: prove2quantum's pipeline drafted each statement (gpt-6.1-sol on Stanford's Sherlock cluster). A blind read-back, written without seeing the paper, is attached to every item. An independent moderator compared each statement against the paper and passed the whole paper without edits.

Deferred results

27 results of the paper are not stated yet, because the library lacks an interface they need:

  • §II Eq.(9): forward classical assistance does not increase unassisted quantum capacity: Evaluated three-resource adaptive channel protocols and their independent operational capacities (hard)
  • §I A Eq.(2): classical capacity and distillability dominate quantum capacity: Evaluated three-resource adaptive channel protocols and their independent operational capacities; gross-output, n/k-regularized distillability (hard)
  • §I A: resource monotonicity: Evaluated three-resource adaptive channel protocols and their independent operational capacities; gross-output, n/k-regularized distillability (hard)
  • §I A and Appendix B Eq.(B1): joint concavity: Evaluated three-resource adaptive channel protocols and their independent operational capacities; gross-output, n/k-regularized distillability (hard)
  • §II Eq.(8): additive contribution of forward classical communication: Evaluated three-resource adaptive channel protocols and their independent operational capacities (hard)
  • §III A Eq.(25): distillability-dependent linear upper bound: A source-specified domain or zero-denominator interpretation for the printed expression. (source-ambiguity)
  • §III A Eq.(27): universal quantum-capacity upper bound: Evaluated three-resource adaptive channel protocols and their independent operational capacities (hard)
  • §III A Eq.(28): forward-classical-resource linear upper bound: A source-specified domain or zero-denominator interpretation for the printed expression. (source-ambiguity)
  • §III A Eq.(29): unlimited-entanglement upper bound: Evaluated three-resource adaptive channel protocols and their independent operational capacities (hard)
  • §III A Eq.(30): teleportation lower bound with surplus entanglement: Evaluated three-resource adaptive channel protocols and their independent operational capacities (hard)
  • §III A Eq.(31): teleportation lower bound with surplus forward communication: Evaluated three-resource adaptive channel protocols and their independent operational capacities (hard)
  • §III A Eq.(32): exact saturation at sufficient entanglement: Evaluated three-resource adaptive channel protocols and their independent operational capacities; attained minimum saturation costs (hard)
  • §III A Eq.(33): concavity interpolation lower bound: Evaluated three-resource adaptive channel protocols and their independent operational capacities; attained minimum saturation costs (hard)
  • §III A Eq.(34): no-feedback teleportation lower bound: Evaluated three-resource adaptive channel protocols and their independent operational capacities (hard)
  • §III A Eq.(35): exact no-feedback capacity with sufficient forward dits: Evaluated three-resource adaptive channel protocols and their independent operational capacities (hard)
  • §III A.1 Eq.(36): unlimited-forward quantum capacity: Evaluated three-resource adaptive channel protocols and their independent operational capacities (hard)
  • §III B Eq.(37): classical entanglement interpolation bound: Evaluated three-resource adaptive channel protocols and their independent operational capacities; attained minimum saturation costs (hard)
  • §III B Eq.(38): distillability-dependent classical upper bound: A source-specified domain or zero-denominator interpretation for the printed expression. (source-ambiguity)
  • §IV Eq.(39): distillability equals quantum capacity with unlimited forward communication: Evaluated three-resource adaptive channel protocols and their independent operational capacities; gross-output, n/k-regularized distillability (hard)
  • §IV Eq.(40): supplied entanglement adds exactly its amount to distillability: Evaluated three-resource adaptive channel protocols and their independent operational capacities; gross-output, n/k-regularized distillability (hard)
  • §IV Eq.(41): forward-only distillability equals unassisted quantum capacity: Evaluated three-resource adaptive channel protocols and their independent operational capacities; gross-output, n/k-regularized distillability (hard)
  • §IV Eq.(42): converse for forward-only distillation: Evaluated three-resource adaptive channel protocols and their independent operational capacities; gross-output, n/k-regularized distillability (hard)
  • §IV: distillability eventually exceeds both communication capacities: Evaluated three-resource adaptive channel protocols and their independent operational capacities; gross-output, n/k-regularized distillability (hard)
  • Appendix C Eqs.(C1)–(C2): equivalence to the Bowen condition: Evaluated three-resource adaptive channel protocols and their independent operational capacities; attained minimum saturation costs (hard)
  • Appendix C Eq.(C3) and following sentence: conditional linear identity: Evaluated three-resource adaptive channel protocols and their independent operational capacities; attained minimum saturation costs (hard)
  • Appendix C Eq.(C4): equivalence to the complete piecewise capacity curve: Evaluated three-resource adaptive channel protocols and their independent operational capacities; attained minimum saturation costs (hard)
  • Appendix C final unnumbered small-entanglement assertion: Unambiguous conjecture scope and a nonvacuous argument for a positive small-entanglement linear interval. (source-ambiguity)

Selected references

  • Inequalities for quantum channels assisted by limited resources, arXiv:quant-ph/0406111v3, https://arxiv.org/abs/quant-ph/0406111v3
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Evaluating Capacities of Bosonic Gaussian ChannelsResearch Paper

Motivation

We show how to compute or at least to estimate various capacity-related quantities for Bosonic Gaussian channels. Among these are the coherent information, the entanglement assisted classical capacity, the one-shot classical capacity, and a new quantity involving the transpose operation, shown to be a general upper bound on the quantum capacity, even allowing for finite errors. All bounds are explicitly evaluated for the case of a one-mode channel with attenuation/amplification and classical noise.

This mission is the statement-level formalization of Evaluating Capacities of Bosonic Gaussian Channels (arXiv:quant-ph/9912067v1). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

24 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is II.B, Eq.(2.9): finite-error transpose capacity bound (II.B, Eq.(2.9): finite-error transpose capacity bound, PDF p. 3). The milestones are the other numbered results, in the paper's order, each quoting the paper.

The paper's own objects are the definition item of this mission. Objects shared across papers come from the prove2quantum library and from earlier papers' missions, listed as references.

Provenance: prove2quantum's pipeline drafted each statement (gpt-6.1-sol on Stanford's Sherlock cluster). A blind read-back, written without seeing the paper, is attached to every item. An independent moderator compared each statement against the paper and passed the whole paper without edits.

Deferred results

22 results of the paper are not stated yet, because the library lacks an interface they need:

  • IV.A, property (A): polynomial action: Mixed-state finite-moment form domains and unbounded CCR polynomial duals (hard)
  • IV.A: infinite unconstrained classical capacity: Operational unrestricted classical coding capacity for arbitrary finite-mode channels (hard)
  • IV.B, Eq.(4.38): covariance and commutator transport: Actual centered mixed-state first/second quadrature form moments (hard)
  • IV.B: canonical completion and complement: Constructed symplectic completion and its canonical unitary with complementary rows (hard)
  • IV.B: asserted Gaussian-environment iff: Source statement lacks a valid pinned theorem under its stated hypotheses (source-ambiguity)
  • IV.C: Gaussian mutual-information maximizer: Mixed-state moment fibers and constructed unique Gaussian representative (hard)
  • IV.C, Eq.(4.41): printed derivative identity: Source statement lacks a valid pinned theorem under its stated hypotheses (source-ambiguity)
  • IV.C: arbitrary moment-constraint attainment: Source statement lacks a valid pinned theorem under its stated hypotheses (source-ambiguity)
  • IV.C: arbitrary quadratic-energy attainment: Source statement lacks a valid pinned theorem under its stated hypotheses (source-ambiguity)
  • IV.C: covariance entropy-exchange formula: General Gaussian purification with reference reflection and covariance spectral calculus (hard)
  • V.A: photon-constrained entanglement-assisted value: All-input photon-energy constrained mutual-information optimization (hard)
  • V.A: coherent Gaussian achieved classical rate: Continuous-ensemble Holevo information and one-shot optimization with photon budget (hard)
  • V.A: printed assisted small-power asymptotic: Source statement lacks a valid pinned theorem under its stated hypotheses (source-ambiguity)
  • V.B, Eq.(5.55): claimed Gaussian coherent optimum: Source statement lacks a valid pinned theorem under its stated hypotheses (source-ambiguity)
  • Appendix A: pure-direction reduction: Source statement lacks a valid pinned theorem under its stated hypotheses (source-ambiguity)
  • Appendix A: nondegenerate pure-range criterion: Source statement lacks a valid pinned theorem under its stated hypotheses (source-ambiguity)
  • Appendix A, Eq.(1.3): constrained minimum sufficient condition: Finite expectations of possibly unbounded selfadjoint constraint operators on a common convex density domain (hard)
  • Appendix B, Eq.(2.1): weighted-L2 unitary dilation: H-valued weighted-L2 unitary and both genuine partial traces (hard)
  • Appendix B: actual complementary kernel: Actual complementary integral operator on L2(muNc) (hard)
  • Appendix B: environmental Weyl representation: Gaussian-weighted translation unitaries on actual L2 equivalence classes (hard)
  • Appendix B: complementary Gaussian characteristic and covariance: Constructed weighted-L2 complementary density and its mixed-state covariance (hard)
  • Appendix B: complementary spectrum and entropy agreement: Actual complementary Gaussian spectrum-to-entropy identification (hard)

Selected references

  • Evaluating Capacities of Bosonic Gaussian Channels, arXiv:quant-ph/9912067v1, https://arxiv.org/abs/quant-ph/9912067v1
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Quantum Information·Captain: Goku

Information capacity formula of quantum optical channelsResearch Paper

Motivation

The applications of the general formulae of channel capacity developed in the quantum information theory to evaluation of information transmission capacity of optical channel are interesting subjects. In this review paper, we will point out that the formulation based on only classical-quantum channel mapping model may be inadequate when one takes into account a power constraint for noisy channel. To define the power constraint well, we should explicitly consider how quantum states are conveyed through a transmission channel. Basing on such consideration, we calculate a capacity formula for an attenuated noisy optical channel with genreral Gaussian state input; this gives certain progress beyond the example in our former paper.

This mission is the statement-level formalization of Information capacity formula of quantum optical channels (arXiv:quant-ph/0105042v1). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

7 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Lossless number-state entropy maximum and capacity (Eqs.(58)-(59), PDF p. 15). The milestones are the other numbered results, in the paper's order, each quoting the paper.

The paper's own objects are the definition item of this mission. Objects shared across papers come from the prove2quantum library and from earlier papers' missions, listed as references.

Provenance: prove2quantum's pipeline drafted each statement (gpt-6.1-sol on Stanford's Sherlock cluster). A blind read-back, written without seeing the paper, is attached to every item. An independent moderator compared each statement against the paper and passed the whole paper without edits.

Deferred results

9 results of the paper are not stated yet, because the library lacks an interface they need:

  • Main result: transmitter-constrained squeezed-state optical capacity, original (53) and (56): A constructed fixed pure squeezed seed and its noisy attenuated displacement alphabet, with measurable modulation mixtures, raw transmitter photon accounting, and operational product-code capacity linked to both Gaussian covariance branches. (hard)
  • Physical Gaussian reduction and attained covariance maximum, (47)–(49): The paper-specific measurable displaced-Gaussian family and raw-moment/covariance interface connecting arbitrary modulation laws to the attained output-covariance optimization in (48)-(49). (hard)
  • Coherent-state specialization of the attenuated noisy capacity, (54): The constructed displaced thermal output family for coherent transmission through attenuation plus classical noise, and its transmitter-constrained operational classical coding capacity. (hard)
  • Squeezing penalty within regime [A]: Physical fixed-seed capacities for the squeezed and coherent displacement alphabets with a common transmitter budget and the regime-(50) comparison. (hard)
  • Photon-loss Holevo bounds in high/low photon regimes, (64)–(65): A quantitatively specified source assertion: Photon-loss Holevo bounds in high/low photon regimes, (64)–(65) (source-ambiguity)
  • Approximate optimum binary single-symbol prior and amplitudes, (79)–(80): A quantitatively specified source assertion: Approximate optimum binary single-symbol prior and amplitudes, (79)–(80) (source-ambiguity)
  • Single-symbol versus collective weak-energy comparison, (81): A quantitatively specified source assertion: Single-symbol versus collective weak-energy comparison, (81) (source-ambiguity)
  • Three equal-angle qubit letters: numerical one-use capacity claim: A quantitatively specified source assertion: Three equal-angle qubit letters: numerical one-use capacity claim (source-ambiguity)
  • Claim that no discrete channel simulates the classical continuous channel: A quantitatively specified source assertion: Claim that no discrete channel simulates the classical continuous channel (source-ambiguity)

Selected references

  • Information capacity formula of quantum optical channels, arXiv:quant-ph/0105042v1, https://arxiv.org/abs/quant-ph/0105042v1
11 thms2 active usersReviewed
Quantum Information·Captain: Goku

Composable Security in the Bounded-Quantum-Storage ModelResearch Paper

Motivation

We present a simplified framework for proving sequential composability in the quantum setting. In particular, we give a new, simulation-based, definition for security in the bounded-quantum-storage model, and show that this definition allows for sequential composition of protocols. Damgard et al. (FOCS '05, CRYPTO '07) showed how to securely implement bit commitment and oblivious transfer in the bounded-quantum-storage model, where the adversary is only allowed to store a limited number of qubits. However, their security definitions did only apply to the standalone setting, and it was not clear if their protocols could be composed. Indeed, we first give a simple attack that shows that these protocols are not composable without a small refinement of the model. Finally, we prove the security of their randomized oblivious transfer protocol in our refined model. Secure implementations of oblivious transfer and bit commitment then follow easily by a (classical) reduction to randomized oblivious transfer.

This mission is the statement-level formalization of Composable Security in the Bounded-Quantum-Storage Model (arXiv:0709.0492v1). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

3 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Measured BB84 uncertainty with explicit smoothing and positivity (Lemma 2.3, PDF p. 6). The milestones are the other numbered results, in the paper's order, each quoting the paper.

The paper's own objects are the definition item of this mission. Objects shared across papers come from the prove2quantum library and from earlier papers' missions, listed as references.

Provenance: prove2quantum's pipeline drafted each statement (gpt-6.1-sol on Stanford's Sherlock cluster). A blind read-back, written without seeing the paper, is attached to every item. An independent moderator compared each statement against the paper and passed the whole paper without edits.

Deferred results

14 results of the paper are not stated yet, because the library lacks an interface they need:

  • Theorem 4.7; precise refinement of the abstract paper result: Concrete BQS-OT hybrid executions and Definition 3.1 security (hard)
  • Theorem 3.2: sequential composition (memory labels corrected using proof): Single-call sequential substitution on corruption-indexed memory-bounded programs (hard)
  • §3, unnumbered: multi-phase security and composition: History-compatible phase-wise simulation with persistent ideal and classical simulator memory (hard)
  • Lemma 4.2: sender security of BQS-OT: Exact malicious-sender execution and ROT sender-corruption simulator (hard)
  • Lemma 4.4: BQS-OT receiver security, no quantum auxiliary input: Receiver simulation with classical auxiliary input and no quantum auxiliary input (hard)
  • Lemma 4.5: BQS-OT receiver security, a normalized pure quantum input of at most β qubits, unknown to the simulator: Uniform receiver simulator for an unknown pure auxiliary state and a two-cut memory profile (hard)
  • Lemma 4.6: BQS-OT receiver security, an arbitrary mixed quantum input of at most β qubits, possibly entangled with the unbounded environment: Reference-preserving receiver execution for arbitrary entangled mixed auxiliary inputs (hard)
  • Theorem B.2: classical OT from randomized OT: Concrete OTfromROT execution with bidirectional typed communication and full security (hard)
  • Theorem C.2: bit commitment from reversed randomized OT: Two-phase OTtoBC execution and one consistent commit/open simulator (hard)
  • Theorem C.3: bounded-storage bit commitment: Role reversal and composition of concrete BQS-TO and two-phase commitment (hard)
  • §1.1, unnumbered: EPR attack on the old one-wait model: Executable old-model teleportation attack with a memory cut and reference recovery (hard)
  • §1.1, unnumbered: precomputed ROT and classical later use: Classical storage and delayed independent use of an oriented ROT sample (hard)
  • §1.1, unnumbered: secure function evaluation from classical UC protocols: Specified SFE functionality/protocol class and a lifting theorem for this bounded-memory model (source-ambiguity)
  • §4.1, unnumbered: role-reversed parallel reflection attack: A choice-labelled parallel distinguishing experiment and its ideal scheduling (source-ambiguity)

Selected references

  • Composable Security in the Bounded-Quantum-Storage Model, arXiv:0709.0492v1, https://arxiv.org/abs/0709.0492v1
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Computable bounds for the discrimination of Gaussian statesResearch Paper

Motivation

By combining the Minkowski inequality and the quantum Chernoff bound, we derive easy-to-compute upper bounds for the error probability affecting the optimal discrimination of Gaussian states. In particular, these bounds are useful when the Gaussian states are unitarily inequivalent, i.e., they differ in their symplectic invariants.

This mission is the statement-level formalization of Computable bounds for the discrimination of Gaussian states (arXiv:0806.1625v2). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

6 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Minkowski spectral bound for Gaussian-state discrimination (Theorem 4, Eqs. (60)–(62), PDF p. 5). The milestones are the other numbered results, in the paper's order, each quoting the paper.

The paper's own objects are the definition item of this mission. Objects shared across papers come from the prove2quantum library and from earlier papers' missions, listed as references.

Provenance: prove2quantum's pipeline drafted each statement (gpt-6.1-sol on Stanford's Sherlock cluster). A blind read-back, written without seeing the paper, is attached to every item. An independent moderator compared each statement against the paper and passed the whole paper without edits.

Selected references

  • Computable bounds for the discrimination of Gaussian states, arXiv:0806.1625v2, https://arxiv.org/abs/0806.1625v2
12 thms2 active usersReviewed
Quantum Information·Captain: Goku

Optimal cloning of unitary transformationsResearch Paper

Motivation

After proving a general no-cloning theorem for black boxes, we derive the optimal universal cloning of unitary transformations, from one to two copies. The optimal cloner is realized by quantum channels with memory, and greately outperforms the optimal measure-and-reprepare cloning strategy. Applications are outlined, including two-way quantum cryptographic protocols.

This mission is the statement-level formalization of Optimal cloning of unitary transformations (arXiv:0804.0129v2). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

10 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Optimal universal one-to-two unitary cloning, with attaining channels (Theorem 1; Eqs. (8)–(10), PDF p. 3). The milestones are the other numbered results, in the paper's order, each quoting the paper.

The paper's own objects are the definition item of this mission. Objects shared across papers come from the prove2quantum library and from earlier papers' missions, listed as references.

Provenance: prove2quantum's pipeline drafted each statement (gpt-6.1-sol on Stanford's Sherlock cluster). A blind read-back, written without seeing the paper, is attached to every item. An independent moderator compared each statement against the paper and passed the whole paper without edits.

Deferred results

1 results of the paper are not stated yet, because the library lacks an interface they need:

  • Paragraph following Theorem 1, controlled-swap realization: Consistent controlled-swap Stinespring realization of Eq. (8) in the stated +/- memory basis (source-ambiguity)

Selected references

  • Optimal cloning of unitary transformations, arXiv:0804.0129v2, https://arxiv.org/abs/0804.0129v2
17 thms2 active usersReviewed
Quantum Information·Captain: Goku

On Differentiable Vectors for Representations of Infinite Dimensional Lie GroupsResearch Paper

Motivation

In this paper we develop two types of tools to deal with differentiability properties of vectors in continuous representations π G→\GL(V)\pi \: G \to \GL(V)πG→\GL(V) of an infinite dimensional Lie group GGG on a locally convex space VVV. The first class of results concerns the space V∞V^\inftyV∞ of smooth vectors. If GGG is a Banach--Lie group, we define a topology on the space V∞V^\inftyV∞ of smooth vectors for which the action of GGG on this space is smooth. If VVV is a Banach space, then V∞V^\inftyV∞ is a Fr'echet space. This applies in particular to C∗C^*C∗-dynamical systems (\cA,G,α)(\cA,G, \alpha)(\cA,G,α), where GGG is a Banach--Lie group. For unitary representations we show that a vector vvv is smooth if the corresponding positive definite function \laπ(g)v,v\ra\la \pi(g)v,v\ra\laπ(g)v,v\ra is smooth. The second class of results concerns criteria for CkC^kCk-vectors in terms of operators of the derived representation for a Banach--Lie group GGG acting on a Banach space VVV. In particular, we provide for each k∈Nk \in \Nk∈N examples of continuous unitary representations for which the space of Ck+1C^{k+1}Ck+1-vectors is trivial and the space of CkC^kCk-vectors is dense.

This mission is the statement-level formalization of On Differentiable Vectors for Representations of Infinite Dimensional Lie Groups (arXiv:1002.1602v3). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

10 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Hilbert-valued smoothness and the inner-product kernel (Theorem 7.1, PDF p. 21). The milestones are the other numbered results, in the paper's order, each quoting the paper.

The paper's own objects are the definition item of this mission. Objects shared across papers come from the prove2quantum library and from earlier papers' missions, listed as references.

Provenance: prove2quantum's pipeline drafted each statement (gpt-6.1-sol on Stanford's Sherlock cluster). A blind read-back, written without seeing the paper, is attached to every item. An independent moderator compared each statement against the paper and passed the whole paper without edits.

Deferred results

42 results of the paper are not stated yet, because the library lacks an interface they need:

  • Lemma 3.3: Finite-order directional manifold calculus, tangent vectors, smooth exponential, and generator domains (hard)
  • Lemma 3.4: Finite-order Ck orbit vectors and iterated partial-generator domains (hard)
  • Lemma 4.2: The Definition 4.1 smooth-vector space, topology and derived action (hard)
  • Lemma 4.3: Smooth-vector seminorms and the actual differential of conjugation (hard)
  • Theorem 4.4: The smooth-vector topology and Bastiani-smooth action into it (hard)
  • Corollary 4.5: The induced smooth-vector space and its Definition 4.1 topology (hard)
  • Proposition 4.6: Smooth compact-open topology and the orbit-map embedding (hard)
  • Lemma 4.10: Distribution-vector dual and smooth-function intertwiner spaces (hard)
  • Proposition 5.4: Canonical smooth-vector locally convex uniform structure (hard)
  • Theorem 6.2: Smooth C-star subalgebra with its derivative topology and unit group (hard)
  • Theorem 7.2: Locally convex Lie-group smooth maps and local smooth matrix coefficients (hard)
  • Corollary 7.3: Smooth orbit vectors and their density for a cyclic unitary representation (hard)
  • Corollary 7.4: Locally convex Lie groups and local scalar smoothness for semidefinite functions (hard)
  • Theorem 8.2: Smooth exponential and generator-domain derivative map (hard)
  • Lemma 8.4: Frechet-Lie exponential curves and a derivative-defined common domain (hard)
  • Theorem 8.5: C1 orbit vectors in Bastiani calculus and the common generator domain (hard)
  • Lemma 9.2: The canonical first graph norm on the generator domain (hard)
  • Lemma 9.3: Iterated generator domains and ordered derived multilinear maps (hard)
  • Theorem 9.4: The exact higher graph norms and successive derived-action spaces (hard)
  • Proposition 9.7: Graph-norm representations, operator-norm derivative maps and Frechet-Ck orbit vectors (hard)
  • Lemma 10.2: The a.e. phase-multiplication representation on L2 (hard)
  • Lemma 10.3: A.e. Lp phase generators and canonical inclusions in L2 (hard)
  • Proposition 10.4: Iterated phase-generator domains and common Lp embeddings (hard)
  • Theorem 11.3: The prescribed countable finite-dimensional direct-limit Lie structure (hard)
  • Theorem 12.4: A pro-Lie realization with compatible smooth projection quotients (hard)
  • Remark 3.2: Generator domains and the fundamental-theorem integral in an incomplete locally convex space (hard)
  • Remark 4.7a: Smooth compact-open Frechet structure and smooth-vector topology (hard)
  • Example 4.8: Product-sequence phase representation and universal locally convex topology quantification (hard)
  • Example 4.9: Affine-function representation and compact/bounded convergence dual topologies (hard)
  • Application 4.10-homogeneous: Smooth homogeneous quotient and distribution-vector parametrization (hard)
  • Footnote 7.1-finite: An unambiguous finite-order regularity hypothesis near the diagonal (source-ambiguity)
  • Remark 8.3: One-parameter generator domains for an isometric Banach representation (hard)
  • Remark 9.5: Higher graph domains, derivatives and the sum norm on the product (hard)
  • Remark 9.6: The projective derivative topology on the infinite common domain (hard)
  • Remark 9.8: Finite-dimensional graph-domain action and the concrete p=2 counterexample (hard)
  • Example 9.9: The Lp phase action on its first graph-norm domain (hard)
  • Example 9.10: Periodic sup-norm representation and its generator domains (hard)
  • Remark 10.5: The concrete p=2n phase representation and its Cn domains (hard)
  • Remark 10.6: Exact phase graph norms and natural Lq norm comparison (hard)
  • Remark 10.7: Frechet-C1 orbit regularity and continuity in the p=2 graph norm (hard)
  • Remark 12.5: The smooth projective-limit realization of R^N and its phase action (hard)
  • Remark 12.6: Seminorm-kernel quotients with their induced norms and factored representations (hard)

Selected references

  • On Differentiable Vectors for Representations of Infinite Dimensional Lie Groups, arXiv:1002.1602v3, https://arxiv.org/abs/1002.1602v3
11 thms2 active usersReviewed
🏆Completed
Quantum Information·Captain: Goku

Integrating representations of Banach--Lie algebrasResearch Paper

Motivation

We give two integrability criteria for representations of Banach--Lie algebras as skew-symmetric unbounded operators on a dense domain of a Hilbert space.

This mission is the statement-level formalization of Integrating representations of Banach--Lie algebras (arXiv:1003.0999v3). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

7 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Product rule for a strongly continuous operator path (Lemma 4, PDF p. 3). The milestones are the other numbered results, in the paper's order, each quoting the paper.

The paper's own objects are the definition item of this mission. Objects shared across papers come from the prove2quantum library and from earlier papers' missions, listed as references.

Provenance: prove2quantum's pipeline drafted each statement (gpt-6.1-sol on Stanford's Sherlock cluster). A blind read-back, written without seeing the paper, is attached to every item. An independent moderator compared each statement against the paper and passed the whole paper without edits.

Deferred results

8 results of the paper are not stated yet, because the library lacks an interface they need:

  • Theorem 1: Actual tangent Banach--Lie algebra identification for the given simply connected G, its exponential curves, smooth orbit maps on the SAME H, and the predicate D subset H-infinity with derived action exactly alpha on D. (hard)
  • Corollary 2: Actual tangent Banach--Lie algebra identification for the given simply connected G, its exponential curves, smooth orbit maps on the SAME H, and the predicate D subset H-infinity with derived action exactly alpha on D. (hard)
  • Corollary 3: Actual tangent Banach--Lie algebra identification for the given simply connected G, its exponential curves, smooth orbit maps on the SAME H, and the predicate D subset H-infinity with derived action exactly alpha on D. (hard)
  • Corollary 8 and equation (3): Canonical intersection of FULL finite-composition domains of the closed operators, and alpha-prime computed from the unique ordered decomposition. (hard)
  • Lemma 11: The actual locally convergent Dynkin BCH product on a symmetric starlike zero-neighbourhood, its chart-domain guards, and delta defined from the inverse differential of the actual right translation. (hard)
  • Lemma 12: The actual locally convergent Dynkin BCH product on a symmetric starlike zero-neighbourhood, its chart-domain guards, and delta defined from the inverse differential of the actual right translation. (hard)
  • Lemma 13: The actual locally convergent Dynkin BCH product on a symmetric starlike zero-neighbourhood, its chart-domain guards, and delta defined from the inverse differential of the actual right translation. (hard)
  • Proposition 14: The actual locally convergent Dynkin BCH product on a symmetric starlike zero-neighbourhood, its chart-domain guards, and delta defined from the inverse differential of the actual right translation. Also the ordered local diffeomorphism F and its computed inverse components x_j(t). (hard)

Selected references

  • Integrating representations of Banach--Lie algebras, arXiv:1003.0999v3, https://arxiv.org/abs/1003.0999v3
8 thms2 active usersReviewed
Quantum Information·Captain: Goku

Information - Disturbance Tradeoff in the Estimation of a Unitary TransformationResearch Paper

Motivation

We address the problem of the information-disturbance trade-off associated to the estimation of a quantum transformation, and show how the extraction of information about the a black box causes a perturbation of the corresponding input-output evolution. In the case of a black box performing a unitary transformation, randomly distributed according to the invariant measure, we give a complete solution of the problem, deriving the optimal trade-off curve and presenting an explicit construction of the optimal quantum network.

This mission is the statement-level formalization of Information - Disturbance Tradeoff in the Estimation of a Unitary Transformation (arXiv:1006.5665v2). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

6 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Attained optimal information–disturbance frontier (§IV C, Eqs.(30)–(34); abstract on PDF p.1, PDF p. 7). The milestones are the other numbered results, in the paper's order, each quoting the paper.

The paper's own objects are the definition item of this mission. Objects shared across papers come from the prove2quantum library and from earlier papers' missions, listed as references.

Provenance: prove2quantum's pipeline drafted each statement (gpt-6.1-sol on Stanford's Sherlock cluster). A blind read-back, written without seeing the paper, is attached to every item. An independent moderator compared each statement against the paper and passed the whole paper without edits.

Selected references

  • Information - Disturbance Tradeoff in the Estimation of a Unitary Transformation, arXiv:1006.5665v2, https://arxiv.org/abs/1006.5665v2
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Cloning of a quantum measurementResearch Paper

Motivation

We analyze quantum algorithms for cloning of a quantum measurement. Our aim is to mimic two uses of a device performing an unknown von Neumann measurement with a single use of the device. When the unknown device has to be used before the bipartite state to be measured is available we talk about 1 -> 2 learning of the measurement, otherwise the task is called 1 -> 2 cloning of a measurement. We perform the optimization for both learning and cloning for arbitrary dimension of the Hilbert space. For 1 -> 2 cloning we also propose a simple quantum network that realizes the optimal strategy.

This mission is the statement-level formalization of Cloning of a quantum measurement (arXiv:1103.5709v2). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

16 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Optimal one-to-two measurement cloning fidelity (§V, Eq.(61): optimal one-to-two cloning fidelity (seed announced in abstract), PDF p. 7). The milestones are the other numbered results, in the paper's order, each quoting the paper.

The paper's own objects are the definition item of this mission. Objects shared across papers come from the prove2quantum library and from earlier papers' missions, listed as references.

Provenance: prove2quantum's pipeline drafted each statement (gpt-6.1-sol on Stanford's Sherlock cluster). A blind read-back, written without seeing the paper, is attached to every item. An independent moderator compared each statement against the paper and passed the whole paper without edits.

Deferred results

3 results of the paper are not stated yet, because the library lacks an interface they need:

  • §IV, Eq.(48): explicit numerical block score coefficients: Numerical Schur score coefficients in Eq.(48) (source-ambiguity)
  • §V, Eqs.(62),(63), p.8 replica formula: printed optimal cloners: Operational optimality of the two printed Eq.(62) block arrays (source-ambiguity)
  • §VI final paragraph and author note [17]: estimate-and-prepare comparison: An operationally specified optimal-estimation-and-prepare strategy (source-ambiguity)

Selected references

  • Cloning of a quantum measurement, arXiv:1103.5709v2, https://arxiv.org/abs/1103.5709v2
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The Schmidt number and partially entanglement breaking channels in infinite dimensionsResearch Paper

Motivation

A definition of the Schmidt number of a state of an infinite dimensional bipartite quantum system is given and properties of the corresponding family of Schmidt classes are considered. The existence of states with a given Schmidt number such that any their countable convex decomposition does not contain pure states with finite Schmidt rank is established. Partially entanglement breaking channels in infinite dimensions are studied. Several properties of these channels well known in finite dimensions are generalized to the infinite dimensional case. At the same time, the existence of partially entanglement breaking channels (in particular, entanglement breaking channels) such that all operators in any their Kraus representations have infinite rank is proved.

This mission is the statement-level formalization of The Schmidt number and partially entanglement breaking channels in infinite dimensions (arXiv:1110.4363v3). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

20 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Proposition 9B: exact k-PEB channels with only infinite-rank nonzero Kraus operators (Proposition 9B: exact k-PEB channels with only infinite-rank nonzero Kraus operators, PDF p. 12). The milestones are the other numbered results, in the paper's order, each quoting the paper.

The paper's own objects are the definition item of this mission. Objects shared across papers come from the prove2quantum library and from earlier papers' missions, listed as references.

Provenance: prove2quantum's pipeline drafted each statement (gpt-6.1-sol on Stanford's Sherlock cluster). A blind read-back, written without seeing the paper, is attached to every item. An independent moderator compared each statement against the paper and passed the whole paper without edits.

Deferred results

1 results of the paper are not stated yet, because the library lacks an interface they need:

  • Proposition 2: Source-pinned infinite-dimensional LOCC class, specifying deterministic versus selected outputs, measurable outcome instruments, round limits and topology. (source-ambiguity)

Selected references

  • The Schmidt number and partially entanglement breaking channels in infinite dimensions, arXiv:1110.4363v3, https://arxiv.org/abs/1110.4363v3
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Quantum Information·Captain: Goku

Quantum Hypothesis Testing and Non-Equilibrium Statistical MechanicsResearch Paper

Motivation

We extend the mathematical theory of quantum hypothesis testing to the general W∗W^*W∗-algebraic setting and explore its relation with recent developments in non-equilibrium quantum statistical mechanics. In particular, we relate the large deviation principle for the full counting statistics of entropy flow to quantum hypothesis testing of the arrow of time.

This mission is the statement-level formalization of Quantum Hypothesis Testing and Non-Equilibrium Statistical Mechanics (arXiv:1109.3804v2). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

17 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Proposition 1.1 (Proposition 1.1, PDF p. 4). The milestones are the other numbered results, in the paper's order, each quoting the paper.

The paper's own objects are the definition item of this mission. Objects shared across papers come from the prove2quantum library and from earlier papers' missions, listed as references.

Provenance: prove2quantum's pipeline drafted each statement (gpt-6.1-sol on Stanford's Sherlock cluster). A blind read-back, written without seeing the paper, is attached to every item. An independent moderator compared each statement against the paper and passed the whole paper without edits.

Deferred results

40 results of the paper are not stated yet, because the library lacks an interface they need:

  • Theorem 3.7: Translation-covariant lattice interactions and canonical tensor inclusions (hard)
  • Theorem 3.8: Translation-covariant lattice interactions and canonical tensor inclusions (hard)
  • Theorem 3.9: Actual CAR quasi-free states, compressions and Fourier symbols (hard)
  • Theorem 4.2: Two-index testing exponents with genuine iterated limits (hard)
  • Theorem 5.1: Genuine W*-standard form and normal positive predual (hard)
  • Proposition 5.2: Unbounded relative Tomita/modular operators and spectral calculus (hard)
  • Proposition 5.3: Extended Araki entropy on normal positive W*-functionals (hard)
  • Proposition 5.4: Source-corrected scope/formula for Proposition 5.4 (source-ambiguity)
  • Proposition 5.5: Unbounded relative Tomita/modular operators and spectral calculus (hard)
  • Lemma 5.6: Unbounded relative Tomita/modular operators and spectral calculus (hard)
  • Lemma 5.7: Unbounded relative Tomita/modular operators and spectral calculus (hard)
  • Theorem 6.1: Unbounded relative Tomita/modular operators and spectral calculus (hard)
  • Proposition 6.2: W*-projection/effect testing and general-index exponent construction (hard)
  • Proposition 6.3: W*-projection/effect testing and general-index exponent construction (hard)
  • Proposition 6.4: Extended Araki entropy on normal positive W*-functionals (hard)
  • Theorem 6.5: W*-projection/effect testing and general-index exponent construction (hard)
  • Theorem 6.6: W*-projection/effect testing and general-index exponent construction (hard)
  • Proposition 6.7: Reversed modular characteristic functions and W*-Stein families (hard)
  • Theorem 6.8: Reversed modular characteristic functions and W*-Stein families (hard)
  • Proposition 7.1: W*-dynamics, relative Hamiltonians and normal-state FCS (hard)
  • Theorem 7.2: quantum hypothesis testing of the arrow of time: W*-dynamics, relative Hamiltonians and normal-state FCS (hard)
  • Theorem 8.1: Spin--fermion model with SF1--SF3 and finite approximants (hard)
  • Theorem 8.2: EBB CAR dynamics, wave operators and on-shell scattering matrix (hard)
  • Theorem 8.3: Source-corrected scope/formula for Theorem 8.3 (source-ambiguity)
  • Generalized tests have the same testing results: W*-projection/effect testing and general-index exponent construction (hard)
  • Section 3.4.1: quantum i.i.d. reduction: Source-corrected scope/formula for Section 3.4.1: quantum i.i.d. reduction (source-ambiguity)
  • Pressure and its convexity: Translation-covariant lattice interactions and canonical tensor inclusions (hard)
  • Open-system multi-parameter FCS: Open-system tensor embeddings and joint spectral FCS (hard)
  • TD FCS local large deviation principle: Source-corrected scope/formula for TD FCS local large deviation principle (source-ambiguity)
  • TD analytic cumulants and central limit theorem: Source-corrected scope/formula for TD analytic cumulants and central limit theorem (source-ambiguity)
  • Scaled spectral lower bounds (6.5)–(6.6): Unbounded relative Tomita/modular operators and spectral calculus (hard)
  • Sufficient analytic moment condition for Stein: Reversed modular characteristic functions and W*-Stein families (hard)
  • W*-open-system entropy production currents: W*-dynamics, relative Hamiltonians and normal-state FCS (hard)
  • W*-FCS transient Evans–Searles symmetry: W*-dynamics, relative Hamiltonians and normal-state FCS (hard)
  • W*-FCS long-time law and local deviations: Source-corrected scope/formula for W*-FCS long-time law and local deviations (source-ambiguity)
  • Finite approximation yields physical FCS: W*-dynamics, relative Hamiltonians and normal-state FCS (hard)
  • Explicit arrow-of-time concentration after Theorem 7.2: Source-corrected scope/formula for Explicit arrow-of-time concentration after Theorem 7.2 (source-ambiguity)
  • Attainment interpretation of the Hoeffding bound: Source-corrected scope/formula for Attainment interpretation of the Hoeffding bound (source-ambiguity)
  • Landauer–Buttiker energy and charge current limits (8.4): EBB CAR dynamics, wave operators and on-shell scattering matrix (hard)
  • Theorem 8.3(1) independently valid thermodynamic conclusion: XY-chain finite-volume Hamiltonian, product Gibbs preparation and FCS cumulants (hard)

Selected references

  • Quantum Hypothesis Testing and Non-Equilibrium Statistical Mechanics, arXiv:1109.3804v2, https://arxiv.org/abs/1109.3804v2
21 thms2 active usersReviewed
Quantum Information·Captain: Goku

Quantum learning algorithms for quantum measurementsResearch Paper

Motivation

We study quantum learning algorithms for quantum measurements. The optimal learning algorithm is derived for arbitrary von Neumann measurements in the case of training with one or two examples. The analysis of the case of three examples reveals that, differently from the learning of unitary gates, the optimal algorithm for learning of quantum measurements cannot be parallelized, and requires quantum memories for the storage of information.

This mission is the statement-level formalization of Quantum learning algorithms for quantum measurements (arXiv:1103.0480v2). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

14 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Three-example qubit learning requires adaptation (Abstract; §V.C and Remark 1: optimal three-example qubit learning requires adaptation, PDF p. 1). The milestones are the other numbered results, in the paper's order, each quoting the paper.

The paper's own objects are the definition item of this mission. Objects shared across papers come from the prove2quantum library and from earlier papers' missions, listed as references.

Provenance: prove2quantum's pipeline drafted each statement (gpt-6.1-sol on Stanford's Sherlock cluster). A blind read-back, written without seeing the paper, is attached to every item. An independent moderator compared each statement against the paper and passed the whole paper without edits.

Deferred results

7 results of the paper are not stated yet, because the library lacks an interface they need:

  • Lemma 5 / Eq.(48), printed unrestricted random-mixture range: Lemma 5 / Eq.(48), printed unrestricted random-mixture range (source-ambiguity)
  • §V.A: strict inferiority of estimating then preparing the estimated measurement: An unrestricted one-use estimate-and-replay-projective-measurement domain with its measurable joint outcome law and actual replica contraction. (hard)
  • Eqs.(82),(A14): printed final two-use scalar formula: Eqs.(82),(A14): printed final two-use scalar formula (source-ambiguity)
  • §V.C: approximate optimal three-use qubit score: §V.C: approximate optimal three-use qubit score (source-ambiguity)
  • §VI: general statement that examples after the second must be sequential: §VI: general statement that examples after the second must be sequential (source-ambiguity)
  • Abstract / §I: requirement of coherent quantum memory: Abstract / §I: requirement of coherent quantum memory (source-ambiguity)
  • §VI: optimal learners for different N do not share initial steps: §VI: optimal learners for different N do not share initial steps (source-ambiguity)

Selected references

  • Quantum learning algorithms for quantum measurements, arXiv:1103.0480v2, https://arxiv.org/abs/1103.0480v2
18 thms2 active usersReviewed
🏆Completed
Quantum Information·Captain: Goku

A generalization of the Entropy Power Inequality to Bosonic Quantum SystemsResearch Paper

Motivation

In most communication schemes information is transmitted via travelling modes of electromagnetic radiation. These modes are unavoidably subject to environmental noise along any physical transmission medium and the quality of the communication channel strongly depends on the minimum noise achievable at the output. For classical signals such noise can be rigorously quantified in terms of the associated Shannon entropy and it is subject to a fundamental lower bound called entropy power inequality. Electromagnetic fields are however quantum mechanical systems and then, especially in low intensity signals, the quantum nature of the information carrier cannot be neglected and many important results derived within classical information theory require non-trivial extensions to the quantum regime. Here we prove one possible generalization of the Entropy Power Inequality to quantum bosonic systems. The impact of this inequality in quantum information theory is potentially large and some relevant implications are considered in this work.

This mission is the statement-level formalization of A generalization of the Entropy Power Inequality to Bosonic Quantum Systems (arXiv:1402.0404v2). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

4 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Three scalar thermal-entropy asymptotics (§IV.B Eq. (86); §VI.B Eqs. (103), (104), PDF p. 17). The milestones are the other numbered results, in the paper's order, each quoting the paper.

The paper's own objects are the definition item of this mission. Objects shared across papers come from the prove2quantum library and from earlier papers' missions, listed as references.

Provenance: prove2quantum's pipeline drafted each statement (gpt-6.1-sol on Stanford's Sherlock cluster). A blind read-back, written without seeing the paper, is attached to every item. An independent moderator compared each statement against the paper and passed the whole paper without edits.

Deferred results

15 results of the paper are not stated yet, because the library lacks an interface they need:

  • §II Eqs. (3)–(5): Concrete arbitrary-n two-input beam-splitter output on full Fock coefficient densities; extended coefficient entropy is already available. (hard)
  • §II Eqs. (6), (7): Full two-input n-mode squeezing channel on general density operators, including phase conjugation. (hard)
  • §II observation following Eq. (5): n-mode Gaussian predicate and finite covariance on the same full-density mixing model. (hard)
  • §II.A Eq. (9): Summed divergence-based displacement Fisher information with genuine derivative/extended-limit semantics. (hard)
  • §II.A Eqs. (12), (13); §IV.A (38), (83); §VI.A (97): Weighted total divergence-based Fisher information on the physical beam-splitter and amplifier outputs. (hard)
  • §II.B Eq. (19), proof §IV.B p.17: An unrestricted every-state entropy asymptotic, without adding a finite-covariance domain. (source-ambiguity)
  • §II.B Eq. (22); §IV.A.1 Eq. (53), p.13: Full additive Gaussian noise map and both full-density mixing channels, characterized beyond moments. (hard)
  • §II.C Eq. (33); §VI.A Eq. (90), p.22: Full squeezing output and its extended total n-mode entropy. (hard)
  • §II.C Eq. (35); §VI.B Eqs. (101), (111), (112): Entropy photon number of the actual arbitrary-input beam-splitter output with infinite entropy allowed. (hard)
  • §II.D observation and Fig. 2, p.11: An exact numerical bound and a specified decay domain for the plotted thermal-candidate gap. (source-ambiguity)
  • §IV.A.2 Eqs. (64), (68), (69): n-mode quadrature displacement orbits and their actual relative-entropy second derivatives. (hard)
  • §IV.A.3 Eqs. (70), (71), completed p.16: Full-density mixing and multimode Weyl displacements with the amplifier B-direction time reversal. (hard)
  • §IV.A.3 Eqs. (81), (82), completed p.17: Directional, rather than merely summed, divergence-Fisher information for both physical output families. (hard)
  • §IV.B Eqs. (85), (87): Finite quadrature moment/covariance interface and normalized heat-channel output in the accepted spectral state model. (hard)
  • §IV.C Eq. (89), Fig. 3 p.19: Independent ordinary classical broadcast code region with full Fock block inputs and an unconditional per-use mean photon constraint. (hard)

Selected references

  • A generalization of the Entropy Power Inequality to Bosonic Quantum Systems, arXiv:1402.0404v2, https://arxiv.org/abs/1402.0404v2
8 thms2 active usersReviewed
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The Functional Calculus Approach to the Spectral TheoremResearch Paper

Motivation

A consistent functional calculus approach to the spectral theorem for strongly commuting normal operators on Hilbert spaces is presented. In contrast to the common approaches using projection-valued measures or multiplication operators, here the functional calculus is not treated as a subordinate but as the central concept. Based on five simple axioms for a "measurable functional calculus", the theory of such calculi is developed in detail, including spectral theory, uniqueness results and construction principles. Finally, the functional calculus form of the spectral theorem is stated and proved, with some proof variants being discussed.

This mission is the statement-level formalization of The Functional Calculus Approach to the Spectral Theorem (arXiv:2003.06130v2). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

49 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Theorem 7.6 (Spectral Theorem: General Case) (Theorem 7.6 (Spectral Theorem: General Case), PDF p. 35). The milestones are the other numbered results, in the paper's order, each quoting the paper.

The paper's own objects are the definition item of this mission. Objects shared across papers come from the prove2quantum library and from earlier papers' missions, listed as references.

Provenance: prove2quantum's pipeline drafted each statement (gpt-6.1-sol on Stanford's Sherlock cluster). A blind read-back, written without seeing the paper, is attached to every item. An independent moderator compared each statement against the paper and passed the whole paper without edits.

Deferred results

2 results of the paper are not stated yet, because the library lacks an interface they need:

  • Example 6.2: Concrete subsequence-tail characters on l-infinity, their bounded diagonal representation on l2 of all increasing subsequences, and the common-kernel anchor-set predicate. (hard)
  • Remark 6.8: arbitrary Borel product analogue: Exact hypotheses and regularity predicate for an arbitrary product of Borel calculi. (source-ambiguity)

Selected references

  • The Functional Calculus Approach to the Spectral Theorem, arXiv:2003.06130v2, https://arxiv.org/abs/2003.06130v2
50 thms2 active usersReviewed
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Quantum Information·Captain: Goku

Metaplectic formulation of the Wigner transform and applicationsResearch Paper

Motivation

We show that the cross Wigner function can be written in the form W(ψ,ϕ)=S^(ψ⊗ϕ^‾)W(\psi, \phi)= \hat S (\psi \otimes \overline{\hat\phi})W(ψ,ϕ)=S^(ψ⊗ϕ^​​) where ϕ^{\hat\phi}ϕ^​ is the Fourier transform of ϕ\phiϕ and S^\hat SS^ is a metaplectic operator that projects onto a linear symplectomorphism SSS consisting of a rotation along an ellipse in phase space (or in the time-frequency space). This formulation can be extended to generic Weyl symbols and yields an interesting fractional generalization of the Weyl-Wigner formalism. It also provides a suitable approach to study the Bopp phase space representation of quantum mechanics, familiar from deformation quantization. Using the "metaplectic formulation" of the Wigner transform we construct a complete set of intertwiners relating the Weyl and the Bopp pseudo-differential operators. This is an important result that allows us to prove the spectral and dynamical equivalence of the Schr"odinger and the Bopp representations of quantum mechanics.

This mission is the statement-level formalization of Metaplectic formulation of the Wigner transform and applications (arXiv:1401.3388v1). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

2 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Periodicity, two elliptic invariants, and coordinate-pair rotations (Remark 5: periodicity and elliptic invariants, PDF p. 5). The milestones are the other numbered results, in the paper's order, each quoting the paper.

The paper's own objects are the definition item of this mission. Objects shared across papers come from the prove2quantum library and from earlier papers' missions, listed as references.

Provenance: prove2quantum's pipeline drafted each statement (gpt-6.1-sol on Stanford's Sherlock cluster). A blind read-back, written without seeing the paper, is attached to every item. An independent moderator compared each statement against the paper and passed the whole paper without edits.

Deferred results

23 results of the paper are not stated yet, because the library lacks an interface they need:

  • Theorem 7 / introductory main result: metaplectic Wigner formula: Independent cross-Wigner L2 extension, exterior L2 product, and canonical metaplectic evolution (hard)
  • Theorem 4: special symplectic flow and metaplectic projection: Genuine metaplectic double cover, its projection, and the identity-based lift of the fixed Hamiltonian flow (hard)
  • Lemma 6: Fourier-pullback formula for the unitary evolution: Canonical self-adjoint graph closure of the Schwartz quadratic realization and its spectral/Stone evolution (hard)
  • Theorem 8: metaplectic formula for general Weyl symbols: Schwartz-kernel correspondence and independent distributional Weyl symbol (18) (hard)
  • Unnumbered: periodic fractional family and its distinguished members: Printed 2theta0 endpoint conflicts with the fixed quadratic evolution; compatible all-L2 family is also unconstructed (source-ambiguity)
  • Theorem 10: regularity of fractional cross Wigner functions: Jointly continuous distribution exterior product on strong duals and compatible S/L2/S-prime Wigner actions (hard)
  • Unnumbered: fractional Moyal identity and window isometry: Printed order of the two window factors in the Moyal identity, plus the all-L2 fractional window (source-ambiguity)
  • Unnumbered: fractional symbol of a rank-one operator: Rank-one Schwartz-to-distribution map for arbitrary L2 vectors and its computed fractional symbol (hard)
  • Theorem 12: inversion, range projection, and distributional adjoint: Distributional transpose used by the printed extension (26) (source-ambiguity)
  • Theorem 12, explicit Hilbert-space clauses (i),(ii) and adjoint (25): Actual fractional L2 window map, its bounded adjoint contraction, and projection onto its independently defined closed range (hard)
  • Theorem 13: fractional kernel formula: Computed formal-adjoint kernel, fractional distributional symbols, and Schwartz-valued fractional Wigner test (hard)
  • Unnumbered equations (31): transport between standard and fractional calculi: Compatible generic distributional symbol and all-L2 Wigner actions of U (hard)
  • Theorem 14: fractional symbol of composition: Partially defined distributional Moyal composition on compatible operator-symbol pairs (hard)
  • Unnumbered equation (33): algebraic properties of the fractional product: Composable domains for both associations and both distributive laws of the fractional product (hard)
  • Unnumbered equations (34),(35): fractional adjoint and reflected-angle kernel formula: Printed parameter-reflection identity (34) is incompatible with conjugation of the fixed generator; generic symbol/kernel actions are also missing (source-ambiguity)
  • Corollary 15: fractional observable expectation formula: Formal-self-adjoint generic operator, fractional distribution symbol, and its evaluation on a Schwartz Wigner function (hard)
  • Unnumbered: standard and fractional position marginals: Printed inverse-U coefficient in the fractional marginal is not the required conjugate transformed symbol; delta-product and Wigner actions are also missing (source-ambiguity)
  • Unnumbered equation (37): conjugation reflects the fractional parameter: Printed reflected-angle equality (37) fails for the actual quadratic evolution; compatible all-L2 family is also missing (source-ambiguity)
  • Theorem 16: Weyl symbol of the phase-space extension: Distributional phase-space extension from the operator kernel and its computed double-phase Weyl symbol (hard)
  • Theorem 20: exact Bopp Weyl symbol: Generic distributional Bopp operator and submersion pullback of an arbitrary tempered Weyl symbol (hard)
  • Unnumbered main result: Weyl–Bopp intertwining relations: Compatible generic distributional Bopp operator, fixed-window isometries, transpose adjoints, and totality over windows (hard)
  • Unnumbered final result: transfer of all spectral clauses of Theorem 17: Specified L2 realizations and eigenfunction domains for the generic operator and its Bopp counterpart (source-ambiguity)
  • Unnumbered final result: transfer of both dynamical clauses of Theorem 18: Generic Bopp and window maps on S/S-prime, with the correctly extended adjoint for reverse solution transfer (hard)

Selected references

  • Metaplectic formulation of the Wigner transform and applications, arXiv:1401.3388v1, https://arxiv.org/abs/1401.3388v1
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Quantum Information·Captain: Goku

Contractivity properties of a quantum diffusion semigroupResearch Paper

Motivation

We consider a quantum generalization of the classical heat equation, and study contractivity properties of its associated semigroup. We prove a Nash inequality and a logarithmic Sobolev inequality. The former leads to an ultracontractivity result. This in turn implies that the largest eigenvalue and the purity of a state with positive Wigner function, evolving under the action of the semigroup, decrease at least inverse polynomially in time, while its entropy increases at least logarithmically in time.

This mission is the statement-level formalization of Contractivity properties of a quantum diffusion semigroup (arXiv:1607.04242v6). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

1 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Order comparison of second derivatives at a common zero minimum (Lemma 3 (Appendix C), PDF p. 29). The milestones are the other numbered results, in the paper's order, each quoting the paper.

The paper's own objects are the definition item of this mission. Objects shared across papers come from the prove2quantum library and from earlier papers' missions, listed as references.

Provenance: prove2quantum's pipeline drafted each statement (gpt-6.1-sol on Stanford's Sherlock cluster). A blind read-back, written without seeing the paper, is attached to every item. An independent moderator compared each statement against the paper and passed the whole paper without edits.

Deferred results

13 results of the paper are not stated yet, because the library lacks an interface they need:

  • Lemma 1: Unbounded spectral functional calculus and state-weighted L2 space (hard)
  • Theorem 3: Canonical n-mode trace-class diffusion and Hilbert-Schmidt generator domain (hard)
  • Theorem 5: Schwartz densities, Wigner transform, and trace-class generator membership (hard)
  • Theorem 6: Diffusion on Schwartz states and extended von Neumann entropy (hard)
  • Theorem 7: Finite local Fisher derivatives for faithful Gaussian densities (hard)
  • Theorem 8: Fisher information at nonfaithful Gaussian states (source-ambiguity)
  • Theorem 9: Displacement Fisher information with output differentiability (hard)
  • Theorem 10: Half-line second differentiability of Gaussian entropy power (hard)
  • Lemma 2: Unbounded logarithms, double commutators and trace-class extensions (hard)
  • Section 5, equations (5.2),(5.7)-(5.9): Operator/Fourier interface with the paper Wigner normalization (hard)
  • Section 5, proof of Theorem 6: Purity curve of the actual canonical diffusion and its Dirichlet energy (hard)
  • Appendix C, equation (C.1): Extended relative entropy of the fixed hybrid Weyl convolution (hard)
  • Appendix C, equations (C.2),(C.6): Weakly measurable essentially bounded operator fields and normal product states (hard)

Selected references

  • Contractivity properties of a quantum diffusion semigroup, arXiv:1607.04242v6, https://arxiv.org/abs/1607.04242v6
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Quantum Information·Captain: Goku

Hadamard quantum broadcast channelsResearch Paper

Motivation

We consider three different communication tasks for quantum broadcast channels, and we determine the capacity region of a Hadamard broadcast channel for these various tasks. We define a Hadamard broadcast channel to be such that the channel from the sender to one of the receivers is entanglement-breaking and the channel from the sender to the other receiver is complementary to this one. As such, this channel is a quantum generalization of a degraded broadcast channel, which is well known in classical information theory. The first communication task we consider is classical communication to both receivers, the second is quantum communication to the stronger receiver and classical communication to other, and the third is entanglement-assisted classical communication to the stronger receiver and unassisted classical communication to the other. The structure of a Hadamard broadcast channel plays a critical role in our analysis: the channel to the weaker receiver can be simulated by performing a measurement channel on the stronger receiver's system, followed by a preparation channel. As such, we can incorporate the classical output of the measurement channel as an auxiliary variable and solve all three of the above capacities for Hadamard broadcast channels, in this way avoiding known difficulties associated with quantum auxiliary variables.

This mission is the statement-level formalization of Hadamard quantum broadcast channels (arXiv:1611.07651v3). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

7 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Theorem 2: exact classical capacity of a Hadamard broadcast channel (Theorem 2, §3.3: classical capacity of a Hadamard broadcast channel (seed paper result), PDF p. 4). The milestones are the other numbered results, in the paper's order, each quoting the paper.

The paper's own objects are the definition item of this mission. Objects shared across papers come from the prove2quantum library and from earlier papers' missions, listed as references.

Provenance: prove2quantum's pipeline drafted each statement (gpt-6.1-sol on Stanford's Sherlock cluster). A blind read-back, written without seeing the paper, is attached to every item. An independent moderator compared each statement against the paper and passed the whole paper without edits.

Selected references

  • Hadamard quantum broadcast channels, arXiv:1611.07651v3, https://arxiv.org/abs/1611.07651v3
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Quantum Information·Captain: Goku

Uniform finite-dimensional approximation of basic capacities of energy-constrained channelsResearch Paper

Motivation

We consider energy-constrained infinite-dimensional quantum channels from a given system (satisfying a certain condition) to any other systems. We show that dealing with basic capacities of these channels we may assume (accepting arbitrarily small error ε\varepsilonε) that all channels have the same finite-dimensional input space -- the subspace corresponding to the m(ε)m(\varepsilon)m(ε) minimal eigenvalues of the input Hamiltonian. We also show that for the class of energy-limited channels (mapping energy-bounded states to energy-bounded states) the above result is valid with substantially smaller dimension m(ε)m(\varepsilon)m(ε). The uniform finite-dimensional approximation allows to prove the uniform continuity of the basic capacities on the set of all quantum channels with respect to the strong (pointwise) convergence topology. For all the capacities we obtain continuity bounds depending only on the input energy bound and the energy-constrained-diamond-norm distance between quantum channels (generating the strong convergence on the set of quantum channels).

This mission is the statement-level formalization of Uniform finite-dimensional approximation of basic capacities of energy-constrained channels (arXiv:1707.05641v2). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

4 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Monotonicity of the perspective of a nonnegative concave function (Lemma 1, PDF p. 9). The milestones are the other numbered results, in the paper's order, each quoting the paper.

The paper's own objects are the definition item of this mission. Objects shared across papers come from the prove2quantum library and from earlier papers' missions, listed as references.

Provenance: prove2quantum's pipeline drafted each statement (gpt-6.1-sol on Stanford's Sherlock cluster). A blind read-back, written without seeing the paper, is attached to every item. An independent moderator compared each statement against the paper and passed the whole paper without edits.

Deferred results

8 results of the paper are not stated yet, because the library lacks an interface they need:

  • Theorem 1: Actual Cchi, Cea, Qbar, Cpbar and regularized C,Q,Cp from Section 4.1: discrete ensembles constrained in average energy, genuine complementary channel/purification, all positive block lengths, additive Hamiltonians and tensor-power input-subspace restrictions. Finiteness must be established on the stated energy domain before taking real differences. (hard)
  • Theorem 2: Actual Cchi, Cea, Qbar, Cpbar and regularized C,Q,Cp from Section 4.1: discrete ensembles constrained in average energy, genuine complementary channel/purification, all positive block lengths, additive Hamiltonians and tensor-power input-subspace restrictions. Finiteness must be established on the stated energy domain before taking real differences. Energy-constrained diamond distance as the supremum of the actual ancilla-amplified channel-difference trace norm over all normalized inputs of energy <= E; the induced metric uniformity and its strong-topology compatibility. (hard)
  • Theorem 3: Actual Cchi, Cea, Qbar, Cpbar and regularized C,Q,Cp from Section 4.1: discrete ensembles constrained in average energy, genuine complementary channel/purification, all positive block lengths, additive Hamiltonians and tensor-power input-subspace restrictions. Finiteness must be established on the stated energy domain before taking real differences. Energy-constrained diamond distance as the supremum of the actual ancilla-amplified channel-difference trace norm over all normalized inputs of energy <= E; the induced metric uniformity and its strong-topology compatibility. (hard)
  • Lemma 2: Actual extended QCMI on arbitrary complete separable tripartite spaces, using the finite-rank-compression supremum with homogeneous evaluation on subnormalized operators, and its compatibility with the trace-class state/channel model. Support-restricted extended mean energy on a common closed subspace of AD. (hard)
  • Lemma 3: Actual relative-entropy mutual information on arbitrary block outputs and references, compatible tensor powers and the energy truncation map. (hard)
  • Lemma 6: Actual block mutual information and energy-constrained diamond distance for energy-limited channels on arbitrary output/reference systems. (hard)
  • Appendix Lemma 7: Actual extended QCMI on arbitrary complete separable tripartite spaces, using the finite-rank-compression supremum with homogeneous evaluation on subnormalized operators, and its compatibility with the trace-class state/channel model. Energy-constrained diamond distance as the supremum of the actual ancilla-amplified channel-difference trace norm over all normalized inputs of energy <= E; the induced metric uniformity and its strong-topology compatibility. (hard)
  • Remark 1: Actual extended QCMI on arbitrary complete separable tripartite spaces, using the finite-rank-compression supremum with homogeneous evaluation on subnormalized operators, and its compatibility with the trace-class state/channel model. Arbitrary block channels and reference/conditioning systems with the input marginal-energy constraints of Lemma 3. (hard)

Selected references

  • Uniform finite-dimensional approximation of basic capacities of energy-constrained channels, arXiv:1707.05641v2, https://arxiv.org/abs/1707.05641v2
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