The entropy photon-number inequalityResearch Paper
Motivation
Shannon's entropy power inequality bounds the entropy of a sum of independent random vectors below by the entropies of the summands; it is a basic tool for classical Gaussian channel capacities. In optical communication, addition is replaced by passive mixing of bosonic modes at a beam splitter. Guha, Erkmen and Shapiro conjectured the sharp bosonic analogue, the entropy photon-number inequality (EPnI), stated in terms of the photon number of the thermal state with the same entropy (ITA 2008). If true, it settles the minimum output entropy of thermal attenuators at fixed input entropy and the capacity regions of bosonic broadcast and wiretap channels, which had been reduced to this inequality (PRA 2007).
This mission asks for a formal proof of the EPnI for finite-energy inputs in any finite number of modes, as stated in an OpenAI preprint dated September 24, 2026 (source). The preprint has not been peer reviewed and its claims have not been independently verified; on the platform the Lean goal is open.
Background
- 1948–1965 — Shannon introduces entropy power; Stam (1959) and Blachman (IEEE IT 1965) prove the entropy power inequality.
- 2004 — Capacity of the pure-loss bosonic channel (PRL 2004) and the minimum-output-entropy conjecture (PRA 2004).
- 2007–2008 — Guha, Shapiro and Erkmen relate broadcast capacity to a minimum-output-entropy conjecture; Guha, Erkmen and Shapiro state the EPnI.
- 2011 — Special cases (one-mode number-diagonal inputs) by Das, Sharma and Muthukrishnan (arXiv:1107.2365).
- 2014 — König and Smith prove a quantum entropy power inequality, including (IEEE IT 2014); De Palma, Mari and Giovannetti prove the exponential form (Nat. Photonics 2014).
- 2015 — Giovannetti, Holevo and García-Patrón solve the Gaussian optimizer conjecture for unconstrained minimum output entropy (CMP 2015).
- 2016–2018 — De Palma, Trevisan and Giovannetti settle one-mode constrained problems (IEEE IT 2017; PRL 2017); De Palma and Trevisan give a rigorous finite-energy conditional EPI (CMP 2018).
- September 2026 — The OpenAI preprint claims the two-input EPnI for all finite-energy inputs (Theorem 1.1, p. 2).
Setting
An -mode bosonic system has Fock space with number basis , . A state is a positive trace-one operator ; it has finite energy if . The von Neumann entropy is (natural log). The thermal entropy per mode is
increasing from to , and the entropy photon number of is , the mean photon number per mode of the product thermal state with the same entropy. For independent inputs and transmissivity , the beam-splitter output is the reduced state of the modes after passive mixing of . No independence among the modes within either input is assumed.
Formalization targets
Goal: Theorem 1.1 (p. 2)
For every finite , every pair of finite-energy -mode states and every ,
Thermal inputs with a common mean photon number within each port give equality.
Significance
The result itself. The EPnI is sharper than the exponential quantum entropy power inequality when the two input entropies differ, which is exactly the regime needed for constrained minimum output entropy. The preprint derives the exact minimum output entropy at fixed input entropy for every tensor power of an identical thermal attenuator, with inputs entangled across modes (Corollary 1.2, p. 2), and the exact capacity region of the degraded two-receiver pure-loss broadcast channel (Corollary 7.1, p. 26), completing the converse of Guha, Shapiro and Erkmen.
Formalizing it. The statement involves infinite-dimensional Fock space, trace-class positive operators, continuous functional calculus for the entropy, and the partial trace after a passive unitary. The Lean development builds these concretely in the number basis. A formal proof would give machine-checked infrastructure for quantum entropy on infinite-dimensional spaces, which Mathlib currently lacks. No machine-checked version of any quantum entropy power inequality is known.
Difficulty
Heat-flow (quantum Fisher information) proofs give the linear and exponential bounds, but these are attained only for equal entropies and do not recover the thermal comparison at unequal entropy levels. The preprint instead minimizes a regularized functional over pairs of inputs and must show that minimizers are thermal. This requires an interpolation theorem for diagonal form comparisons (Theorem 3.1, p. 8), attainment and Gibbs regularity of minimizers in infinite dimensions (Lemma 4.1, Proposition 4.2, pp. 15–16), a component entropy-Hessian estimate, and a stationarity identity whose cancellation forces convergence to thermal inputs (Section 6). Compactness relies on the finite-energy hypothesis; without it entropies can be infinite.
Formalization scope
Fock nislp (fun _ : Fin n → ℕ => ℂ) 2. AStateis a positive bounded operator whose diagonal in the number basis sums (HasSum) to .FiniteEnergy ρis summability of .entropy ρis the sum of diagonal entries of ; for finite-energy states it is finite, so thetsumis the true entropy.gInv s = sInf {t ≥ 0 | s ≤ g t}, the inverse of on .IsBeamSplitterOutput η ρA ρB ρCrequires every number-basis entry of to be the (convergent) partial-trace sum of the explicitly given beam-splitter coefficients applied to ; the inputs are arbitrary density matrices, so internal entanglement is allowed.- The hypotheses are satisfiable (e.g. vacuum or thermal inputs) and the conclusion is the inequality as stated.
Selected references
- OpenAI, The entropy photon-number inequality, OpenAI Math Release preprint, September 24, 2026. https://github.com/openai/math/blob/adc7f1241b42e322a6451854ab7e4b4c146bf78a/preprints/The-entropy-photon-number-inequality-September-24-2026/paper.pdf
- S. Guha, B. I. Erkmen, J. H. Shapiro, The entropy photon-number inequality and its consequences, ITA Workshop 2008, 128–130. https://doi.org/10.1109/ITA.2008.4601037
- S. Guha, J. H. Shapiro, B. I. Erkmen, Classical capacity of bosonic broadcast communication and a minimum output entropy conjecture, Phys. Rev. A 76 (2007), 032303. https://doi.org/10.1103/PhysRevA.76.032303
- R. König, G. Smith, The entropy power inequality for quantum systems, IEEE Trans. Inf. Theory 60 (2014), 1536–1548. https://doi.org/10.1109/TIT.2014.2298436
- G. De Palma, A. Mari, V. Giovannetti, A generalization of the entropy power inequality to bosonic quantum systems, Nat. Photonics 8 (2014), 958–964. https://doi.org/10.1038/nphoton.2014.252
- G. De Palma, D. Trevisan, The conditional entropy power inequality for bosonic quantum systems, Comm. Math. Phys. 360 (2018), 639–662. https://doi.org/10.1007/s00220-017-3082-8
- V. Giovannetti, A. S. Holevo, R. García-Patrón, A solution of Gaussian optimizer conjecture for quantum channels, Comm. Math. Phys. 334 (2015), 1553–1571. https://doi.org/10.1007/s00220-014-2150-6
- V. Giovannetti, S. Guha, S. Lloyd, L. Maccone, J. H. Shapiro, H. P. Yuen, Classical capacity of the lossy bosonic channel: the exact solution, Phys. Rev. Lett. 92 (2004), 027902. https://doi.org/10.1103/PhysRevLett.92.027902
- C. E. Shannon, A mathematical theory of communication, Bell Syst. Tech. J. 27 (1948). https://doi.org/10.1002/j.1538-7305.1948.tb00917.x