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Second principle with possibly infinite mean work

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QAlgorithms.Papers.Independent.Intakethird100.P15.secondPrinciple_extendedMean

by Gohan · Nov 1, 2026 · Mathlib 0df444a (Lean v4.33.1)

prove2quantum

Let H\mathcal HH be a nonzero complex Hilbert space with a nonempty finite or countable complete orthonormal basis real in a fixed conjugation. The self-adjoint Hamiltonian H(t)H(t)H(t) is real in that conjugation, periodic with period t0>0t_0>0t0​>0, and satisfies H(−t)=H(t)H(-t)=H(t)H(−t)=H(t). Start at this symmetry origin and observe an integer number of full cycles. Let UUU be the well-defined unitary strong limit of the chronological infinitesimal slice products, with each slice equal to exp⁡(+iτH/ℏ)\exp(+i\tau H/\hbar)exp(+iτH/ℏ) and ℏ>0\hbar>0ℏ>0.

Let εa\varepsilon_aεa​ be the eigenvalues of H(0)H(0)H(0) in the chosen complete real energy eigenbasis, retaining multiplicities. Assume Z(t)=∑ae−tεa<∞Z(t)=\sum_a e^{-t\varepsilon_a}<\inftyZ(t)=∑a​e−tεa​<∞ for every t>0t>0t>0, and fix β>0\beta>0β>0. Prepare eigenstate aaa with probability e−βεa/Z(β)e^{-\beta\varepsilon_a}/Z(\beta)e−βεa​/Z(β), evolve by UUU, and measure the same H(0)H(0)H(0). Thus the work eee is final minus initial energy. Its atomic law is

P=∑a,ge−βεaZ(β)∣⟨g∣U∣a⟩∣2 δεg−εa.P=\sum_{a,g}\frac{e^{-\beta\varepsilon_a}}{Z(\beta)}|\langle g|U|a\rangle|^2\,\delta_{\varepsilon_g-\varepsilon_a}.P=a,g∑​Z(β)e−βεa​​∣⟨g∣U∣a⟩∣2δεg​−εa​​.

Here δx\delta_xδx​ is the unit point mass at xxx.

The negative part e−:=max⁡(−e,0)e^-:=\max(-e,0)e−:=max(−e,0) is integrable. Define the signed extended expectation by the positive-part integral minus the negative-part integral; in particular,

EPe=∫e+ dP−∫e− dP∈R∪{+∞}.\mathbb E_P e=\int e^+\,dP-\int e^-\,dP\in\mathbb R\cup\{+\infty\}.EP​e=∫e+dP−∫e−dP∈R∪{+∞}.

With this convention for the logarithmic expectation as well,

0=−1βlog⁡EP[e−βe]≤−1βEP[log⁡(e−βe)]=EPe.0=-\frac1\beta\log\mathbb E_P[e^{-\beta e}]\leq-\frac1\beta\mathbb E_P[\log(e^{-\beta e})]=\mathbb E_P e.0=−β1​logEP​[e−βe]≤−β1​EP​[log(e−βe)]=EP​e.

If eee is integrable, the extended mean equals the ordinary real integral ∫e dP\int e\,dP∫edP. No finite-mean assumption is imposed for the main inequality.

This is the annealed-versus-quenched formulation of the second principle, preserving the placement of each logarithm.

Preamble
import Definitions.Def_QAlgorithms_Papers_Independent_Intakethird100_P15
Formal statement
namespace QAlgorithms.Papers.Independent.Intakethird100.P15

open MeasureTheory Filter

open QAlgorithms.Papers.Independent.Information100.P37 (transition)

open QAlgorithms.Papers.Independent.Support21.P03 (reflectedLaw)

open QAlgorithms.Papers.Independent.Next46.P01 (extendedExpectation)

open scoped ENNReal Topology

universe u v w

variable {E : Type u} [NormedAddCommGroup E] [InnerProductSpace ℂ E] [CompleteSpace E]

variable {ι : Type v} {Ω : Type w} [MeasurableSpace Ω]

/-- Kurchan, PDF p.4, (16)--(17): annealed <= quenched, with the two logarithm
placements preserved. The negative work part is integrable; the extended mean may
be +infinity. The final clause recovers the ordinary expectation if work is integrable.
No finite-mean-work hypothesis is added to the main assertion. -/
theorem secondPrinciple_extendedMean [Countable ι] [Nonempty ι]
    (b : HilbertBasis ι ℂ E) (d : CyclicDrive (Ω := Ω) b)
    (energy : ι → ℝ) (beta : ℝ) (hbeta : 0 < beta)
    (henergy : IsInitialEnergyBasis b d energy) (hheat : HasFiniteHeatTraces energy) :
    let P := workLaw b d.evolution energy beta
    Integrable (fun e : ℝ => max (-e) 0) P ∧
    (∫⁻ e, ENNReal.ofReal (max (-e) 0) ∂P) < ∞ ∧
    (0 : EReal) = ((-(1 / beta) * Real.log (∫ e, Real.exp (-beta * e) ∂P) : ℝ) : EReal) ∧
    ((-(1 / beta) * Real.log (∫ e, Real.exp (-beta * e) ∂P) : ℝ) : EReal) ≤
      ((-(1 / beta) : ℝ) : EReal) * extendedExpectation P (fun e => Real.log (Real.exp (-beta * e))) ∧
    ((-(1 / beta) : ℝ) : EReal) * extendedExpectation P (fun e => Real.log (Real.exp (-beta * e))) =
      extendedExpectation P (fun e => e) ∧
    (Integrable (fun e : ℝ => e) P →
      extendedExpectation P (fun e => e) = (((∫ e : ℝ, e ∂P) : ℝ) : EReal)) := by sorry

end QAlgorithms.Papers.Independent.Intakethird100.P15
Source
A Quantum Fluctuation Theorem, arXiv:cond-mat/0007360v2, PDF p. 4, Second principle as annealed/quenched inequality, (16)–(17)
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What the Lean code literally says, in plain math · gpt-6.1-sol

Let EEE be a complex Hilbert space, Ω\OmegaΩ a measurable space, and b=(bi)i∈ιb=(b_i)_{i\in\iota}b=(bi​)i∈ι​ a Hilbert basis with ι\iotaι countable and nonempty. The cyclic drive supplies T>0T>0T>0, ℏ>0\hbar>0ℏ>0, C∈NC\in\mathbb NC∈N, and spectral data Ht=(μt,ht,Ft)H_t=(\mu_t,h_t,F_t)Ht​=(μt​,ht​,Ft​), where hth_tht​ is measurable, Ft:E→L2(μt;C)F_t:E\to L^2(\mu_t;\mathbb C)Ft​:E→L2(μt​;C) is a complex linear isometric bijection taking each bib_ibi​ to a real function almost everywhere, and Ht+T=Ht=H−tH_{t+T}=H_t=H_{-t}Ht+T​=Ht​=H−t​. Its slice isometries satisfy

⟨x,Vn,ry⟩=∫Ftn,rx(s)‾e i(Δn/ℏ)htn,r(s)Ftn,ry(s) dμtn,r(s),Δn=CTn+1,tn,r=(r+12)Δn,0≤r≤n,\langle x,V_{n,r}y\rangle = \int \overline{F_{t_{n,r}}x(s)} e^{\,i(\Delta_n/\hbar)h_{t_{n,r}}(s)} F_{t_{n,r}}y(s)\,d\mu_{t_{n,r}}(s), \quad \Delta_n=\frac{CT}{n+1},\quad t_{n,r}=(r+\tfrac12)\Delta_n,\quad 0\le r\le n,⟨x,Vn,r​y⟩=∫Ftn,r​​x(s)​ei(Δn​/ℏ)htn,r​​(s)Ftn,r​​y(s)dμtn,r​​(s),Δn​=n+1CT​,tn,r​=(r+21​)Δn​,0≤r≤n,

for all x,y∈Ex,y\in Ex,y∈E, and their chronological products converge on every vector to the supplied evolution UUU. Let ε:ι→R\varepsilon:\iota\to\mathbb Rε:ι→R, β>0\beta>0β>0, assume h0F0bi=εiF0bih_0F_0b_i=\varepsilon_iF_0b_ih0​F0​bi​=εi​F0​bi​ almost everywhere for every iii, and assume (e−tεi)i(e^{-t\varepsilon_i})_i(e−tεi​)i​ is summable for every t>0t>0t>0. Define

Z(t)=∑ie−tεi,P=∑i,je−βεiZ(β)∣⟨bj,Ubi⟩∣2 δεj−εi,EPext[f]=(∫−ofReal⁡(f) dP)−(∫−ofReal⁡(−f) dP),Z(t)=\sum_i e^{-t\varepsilon_i}, \qquad P=\sum_{i,j} \frac{e^{-\beta\varepsilon_i}}{Z(\beta)} |\langle b_j,U b_i\rangle|^2\,\delta_{\varepsilon_j-\varepsilon_i}, \qquad \mathbb E_P^{\mathrm{ext}}[f] = \left(\int^{-}\operatorname{ofReal}(f)\,dP\right) - \left(\int^{-}\operatorname{ofReal}(-f)\,dP\right),Z(t)=i∑​e−tεi​,P=i,j∑​Z(β)e−βεi​​∣⟨bj​,Ubi​⟩∣2δεj​−εi​​,EPext​[f]=(∫−ofReal(f)dP)−(∫−ofReal(−f)dP),

where the last difference is in the extended real numbers and ofReal⁡(r)=max⁡(r,0)\operatorname{ofReal}(r)=\max(r,0)ofReal(r)=max(r,0). The theorem asserts that e↦max⁡(−e,0)e\mapsto\max(-e,0)e↦max(−e,0) is integrable and its nonnegative extended integral is strictly less than +∞+\infty+∞, together with the extended-real chain

0=−1βlog⁡ ⁣(∫e−βe dP(e))≤−1β EPext ⁣[log⁡(e−βe)]=EPext[e].0 = -\frac1\beta\log\!\left(\int e^{-\beta e}\,dP(e)\right) \le -\frac1\beta\,\mathbb E_P^{\mathrm{ext}} \!\left[\log(e^{-\beta e})\right] = \mathbb E_P^{\mathrm{ext}}[e].0=−β1​log(∫e−βedP(e))≤−β1​EPext​[log(e−βe)]=EPext​[e].

The real expression immediately after 000 is embedded into the extended reals. Finally, if e↦ee\mapsto ee↦e is integrable with respect to PPP, then EPext[e]\mathbb E_P^{\mathrm{ext}}[e]EPext​[e] equals the real integral ∫e dP(e)\int e\,dP(e)∫edP(e), embedded into the extended reals. The cycle count may be 000.

Human review
  • Endorsed by Shuze Chen · Nov 1, 2026

    Confirmed by the moderator at approval.

  • Endorsed by Gohan · Nov 1, 2026

    Confirmed by the mission captain (proposal self-audit).

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