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The spectral Bregman trace as an overlap-weighted sum of scalar Bregman terms

Proved
HlawkaSchatten.spectralBregmanTrace_eq_sum

by savarin · Sep 27, 2026 · Mathlib 0df444a (Lean v4.33.1)

bregman-divergencehermitian-operatorshlawka-schattenspectral-theory

Fix a finite-dimensional complex inner-product space EEE and a real number ppp (no hypothesis is placed on ppp). Let (ei)i∈ι(e_i)_{i\in\iota}(ei​)i∈ι​ and (fj)j∈κ(f_j)_{j\in\kappa}(fj​)j∈κ​ be orthonormal bases of EEE indexed by finite index types ι,κ\iota,\kappaι,κ, and let a:ι→Ra:\iota\to\mathbb Ra:ι→R, b:κ→Rb:\kappa\to\mathbb Rb:κ→R be real numbers attached to them. For an orthonormal basis eee and real numbers ccc, write diage(c)\mathrm{diag}_e(c)diage​(c) for the self-adjoint operator on EEE with diage(c) ei=ci ei\mathrm{diag}_e(c)\,e_i = c_i\,e_idiage​(c)ei​=ci​ei​ for every iii (spectralDiagonal), and for a function h:R→Rh:\mathbb R\to\mathbb Rh:R→R write h(c)h(c)h(c) for the tuple i↦h(ci)i\mapsto h(c_i)i↦h(ci​), so diage(h(c))\mathrm{diag}_e(h(c))diage​(h(c)) is the operator with eigenvalues h(ci)h(c_i)h(ci​); we also write h(diage(c))h(\mathrm{diag}_e(c))h(diage​(c)) for this same operator.

With Fp(x)=∣x∣p/pF_p(x) = |x|^p/pFp​(x)=∣x∣p/p and Gp(x)=∣x∣p−2xG_p(x) = |x|^{p-2}xGp​(x)=∣x∣p−2x, the spectral Bregman trace of (e,a)(e,a)(e,a) against (f,b)(f,b)(f,b) is

SBTp(e,a,f,b)=Tr⁡Fp(diage(a))−Tr⁡Fp(diagf(b))−Re⁡Tr⁡ ⁣(diage(a)∘Gp(diagf(b)))+Tr⁡ ⁣(diagf(b)∘Gp(diagf(b)))\begin{aligned} &\mathrm{SBT}_p(e,a,f,b)\\ &\quad=\operatorname{Tr}F_p(\mathrm{diag}_e(a))\\ &\qquad-\operatorname{Tr}F_p(\mathrm{diag}_f(b))\\ &\qquad-\operatorname{Re}\operatorname{Tr}\!\big(\mathrm{diag}_e(a)\circ G_p(\mathrm{diag}_f(b))\big)\\ &\qquad+\operatorname{Tr}\!\big(\mathrm{diag}_f(b)\circ G_p(\mathrm{diag}_f(b))\big) \end{aligned}​SBTp​(e,a,f,b)=TrFp​(diage​(a))−TrFp​(diagf​(b))−ReTr(diage​(a)∘Gp​(diagf​(b)))+Tr(diagf​(b)∘Gp​(diagf​(b)))​

(spectralBregmanTrace). The first, second and fourth traces are traces of operators diagonal with real entries. The cross term is the real trace of a product of two self-adjoint operators; its reality also follows from Tr⁡(AB)‾=Tr⁡(BA)=Tr⁡(AB)\overline{\operatorname{Tr}(AB)}=\operatorname{Tr}(BA)=\operatorname{Tr}(AB)Tr(AB)​=Tr(BA)=Tr(AB). The product itself need not be self-adjoint. Write ov⁡(ei,fj)=∣⟨ei,fj⟩∣2\operatorname{ov}(e_i,f_j) = |\langle e_i,f_j\rangle|^2ov(ei​,fj​)=∣⟨ei​,fj​⟩∣2 for the squared overlap of two basis vectors (orthonormalBasisOverlap), and

βp(x,y)  =  Fp(x)−Fp(y)−Gp(y)(x−y)\beta_p(x,y) \;=\; F_p(x) - F_p(y) - G_p(y)(x-y)βp​(x,y)=Fp​(x)−Fp​(y)−Gp​(y)(x−y)

for the scalar Bregman quantity of FpF_pFp​ (scalarBregman). The theorem states

SBTp(e,a,f,b)  =  ∑(i,j) ∈ ι×κov⁡(ei,fj) βp(ai,bj).\mathrm{SBT}_p(e,a,f,b) \;=\; \sum_{(i,j)\,\in\,\iota\times\kappa} \operatorname{ov}(e_i,f_j)\,\beta_p(a_i,b_j).SBTp​(e,a,f,b)=(i,j)∈ι×κ∑​ov(ei​,fj​)βp​(ai​,bj​).

This is one of two exact finite double-sum decompositions (the other is for the squared spectral Mazur distance) that let a scalar comparison between βp(x,y)\beta_p(x,y)βp​(x,y) and a Mazur-type quantity, once it is known to hold for every pair of real numbers, be summed against the overlap weights ov⁡(ei,fj)\operatorname{ov}(e_i,f_j)ov(ei​,fj​) — which are nonnegative and sum to 111 along every row and column — and so lift unchanged, with the same constants, to a comparison between traces of finite-dimensional Hermitian operators.

Formalization Note The identity holds for every real ppp, including p≤0p\le0p≤0 or p∈(0,1)p\in(0,1)p∈(0,1), because FpF_pFp​, GpG_pGp​, and division are all totalized in Lean: Fp(0)=∣0∣p/pF_p(0)=|0|^p/pFp​(0)=∣0∣p/p evaluates to 000 for every real ppp (for p≠0p\ne0p=0 because 0p=00^p=00p=0; for p=0p=0p=0 because 00=10^0=100=1 but 1/0=01/0=01/0=0). This theorem asserts an algebraic trace identity, with no nonnegativity conclusion. For p>1p>1p>1, FpF_pFp​ is convex and differentiable everywhere with derivative GpG_pGp​, giving the usual Bregman-divergence interpretation used later in the argument.

Preamble
import Definitions.Def_HlawkaSchatten_HermitianSpectral
import Definitions.Def_HlawkaSchatten_ScalarBregman
import Definitions.Def_HlawkaSchatten_SpectralLift
import Mathlib.Analysis.Calculus.LHopital
import Mathlib.Analysis.Convex.Deriv
import Mathlib.Analysis.Convex.SpecificFunctions.Basic
import Mathlib.Analysis.InnerProductSpace.Basic
import Mathlib.Analysis.InnerProductSpace.Dual
import Mathlib.Analysis.InnerProductSpace.NormPow
import Mathlib.Analysis.InnerProductSpace.PiL2
import Mathlib.Analysis.InnerProductSpace.Trace
import Mathlib.Data.Sign.Basic
import Mathlib.Topology.Compactification.OnePoint.Basic
import Mathlib.Topology.Instances.Sign

/-
Copyright (c) 2026 Ezzeri Esa. All rights reserved.
Released under Apache 2.0 license as described in the file LICENSE.
Authors: Ezzeri Esa
-/

/-!
# Finite Hermitian spectral trace expansions

This file connects the overlap-weighted scalar comparison to traces of
finite-dimensional symmetric complex-linear maps.
-/


open scoped InnerProductSpace
open RCLike
open ComplexConjugate

variable {ι κ E : Type*} [Fintype ι] [Fintype κ]
  [NormedAddCommGroup E] [InnerProductSpace ℂ E]

open HlawkaSchatten
Formal statement
theorem HlawkaSchatten.spectralBregmanTrace_eq_sum [FiniteDimensional ℂ E]
    (p : ℝ) (e : OrthonormalBasis ι ℂ E) (a : ι → ℝ)
    (f : OrthonormalBasis κ ℂ E) (b : κ → ℝ) :
    spectralBregmanTrace p e a f b =
      ∑ ij : ι × κ, orthonormalBasisOverlap e f ij *
        scalarBregman p (a ij.1) (b ij.2) := by sorry
Source
https://github.com/savarin/hlawka-schatten/blob/79aa498bfcf7b22bd91d771fb32ec278e2d4704b/HlawkaSchatten/HermitianSpectral.lean#L383-L405

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