Classical capacity of fermionic product channels: An Explicit Formula for the Gaussian Capacity, Which Equals the One-Shot Capacity for n ≤ 2Research Paper
Motivation
Sending classical messages through a quantum device requires choosing input states that remain distinguishable after noise. The one-shot classical capacity measures the best information rate when each channel use is signaled with a separate input state. For many channels the optimization is difficult because it ranges over all ensembles of quantum states. Fermionic systems provide a finite-dimensional setting in which the noise has a direct description on elementary operators, but the optimal signaling states still need not be obvious. Bravyi's 2005 paper isolates a family of fermionic product channels, computes the best rate from Gaussian input states for any number of qubits, and proves that this restricted rate is the full one-shot rate for one or two qubits.
Setting
The system has qubits, with computational basis indexed by bit strings . The Jordan–Wigner Majorana operators are tensor products of Pauli matrices: has on qubits before , on qubit , and identity afterwards; replaces with . Their ordered monomials , , form a basis of all operators on the qubits. The paper gives these operators and their monomials in Eq. (3).
A fermionic product channel is determined by attenuation coefficients . On each monomial it acts by , and linearity defines it on every operator. A state is a positive semidefinite matrix of trace one. For a finite ensemble of output states , with nonnegative weights summing to one, its Holevo quantity in bits is
The supremum of over all finite ensembles of outputs of is . A Gaussian state has the specific form of Definition 1: , each , and for Hermitian quadratic and linear combinations of Majorana operators. Requiring Gaussian input states gives . Setting gives an even Gaussian state. These are separate classes; the even class supplies an intermediate entropy minimum. Definition 1 and Eq. (13) are on page 4.
Formalization targets
Gaussian capacity
Write for the coefficients in decreasing order, and let . The main formula, Theorem 1 and Eq. (6), is
It holds for every and every unsorted . The milestones identify the covariance and Gaussian-preservation facts, the exact even and general Gaussian minimum-output entropies, and an ensemble attaining the capacity.
Full one-shot capacity for at most two qubits
The second clause of Theorem 1 states
Thus restricting the input ensemble to Gaussian states loses no one-shot capacity in these dimensions. The paper does not prove this equality for arbitrary .
Significance
The formula replaces an optimization over arbitrary finite Gaussian ensembles with binary entropies of sorted attenuation coefficients. In the one- and two-qubit cases it also settles the unrestricted one-shot optimization for this channel family. The intermediate result relates signaling directly to minimum output entropy; the even-Gaussian and Gaussian minima make the distinction between the two state classes explicit. These relationships are established in Sections II–IV of the paper.
The mathematical results are proved in the 2005 paper. This mission asks for machine-checked proofs of their exact finite-dimensional statements. The definitions of bit-valued von Neumann entropy, finite output ensembles, ordered Majorana monomials, Gaussian-state predicates, and covariance matrices can support later work on fermionic channels. The submitted goal and milestones are presently proof obligations rather than claims of existing Lean proofs.
Difficulty
The channel is simple on each Majorana monomial, but the entropy of a general output state is not determined by its one- and two-point correlations. Even within the Gaussian class, optimizing only the even Gaussian states gives a different formula from optimizing all Gaussian states: linear Majorana terms change the optimum. A direct search over density matrices therefore does not expose the closed expression in Theorem 1. For the unrestricted two-qubit clause, one must also relate arbitrary states to the Gaussian class; the paper invokes a three-qubit parity result for that step. The distinctions and parity result appear in Sections III–IV.
Formalization scope
Lean represents qubit basis vectors by Fin n → Fin 2 and operators by complex matrices on that finite type. Majorana indices start at zero in Lean, so the paper's correspond to consecutive indices . The Jordan–Wigner tensor factor at coordinate acts on qubit ; the monomial product follows increasing Majorana index. The channel is defined on all matrices by the trace-orthogonal monomial expansion of Eq. (4), not merely on covariance matrices. Attenuations may equal zero or one. Entropies use logarithms to base two, with .
Every capacity uses a real supremum over all finite normalized ensembles, with arbitrary ensemble size. The inputs are density matrices, and their channel outputs must be density matrices. The Gaussian capacity requires every input to satisfy Definition 1; Lemma 2 ensures these outputs are Gaussian too. The minimum-output quantities are real infima over their stated input classes, and the corresponding milestone theorems assert attainment. For the actual channels the relevant sets are nonempty and bounded: the maximally mixed state supplies an output state, while every Holevo quantity lies between zero and . This representation rules out restricting the Gaussian ensemble to the displayed optimizing family, assuming the goal's coefficients are initially sorted, or replacing bit entropy with natural-log entropy.
The development needs finite-matrix functional calculus, positivity, matrix exponentials, permutation and singular-value reasoning, and finite ensemble entropy bounds. Contributions to those reusable layers and to the paper's covariance, Gaussian-preservation, and minimum-output results are within scope. Lemma 3 is stated in its even-Gaussian form, which its proof establishes; the displayed lemma says only “Gaussian.”
Selected references
- Sergey Bravyi, Classical capacity of fermionic product channels, arXiv preprint quant-ph/0507282v1, 2005. arXiv