Explorerβ€ΊQuantum Computingβ€ΊQuantum Physics
Research PaperResearchia:202605.04018

The structure of gauge invariant Gaussian quantum operations on finite Fermion systems

Eric A. Carlen

Abstract

Let ${\mathcal H}_1$ be a finite dimensional complex Hilbert space. Let $ψ\mapsto Z(ψ)$ be a canonical anti-commutation relations (CAR) field over ${\mathcal H}_1$ acting irreducibly on a Hilbert space ${\mathord{\mathscr K}}$. The $$-algebra ${\mathscr A}_{{\mathcal H}_1}$ generated by the $Z(ψ)$, $ψ\in {\mathcal H}_1$, is simply all operators on ${\mathscr K}$. However, the CAR field endows ${\mathscr A}_{{\mathcal H}_1}$ with additional structure, and we are concerned with quantum operation...

Submitted: May 4, 2026Subjects: Quantum Physics; Quantum Computing

Description / Details

Let H1{\mathcal H}_1 be a finite dimensional complex Hilbert space. Let Οˆβ†¦Z(ψ)ψ\mapsto Z(ψ) be a canonical anti-commutation relations (CAR) field over H1{\mathcal H}_1 acting irreducibly on a Hilbert space K{\mathord{\mathscr K}}. The βˆ—*-algebra AH1{\mathscr A}_{{\mathcal H}_1} generated by the Z(ψ)Z(ψ), ψ∈H1ψ\in {\mathcal H}_1, is simply all operators on K{\mathscr K}. However, the CAR field endows AH1{\mathscr A}_{{\mathcal H}_1} with additional structure, and we are concerned with quantum operations whose acting in harmony with this structure. In particular, there is a gauge automorphism group generated by ``second quantizing'' Οˆβ†¦eitψψ\mapsto e^{it}ψ. The fixed point algebra of the gauge group, GH1{\mathscr G}_{{\mathcal H}_1}, is a sub-algebra of AH1{\mathscr A}_{{\mathcal H}_1} studied by Araki and Wyss. It contains the density matrices of an important class of states, the gauge invariant Gaussian states, SGIG{\mathfrak S}_{GIG}. Our focus is on semigroups {etL}tβ‰₯0\{e^{t{\mathscr L}}\}_{t\geq 0} of quantum operations on AH1{\mathscr A}_{{\mathcal H}_1} that map SGIG{\mathfrak S}_{GIG} into itself. Each etLe^{t{\mathscr L}} is one-to-one, and our first main result is a structure theorem forsuch quantum operations on GH1{\mathscr G}_{{\mathcal H}_1} that map SGIG{\mathfrak S}_{GIG} into itself. We apply this to study semigroups of quantum operations on GH1{\mathscr G}_{{\mathcal H}_1} that map SGIG{\mathfrak S}_{GIG} into itself. Our second main result is a structure theorem showing that they are parameterized by pairs (G,A)(G,A) where GG is a contraction semigroup generator on H1{\mathcal H}_1, and 0≀Aβ‰€βˆ’Gβˆ’Gβˆ—0 \leq A \leq -G -G^*. We then show that each of these semigroups has a natural extension to the full CAR algebra AH1{\mathscr A}_{{\mathcal H}_1}. Further results are obtained under further assumptions on the pair (G,A)(G,A).


Source: arXiv:2605.00784v1 - http://arxiv.org/abs/2605.00784v1 PDF: https://arxiv.org/pdf/2605.00784v1 Original Link: http://arxiv.org/abs/2605.00784v1

Please sign in to join the discussion.

No comments yet. Be the first to share your thoughts!

Access Paper
View Source PDF
Submission Info
Date:
May 4, 2026
Topic:
Quantum Computing
Area:
Quantum Physics
Comments:
0
Bookmark
The structure of gauge invariant Gaussian quantum operations on finite Fermion systems | Researchia