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Perturbative anomalies in quantum mechanics

Maxim Gritskov, Andrey Losev, Saveliy Timchenko

Abstract

In this work, we propose a cohomological approach to studying perturbative anomalies in quantum mechanics. The Hamiltonian $\hat{H}$ together with the symmetry generator $\hat{S}$ forms a unitary representation of the two-dimensional Abelian Lie algebra $g\cong \mathbb{R}^{2}$ on the Hilbert space $V$. We show that perturbations of such a system are related to the first Chevalley-Eilenberg cohomology group $H^{1}_{CE}(\mathbb{R}^{2},\mathfrak{u}(V))$. In turn, the perturbative anomalies of the symmetry $\hat{S}$ are related to the second cohomology group $H^{2}_{CE}(\mathbb{R}^{2},\mathfrak{u}(V))$.

Perturbative anomalies in quantum mechanics

Abstract

In this work, we propose a cohomological approach to studying perturbative anomalies in quantum mechanics. The Hamiltonian together with the symmetry generator forms a unitary representation of the two-dimensional Abelian Lie algebra on the Hilbert space . We show that perturbations of such a system are related to the first Chevalley-Eilenberg cohomology group . In turn, the perturbative anomalies of the symmetry are related to the second cohomology group .
Paper Structure (7 sections, 8 theorems, 43 equations)

This paper contains 7 sections, 8 theorems, 43 equations.

Key Result

Proposition 2.2

The first cohomology group $H^1(\mathfrak{g},V\otimes V^*)$ corresponds to the nontrivial infinitesimal deformations of a Lie algebra representation $\rho$.

Theorems & Definitions (18)

  • Definition 2.1
  • Proposition 2.2
  • Proposition 2.3
  • Example 2.4
  • Lemma 2.5
  • proof
  • Lemma 2.6
  • proof
  • Lemma 2.7
  • proof
  • ...and 8 more