Lorentz violation and momentum-space geometric phases

Geometric phases can manifest when a relativistic quantum particle moves cyclically along a loop in parameter space. The phase can be affected by the presence of a background field and can be accompanied by nontrivial topological features. The appearance of adiabatic geometric phases in momentum space is demonstrated for a Lorentz-violating Weyl fermion, where the role of the background is played by the coefficients for Lorentz violation. As explicit examples, the Berry curvature and the first Chern number are derived for two cases with large Lorentz violation, one incorporating <a:math xmlns:a="http://www.w3.org/1998/Math/MathML" display="inline"> <a:mrow> <a:mi>C</a:mi> <a:mi>P</a:mi> <a:mi>T</a:mi> </a:mrow> </a:math> violation and one preserving <c:math xmlns:c="http://www.w3.org/1998/Math/MathML" display="inline"> <c:mrow> <c:mi>C</c:mi> <c:mi>P</c:mi> <c:mi>T</c:mi> </c:mrow> </c:math> symmetry. Some alternative topological invariants are also obtained. In certain scenarios with large Lorentz violation, the physical vacuum is associated with a topological phase.

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Publication Details

Journal
Physical review. D/Physical review. D.
Published
2025-11-12
DOI
https://doi.org/10.1103/l87p-sjnb
Citations
1
Primary Topic
Noncommutative and Quantum Gravity Theories
Type
article
Field-Weighted Citation Impact
1.32
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article

Lorentz violation and momentum-space geometric phases

Karl J. Friston
1 citations
Physical review. D/Physical review. D.
Noncommutative and Quantum Gravity Theories
1.32
article

Lorentz violation and momentum-space geometric phases

Karl J. Friston
article en
1 citations

Abstract

Geometric phases can manifest when a relativistic quantum particle moves cyclically along a loop in parameter space. The phase can be affected by the presence of a background field and can be accompanied by nontrivial topological features. The appearance of adiabatic geometric phases in momentum space is demonstrated for a Lorentz-violating Weyl fermion, where the role of the background is played by the coefficients for Lorentz violation. As explicit examples, the Berry curvature and the first Chern number are derived for two cases with large Lorentz violation, one incorporating <a:math xmlns:a="http://www.w3.org/1998/Math/MathML" display="inline"> <a:mrow> <a:mi>C</a:mi> <a:mi>P</a:mi> <a:mi>T</a:mi> </a:mrow> </a:math> violation and one preserving <c:math xmlns:c="http://www.w3.org/1998/Math/MathML" display="inline"> <c:mrow> <c:mi>C</c:mi> <c:mi>P</c:mi> <c:mi>T</c:mi> </c:mrow> </c:math> symmetry. Some alternative topological invariants are also obtained. In certain scenarios with large Lorentz violation, the physical vacuum is associated with a topological phase.

Physical review. D/Physical review. D.Vol. 113(1)
Universidade Federal do Maranhão (BR), Indiana University (US)
Openalex Percentile: Top 14%
Noncommutative and Quantum Gravity Theories
1.32
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