Non-Abelian Geometric Phases Carried by the Spin Fluctuation Tensor
arXiv:1702.08564 · doi:10.1063/1.5018188
Abstract
The expectation values of the first and second moments of the quantum mechanical spin operator can be used to define a spin vector and spin fluctuation tensor, respectively. The former is a vector inside the unit ball in three space, while the latter is represented by an ellipsoid in three space. They are both experimentally accessible in many physical systems. By considering transport of the spin vector along loops in the unit ball it is shown that the spin fluctuation tensor picks up geometric phase information. For the physically important case of spin one, the geometric phase is formulated in terms of an SO(3) operator. Loops defined in the unit ball fall into two classes: those which do not pass through the origin and those which pass through the origin. The former class of loops subtend a well defined solid angle at the origin while the latter do not and the corresponding geometric phase is non-Abelian. To deal with both classes, a notion of generalized solid angle is introduced, which helps to clarify the interpretation of the geometric phase information. The experimental systems that can be used to observe this geometric phase are also discussed.
27 pages, 7 figures
References in corpus (5)
- Geometric phases in quantum information
- Quantum geometric phase in Majorana's stellar representation: Mapping onto a many-body Aharonov-Bohm phase
- Characterizing the energy gap and demonstrating an adiabatic quench in an interacting spin system
- Geometric Phases for Mixed States of the Kitaev Chain
- Exploring Non-Abelian Geometric Phases in Spin-1 Ultracold Atoms
Cited by in corpus (7)
- Exploring Non-Abelian Geometric Phases in Spin-1 Ultracold Atoms
- Observation of spin-tensor induced topological phase transitions of triply degenerate points with a trapped ion
- Quantum spiral spin-tensor magnetism
- Spin-tensor Meissner currents of ultracold bosonic gas in an optical lattice
- Synthetic Hall tube of interacting fermions
- Robust Weyl points in a 1D superlattice with transverse spin-orbit coupling
- A new light on the FKMM invariant and its consequences