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Geometric phase in eigenspace evolution of invariant and adiabatic action operators
1Department of Physics, The University of Hong Kong, Pokfulam Road, Hong Kong, China.
Physical Review Letters
|August 11, 2005
Summary
This study generalizes geometric phase theory to N-fold degenerate eigenspaces, revealing holonomy that captures geometric state evolution, even for non-cyclic processes.
Area of Science:
- Quantum mechanics
- Differential geometry
- Topology
Background:
- Geometric phase, also known as Berry phase, describes phase changes in quantum systems undergoing cyclic evolution.
- Degenerate systems present unique challenges in defining and understanding geometric phases.
- The Stiefel and Grassmann manifolds are fundamental in understanding vector bundles and holonomy.
Purpose of the Study:
- To generalize the theory of geometric phase to N-fold degenerate eigenspaces.
- To interpret the geometric phase as a holonomy derived from a universal U(N) bundle.
- To formulate a rigorous theory for geometric phase in adiabatic evolution of eigenspaces.
Main Methods:
- Generalization of geometric phase theory for degenerate eigenspaces.
- Interpretation of geometric phase as holonomy over a Grassmann manifold.
- Formulation of a rigorous theory for adiabatic evolution using pullback U(N) bundles.
Main Results:
- The geometric phase for N-fold degenerate eigenspaces is identified as a holonomy from the universal Stiefel U(N) bundle.
- This holonomy accurately captures the geometric features of state evolution, irrespective of cyclicity.
- A theory for geometric phase in adiabatic evolution of eigenspaces is established, linked to a pullback U(N) bundle.
Conclusions:
- The generalized geometric phase provides a robust framework for understanding state evolution in degenerate quantum systems.
- Holonomy offers a powerful geometric interpretation of phase evolution, extending beyond cyclic processes.
- The developed theory is crucial for analyzing complex quantum dynamics and geometric properties.