Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

Physics Letters A

Nonadiabatic geometric spinor phase in rotating magnetic fields

Apoorva G. Wagh, Veer Chand Rakhecha

Published Oct 1, 1992• 31 citations
Publisher
DOI
10.1016/0375-9601(92)90775-h

Related papers

Geometric Phase Associated with Spinor Rotations

Apoorva G. Wagh, Veer Chand Rakhecha

Springer eBooks•Jan 1, 1993•4 citations

Nonadiabatic dynamics and geometric phase of an ultrafast rotating electron spin

Xing-Yan Chen, Tongcang Li, Zhang‐qi Yin

arXiv:1811.01641•中国科学通报:英文版•Feb 26, 2019•25 citations

Geometric phase of spin-1 in a rotating magnetic field

张晓燕, 胡连

Chinese Optics Letters•Jan 1, 2006•0 citations

Interacting spin pairs in rotational magnetic fields and geometric phase

Xin Li

Physics Letters A•May 30, 2008•9 citations

Dynamics and geometric phase of two spins with exchange coupling in a rotating magnetic field

Chang-Tan Xu, J.-Q. Liang

Physics Letters A•Mar 30, 2006•9 citations

Exact fixed-angle spinor evolutions via the rotating-frame formalism

Apoorva G. Wagh, Veer Chand Rakhecha

We examine spinor evolutions in a general time-dependent magnetic field B. We derive a condition the B variation must satisfy in order that the effective field direction ${\mathbf{r}\mathbf{\^{}}}_{\mathrm{B}}^{\ensuremath{'}}$ for a frame rotating with B becomes stationary in that frame. This condition is both sufficient and necessary for B to bring about a spinor evolution which exactly maintains a fixed angle between the spin and B. The adiabatic evolution used by Berry is just a special case, albeit only approximate, of these fixed-angle evolutions. To the other extreme of the fixed-angle evolutions, the nontrivial parallel transportation occurs, which is exact, necessarily nonadiabatic, and yields a pure geometric phase. Hence an experiment aimed at observing the geometric phase should seek to effect not an adiabatic evolution but a parallel transportation.

Physical Review A•Sep 1, 1993•37 citations
We examine spinor evolutions in a general time-dependent magnetic field B. We derive a condition the B variation must satisfy in order that the effective field direction ${\mathbf{r}\mathbf{\^{}}}_{\mathrm{B}}^{\ensuremath{'}}$ for a frame rotating with B becomes stationary in that frame. This condition is both sufficient and necessary for B to bring about a spinor evolution which exactly maintains a fixed angle between the spin and B. The adiabatic evolution used by Berry is just a special case, albeit only approximate, of these fixed-angle evolutions. To the other extreme of the fixed-angle evolutions, the nontrivial parallel transportation occurs, which is exact, necessarily nonadiabatic, and yields a pure geometric phase. Hence an experiment aimed at observing the geometric phase should seek to effect not an adiabatic evolution but a parallel transportation.