Summary
For a time-dependent quantum system, the instantaneous stationary Schrödinger equation is not covariant under gauge transformation. Therefore, the formal definition of the Berry phase may depend on the choice of mutually gauge-equivalent Hamiltonians. It is shown that the Lewis-Riesenfeld phase is manifestly gauge independent. The generalized time-dependent harmonic oscillator is used as an example to demonstrate this result.
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References
Shapere A. andWiclzek F.,Geometric Phase in Physics (World Scientific, Singapore) 1989.
Berry M. V.,Proc. R. Soc. London, Ser. A,392 (1984) 45.
Liang J. Q. andDing X. X.,Phys. Lett. A,153 (1991) 273.
Liang J. Q. andMüller-Kirstein H. J. W.,Ann. Phys. (N.Y.),219 (1992) 42.
Giavarini G., Gozzi E., Rohrlich D. andThacker W. D.,Phys. Lett. A,138 (1989) 235.
Kobe D. H.,J. Phys. A,23 (1990) 4249.
Lewis H. R. andRiesenfeld W. B.,J. Math. Phys.,10 (1969) 1458.
Jing-Bo Gao, Jing-Bo Xu andTie-Zhing Qian,Ann. Phys. (N.Y.),204 (1990) 235.
Berry M. V.,J. Phys. A,18 (1985) 5.
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Wei, LF., Liang, JQ. & Li, BZ. Gauge independence of Lewis-Riesenfeld phases. Nuov Cim B 110, 1357–1361 (1995). https://doi.org/10.1007/BF02723119
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DOI: https://doi.org/10.1007/BF02723119