Summary
We show that non-relativistic quantum mechanics is invariant under a local gauge transformation even in the absence of any external electromagnetic field, provided we do not exclude the arbitrary phase factor in the coordinate representation of the wave vector. A generalised, gauge-invariant form of the Schroedinger equation, as well as gauge-invariant canonical momentum and Hamiltonian operators are introduced. In the presence of an electromagnetic field, the new Hamiltonian operator turns out to be identical with the «energy operator» introduced by K. H. Yang. A previously derived result, proving thenon-equivalence of the minimal-coupling and the multipolar forms of matter-radiation interaction, is shown to follow as a corollary.
References
L. H. Ryder:Quantum Field Theory (Cambridge University Press, Cambridge, 1984).
R. Mills:Am. J. Phys.,57, 493 (1989).
D. H. Kobe:Am. J. Phys.,46, 342 (1978).
P. A. M. Dirac:The Principles of Quantum Mechanics, 4th edition (1967). In sect. 22, eq. (35) Dirac shows that the quantum condition [q k, pk]=iħ definesp k only to within an additive arbitrary partial (space) derivative, which corresponds to an arbitrary phase factor in the coordinate representation.
P. A. M. Dirac:The Principles of Quantum Mechanics, 4th edition (1967). In sect. 27, eq. (4) Dirac shows that the linear-superposition principle and the requirement of unitarity determine the time derivative only to within an additive pure imaginary number (corresponding to an arbitrary phase factor).
K. H. Yang:Ann. Phys. (N.Y.),101, 62 (1976).
D. K. Kobe andA. L. Smirl:Am. J. Phys.,46, 624 (1978).
T. K. Rai Dastidar: submitted toPhis. Rev. Lett.
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Rai Dastidar, T.K., Dastidar, K.R. Gauge Invariance in non-relativistic quantum mechanics. Nuov Cim B 109, 1115–1118 (1994). https://doi.org/10.1007/BF02723234
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DOI: https://doi.org/10.1007/BF02723234