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Physics Letters A

On the interpretation of the spinor phase change in a magnetic field in neutron interferometry

A. O. Barut, Mirjana Božić

Published Oct 1, 1990• 5 citations
Publisher
DOI
10.1016/0375-9601(90)90211-6

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Cambridge University Press eBooks•Dec 5, 2024•0 citations
If a spin-½ particle is placed in a constant uniform magnetic field for a time t during which, classically, the Larmor precession angle would be θ, then according to quantum mechanics the components of the spin part of the wave function undergo phase changes of ±θ/2. Hence, corresponding to a classical precession of 2π radians, there is a sign change of the spinor, whatever the initial polarization may be. Bernstein pointed out that this sign change can be observed by coherently splitting a fermion beam, subjecting one part to the magnetic field, and coherently recombining the parts. Evidently, the same interference effect can be achieved by subjecting the two parts of the beam to fields which would classically cause precessions of π radians in opposite senses. He noted advantages in studying neutral rather than charged particles, and outlined a proposal for an interferometry experiment with neutrons. The recent invention and application of a remarkable single-crystal neutron interferometer greatly increases the feasibility of observing the sign change. In the experiment of Ref. 3 a neutron beam is split, and the two parts follow paths of different elevations. The interference of the recombined parts exhibits the effect of gravitational potential difference between the two elevations. In the experiment which we propose, the paths could be kept at the same elevation, but phase differences would be produced by appropriate magnetic fields.
When a moving magnetic dipole enters a strong electric field the velocity of the magnet changes by a tiny amount. When a polarized, coherent beam of magnetic particles is split, the two parts passed through strong electric fields of opposite sign, then rejoined, interference patterns are observed due to the phase shift between the de Broglie waves of the two branches. Two recent, extremely delicate experiments, one using neutron interferometry and the second using F nuclei in TlF molecules, are reviewed and interpreted in this way. The fractional velocity change was 1 part in for the neutrons and 1 in for the TlF molecules. This explains the phase shift discussed by Aharonov and Casher and, contrary to their statement, is not equivalent to an Aharonov - Bohm effect. The latter requires that a de Broglie wave phase shift be produced by a vector potential in the absence of a field.
Spinor wave functions; classical Lagrangian and Hamiltonian of a charged particle in an electromagnetic field, and its quantum Hamiltonian; gauge invariance; spin magnetic moment in a uniform magnetic field; magnetic resonance; the Stern--Gerlach experiment; neutron interferometry and rotations of spinor wave functions; treatment of a particle in a uniform magnetic field with and without the inclusion of spin degrees of freedom; Ahronov--Bohm effect for a charged spinless particle confined in a cylindrical shell.