Spin-Rotation Coupling

November 29, 2016 10:39 am Published by

The effect of spin–rotation coupling, refereed to as SagnacMashhoon phase, has been measured by our group for the first time with neutrons in a polarometric experiment 1. The basis of the Sagnac effect lies in the influence of rotation on the phase of light passing through an interferometer. An inertial observer in the frame of an rotating interferometer of frequency , will observe that the wave vector of any radiation is . Thus a phase shift proportional to the scalar product of rotation frequency and area of the interferometer occurs. This phase shift can be extended to include the intrinsic spin of a quantum mechanical particle when replacing the orbital angular momentum, denoted as , by the total angular momentum . This results in an additional phase shift due to the spin-rotation coupling. In a paper published in 1998 2 Iranian born physicist Bahram Mashhoon proposed a neutron interferometric test of the Sagnac-Mashhoon phase, where a longitudinal polarized beam passes through a slowly rotating spin flipper placed in one arm, is proposed.

To describe the interaction of the spin of a free neutron in a magnetic field with angular velocity the PauliSchrödinger equation has to be solved for a particle propagating in − direction in a uniformly rotating magnetic field given by which gives  (see here for details of the derivation). The Pauli equation in a rotating magnetic field for plane waves is analytically solvable and in this particular case given by , where generates the rotation of the initial spin state  ,  which cab be expressed as  . The square of the magnitude of the rotation vector is given by a Pythagorean equation , where we used the definition of the Larmor frequency . The solution from above contains the coupling term and describes the evolution of the spin states for both the rotating and the static field (). Instead of a flip it is better to choose a multiple of in which case the dynamical part becomes disengaged from the spinor function and the phase shift can be attributed purely to a geometric phase.


If we prepare the incident beam in our polarimetric setup, which is depicted above (left), to be  the effect of the spin–rotation coupling can be seen when we choose to represent the initial state as a superposition of and states. The outcome of the spinor function in this set-up after a time and a rotation changes to initial state to  . The corresponding change in the polarization vector (from ) is . For higher precision and feasibility it is more convenient to keep constant and scan a relative phase, just like in an interferometer experiment where phase shifter scans are performed. The observed phase shift is plotted above (right) as a function of the frequency. A linear behaviour is clearly seen, as theoretically expected. All results are within the error bounds of the expected values predicted by the Pauli–Schrödinger equation. The final average contrast of 95.23(84)% confirms the high reliability of our measurement.


A scheme of the original proposed measurement for spin- particles is shown aside. Polarized neutrons initially propagating in +y− direction are split into two arms of an interferometer of which one contains a static spin flipper and the other one a rotating spin flipper whose angular velocity vector is parallel to the initial neutron spin. The first proposals of the experiment suggested the use of a mechanically rotating coil, analogous to the HWP in the optical interferometer scheme, but it was pointed out later that this situation is physically equivalent to a static quadrate recoil producing a rotating magnetic field . The experimental realization of the interferometric setup is an ongoing project and foreseen to be achieved in 2018.

1. B. Demirel, S. Sponar, and Y. Hasegawa, New. J. of Phys. A 17, 023065 (2015)

2. B. Mashhoon, R. Neutze, M. Hannah, and G. E. Stedman, Phys. Lett. A 249, 161 (1998)