Spin particles not in a magnetic field

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Determining the magnetic moment of spin particles in a zero magnetic field (\vec{B} = 0) presents challenges, as traditional methods may not yield conclusive results. The Aharonov-Bohm effect suggests that it is possible to create a region where the magnetic field is absent, yet a vector potential exists, allowing for interference measurements. Additionally, accelerating the particles could enable the measurement of electric polarization, as moving magnetization can manifest as polarization. These methods provide potential avenues for investigating the properties of spin particles in a zero magnetic field. Overall, while direct measurement may be difficult, alternative approaches could offer insights into their magnetic moments.
denjay
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If spin particles are in \vec{B} = 0, then is it impossible to determine their magnetic moment at a given time given any investigative method?
 
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I think you could use something like Aharonov-Bohm: create a region where B is 0 but A is not and interfere. Alternatively, you could accelerate these particles and measure their electric polarization (a moving magnetization becomes a polarization)
 
Thread 'Motional EMF in Faraday disc, co-rotating magnet axial mean flux'
So here is the motional EMF formula. Now I understand the standard Faraday paradox that an axis symmetric field source (like a speaker motor ring magnet) has a magnetic field that is frame invariant under rotation around axis of symmetry. The field is static whether you rotate the magnet or not. So far so good. What puzzles me is this , there is a term average magnetic flux or "azimuthal mean" , this term describes the average magnetic field through the area swept by the rotating Faraday...
It may be shown from the equations of electromagnetism, by James Clerk Maxwell in the 1860’s, that the speed of light in the vacuum of free space is related to electric permittivity (ϵ) and magnetic permeability (μ) by the equation: c=1/√( μ ϵ ) . This value is a constant for the vacuum of free space and is independent of the motion of the observer. It was this fact, in part, that led Albert Einstein to Special Relativity.

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