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What is the four-vector related to electric and magnetic dipole moment?
The discussion centers on the four-vector representation of electric and magnetic dipole moments, specifically addressing the electromagnetic tensor ##F^{\mu\nu}## and its relationship to the dipole moments represented by the anti-symmetric rank 2 tensor ##M^{\mu\nu}##. It is established that there is no four-vector that describes dipole moments; instead, they form an anti-symmetric rank 2 tensor. The interaction term proportional to ##F_{\mu\nu}M^{\mu\nu}## can be included in the Lagrangian density to describe dipole interactions. The conversation also touches on the implications of restricting to the ##SO(3)## subgroup of spatial rotations.
PREREQUISITESThis discussion is beneficial for theoretical physicists, students of electromagnetism, and researchers interested in advanced topics related to dipole moments and tensor analysis in field theory.
It is not the field tensor ##F^{\mu\nu}##, it is a separate anti-symmetric rank 2 tensor ##M^{\mu\nu}##. It is true that it is constructed from the electric and magnetic dipole moments in the same way ##F## is constructed from the electric and magnetic fields. You can then put an interaction term proportional to ##F_{\mu\nu}M^{\mu\nu}## into the Lagrangian density, effectively describing the dipole interactions.sweet springs said:I have never think about that. How about electromagnetic tensor ##F^{\mu\nu}## represented by ##\mathbf{P}## and ##\mathbf{M}## instead of ##\mathbf{E}## and ##\mathbf{B}## ? I am not sure at all ##\epsilon## and ##\mu## are constant in Lorentz transformation.
Best.