Abstract
We derive electromagnetomotive force fields for charged particlesmoving in a rotating Hall sample, satisfying a twofold U(1) gaugeinvariance principle. It is then argued that the phase coherenceproperty of quantization of the line integral of total collectiveparticle momentum into multiples of Planck's quantum of action issolely responsible for quantization in the Hall state. As aconsequence, the height of the Hall quantization steps should remaininvariant in a rapidly rotating Hall probe. Quantum Hall particleconductivities do not depend on charge and mass of the electron, andare quantized in units of the inverse of Planck's action quantum.
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