Spin rotation as an element of polarization experiments on elastic electron-proton scattering
arXiv:0904.1671 · doi:10.1016/j.physleta.2010.01.009
Abstract
The validity of some rules in the classical theory of spin, which are followed by the Bargmann--Michel--Telegdi formula for a relativistic particle spin rotation in a constant homogeneous magnetic field, is analyzed. In the framework of the quantum theory, we give examples where these rules are violated. Consequences for polarization experiments are discussed.
9 pages, no figures, published version
References in corpus (12)
- Measurement of GEp/GMp in ep -> ep to Q2 = 5.6 GeV2
- Proton elastic form factor ratios to = 3.5 GeV by polarization transfer
- How to reconcile the Rosenbluth and the polarization transfer method in the measurement of the proton form factors
- Precision Rosenbluth measurement of the proton elastic form factors
- Two-photon exchange in elastic electron-nucleon scattering
- Measurements of electron-proton elastic cross sections for
- The two-photon exchange contribution to elastic electron-nucleon scattering at large momentum transfer
- How well do we know the electromagnetic form factors of the proton?
- resonance contribution to two-photon exchange in electron-proton scattering
- Proton G_E/G_M from beam-target asymmetry
- Contribution of spin 1/2 and 3/2 resonances to two-photon exchange effects in elastic electron-proton scattering
- Electromagnetic form factors and polarizations of non-Dirac particles with rest spin 1/2
Cited by in corpus (4)
- Lagrangian for Frenkel electron and position's non-commutativity due to spin
- Variational problem for the Frenkel and the Bargmann-Michel-Telegdi (BMT) equations
- Electromagnetic properties of non-Dirac particles with rest spin 1/2
- Magnetic moment operator of non-Dirac particles and some elements of polarization -experiments