Position Space Interpretation for Generalized Parton Distributions
Position Space Interpretation for Generalized Parton Distributions
Position Space Interpretation for Generalized Parton Distributions
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physical origin <strong>for</strong> ⊥ distortion<br />
anomalous magnetic moment coupling in Dirac eq:<br />
iκ<br />
2M ¯qσµν qF µν =<br />
↩→<br />
iκ<br />
]<br />
[¯qσ ij qF ij + 2¯qσ 0ν qF 0ν<br />
2M<br />
[<br />
]<br />
κ ⃗σ · ⃗B + (σ × ⃗p) · ⃗E<br />
back<br />
moving spin 1 2<br />
particle with anomalous magnetic moment has<br />
(viewed from observer at rest) transverse electric dipole<br />
moment, which is perp. to both its spin and momentum.<br />
↩→ ⊥ distortion of q(x,b ⊥ ) is consequence of Lorentz invariance<br />
<strong>for</strong> Dirac particle with anomalous magnetic moment.<br />
<strong>Position</strong> <strong>Space</strong> <strong>Interpretation</strong> <strong>for</strong> <strong>Generalized</strong> <strong>Parton</strong> <strong>Distributions</strong> – p.54/55