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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

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