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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Proof that B ⊥ |p + ,R ⊥ = 0 ⊥ 〉 = 0<br />
↩→<br />
Use<br />
e −iv ⊥·B ⊥<br />
|p + ,p ⊥ , λ〉 = |p + ,p ⊥ + p + v ⊥ , λ〉<br />
∫<br />
∫<br />
e −iv ⊥·B ⊥<br />
d 2 p ⊥ |p + ,p ⊥ , λ〉 = d 2 p ⊥ |p + ,p ⊥ , λ〉<br />
↩→<br />
B ⊥<br />
∫<br />
d 2 p ⊥ |p + ,p ⊥ , λ〉 = 0<br />
back<br />
<strong>Position</strong> <strong>Space</strong> <strong>Interpretation</strong> <strong>for</strong> <strong>Generalized</strong> <strong>Parton</strong> <strong>Distributions</strong> – p.47/55