Abstract:The Fourier transform of generalized parton distribution functions at ξ = 0 describes the distribution of partons in the transverse plane. The physical significance of these impact parameter dependent parton distribution functions is discussed. In particular, it is shown that they satisfy positivity constraints which justify their physical interpretation as a probability density. The generalized parton distribution H is related to the impact parameter distribution of unpolarized quarks for an unpolarized nucle… Show more
“…This interpretation becomes even more transparent after switching to an impact parameter representation [8,9,10,11] …”
Section: Initial (Final) State Interactions and Transverse Spin Amentioning
confidence: 99%
“…If the target is polarized in the x-direction in the infinite momentum frame, the unpolarized impact parameter dependent PDFs for flavor q reads [11] …”
Section: Simple Models For the Final State Interactionsmentioning
We illustrate how an axial asymmetry in impact parameter dependent parton distributions can give rise to an axial asymmetry for the transverse momentum of the leading quark in the photoproduction of hadrons. The effect is related to the asymmetry originating from the Wilson-line phase factor in gauge invariant Sivers distributions. The single spin asymmetry arising from the asymmetry of the impact parameter dependent parton distributions is shown to exhibit a pure sin φ dependence.
“…This interpretation becomes even more transparent after switching to an impact parameter representation [8,9,10,11] …”
Section: Initial (Final) State Interactions and Transverse Spin Amentioning
confidence: 99%
“…If the target is polarized in the x-direction in the infinite momentum frame, the unpolarized impact parameter dependent PDFs for flavor q reads [11] …”
Section: Simple Models For the Final State Interactionsmentioning
We illustrate how an axial asymmetry in impact parameter dependent parton distributions can give rise to an axial asymmetry for the transverse momentum of the leading quark in the photoproduction of hadrons. The effect is related to the asymmetry originating from the Wilson-line phase factor in gauge invariant Sivers distributions. The single spin asymmetry arising from the asymmetry of the impact parameter dependent parton distributions is shown to exhibit a pure sin φ dependence.
“…In the limit where the momentum transfer ∆ to the nucleon is purely transverse, i.e. ∆ = (0, ∆ ⊥ ) and ξ = 0, GPDs regain a probabilistic interpretation [4]. In the 2 forward limit (∆ = 0), these distributions reduce to the Feynman parton distributions.…”
Section: Matrix Elements Of the Light Cone Operatormentioning
confidence: 99%
“…Generalized parton distributions (GPDs) [1,2] describe the coherence of two different hadron wave functions ψ † (x + ξ/2) ψ(x − ξ/2), one where the parton carries fractional momentum x + ξ/2 and one where this fraction is x − ξ/2, from which further information on the transverse distribution of partons can be drawn [3,4]. In the limit where the momentum transfer ∆ to the nucleon is purely transverse, i.e.…”
Section: Matrix Elements Of the Light Cone Operatormentioning
We present here the latest results from the QCDSF collaboration for (moments of) structure functions and generalized form factors in full QCD with N f = 2 O(a)-improved Wilson fermions based on simulations closer to the chiral and continuum limit.
“…Recent calculations using the GPD's have provided insight into the transverse distribution of partons within the nucleon [62,2]. GPDs using form factor input have also provided new methods of calculating the charge distributions of nucleons [63,64,65] without resorting to the Breit frame transformations.…”
Section: Generalized Parton Distributionsmentioning
Knowledge of the electric and magnetic elastic form factors of the nucleon is essential for an understanding of nucleon structure. Of the form factors, the electric form factor of the neutron has been measured over the smallest range in Q 2 and with the lowest precision. Jefferson Lab experiment 02-013 used a novel new polarized 3 He target to nearly double the range of momentum transfer in which the neutron form factor has been studied and to measure it with much higher precision. Polarized electrons were scattered off this target, and both the scattered electron and neutron were detected. G n E was measured to be 0.0242 ± 0.0020(stat) ± 0.0061(sys) and 0.0247 ± 0.0029(stat) ± 0.0031(sys) at Q 2 = 1.7 and 2.5 GeV 2 , respectively.
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