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Languages : en
Pages : 0
Book Description
Measurement of Deeply Virtual Compton Scattering at HERA
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Category :
Languages : en
Pages : 0
Book Description
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Category :
Languages : en
Pages : 0
Book Description
Measurement of Deeply Virtual Compton Scattering and Its T-dependence at HERA
Author:
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Category :
Languages : en
Pages : 21
Book Description
Publisher:
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Category :
Languages : en
Pages : 21
Book Description
Measurement of Deeply Virtual Compton Scattering at HERA
Author: Rainer Stamen
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Languages : en
Pages : 99
Book Description
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Category :
Languages : en
Pages : 99
Book Description
Measurement of Deeply Virtual Compton Scattering Using the ZEUS Detector at HERA
Author: Iwona Grabowska-Bold
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Languages : en
Pages :
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Languages : en
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Book Description
A Measurement of the Q2-, W- and T-dependences of Deeply Virtual Compton Scattering at HERA
Author: ZEUS Collaboration
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Languages : en
Pages : 18
Book Description
Publisher:
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Category :
Languages : en
Pages : 18
Book Description
Measurement of Deeply Virtual Compton Scattering Cross Sections with the ZEUS Detector at HERA
Author: Amir Stern
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Languages : en
Pages : 123
Book Description
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Category :
Languages : en
Pages : 123
Book Description
Deeply Virtual Compton Scattering at 6 GeV.
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Languages : en
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Book Description
The authors propose a measurement of the Deep Virtual Compton Scattering process (DVCS) ep → ep[gamma] in Hall A at Jefferson Lab with a 6 GeV beam. The authors are able to explore the onset of Q2 scaling, by measuring a beam helicity asymmetry for Q2 ranging from 1.5 to 2.5 GeV2 at x{sub B} ≈ 0.35. At this kinematics, the asymmetry is dominated by the DVCS Bethe-Heitler (BH) interference, which is proportional to the imaginary part of the DVCS amplitude amplified by the full magnitude of the BH amplitude. The imaginary part of the DVCS amplitude is expected to scale early. Indeed, the imaginary part of the forward Compton amplitude measured in deep inelastic scattering (via the optical theorem) scales at Q2 as low as 1 GeV2. If the scaling regime is reached, they make an 8% measurement of the skewed parton distributions (SPD) contributing to the DVCS amplitude. Also, this experiment allows them to separately estimate the size of the higher-twist effects, since they are only suppressed by an additional factor 1/Q compared to the leading-twist term, and have a different angular dependence. They use a polarized electron beam and detect the scattered electron in the HRSe, the real photon in an electromagnetic calorimeter (under construction) and the recoil proton in a shielded scintillator array (to be constructed). This allows them to determine the difference in cross-sections for electrons of opposite helicities. This observable is directly linked to the SPD's. The authors estimate that 25 days of beam (600 hours) are needed to achieve this goal.
Publisher:
ISBN:
Category :
Languages : en
Pages :
Book Description
The authors propose a measurement of the Deep Virtual Compton Scattering process (DVCS) ep → ep[gamma] in Hall A at Jefferson Lab with a 6 GeV beam. The authors are able to explore the onset of Q2 scaling, by measuring a beam helicity asymmetry for Q2 ranging from 1.5 to 2.5 GeV2 at x{sub B} ≈ 0.35. At this kinematics, the asymmetry is dominated by the DVCS Bethe-Heitler (BH) interference, which is proportional to the imaginary part of the DVCS amplitude amplified by the full magnitude of the BH amplitude. The imaginary part of the DVCS amplitude is expected to scale early. Indeed, the imaginary part of the forward Compton amplitude measured in deep inelastic scattering (via the optical theorem) scales at Q2 as low as 1 GeV2. If the scaling regime is reached, they make an 8% measurement of the skewed parton distributions (SPD) contributing to the DVCS amplitude. Also, this experiment allows them to separately estimate the size of the higher-twist effects, since they are only suppressed by an additional factor 1/Q compared to the leading-twist term, and have a different angular dependence. They use a polarized electron beam and detect the scattered electron in the HRSe, the real photon in an electromagnetic calorimeter (under construction) and the recoil proton in a shielded scintillator array (to be constructed). This allows them to determine the difference in cross-sections for electrons of opposite helicities. This observable is directly linked to the SPD's. The authors estimate that 25 days of beam (600 hours) are needed to achieve this goal.
Future Measurements of Deeply Virtual Compton Scattering at HERMES
Author:
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Category :
Languages : en
Pages : 12
Book Description
Publisher:
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Languages : en
Pages : 12
Book Description
Future Measurements of Deeply Virtual Compton Scattering
Author: V. A. Korotkov
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Languages : en
Pages : 12
Book Description
Publisher:
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Category :
Languages : en
Pages : 12
Book Description
Deeply Virtual Compton Scattering at JLab Hall A.
Author:
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Category :
Languages : en
Pages :
Book Description
The deeply virtual Compton scattering reaction has been investigated in the Hall A of the Jefferson Laboratory by measuring longitudinally polarized (e, e'gamma) cross sections, in the valence quark region, for protons and neutrons. In the proton channel, experimental results strongly support the factorization of the cross section at Q2 as low as 2 GeV2, opening the path to systematic measurements of generalized parton distributions (GPDs). In the neutron case, preliminary data show sensitivity to the angular momentum of quarks.
Publisher:
ISBN:
Category :
Languages : en
Pages :
Book Description
The deeply virtual Compton scattering reaction has been investigated in the Hall A of the Jefferson Laboratory by measuring longitudinally polarized (e, e'gamma) cross sections, in the valence quark region, for protons and neutrons. In the proton channel, experimental results strongly support the factorization of the cross section at Q2 as low as 2 GeV2, opening the path to systematic measurements of generalized parton distributions (GPDs). In the neutron case, preliminary data show sensitivity to the angular momentum of quarks.