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90 Chapter 7. Off-Shell Ambiguities 2 1 A LT A LT A LT 0 -1 -2 1 0.5 0 -0.5 -1 1 0.5 0 -0.5 -1 1 0.5 Q 2 = 1.08 (GeV) 2 Q 2 = 3.11 (GeV) 2 Q 2 = 6.74 (GeV) 2 A LT 0 -0.5 Q 2 = 12.2 (GeV) 2 -1 0 100 200 300 400 500 p m Figure 7.8 The left-right asymmetry for the 12 C(e, e ′ p) 11 B(1p −1 3/2 ) reaction at four different energies, calculated in a Glauber framework. The solid (dashed) curves are obtained with the CC2 (CC1) current operator.
91 A LT 1 0.5 0 OMEA (CC2) OMEA (CC1) RMSGA (CC2) RMSGA (CC1) -0.5 -1 1 0.5 p 3/2 p 1/2 A LT 0 -0.5 -1 0 50 100 150 200 250 300 350 400 450 500 p m [MeV/c] Figure 7.9 The left-right asymmetry A LT for both 1p 3/2 and 1p 1/2 knockout from 16 O in the kinematics of Ref. [15].
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De Eikonale Benadering in Dirac-Ge
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ii CONTENTS 10 Conclusion and Outlo
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2 Chapter 1. Introduction the stron
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4 Chapter 1. Introduction a wide Q
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6 Chapter 2. Reaction Observables a
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8 Chapter 2. Reaction Observables a
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10 Chapter 2. Reaction Observables
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Chapter 3 Relativistic Bound State
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3.1. Formalism 15 content to the me
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3.2. Results 17 12 C 16 O proton ne
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3.2. Results 19 have verified that
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3.2. Results 21 where the positive
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3.2. Results 23 Figure 3.4 Nucleon
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26 Chapter 4. Off-Shell Electron-Pr
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28 Chapter 4. Off-Shell Electron-Pr
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Chapter 5 The Eikonal Final State I
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5.2. A Consistent Approach to Final
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5.2. A Consistent Approach to Final
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5.3. Optical Potentials and the Eik
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Page 45 and 46: 5.4. The Glauber Approach 41 where
Page 47 and 48: 5.4. The Glauber Approach 43 Figure
Page 49 and 50: 5.4. The Glauber Approach 45 shape
Page 51 and 52: 5.4. The Glauber Approach 47 ε pp
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Page 55 and 56: 5.4. The Glauber Approach 51 so tha
Page 57 and 58: 5.4. The Glauber Approach 53 1.2 1
Page 59 and 60: 5.5. Higher Order Eikonal Correctio
Page 61 and 62: Chapter 6 Final State Interactions
Page 63 and 64: 6.1. 16 O(e, e ′ p) 15 N 59 d 5
Page 65 and 66: 6.1. 16 O(e, e ′ p) 15 N 61 ρ [(
Page 67 and 68: 6.1. 16 O(e, e ′ p) 15 N 63 12 C(
Page 69 and 70: 6.1. 16 O(e, e ′ p) 15 N 65 CEA w
Page 71 and 72: 6.1. 16 O(e, e ′ p) 15 N 67 Figur
Page 73 and 74: 6.1. 16 O(e, e ′ p) 15 N 69 0.4 0
Page 75 and 76: 6.2. 12 C(e, e ′ p) 11 B 71 0 -0.
Page 77 and 78: 6.2. 12 C(e, e ′ p) 11 B 73 ρ [(
Page 79 and 80: 6.2. 12 C(e, e ′ p) 11 B 75 P n P
Page 81 and 82: Chapter 7 Off-Shell Ambiguities A m
Page 83 and 84: 79 momentum region. Since these exc
Page 85 and 86: 81 R L [fm 3 ] R T [fm 3 ] R TT [fm
Page 87 and 88: 83 R L [fm 3 ] R T [fm 3 ] 0.04 0.0
Page 89 and 90: 85 manner, we will from here on onl
Page 91 and 92: 87 R CC1/CC2 R CC1/CC2 R CC1/CC2 R
Page 93: 89 The relation obtained in Eq. (7.
Page 98 and 99: 94 Chapter 8. Relativistic Effects
Page 107 and 108: Chapter 9 Nuclear Transparency The
Page 109 and 110: 9.1. Theoretical Background 105 Req
Page 111 and 112: 9.1. Theoretical Background 107 few
Page 113 and 114: 9.2. Review of Experimental Results
Page 115 and 116: 9.2. Review of Experimental Results
Page 117 and 118: 9.3. Nuclear Transparency Calculati
Page 125 and 126: Chapter 10 Conclusion and Outlook I
Page 127 and 128: 123 with increasing Q 2 the uncerta
Page 129 and 130: Bibliography [1] V. Pandharipande,
Page 131 and 132: Bibliography 127 [42] J. Kelly, Phy
Page 133 and 134: Bibliography 129 [85] A. Saha, W. B
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