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80 Chapter 7. Off-Shell Ambiguities R L [fm 3 ] R T [fm 3 ] 30 20 10 0 30 20 10 0 1 CC2 DON WT CC1 R TT [fm 3 ] R TL [fm 3 ] 0.5 0 -0.5 -1 10 0 -10 -20 -30 -40 0 100 200 300 100 200 300 p m [MeV/c] p m [MeV/c] Figure 7.2 The different structure functions versus missing momentum for 1p 3/2 knockout from 16 O in the kinematics of Ref. [15]. The calculations in the left column imposed current conservation by replacing the longitudinal component of the vector current operator (Eq. (4.5)), while for the results in the right column the charge density operator was modified according to Eq. (4.7). The curves refer to the different off-shell prescriptions as they were introduced in Sec. 4.
81 R L [fm 3 ] R T [fm 3 ] R TT [fm 3 ] 30 20 10 0 30 20 10 0 1 0.8 0.6 0.4 0.2 0 10 CC2 DON WT CC1 R TL [fm 3 ] 0 -10 -20 0 100 200 300 100 200 300 p m [MeV/c] p m [MeV/c] Figure 7.3 Same as in Fig. 7.2, but for 1p 1/2 knockout.
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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
Page 35 and 36: Chapter 5 The Eikonal Final State I
Page 37 and 38: 5.2. A Consistent Approach to Final
Page 39 and 40: 5.2. A Consistent Approach to Final
Page 41 and 42: 5.3. Optical Potentials and the Eik
Page 43 and 44: 5.3. Optical Potentials and the Eik
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
Page 53 and 54: 5.4. The Glauber Approach 49 1250 1
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: 79 momentum region. Since these exc
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 and 94: 89 The relation obtained in Eq. (7.
Page 95: 91 A LT 1 0.5 0 OMEA (CC2) OMEA (CC
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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