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94 Chapter 8. Relativistic Effects R R R R L [fm 3 T [fm 3 TL [fm 3 TT [fm 3 ] ] ] ] 8 6 4 2 0 20 15 10 5 0 0.5 0 -0.5 -1 -1.5 -2 0.2 0.1 0 -0.1 0 200 400 s 1/2 p 3/2 p m [MeV/c] 0 200 400 p m [MeV/c] Figure 8.1 The unpolarized structure functions for the 12 C(e, e ′ p) knockout experiment of Ref. [98]. The solid line presents fully relativistic eikonal calculations with Cooper optical potentials, while for the dashed results, the coupling between the lower components of the bound and scattering state has been reduced to zero.
95 σ Rel/Non-Rel 1.2 1 CC1 CC2 1.1 R L Rel/Non-Rel 1 0.9 1.01 R T Rel/Non-Rel 1 R TT Rel/Non-Rel 0.99 3 2 1 0 R TL Rel/Non-Rel 4 2 0 0 2 4 6 8 10 12 14 16 18 20 Q 2 [(GeV/c) 2 ] Figure 8.2 The Q 2 dependence of the sensitivity of the (e,e’p) structure functions to dynamical relativistic effects. The curves show for 1p 3/2 knockout from 12 C the ratio of the fully relativistic results to the predictions when the coupling between the lower components has been omitted. These calculations were performed in the maximum of the 1p 3/2 momentum distribution (p m ≃ 100 MeV/c). Calculations are performed for both the CC1 and CC2 current operator in the Glauber framework.
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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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5.3. Optical Potentials and the Eik
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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 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 and 94: 89 The relation obtained in Eq. (7.
Page 95: 91 A LT 1 0.5 0 OMEA (CC2) OMEA (CC
Page 100 and 101: 96 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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