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42 Chapter 5. The Eikonal Final State Cross section [mb] 10 2 10 σ tot σ el pp Cross section [mb] 10 2 10 σ tot σ el pn 10 -1 1 10 Proton momentum [GeV/c] Figure 5.5 Total and elastic cross sections for pp and pn scattering as a function of the lab proton momentum. The data were taken from Ref. [64].
5.4. The Glauber Approach 43 Figure 5.6 This picture, that was taken from Ref. [6] shows the absolute contributions from the spin-dependent terms to the differential pp scattering cross section at small angles.
Page 1: De Eikonale Benadering in Dirac-Ge
Page 4 and 5: ii CONTENTS 10 Conclusion and Outlo
Page 6 and 7: 2 Chapter 1. Introduction the stron
Page 8 and 9: 4 Chapter 1. Introduction a wide Q
Page 10 and 11: 6 Chapter 2. Reaction Observables a
Page 12 and 13: 8 Chapter 2. Reaction Observables a
Page 14 and 15: 10 Chapter 2. Reaction Observables
Page 17 and 18: Chapter 3 Relativistic Bound State
Page 19 and 20: 3.1. Formalism 15 content to the me
Page 21 and 22: 3.2. Results 17 12 C 16 O proton ne
Page 23 and 24: 3.2. Results 19 have verified that
Page 25 and 26: 3.2. Results 21 where the positive
Page 27: 3.2. Results 23 Figure 3.4 Nucleon
Page 30 and 31: 26 Chapter 4. Off-Shell Electron-Pr
Page 32 and 33: 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: 5.4. The Glauber Approach 41 where
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 98 and 99:
94 Chapter 8. Relativistic Effects
Page 100 and 101:
Page 102 and 103:
Page 104 and 105:
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
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Page 121 and 122:
Page 123 and 124:
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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