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1 Microscopic Cluster Models |
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1 | (66) |
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1 | (4) |
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1.2 Choice of the Nucleon-Nucleon Interaction |
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5 | (2) |
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1.3 The Resonating Group Method |
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7 | (4) |
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7 | (3) |
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1.3.2 Example: Overlap Kernel of the α + n System |
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10 | (1) |
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1.4 The Generator Coordinate Method |
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11 | (6) |
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11 | (1) |
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1.4.2 Slater Determinants and GCM Basis Functions |
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12 | (3) |
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1.4.3 Equivalence Between RGM and GCM |
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15 | (1) |
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1.4.4 Two-Cluster Angular-Momentum Projection |
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16 | (1) |
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1.5 Matrix Elements Between Slater Determinants |
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17 | (11) |
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1.5.1 General Presentation |
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17 | (3) |
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1.5.2 Spin and Isospin Factorization |
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20 | (2) |
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1.5.3 The Spin-Orbit Interaction |
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22 | (1) |
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1.5.4 Matrix Elements Between Individual Orbitals |
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22 | (1) |
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1.5.5 Example: α + n Overlap Kernel |
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23 | (2) |
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1.5.6 GCM Kernels of α + N Systems |
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25 | (3) |
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1.6 Approximations of the RGM |
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28 | (4) |
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1.6.1 Eigenvalues of the Overlap Kernel |
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28 | (2) |
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1.6.2 Reformulation of the RGM Equation |
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30 | (1) |
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1.6.3 The Orthogonality Condition Model |
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31 | (1) |
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1.7 Recent Developments of the GCM |
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32 | (15) |
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32 | (1) |
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1.7.2 Internal Wave Functions |
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32 | (5) |
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1.7.3 Multicluster Angular-Momentum Projection |
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37 | (1) |
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1.7.4 Multichannel Two-Cluster Systems |
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38 | (3) |
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1.7.5 Multicluster Models |
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41 | (6) |
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1.8 Scattering States With the GCM |
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47 | (4) |
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47 | (1) |
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48 | (1) |
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1.8.3 The Microscopic R-matrix Method |
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49 | (2) |
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1.9 Applications of the GCM |
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51 | (10) |
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1.9.1 The 2x + 3x Systems |
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51 | (4) |
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1.9.2 Other Applications of the Multicluster Model |
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55 | (2) |
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1.9.3 Multichannel Study of the 17F(p, 7)18Ne Reaction |
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57 | (3) |
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1.9.4 12Be as an Example of a Light Exotic Nucleus |
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60 | (1) |
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61 | (6) |
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62 | (5) |
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2 Neutron Halo and Breakup Reactions |
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67 | (54) |
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68 | (3) |
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2.2 Coulomb Breakup at Intermediate/High Energies |
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71 | (3) |
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2.3 Coulomb Breakup and Soft E1 Excitation of 1n Halo Nuclei |
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74 | (22) |
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2.3.1 Coulomb Breakup of 11Be and Characteristic Feature of Soft E1 Excitation of One-Neutron Halo Nuclei |
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74 | (8) |
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2.3.2 Spectroscopy Using Coulomb Breakup of 1n Halo Nuclei - Application to 19C |
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82 | (5) |
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2.3.3 Application to the Radiative Capture Reaction 14C(n, y)15C of Astrophysical Interest |
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87 | (4) |
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2.3.4 Inclusive Coulomb Breakup of 31Ne |
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91 | (5) |
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2.4 Coulomb Breakup and Soft E1 Excitation of 2n Halo Nuclei |
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96 | (5) |
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2.4.1 Exclusive Coulomb Breakup of 11Li |
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97 | (4) |
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2.5 Spectroscopy of Unbound States via the Nuclear Breakup |
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101 | (13) |
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2.5.1 Inelastic Scattering of 14Be |
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103 | (2) |
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2.5.2 Breakup of 14Be With a Proton Target and Spectroscopy of 13Be |
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105 | (9) |
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114 | (7) |
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116 | (5) |
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3 Breakup Reaction Models for Two- and Three-Cluster Projectiles |
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121 | (44) |
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122 | (1) |
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3.2 Projectile and Reaction Models |
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123 | (2) |
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3.3 Semiclassical Approximation |
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125 | (6) |
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3.3.1 Time-Dependent Schrodinger Equation |
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125 | (1) |
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126 | (1) |
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3.3.3 Resolution at the First Order of the Perturbation Theory |
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127 | (2) |
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3.3.4 Numerical Resolution |
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129 | (2) |
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3.4 Eikonal Approximations |
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131 | (7) |
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3.4.1 Dynamical Eikonal Approximation |
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131 | (1) |
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131 | (2) |
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3.4.3 Standard Eikonal Approximation |
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133 | (2) |
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3.4.4 Coulomb-Corrected Eikonal Approximation |
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135 | (3) |
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3.5 Continuum-Discretized Coupled-Channel Method |
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138 | (4) |
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3.6 Breakup Reactions of Two-Body Projectiles |
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142 | (6) |
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142 | (2) |
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3.6.2 Two-Body Breakup of Exotic Nuclei |
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144 | (2) |
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3.6.3 Application to Nuclear Astrophysics |
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146 | (2) |
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3.7 Breakup Reactions of Three-Body Projectiles |
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148 | (10) |
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3.7.1 Three-Cluster Model of Projectile |
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148 | (5) |
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3.7.2 Dipole Strength Distribution |
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153 | (1) |
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3.7.3 The CCE Approximation for Three-Body Projectiles |
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154 | (2) |
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3.7.4 The CDCC Approximation for Three-Body Projectiles |
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156 | (2) |
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158 | (7) |
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160 | (5) |
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4 Clustering Effects Within the Dinuclear Model |
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165 | (64) |
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166 | (1) |
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4.2 Adiabatic or Diabatic Potentials Between Nuclei |
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166 | (9) |
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4.2.1 Two-Center Shell Model |
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167 | (1) |
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4.2.2 Calculation of Adiabatic and Diabatic Potentials |
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168 | (2) |
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4.2.3 The Motion of the Neck |
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170 | (3) |
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4.2.4 Repulsive Potentials by the Quantization of Kinetic Energy |
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173 | (2) |
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4.3 Nuclear Molecules, Hyperdeformed Nuclear Structures |
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175 | (5) |
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4.3.1 Hyperdeformed States Directly Formed in the Scattering of 48Ca + 140 Ce and 90Zr + 90 Zr |
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176 | (2) |
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4.3.2 Hyperdeformed States Formed by Neutron Emission from the Dinuclear System |
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178 | (2) |
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4.4 Normal Deformed and Superdeformed Nuclei |
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180 | (9) |
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4.4.1 Internuclear Potential, Moments of Inertia, Quadrupole and Octupole Moments of the Dinuclear Shape |
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180 | (1) |
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4.4.2 Parity Splitting in Heavy Nuclei |
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181 | (4) |
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4.4.3 Cluster Effects in the Ground State and Superdeformed Bands of 60Zn |
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185 | (2) |
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4.4.4 Decay Out Phenomenon of Superdeformed Bands in the Mass Region A 190 |
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187 | (2) |
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4.5 Complete Fusion and Quasifission in the Dinuclear Model |
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189 | (23) |
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4.5.1 Reaction Models for Fusion With Adiabatic and Diabatic Potentials |
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189 | (1) |
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4.5.2 Problems of Adiabatic Treatment of Fusion |
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190 | (2) |
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4.5.3 Fusion to Superheavy Nuclei |
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192 | (12) |
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4.5.4 Production of Neutron-Deficient Isotopes of Pu |
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204 | (1) |
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4.5.5 Master Equations for Nucleon Transfer |
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205 | (4) |
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4.5.6 Results for Quasifission |
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209 | (3) |
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4.6 Multinucleon Transfer Reactions |
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212 | (4) |
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4.6.1 Production of Heaviest Nuclei in Transfer Reactions |
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212 | (2) |
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4.6.2 Transfer Products in Cold Fusion Reactions |
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214 | (1) |
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4.6.3 Production of Neutron-Rich Isotopes in Transfer Reactions |
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215 | (1) |
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4.7 Binary and Ternary Fission in the Scission-Point Model |
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216 | (7) |
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4.7.1 Fission Potential With the Dinuclear System Model |
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217 | (3) |
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220 | (2) |
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222 | (1) |
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4.8 Selected Summarizing and Concluding Remarks |
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223 | (6) |
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224 | (5) |
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5 Nuclear Alpha-Particle Condensates |
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229 | (70) |
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230 | (3) |
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5.2 Formulation of Alpha-Condensation: THSR Wave Function and OCM Approach |
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233 | (6) |
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5.2.1 Resonating Group Method (RGM) |
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233 | (1) |
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234 | (2) |
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5.2.3 nα Boson Wave Function and OCM |
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236 | (2) |
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5.2.4 Single α-Particle Density Matrix and Occupation Probabilities |
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238 | (1) |
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5.3 THSR Wave Function versus Brink Wave Function for 8Be |
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239 | (4) |
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5.4 Alpha-Gas Like States in Light Nuclei |
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243 | (28) |
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243 | (12) |
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255 | (9) |
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5.4.3 Heavier 4n Nuclei: Gross-Pitaevskii Equation |
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264 | (3) |
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5.4.4 Hoyle-Analogue States in Non-4n Nuclei: 11B and 13C |
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267 | (4) |
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5.5 Clusters in Nuclear Matter and α-Particle Condensation |
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271 | (21) |
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5.5.1 Nuclear Clusters in the Medium |
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271 | (2) |
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5.5.2 Four-Particle Condensates and Quartetting in Nuclear Matter |
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273 | (9) |
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5.5.3 Reduction of the α-Condensate with Increasing Density |
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282 | (4) |
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5.5.4 `Gap' Equation for Quartet Order Parameter |
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286 | (6) |
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5.6 Summary and Conclusions |
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292 | (7) |
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294 | (5) |
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6 Cluster in Nuclei: Experimental Perspectives |
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299 | |
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300 | (1) |
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6.2 Population of Cluster States |
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300 | (12) |
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300 | (6) |
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6.2.2 In-Beam Induced Reactions |
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306 | (6) |
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312 | (9) |
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313 | (2) |
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6.3.2 Solid Hydrogen Targets |
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315 | (3) |
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318 | (3) |
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321 | (23) |
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6.4.1 Gamma-Ray Spectroscopy |
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321 | (3) |
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6.4.2 Charged Particle Detectors |
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324 | (9) |
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333 | (1) |
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6.4.4 Mass Spectrometers, Mass Separators and Combined Setup |
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334 | (3) |
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6.4.5 Particle Identification |
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337 | (5) |
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6.4.6 Electronics and Data AcQuisition (DAQ) Systems |
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342 | (2) |
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344 | (4) |
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6.5.1 Complete Kinematics |
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344 | (1) |
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6.5.2 Particle Reconstruction |
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345 | (1) |
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6.5.3 Total Final State Kinetic Energy (TKE) |
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346 | (1) |
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347 | (1) |
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348 | (2) |
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350 | |
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350 | |