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1 | (38) |
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What is a giant resonance? |
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1 | (3) |
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Classification of giant-resonance modes |
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4 | (3) |
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4 | (1) |
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4 | (3) |
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7 | (4) |
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First evidence for IVGDR excitation |
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7 | (1) |
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Further systematic studies of the IVGDR |
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7 | (2) |
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9 | (2) |
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The isoscalar giant resonances |
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11 | (4) |
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12 | (1) |
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The isoscalar giant monopole resonance |
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12 | (3) |
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Other isoscalar multipole strength |
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15 | (1) |
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15 | (3) |
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The isovector giant quadrupole resonance (IVGQR) |
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16 | (1) |
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The isovector giant monopole resonance (IVGMR) |
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16 | (2) |
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Spin-flip or magnetic resonances |
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18 | (5) |
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18 | (1) |
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The 0hω, L = 0 resonances |
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19 | (3) |
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The 1hω, ΔL = 1 transitions |
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22 | (1) |
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23 | (1) |
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23 | (1) |
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Damping of giant resonances |
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23 | (3) |
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The width T of the resonance |
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23 | (2) |
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Decay of the giant resonance |
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25 | (1) |
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26 | (2) |
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28 | (4) |
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32 | (7) |
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The time scale associated with fission |
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32 | (2) |
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34 | (1) |
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The incompressibility of nuclear matter |
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35 | (2) |
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Multipole strength distribution in nuclei with a neutron excess |
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37 | (2) |
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Theoretical frameworks relevant for GR studies |
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39 | (58) |
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General concepts and sum rules |
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39 | (22) |
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39 | (1) |
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39 | (7) |
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Transition rates and single-particle units |
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46 | (5) |
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51 | (7) |
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58 | (3) |
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61 | (5) |
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61 | (1) |
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Compression and polarisation modes |
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62 | (4) |
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66 | (12) |
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66 | (2) |
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Tamm-Dancoff approximation (TDA) |
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68 | (4) |
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72 | (6) |
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Direct reaction theory relevant for GR studies |
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78 | (19) |
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78 | (1) |
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79 | (1) |
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80 | (2) |
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Coupled-channels method and distorted-wave Born approximation |
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82 | (2) |
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Optical potentials from folding models |
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84 | (5) |
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Transition potentials: folding and implicit-folding models |
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89 | (8) |
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Experimental methods used in GR studies |
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97 | (59) |
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97 | (1) |
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Tools for isoscalar non-spin-flip transitions |
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98 | (28) |
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98 | (14) |
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Inelastic scattering of heavy ions at 30-100 MeV/u bombarding energies |
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112 | (7) |
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Inelastic proton scattering |
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119 | (7) |
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Tools for isovector non-spin-flip excitations |
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126 | (18) |
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126 | (1) |
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γ-absorption: real photons |
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127 | (1) |
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128 | (1) |
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Absorption of virtual photons: Coulomb excitation |
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129 | (10) |
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Charge-exchange reactions |
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139 | (5) |
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Tools for isoscalar and isovector excitations: (e,e') |
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144 | (4) |
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Tools for spin-flip resonances |
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148 | (8) |
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148 | (1) |
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Hadronic probes for spin-flip transitions |
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149 | (1) |
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150 | (2) |
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152 | (1) |
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153 | (2) |
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155 | (1) |
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Properties of isoscalar electric GRs |
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156 | (47) |
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156 | (1) |
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The isoscalar giant monopole resonance |
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156 | (14) |
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156 | (1) |
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The data for A ≥ 90 nuclei |
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157 | (2) |
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The ISGMR in light nuclei |
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159 | (10) |
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The ISGMR in light nuclei: concluding remarks |
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169 | (1) |
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Isoscalar ΔL = 1 strength |
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170 | (8) |
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170 | (3) |
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1hω isoscalar dipole strength |
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173 | (1) |
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3hω isoscalar dipole strength |
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173 | (5) |
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The isoscalar giant quadrupole resonance (ISGQR) |
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178 | (10) |
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178 | (1) |
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The ISGQR in A ≥ 90 nuclei |
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179 | (6) |
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The ISGQR in 40 ≤ A < 90 nuclei |
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185 | (2) |
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The ISGQR in 16 ≤ A < 40 nuclei |
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187 | (1) |
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188 | (1) |
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188 | (2) |
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188 | (1) |
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189 | (1) |
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189 | (1) |
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190 | (1) |
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Isoscalar ΔL ≥ 4 strength |
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190 | (1) |
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The effect of deformation on the ISGQR and ISGMR |
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190 | (13) |
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190 | (2) |
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Calculations on the effect of deformation for the ISGMR and ISGQR |
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192 | (7) |
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Experimental information on the ISGQR and ISGMR strength distributions in deformed nuclei |
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199 | (4) |
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203 | (53) |
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203 | (5) |
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The isovector giant monopole resonance (IVGMR) |
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208 | (10) |
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208 | (1) |
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Pion charge-exchange reactions |
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209 | (4) |
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Heavy-ion charge-exchange reactions |
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213 | (3) |
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216 | (2) |
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The isovector giant dipole resonance |
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218 | (25) |
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218 | (1) |
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The giant dipole resonance in A < 50 nuclei |
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218 | (16) |
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The IVGDR in light nuclei |
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234 | (4) |
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238 | (5) |
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The isovector giant quadrupole resonance (IVGQR) |
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243 | (13) |
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243 | (2) |
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The IVGQR studied by interference effects in reactions involving photons |
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245 | (8) |
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The IVGQR in electron scattering |
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253 | (1) |
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254 | (2) |
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Spin-flip transitions in charge-exchange reactions |
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256 | (77) |
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Introduction: a qualitative discussion |
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256 | (2) |
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The Gamow-Teller resonance: the τ - channel |
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258 | (43) |
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258 | (2) |
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The Gamow-Teller sum rule |
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260 | (3) |
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(p, n) reactions - reaction mechanism |
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263 | (13) |
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L = 0 strength from 0° (p, n) cross sections |
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276 | (14) |
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Spin-transfer information from polarisation experiments |
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290 | (5) |
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295 | (6) |
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The GT resonance: the τ+ channel |
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301 | (6) |
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Introduction: the (n, p) and (t, 3He) channels |
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301 | (1) |
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The (n, p) reaction: experimental data |
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302 | (5) |
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The 1hω and 2hω spin-flip strength |
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307 | (22) |
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General features and calculated strength distributions |
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307 | (2) |
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309 | (4) |
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The spin-isospin 1hω ΔL = 1 strength |
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313 | (12) |
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The spin-isospin 2hω strength |
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325 | (4) |
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329 | (4) |
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The 0hω ΔL = 0 transitions |
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330 | (1) |
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The 1hω Δ = 1 transitions |
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331 | (1) |
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The evidence for 2hω ΔL = 0 1+ strength |
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332 | (1) |
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The evidence for 2hω ΔL = 2 strength |
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332 | (1) |
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Spin-flip strength from inelastic scattering |
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333 | (29) |
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333 | (3) |
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336 | (21) |
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336 | (1) |
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337 | (18) |
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The orbital M1 (scissors) mode |
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355 | (2) |
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The ΔL = 1 spin-flip strength |
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357 | (3) |
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360 | (2) |
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362 | (61) |
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362 | (3) |
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365 | (13) |
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Compound and direct particle decay, the hybrid model |
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365 | (3) |
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368 | (1) |
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Beyond the RPA: damping due to collisions |
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369 | (4) |
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The escape width in a model with collision damping |
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373 | (5) |
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Experiments on particle decay in A ≥ 90 nuclei |
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378 | (24) |
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378 | (1) |
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379 | (2) |
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General features of a neutron-decay spectrum |
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381 | (2) |
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Statistical-model calculations for particle decay |
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383 | (3) |
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Quasi-free scattering and direct decay |
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386 | (2) |
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388 | (11) |
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Evidence for pre-equilibrium decay |
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399 | (3) |
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Other GR decay modes in A ≥ 90 nuclei |
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402 | (6) |
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402 | (3) |
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Fission decay of GRs in the actinide region |
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405 | (3) |
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Particle decay in A ≤ 90 nuclei |
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408 | (11) |
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408 | (1) |
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The decay of the IVGDR in A < 90 nuclei |
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408 | (4) |
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The decay of the ISGMR and ISGQR in A ≤ 90 nuclei |
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412 | (2) |
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α0 angular correlation functions with emphasis on 40Ca; multipole identification and branching ratio |
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414 | (5) |
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What did we learn from GR decay experiments? |
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419 | (4) |
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Main features of decay spectra |
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419 | (1) |
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Decay experiments and microscopic structure of GRs |
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420 | (1) |
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Multipole identification from decay experiments |
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421 | (2) |
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423 | (50) |
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423 | (5) |
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423 | (3) |
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The one-dimensional harmonic vibrator |
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426 | (2) |
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Double-charge-exchange resonances |
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428 | (10) |
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428 | (3) |
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Measurements on DCX reactions |
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431 | (7) |
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Multiphonon excitation in heavy-ion scattering |
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438 | (9) |
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438 | (3) |
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Experimental observation of the two-phonon ISGQR in 40Ca |
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441 | (6) |
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Double-IVGDR Coulomb excitation |
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447 | (14) |
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Cross-section calculations |
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447 | (4) |
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Evidence for multiphonon excitation from inclusive reactions |
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451 | (3) |
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Direct observation of the DGDR in heavy-ion collisions |
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454 | (5) |
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Summary of DGDR experiments in relativistic heavy-ion scattering |
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459 | (2) |
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The cross-section problem |
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461 | (10) |
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The effect of the Pauli principle |
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462 | (2) |
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A microscopic calculation |
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464 | (1) |
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Macroscopic models mimicking anharmonic components |
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465 | (2) |
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Phonon mixing and non-linear effects in the excitation mechanism |
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467 | (2) |
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Phonon damping and DGDR excitation cross section |
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469 | (2) |
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471 | (2) |
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The giant dipole resonance in hot nuclei |
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473 | (62) |
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473 | (7) |
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473 | (4) |
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Excitation and decay of hot nuclei: general remarks |
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477 | (2) |
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General features of a γ-decay spectrum |
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479 | (1) |
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Formation and decay of the initial system |
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480 | (10) |
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480 | (1) |
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Statistical γ-decay and its relation to particle decay |
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481 | (4) |
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Formation of compound systems: reaction mechanism and excitation energy |
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485 | (5) |
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The dependence of IVGDR parameters on energy and spin |
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490 | (23) |
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The width of the IVGDR from shape changes and fluctuations |
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492 | (9) |
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Nucleon-nucleon collisions and the IVGDR width |
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501 | (6) |
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Nuclear shape and angular distribution of the IVGDR γ-decay |
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507 | (4) |
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How to distinguish experimentally Einit and Jinit effects |
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511 | (2) |
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Experimental results and their analysis |
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513 | (22) |
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513 | (2) |
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Shape evolution as a function of J |
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515 | (5) |
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The IVGDR width as a function of the temperature T |
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520 | (6) |
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A phenomenological function of the IVGDR width Λ(T, J, A) |
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526 | (2) |
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Measurements at very high excitation energies |
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528 | (5) |
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What did we learn about the IVGDR in hot and fast-rotating nuclei? |
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533 | (2) |
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535 | (48) |
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IVGDR γ-decay used as a time clock in fission |
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535 | (5) |
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535 | (2) |
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Fission delay time extracted from the 229Np* γ-spectrum |
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537 | (3) |
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The difference in neutron-proton radii, ΔRnp |
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540 | (17) |
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540 | (2) |
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Isospin mixing in the ground state due to ΔRnp |
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542 | (1) |
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Experimental determination of ΔRnp through (α, α'): method I |
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542 | (10) |
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Experimental determination of ΔRnp through charge-exchange reactions: method II |
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552 | (5) |
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Isospin mixing at high excitation energies |
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557 | (1) |
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Incompressibility of nuclei and nuclear matter |
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558 | (14) |
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558 | (3) |
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Nuclear incompressibilities |
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561 | (2) |
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From nuclear to nuclear-matter incompressibility |
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563 | (7) |
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Incompressibility and the ISGDR |
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570 | (2) |
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Multipole strength functions in unstable nuclei |
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572 | (11) |
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The quadrupole and dipole response functions for 28O |
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572 | (5) |
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The monopole response in Ca isotopes |
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577 | (2) |
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Experiments on multipole strength in nuclei with neutron excess |
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579 | (4) |
Bibliography |
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583 | (34) |
Index |
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617 | |