1992
DOI: 10.1016/0375-9474(92)90274-n
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Fusion of 28Si + 68Zn, 32S + 64Ni, 37Cl + 59Co and 45Sc + 51V in the vicinity of the Coulomb barrier

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Cited by 99 publications
(42 citation statements)
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“…Even though the approach of CCFUS provides an elegant mathematical solution to the matrix diagonalization problem it ignores all the states where the same phonon appears more than once, e.g., the double-phonon states. Dasgupta et al (1992) and Kruppa et al (1993) pointed out that in some cases the coupling of a state like (b † i ) 2 | 0 to the ground state can be stronger than the coupling of a state like Kruppa et al (1993) considered quadrupole and octupole phonons, but included their double-phonon states as well diagonalizing the resulting 6 × 6 matrix. Dasgupta et al (1992) excluded all multiplephonon states, so for n different types of phonons they numerically diagonalized an (n + 1) × (n + 1) matrix instead of analytically diagonalizing an 2 n × 2 n matrix.…”
Section: B Simplified Coupled-channels Modelsmentioning
confidence: 99%
See 1 more Smart Citation
“…Even though the approach of CCFUS provides an elegant mathematical solution to the matrix diagonalization problem it ignores all the states where the same phonon appears more than once, e.g., the double-phonon states. Dasgupta et al (1992) and Kruppa et al (1993) pointed out that in some cases the coupling of a state like (b † i ) 2 | 0 to the ground state can be stronger than the coupling of a state like Kruppa et al (1993) considered quadrupole and octupole phonons, but included their double-phonon states as well diagonalizing the resulting 6 × 6 matrix. Dasgupta et al (1992) excluded all multiplephonon states, so for n different types of phonons they numerically diagonalized an (n + 1) × (n + 1) matrix instead of analytically diagonalizing an 2 n × 2 n matrix.…”
Section: B Simplified Coupled-channels Modelsmentioning
confidence: 99%
“…Dasgupta et al (1992) and Kruppa et al (1993) pointed out that in some cases the coupling of a state like (b † i ) 2 | 0 to the ground state can be stronger than the coupling of a state like Kruppa et al (1993) considered quadrupole and octupole phonons, but included their double-phonon states as well diagonalizing the resulting 6 × 6 matrix. Dasgupta et al (1992) excluded all multiplephonon states, so for n different types of phonons they numerically diagonalized an (n + 1) × (n + 1) matrix instead of analytically diagonalizing an 2 n × 2 n matrix. The resulting simplified coupled channels code is named CCMOD (Dasgupta et al, 1992).…”
Section: B Simplified Coupled-channels Modelsmentioning
confidence: 99%
“…It was shown in Ref. [2] that coupling to the 3 − 1 state in 16 O at 6.13 MeV using the simplified CC code CCMOD [15], which uses the linear coupling approximation, resulted in a deterioration in the agreement with the measured barrier distribution. This effect is related to the neglect of the higher-order terms in the CC calculations [17,25].…”
Section: Approximations Used In Solving the Coupled Equationsmentioning
confidence: 99%
“…The CC description is expected to be simpler for systems involving the fusion of closed-shell nuclei due to the presence of relatively few low-lying collective states. An example is the 16 O+ 144 Sm system, where a good description [10] of the experimental barrier distribution was obtained with a simplified CC model [14,15]. This description was somewhat fortuitous in view of the approximations used in this model.…”
Section: Introductionmentioning
confidence: 99%
“…This is the most difficult problem in the fusion of massive nuclei, and there are still large ambiguities in theoretical predictions of fusion cross sections. Because of this reason, one often employs a simplified coupled-channels treatment for the barrier penetration prior to the touching configuration [5,7], which is essentially based on the constant coupling approximation [8] or a variant [9].…”
Section: Introductionmentioning
confidence: 99%