1980
DOI: 10.1007/3-540-09965-4_25
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Review of models for fusion

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Cited by 8 publications
(4 citation statements)
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“…Let us indeed consider the partial wave I~ for which Vc+Ic(lc+l)h2/2#r~ is equal to E. For l< l~, the transmission coefficients are close to unity and for t> I~ they are close to zero. The sum in (1) is thus approximately limited to tc and one finds the usual high-energy behaviour [2][3][4]8] ar ~-~r~(l -VIE).…”
Section: =0mentioning
confidence: 99%
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“…Let us indeed consider the partial wave I~ for which Vc+Ic(lc+l)h2/2#r~ is equal to E. For l< l~, the transmission coefficients are close to unity and for t> I~ they are close to zero. The sum in (1) is thus approximately limited to tc and one finds the usual high-energy behaviour [2][3][4]8] ar ~-~r~(l -VIE).…”
Section: =0mentioning
confidence: 99%
“…0340-2193/82/0306/0079/$02.00 either when the Coulomb plus centrifugal barrier has been passed through, either when a critical distance of approach r~ has been reached [8,[2][3][4]. The fusion cross section is defined as [2] a r = 7t22 ~ (i + (-1) '+ 2, 5/(2I + 1)) (21 + 1) T z…”
Section: Principlementioning
confidence: 99%
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“…The results obtained elucidated to a considerable extent the picture of this interesting phenomenon and deserve a special consideration. Several publications considered various aspects of this problem (Schroder and Huizenga 1977, Birkelund et a1 1979, Nix and Sierk 1979, Krappe 1979, Swiatecki 1980, b, Vaz et a1 1981. To summarise the data accumulated one can say that at present the use of the A 3 6 0 ion beams looks unpromising for SHE synthesis in complete-fusion reactions.…”
Section: E*mentioning
confidence: 99%