Matches in SemOpenAlex for { <https://semopenalex.org/work/W2051463932> ?p ?o ?g. }
- W2051463932 endingPage "567" @default.
- W2051463932 startingPage "556" @default.
- W2051463932 abstract "The differential cross sections for the reactions $^{63,65}mathrm{Cu}(t,p)^{65,67}mathrm{Cu}$ were measured at ${E}_{t}=3.2, 3.0, mathrm{and} 2.8$ MeV. For $L=0$ ground-state transitions, the energy dependence of the values of the differential cross sections is strong and exponential, while the angular distribution shape, which is of a clear diffraction pattern in sharp contrast to the case of the sub-Coulomb ($d,p$) reaction, does not change with small energy variation. The reactions proceed well below the Coulomb barrier of the entrance channel, yet through a direct process. A definite difference is observed between the angular distributions for the two ground-state transitions. The zero-range distorted-wave Born approximation can reproduce the energy dependence of the differential cross sections and the trend of isotope dependence of the angular distribution. In distorted-wave Born approximation calculations, a definite nuclear optical potential is needed for the triton-nucleus channel which is below the Coulomb barrier, in sharp contrast to the sub-Coulomb ($d,p$) reaction. The triton-nucleus optical potential below the Coulomb barrier is nearly equal to the optical potential that works at energies of a few tens of MeV. The angular distribution for an $L=2$ transition is forward-rising, though not diffractionlike, and can be reproduced on the whole by the zero-range distorted-wave Born approximation. It is confirmed for the first time that the ($t,p$) reaction below the Coulomb barrier of the entrance channel takes place in an extended region outside the nucleus. It is argued and concluded on various grounds that the ($t,p$) angular distribution shape below the Coulomb barrier of the entrance channel is sensitive to the radial two-neutron from factor outside the nucleus. Physical implications of the revealed features are discussed, especially on the coherence of the two-particle form factor and the proton and neutron distributions in the nuclear surface region.NUCLEAR REACTIONS $^{63,65}mathrm{Cu}(t,p)$, $E=2.8, 3.0, 3.2$ MeV; measured $ensuremath{sigma}(E;ensuremath{theta})$; DWBA analysis. Enriched $^{63}mathrm{Cu}$, natural Cu targets, resolution 200 keV; $ensuremath{theta}=10ensuremath{-}165ifmmode^circelsetextdegreefi{}$. Revealed features below the Coulomb barrier, sensitivity to the form factor." @default.
- W2051463932 created "2016-06-24" @default.
- W2051463932 creator A5009965187 @default.
- W2051463932 creator A5016970427 @default.
- W2051463932 creator A5071560799 @default.
- W2051463932 creator A5089818516 @default.
- W2051463932 date "1976-02-01" @default.
- W2051463932 modified "2023-10-03" @default.
- W2051463932 title "Features of the (t,p) reaction below the Coulomb barrier of the entrance channel" @default.
- W2051463932 cites W1501093122 @default.
- W2051463932 cites W1589237550 @default.
- W2051463932 cites W1965673110 @default.
- W2051463932 cites W1966504497 @default.
- W2051463932 cites W1968040809 @default.
- W2051463932 cites W1968087374 @default.
- W2051463932 cites W1971674544 @default.
- W2051463932 cites W1971932634 @default.
- W2051463932 cites W1972205889 @default.
- W2051463932 cites W1973972023 @default.
- W2051463932 cites W1975914728 @default.
- W2051463932 cites W1981355541 @default.
- W2051463932 cites W1985681532 @default.
- W2051463932 cites W1992600143 @default.
- W2051463932 cites W1993302941 @default.
- W2051463932 cites W1993945298 @default.
- W2051463932 cites W1996125762 @default.
- W2051463932 cites W1996275737 @default.
- W2051463932 cites W1997563329 @default.
- W2051463932 cites W1998541669 @default.
- W2051463932 cites W1998952398 @default.
- W2051463932 cites W1999695511 @default.
- W2051463932 cites W2002478407 @default.
- W2051463932 cites W2004824472 @default.
- W2051463932 cites W2008611632 @default.
- W2051463932 cites W2009636305 @default.
- W2051463932 cites W2012050441 @default.
- W2051463932 cites W2014886806 @default.
- W2051463932 cites W2016181203 @default.
- W2051463932 cites W2016687205 @default.
- W2051463932 cites W2016952467 @default.
- W2051463932 cites W2021070244 @default.
- W2051463932 cites W2023784002 @default.
- W2051463932 cites W2029223436 @default.
- W2051463932 cites W2029777362 @default.
- W2051463932 cites W2030450208 @default.
- W2051463932 cites W2031402410 @default.
- W2051463932 cites W2032693919 @default.
- W2051463932 cites W2036970940 @default.
- W2051463932 cites W2047274954 @default.
- W2051463932 cites W2050872219 @default.
- W2051463932 cites W2053953599 @default.
- W2051463932 cites W2056503617 @default.
- W2051463932 cites W2058076843 @default.
- W2051463932 cites W2058995743 @default.
- W2051463932 cites W2062324853 @default.
- W2051463932 cites W2063787907 @default.
- W2051463932 cites W2063905787 @default.
- W2051463932 cites W2067054054 @default.
- W2051463932 cites W2070906747 @default.
- W2051463932 cites W2072303748 @default.
- W2051463932 cites W2076478853 @default.
- W2051463932 cites W2078448428 @default.
- W2051463932 cites W2090074380 @default.
- W2051463932 cites W2092080459 @default.
- W2051463932 cites W2094608435 @default.
- W2051463932 cites W2094689305 @default.
- W2051463932 cites W2095030487 @default.
- W2051463932 cites W2241538498 @default.
- W2051463932 cites W2249924119 @default.
- W2051463932 cites W2278273093 @default.
- W2051463932 cites W2279683715 @default.
- W2051463932 cites W2291171117 @default.
- W2051463932 cites W2314338151 @default.
- W2051463932 cites W2314354690 @default.
- W2051463932 cites W2319310090 @default.
- W2051463932 cites W2488620602 @default.
- W2051463932 cites W2600711790 @default.
- W2051463932 cites W3021129094 @default.
- W2051463932 cites W3024827764 @default.
- W2051463932 cites W3117260649 @default.
- W2051463932 cites W35473614 @default.
- W2051463932 cites W4230804862 @default.
- W2051463932 doi "https://doi.org/10.1103/physrevc.13.556" @default.
- W2051463932 hasPublicationYear "1976" @default.
- W2051463932 type Work @default.
- W2051463932 sameAs 2051463932 @default.
- W2051463932 citedByCount "3" @default.
- W2051463932 crossrefType "journal-article" @default.
- W2051463932 hasAuthorship W2051463932A5009965187 @default.
- W2051463932 hasAuthorship W2051463932A5016970427 @default.
- W2051463932 hasAuthorship W2051463932A5071560799 @default.
- W2051463932 hasAuthorship W2051463932A5089818516 @default.
- W2051463932 hasConcept C113612514 @default.
- W2051463932 hasConcept C121332964 @default.
- W2051463932 hasConcept C147120987 @default.
- W2051463932 hasConcept C156137748 @default.
- W2051463932 hasConcept C159985019 @default.
- W2051463932 hasConcept C184779094 @default.