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123QFyieldtreatedbyKRA-F56PotentialenergyoftheDNSMassyieldsofthereaction48Ca+244PucalculatedwithDIFFandKRA-F,respectively.(a)MassrangefromA1=50toA1=ACN/2.(b)MassrangefromB-GPoint(A1=19)toincidentChannel(A1=48).10(a)Thedrivingpotentialofthereaction48Ca+244PuasafunctionofthefragmentA1.Theopencirclesstandforthedrivingpotential,inwhichthepotentialvalueatA1=113isartificiallysubstitutedbythatofA1=112.(b)ThemassyieldsshownbyblacksquaresandstarsasafunctionofthefragmentA1underthedrivingpotentialgivenbyblacksquaresin(a)(exceptatA1=113,atallotherplaces,theopencirclesarelocatedontheblacksquares),calculatedbyDIFFandKRA-F,respectively.Opencirclesaretheyields’distributionunderthedrivingpotentialbyopencircles.动力学形变的影响1314Thepotentialenergysurface(thedrivingpotential)PESforthereaction48Ca+244Puasafunctionofquadrupoledeformationsintheentrancechannel(A1=48).171819202122Thetimeevolutionofthemassyieldsofthereaction48Ca+244PucalculatedwithDIFFwitht0=10−22s.
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