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Dirac Coupled-channel Analyses of Polarized Proton Scatterings to the 2$^+$ Gamma Vibrational Band in $^{24}$Mg and $^{26}$Mg

机译:偏振质子散射的Dirac耦合通道分析   2 $ $ ^ + $ Gamma振动带,$ ^ {24} $ mg和$ ^ {26} $ mg

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摘要

Dirac coupled channel calculations are performed phenomenologically for thehigh-lying excited states that belong to the 2$^+$ gamma vibrational band atthe 800-MeV polarized proton inelastic scatterings from the s-d shell nuclei,$^{24}$Mg and $^{26}$Mg. Optical potential model is used and scalar andtime-like vector potentials are considered as direct potentials. First-ordervibrational collective models are used to obtain the transition opticalpotentials in order to accommodate the high-lying excited vibrationalcollective states. The complicated Dirac coupled channel equations are solvedphenomenologically to reproduce the differential cross section and analyzingpower data by varying the optical potential and deformation parameters. It is found that the relativistic Dirac coupled channel calculation coulddescribe the high-lying excited states of the 2$^+$ gamma vibrational band atthe 800-MeV polarized proton inelastic scatterings from s-d shell nuclei$^{24}$Mg and $^{26}$Mg reasonably well, showing better agreement with theexperimental data compared to the results obtained from the nonrelativisticcalculations. Calculated deformation parameters for the excited states areanalyzed and compared with those of nonrelativistic calculations.
机译:狄拉克耦合通道的计算是从现象学上对高激发态进行的,该激发态是在sd壳核的800MeV极化质子非弹性散射,$ ^ {24} $ Mg和$ ^ { 26} $ Mg。使用光学势模型,并将标量和类似时间的矢量势视为直接势。一阶振动集合模型用于获得跃迁光势,以适应高激发振动集合态。现象学上解决了复杂的狄拉克耦合通道方程,通过改变光势和变形参数来再现微分截面并分析功率数据。发现相对论狄拉克耦合通道计算可以描述来自sd壳核$ ^ {24} $ Mg和$ ^ {的800MeV极化质子非弹性散射处2 $ ^ + $伽马振动带的高激发态。 26} $ Mg相当好,与从非相对论计算获得的结果相比,与实验数据显示出更好的一致性。分析了激发态的变形参数,并将其与非相对论计算的变形参数进行了比较。

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    Shim, Sugie;

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