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Semileptonic decay of heavy baryons in a constituent quark model.

机译:构成夸克模型中重子的半轻子衰变。

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摘要

The semileptonic decays of heavy baryons, Λ Q and ΛQ are treated in the framework of a constituent quark model. Both nonrelativistic and semirelativistic Hamiltonians are used to obtain the baryon wave functions from a fit to the spectra, and the wave functions are expanded in both the harmonic oscillator and Sturmian bases. The latter basis leads to form factors in which the kinematic dependence on the square of the momentum transfer (q 2) is in the form of multipoles, and the resulting form factors fall faster as a function of q2 in the available kinematic ranges. As a result, decay rates obtained in the two models using the Sturmian basis are significantly smaller than those obtained using the harmonic oscillator basis. In the case of the Λc, decay rates calculated using the Sturmian basis are closer to the experimentally reported rates. However, we find a semileptonic branching fraction for the Λ c to decay to excited Λ* states of 11% to 19%, in contradiction with what is assumed in available experimental analyses. Our prediction for the Λb semileptonic decays is that decays to the ground state Λc provide a little less than 70% of the total semileptonic decay rate. For the decays Λ b → Λc the analytic form factors we obtain satisfy the relations expected from heavy-quark effective theory at the non-recoil point, at leading and next-to-leading orders in the heavy-quark expansion. In addition, some features of the heavy-quark limit are shown to naturally persist as the mass of the heavy quark in the daughter baryon is decreased.; For the case of OQ decays there are no experimentally determined rates. However, we find that our analytical and numerical results for the form factors and rates of OQ decays compare well with HQET predictions. Our results indicate a significant inelastic branching fraction for Ob → O c(*) decays, which is about 35% in all of our models. For Oc → xi (*) decays the elastic fraction dominates (about 84%) but it does not saturate the decay.
机译:重质重子ΛQ和ΛQ的半轻子衰变在构成夸克模型的框架内进行处理。非相对论和半相对论的哈密顿量都用于通过拟合光谱获得重子波函数,并且该波函数在谐波振荡器和Sturmian基中都得到扩展。后一个基础导致了形状因数,其中运动对动量传递平方(q 2)的依赖关系是多极形式,并且在可用运动范围内,所得形状因数随q2的变化而下降得更快。结果,在两个模型中使用Sturmian基础获得的衰减率显着小于使用谐波振荡器基础获得的衰减率。在Λc的情况下,使用Sturmian基础计算的衰减速率更接近实验报告的速率。但是,我们发现Λc的半轻质支化分数衰减到11%到19%的激发Λ*状态,这与现有的实验分析所假定的相反。我们对Λb半瘦子衰变的预测是,衰减到基态Λc占总半瘦子衰变率的不到70%。对于衰变Λb→Λc,我们获得的解析形状因子满足重夸克有效理论在非反冲点,重夸克展开中的前导和次先阶时所期望的关系。另外,随着子重子中重夸克质量的减少,重夸克极限的某些特征显示为自然存在。对于OQ衰减的情况,没有实验确定的速率。但是,我们发现我们对OQ衰减的形状因数和速率的分析和数值结果与HQET预测具有很好的对比。我们的结果表明,Ob→O c(*)衰减具有显着的非弹性分支分数,在我们所有模型中均约为35%。对于Oc→xi(*)衰减,弹性分数占主导地位(约84%),但不会使衰减饱和。

著录项

  • 作者

    Pervin, Muslema.;

  • 作者单位

    The Florida State University.;

  • 授予单位 The Florida State University.;
  • 学科 Physics Nuclear.; Physics Elementary Particles and High Energy.
  • 学位 Ph.D.
  • 年度 2005
  • 页码 74 p.
  • 总页数 74
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类 原子核物理学、高能物理学;高能物理学;
  • 关键词

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