The QCD light-front Hamitonian equation derived from quantization at fixed LFtime provides a causal, frame-independent, method for computing hadronspectroscopy and dynamical observables. de Alfaro, Fubini, and Furlan (dAFF)have made an important observation that a mass scale can appear in theequations of motion without affecting the conformal invariance of the action ifone adds a term to the Hamiltonian proportional to the dilatation operator orthe special conformal operator. If one applies the dAFF procedure to the QCDlight-front Hamiltonian, it leads to a color confining potential $\kappa^4\zeta^2$ for mesons, where $\zeta^2$ is the LF radial variable conjugate to the$q \bar q$ invariant mass squared. The same result, including spin terms, isobtained using light-front holography if one modifies the AdS$_5$ action by thedilaton $e^{\kappa^2 z^2}$ in the fifth dimension $z$. When one generalizesthis procedure using superconformal algebra, the resulting light-fronteigensolutions provide a unified Regge spectroscopy of meson, baryon, andtetraquarks, including remarkable supersymmetric relations between the massesof mesons and baryons and a universal Regge slope. The pion $q \bar q$eigenstate has zero mass at $m_q=0.$ The superconformal relations also can beextended to heavy-light quark mesons and baryons. AdS/QCD also predicts theanalytic form of the nonperturbative running coupling in agreement with theeffective charge measured from measurements of the Bjorken sum rule. The massscale underlying hadron masses can be connected to the mass parameter in theQCD running coupling. The result is an effective coupling $\alpha_s(Q^2)$defined at all momenta. One also obtains empirically viable predictions forspacelike and timelike hadronic form factors, structure functions, distributionamplitudes, and transverse momentum distributions.
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机译:从固定的LFtime量化导出的QCD光前哈密顿方程提供了一种因果关系的,与帧无关的方法,用于计算强子光谱和动态可观察物。 de Alfaro,Fubini和Furlan(dAFF)做出了重要观察,如果将一个与膨胀算子或特殊保形算子成比例的哈密顿量项添加到运动方程中,则在不影响作用的保形不变性的情况下,质量标可以出现在运动方程中。如果将dAFF程序应用于QCDlight-front哈密顿量,则会导致介子的颜色限制潜力$ \ kappa ^ 4 \ zeta ^ 2 $,其中$ \ zeta ^ 2 $是与$ q共轭的LF径向变量。 \ bar q $不变质量的平方。如果使用第五维$ z $中的狄拉顿$ e ^ {\ kappa ^ 2 z ^ 2} $修改AdS $ _5 $动作,则可以使用光前全息术获得相同的结果,包括旋转项。当使用超共形代数推广这一过程时,所得的光前本征解提供了介子,重子和四夸克的统一Regge光谱,包括介子和重子的质量之间的显着超对称关系以及通用Regge斜率。介子$ q \ bar q $本征态在$ m_q = 0处的质量为零。超共形关系也可以扩展为重轻的夸克介子和重子。 AdS / QCD还可以预测非扰动耦合的解析形式,并与根据Bjorken和规则测得的有效电荷相一致。潜在的强子质量的质量标度可以连接到QCD运行耦合中的质量参数。结果是在所有时刻都定义了有效耦合$ \ alpha_s(Q ^ 2)$。人们还获得了像时空一样的强子形状因子,结构函数,分布幅度和横向动量分布的经验上可行的预测。
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