论文标题
对相对论旋转0颗粒的深度非谐调性
Deep anharmonicity to relativistic spin-0 particles in the spherical regime
论文作者
论文摘要
我们提出了在量子状态下移动的相对论旋转0电荷的振荡器建模,电磁场的最小耦合。我们不是扰动无旋转状态的方法,而是直接在整数依赖性水平下进行非谐调。这样,静止质量能量的带电粒子保持为280 MEV。在熟悉的类似北京的近似值中,我们还提高了对第三和第四的订单的深入近似值,在$ 7.5 \,{\ rm fm} $的第三和第四平衡中。此外,我们已经建立了一个更紧密的高阶近似协议,并且具有$ 0.43 \,{\ rm fm^{ - 1}} $的宽度范围为$ 0.43 \。尽管标量和矢量电位之间的平等以可解决的形式产生输出,但改进的近似值可提供与空间无关的休息质量,作为没有外部场的“纯振荡器”。在没有标量分布的情况下,最小的耦合也可能导致平衡距离的振荡,因此我们考虑了超能量的增加,在80至100 MEV的深度范围内,摩尔斯的潜力转移了变化。由于转移的结果,得出的结论是,带电粒子的潜在深度会影响相对论的能量水平,在这种情况下,我们发现大约200 MEV用于颗粒,而将近-10 meV用于抗粒子。除了负能量状态外,典型的概率图显示了旋转零电荷分布之后的波段为($ n = 0 $ $ \ ell = 0 $)和($ n = 1 $,$ \ ell = 1 $),与相对主义能量相对应。通过考虑到具有$ v_ {v}(r)\ neq 0 $和$ v_ {s}(r)= 0 $的klein-gordon anharmonicity的深近似,可以引入近似可溶性的相关振动模型。
We present an oscillator modeling of the relativistic spin-0 charges moving in the quantum states with minimum coupling of electromagnetic fields. Rather than perturbative approach to spinless regime, we put into operation directly under integer dependent levels for anharmonicity. In this way, the charged particle of rest mass energy kept as 280 MeV. Within the familiar Pekeris-like approximation, we have also improved the deep approximation to the orders of third and fourth near equilibrium of $7.5\,{\rm fm}$. Moreover, we have founded a closer agreement of high order approximation and given potential which has width range of $0.43\,{\rm fm^{-1}}$. Although equality between scalar and vector potentials give output in the solvable form, the improved approximation provides the spatial-independent rest mass as a "pure oscillator" without external field. In the absence of scalar distribution, minimal coupling might also leads to an oscillation at equilibrium distances, so we have considered an adding of extra-energy giving shifted Morse potential in the depth range 80 to 100 MeV. As a result of the shift, it has been concluded that the potential depth of the charged particle affects the relativistic energy levels where we have found about 200 MeV being for particles and nearly -10 MeV being for anti-particles. Besides negative energy states, the typical probability picture showing spin-zero charge distribution has been followed by the wavefunctions as ($n=0$ $\ell=0$) and ($n=1$, $\ell=1$) corresponding to relativistic energies. By taking into account a deep approximation to Klein-Gordon anharmonicity with $V_{v}(r)\neq 0$ and $V_{s}(r)=0$, one can introduced approximate-solvable relativistic oscillatory model.