In this paper, the physical nature of quantum usual and self-friction (SF) harmonic oscillators is presented. The procedure for studying these harmonic oscillators is identical; therefore, we can benefit from the theory of the usual harmonic oscillator. To study the SF harmonic oscillator, using analytical formulae for the $$L^{{(p_{l}^{ * } )}}$$ -SF Laguerre polynomials ( $$L^{{(p_{l}^{ * } )}}$$ -SFLPs) and $$L^{{(\alpha^{*} )}}$$ -modified SFLPs ( $$L^{{(\alpha^{*} )}}$$ -MSFLPs) in standard convention, the $$V^{{(p_{l}^{ * } )}}$$ -SF potentials ( $$V^{{(p_{l}^{ * } )}}$$ -SFPs), $$V^{{(\alpha^{*} )}}$$ -modified SFPs ( $$V^{{(\alpha^{*} )}}$$ -MSFPs), $$F^{{(p_{l}^{ * } )}}$$ -SF forces ( $$F^{{(p_{l}^{ * } )}}$$ -SFFs) and $$F^{{(\alpha^{*} )}}$$ -modified SFFs ( $$F^{{(\alpha^{*} )}}$$ -MSFFs) are investigated, where $$p_{l}^{ * } = 2l + 2 - \alpha^{*}$$ and $$\,\alpha^{*}$$ is the integer ( $$\alpha^{*} = \alpha$$ , $$\, - \infty < \alpha \le 2)$$ or non-integer ( $$\alpha^{*} \ne \alpha$$ , $$\, - \infty < \alpha < 3)$$ SF quantum number. We note that the potentials ( $$V^{{(p_{l}^{ * } )}}$$ -SFPs and $$V^{{(\alpha^{*} )}}$$ -MSFPs), and forces ( $$F^{{(p_{l}^{ * } )}}$$ -SFFs and $$F^{{(\alpha^{*} )}}$$ -MSFFs), respectively, are independent functions. It is shown that the numerical values of these independent functions are the same, i.e., $$V_{num}^{{(p_{l}^{ * } )}} = V_{num}^{{(\alpha^{*} )}}$$ and $$F_{num}^{{(p_{l}^{ * } )}} = F_{num}^{{(\alpha^{*} )}}$$ . The dependence of the SF harmonic oscillator as a function of the distance is analyzed. The presented relationships are valid for arbitrary values of parameters.
Read full abstract