An Internally Disclosed Structure of the Uranium Family

In the framework of the new theory [1] of an atom with orbits quantized by leptonic families, in the arbitrary case of an atom $X_{Z}^{A},$ the numbers of isotopes $I$ of its root $X_{Z}^{2Z}$ of lepton $(N_{l}^{I})$ and antineutrino $(N_{{\bar \nu_{l}}}^{I})$ orbits are equal to $$N_{l}^{I}=Z, \, \, \, \, N_{{\bar \nu_{l}}}^{I}=\left\{ {\begin{array}{l} {\, \, \, \, 2L_{l}\quad \mbox{for}\quad Z=N=1,}\\ {2ZL_{l}\quad \mbox{for}\quad Z=N>1.} \end{array}}\right. \eqno(1)$$ Such a principle clearly shows that the total number $N_{full}^{I}$ of isotopes that constitute the same atomic family is intimately connected with the quantity of lepton flavors $$N_{full}^{I}=N_{l}^{I}+N_{{\bar \nu_{l}}}^{I}. \eqno(2)$$ If we choose $H_{1}^{2}$ from the united system of atomic roots $X_{Z}^{2Z},$ its family at $(l=\epsilon,$ $e,$ $\mu,$ $\tau,...)$ consists of ten atoms. The helium family includes eighteen forms of atomic systems. Then it is possible, from (1) and (2), to predict the availability in nature of $63189$ isotope forms of $118$ types of atomic systems. Among them, the uranium family includes $828$ types of atoms. [1] R.S. Sharafiddinov, Phys. Essays {\bf 32}, 358 (2019); Bull. Am. Phys. Soc. {\bf 63}(4), L01.00041 (2018).