The orbital loops observed experimentally of \(p\), \(d\) and \(f\) orbits are due to the weak \(E\) fields generated by spinning \(T^{+}\) particles. These fields have a positive and negative end (two opposing loops to one field) and the number of loop pairs increases with the number of unpaired \(T^{+}\) particles in the nucleus.
The loops appears when the \(T^{+}\) are in unpaired orbits. In such cases, under experimental conditions to measure electric fields, their orbits space out such that the generated \(E\) fields have the least interaction and do not overlap.
Those distorted elongated spheres are not electron clouds.
