A systematic way to construct the power spectra of the atom?

Probably an ordered matrix power series, and probably something for which I have no real answer. Now that I mentioned it, I will likely look around and borrow steal ideas.  But it is  one of those things where I am not the expert. I am not sure how far I want to push this. It seems to be we are counting power spectra up from the ground, and generating axis of symmetry for each count. Those axis should appear as the coefficient of a symmetric matrix to the power defined by the exponent separations. I do not et understand it all, but its a bit like placing the digits of a numbering system in the proper location of a spherical number line.

My spectral chart is a good starting point, it is to the right in one of the pages on this blog. The Laplace guy from ancient France worked part of the problem.

In mathematics, spherical harmonics are the angular portion of a set of solutions to Laplace's equation. Represented in a system of spherical coordinates, Laplace's spherical harmonics are a specific set of spherical harmonics that forms an orthogonal system, first introduced by Pierre Simon de Laplace in 1782.^[1] 

Our boundary condition is the Higgs bandwidth areoung the atom, includes all phase velues generated by the polynomial. Our condition should be Gauss^2. Follow the references for iterative methods that work with sparse matrices, generated by our hyperbolic power series; would be my guess. The bubbles already computed the maximum entropy modes, so we are working the reverse Planck curve, finding the 'box' that generates the Planck curve. We are decoding, not encoding. Adding the Bosons is optional, it increases the resolution. But we should see the quark and chromodynamics modes. What about the precision of the most irrational number? That should increase with energy.

Pretty Bubbles