<u>Axial Nucleus Density</u> for DFT, Symmetry Axis Rotating Toward Electron Clusters with ½, Zeta Related to Two Locked-at-180^o Dirac Monopoles, Inter-dimensional Hemispherical (r_#,θ_#,φ_#,z) Relativity Stress

I provide a DFT axial nucleus density to apply that is not in current set.

• Based upon ‘extra 1/r’ generating net-2-interaction, so ^(-4)+^(-3) as no density near the nucleus, but instead starting at Bohr-H (a₀) *adjusted for nucleon counts.
  
  Concentrated at two poles understood as the subshell-s direction, Quantum Number (N,0,x,x) as Quantitized Hemispherical (r_#, θ_#=0, φ_#, z=±½).
  
  Rotating that nucleostatic axis by ½ energy towards strongest electron cluster versus ½ energy as linear acceleration of electrons towards that nucleostatic axis XC-Diff (X1)
  
  With DFT (X1) XC-diff understood as two locked-at-180^o Dirac monopole, never alone at the particle surface (r_e) poles.
  
  With interdimensional transfers in a limited relativity with added cosine-θ-variant for static precursor B-field understood by that hemispherical frame-of-reference
  
  Position-in-field scaling as (r/a₀)^M/N

This generates:

• Better densities for DFT
  
  3D settling, from chaos, path for TDDFT
  
  Physical models underlying equations
  
  Acceleration-vectors alternative for computational modeling