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This paper applies the Scretching–Planck (SP) density–phase representation, \(ψ=√ P\,eiS/\), to supersymmetric quantum mechanics and selected string models. For a real, nodeless ground state, the balance \(E_0=V+QSP[P_0]\) expresses the superpotential as \(W=-√m/2\,u_0\), where \(u_0\) is the osmotic velocity of the ground-state density. The same density gives the partner potential \(V-(^2/2m)(ln P_0)''\). Five numerical benchmarks agree within \(2.3×10⁻⁴\) at the grid resolution used, and the iterated factorization reproduces the first six hydrogen energies within \(6.2×10⁻⁶\) Ry. For the factorization branch considered, a normalizable zero mode signals unbroken supersymmetry. The paper then examines the cancellation of bosonic and fermionic zero-point energies. A cutoff estimate with superpartners near \(2\) TeV gives a residual vacuum energy \(6.4×10⁵⁹\) times the observed dark-energy density. In the string examples, regularized oscillator sums contribute to the intercepts in the critical bosonic and superstring theories, with \(D=26\) and \(D=10\), respectively. The bosonic level counts are \(24\) and \(324\), and the oscillator contributions cancel in the Ramond sector. For circle compactification, SP phase circulation quantizes momentum, and T-duality exchanges momentum and winding. Four additional massless vectors appear at the self-dual radius in the bosonic circle model. The paper compares the charge-matched Kaluza–Klein scale of \(5.215×10¹⁷\) GeV with the coupling-dependent heterotic scale \(g(5.265×10¹⁷\,GeV)\). The scales agree within about 1% at \(g=1\), while the separate self-dual matching condition gives \(g^2=8πα\). Finally, writing the dilaton as \(P=e-2Φ\) turns its string-frame kinetic term into the density-gradient expression \((∇ P)^2/P\) and gives the Einstein-frame conformal factor \(P2/(D-2)\). Ten solved problems are included.
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Daniel Scretching (2026) studied this question.
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