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A M Escobar-Ruiz

Publications and source records attributed to A M Escobar-Ruiz.

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Nodal algebraic curves and entropy diagnostics in degenerate two-dimensional harmonic-oscillator shells

Degeneracy allows the nodal structure of a quantum state to vary without changing its energy. We study this effect for real superpositions in the fixed-energy shells of the two-dimensional isotropic harmonic oscillator. In Cartesian coordinates $(x,y)$, any such state in the $N$th shell has the parametrized form $ψ_N(x,y;\mathbf{c})=ψ_0(x,y)\,P_N(x,y;\mathbf{c})$, where $ψ_0$ is the non-vanishing ground state and the real coefficients $\mathbf{c}$ determine the polynomial factor $P_N$. The nodal set is exactly the algebraic curve $P_N=0$. Thus, varying $\mathbf{c}$ reshapes this curve at fixed energy. We show that its topology can change only when it develops a finite singular point, $P_N=\nabla P_N=0$, or when two asymptotic nodal directions merge. We characterize this geometry using three diagnostics: the nodal-domain entropy $S_{\rm dom}$, the Cartesian mutual information $I(x;y)$, and the entropic uncertainty sum $S_r+S_p$, which respectively probe probability redistribution among nodal domains, coordinate correlations, and global position-momentum delocalization. The lowest shells reveal a clear hierarchy. For $N=1$, mixing only rotates a nodal line. Along a representative $N=2$ path, a closed conic passes through parallel lines into a hyperbola-type curve; $S_{\rm dom}$ clearly detects this transition, while $S_r+S_p$ remains smooth. For $N=3$, merging asymptotic directions brings smooth cubic branches close together and enhances both $S_{\rm dom}$ and $I(x;y)$. These signatures are accessible in Hermite-Gaussian structured light and nearly isotropic trapped oscillators.

quant-ph

Superintegrability and choreographic obstructions in dihedral $n$-body Hamiltonian systems

We study planar $n$-body Hamiltonians with quadratic pair interactions whose coupling pattern is invariant under the dihedral group $D_n$. After the center of mass is removed, the dynamics separates into label-Fourier modes. This makes it possible to distinguish three notions that are often conflated: commensurability of the normal frequencies, maximal superintegrability of the full relative Hamiltonian, and realization of choreographic space--time symmetry. We prove that a periodic configuration is $C_n$-equivariant if and only if every label-Fourier coefficient acquires under the time shift $T/n$ the character phase prescribed by cyclic relabeling. For harmonic motion this criterion determines the complete equivariant subspace of initial data and its codimension. Thus, a resonant orbit may be periodic without being a choreography. The cases $n=4,5,6$ illustrate the obstruction. In particular, $n=6$ is the first case with three inequivalent internal branches: the nondegenerate $1{:}2{:}3$ resonance admits a phase-matched three-branch choreography, whereas the exactly degenerate $1{:}2{:}2$ spectrum is incompatible with simultaneous $m=2$ and Nyquist $m=3$ excitation. A choreography on the latter surface survives only in a compatible invariant subspace. Resonant data outside the equivariant subspace can instead organize into synchronized multi-trace fragments.

math-ph