Bivariate quantum signal processing simulates non-Hermitian Hamiltonians H_eff = H_R + i H_I with query-optimal complexity O((α_R + β_I)T + log(1/ε)/log log(1/ε)) in the separate-oracle model.
Feshbach, Unified theory of nuclear reactions, Annals of Physics5, 357 (1958)
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Cavity photons screen attractive or repulsive interactions in a quantum-dot Kitaev chain, allowing the system to reach the sweet spot for poor man's Majorana bound states.
NEGF calculation of 236U(γ,f) cross sections between 5-6 MeV reproduces experimental data including sub-barrier suppression and shows first-eigenchannel dominance, supporting Bohr-Wheeler microscopically.
A two-channel model demonstrates stabilization of three-body resonances into bound states in the continuum via parameter tuning, shown in 1D mass-imbalanced and 3D Efimov systems with magnetic field control.
An educational exposition of Feshbach resonances in Li-6 using basic quantum mechanics to illustrate magnetic tuning of atomic interactions.
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Stabilization of three-body resonances to bound states in a continuum
A two-channel model demonstrates stabilization of three-body resonances into bound states in the continuum via parameter tuning, shown in 1D mass-imbalanced and 3D Efimov systems with magnetic field control.