Noninteracting fermions with effective mass m_eff(x) ~ |x|^α form a determinantal point process whose large-N scaled kernel near the origin is a sum of two Bessel kernels with different indices rather than standard Airy or single-Bessel forms.
Title resolution pending
4 Pith papers cite this work. Polarity classification is still indexing.
4
Pith papers citing it
verdicts
UNVERDICTED 4representative citing papers
Symmetry class alone sets SWSSB correlation length growth to exponential (Z2, tc ~ ln L) or algebraic (U(1), tc ~ L^alpha with alpha filling-dependent) in open quantum systems, independent of spectral gap.
A blockade-restricted long-range model for Rydberg-cavity systems yields a distinct blockaded ferromagnetic/superradiant phase at equilibrium and long-range many-body scars with logarithmic entanglement dynamics out of equilibrium.
Diffusion maps identify quantum phase transitions in Bose-Hubbard systems, including symmetry-protected topological phases and ergodic vs. many-body localized regimes, without prior order parameters or handcrafted observables.
citing papers explorer
-
Sluggish quantum mechanics of noninteracting fermions with spatially varying effective mass
Noninteracting fermions with effective mass m_eff(x) ~ |x|^α form a determinantal point process whose large-N scaled kernel near the origin is a sum of two Bessel kernels with different indices rather than standard Airy or single-Bessel forms.
-
Universal Dynamical Scaling of Strong-to-Weak Spontaneous Symmetry Breaking in Open Quantum Systems
Symmetry class alone sets SWSSB correlation length growth to exponential (Z2, tc ~ ln L) or algebraic (U(1), tc ~ L^alpha with alpha filling-dependent) in open quantum systems, independent of spectral gap.
-
Kinetically constrained cavity QED: from blockaded ferromagnetism to long-range quantum scars
A blockade-restricted long-range model for Rydberg-cavity systems yields a distinct blockaded ferromagnetic/superradiant phase at equilibrium and long-range many-body scars with logarithmic entanglement dynamics out of equilibrium.
-
Unsupervised Learning of Quantum Phase Transitions for Bose-Hubbard lattice systems
Diffusion maps identify quantum phase transitions in Bose-Hubbard systems, including symmetry-protected topological phases and ergodic vs. many-body localized regimes, without prior order parameters or handcrafted observables.