Crystalline antiunitary symmetry in altermagnets selects pairing that produces robust nodal topological superconducting phases with Majorana flat bands and chiral edge states.
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Quantum fluctuations shift the Higgs mode eigenfrequency below the 2Δ gap in s-wave superconductors, producing an undamped pole that yields sharper signals in THG and Raman scattering.
Experimental preparation of a Dirac spin liquid candidate in a 114-atom Rydberg kagome array shows correlations consistent with a gapless U(1) state.
Symmetry and conservation laws alone yield nonlinear fluctuating hydrodynamics equations whose sound and heat modes both flow to a KPZ fixed point with dynamical exponent 3/2, confirmed by simulations matching the Prahofer-Spohn function.
DMRG calculations find trivial paramagnets on four Archimedean lattices, collinear Neel order on four others, competing phases including a possible spin liquid on the triangular lattice, and a likely Dirac spin liquid on the kagome lattice for the quantum dipolar XY model.
Quantum fluctuations melt classical quasiperiodic attractors in open driven-dissipative systems, producing finite Liouvillian lifetimes that vanish algebraically toward the classical limit with universal scaling in size and time.
A universal s-wave resonance is accessible in dipolar fermionic spin mixtures via microwave parameters, enabling tunable interactions and tetratomic bound states without losing shielding.
A purely electronic model for exciton-polarons in moiré lattices predicts density-dependent mass renormalization and sign change near correlated insulators.
Derivative feedback in PID control affects both conditional and unconditional squeezing of a mechanical quadrature in an optomechanical system and enables tracking of desired signals.
citing papers explorer
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Nodal Topological Superconductivity Driven by Crystalline Antiunitary Symmetry in Altermagnets
Crystalline antiunitary symmetry in altermagnets selects pairing that produces robust nodal topological superconducting phases with Majorana flat bands and chiral edge states.
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Quantum fluctuations and the emergence of in-gap Higgs mode in superconductors
Quantum fluctuations shift the Higgs mode eigenfrequency below the 2Δ gap in s-wave superconductors, producing an undamped pole that yields sharper signals in THG and Raman scattering.
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Dirac Spin Liquid Candidate in a Rydberg Quantum Simulator
Experimental preparation of a Dirac spin liquid candidate in a 114-atom Rydberg kagome array shows correlations consistent with a gapless U(1) state.
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Symmetry-based nonlinear fluctuating hydrodynamics in one dimension
Symmetry and conservation laws alone yield nonlinear fluctuating hydrodynamics equations whose sound and heat modes both flow to a KPZ fixed point with dynamical exponent 3/2, confirmed by simulations matching the Prahofer-Spohn function.
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Ground states of quantum XY dipoles on the Archimedean lattices
DMRG calculations find trivial paramagnets on four Archimedean lattices, collinear Neel order on four others, competing phases including a possible spin liquid on the triangular lattice, and a likely Dirac spin liquid on the kagome lattice for the quantum dipolar XY model.
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Universal quantum melting of quasiperiodic attractors in driven-dissipative cavities
Quantum fluctuations melt classical quasiperiodic attractors in open driven-dissipative systems, producing finite Liouvillian lifetimes that vanish algebraically toward the classical limit with universal scaling in size and time.
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Tunable Field-Linked $s$-wave Interactions in Dipolar Fermi Mixtures
A universal s-wave resonance is accessible in dipolar fermionic spin mixtures via microwave parameters, enabling tunable interactions and tetratomic bound states without losing shielding.
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Purely electronic model for exciton-polaron formation in moir\'e heterostructures
A purely electronic model for exciton-polarons in moiré lattices predicts density-dependent mass renormalization and sign change near correlated insulators.
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Squeezing and measurement of a mechanical quadrature via PID feedback
Derivative feedback in PID control affects both conditional and unconditional squeezing of a mechanical quadrature in an optomechanical system and enables tracking of desired signals.