Moiré strain Skyrmions form an elastic ground-state lattice in twisted bilayers and display a chirality-dependent Skyrmion Hall effect under interlayer sliding whose angle is inversely proportional to the twist angle.
Castro Neto, F
8 Pith papers cite this work. Polarity classification is still indexing.
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cond-mat.mes-hall 2 cond-mat.mtrl-sci 2 cond-mat.str-el 2 physics.chem-ph 1 physics.comp-ph 1years
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High magnetic fields directly enhance the amplitude and correlation length of stripe order in a cuprate superconductor far above the vortex melting transition, indicating a coupling mechanism independent of superconductivity suppression.
A reorganized Hartree-Fock framework imposes tunable orbital locality by pairing local degrees of freedom with local solution conditions, maintaining efficient SCF optimization and competitive reaction-energy accuracy.
Exact vs. restricted particle-hole dynamics in graphene flakes after optical quench shows periodic structures captured by low-order excitations but confined ones require higher-order contributions, positioning the setup as a quantum-computing benchmark.
DFT study reports that As substitution and interstitial doping in MoS2 monolayer introduce midgap defect states and shift the Fermi level to produce p-type or n-type character depending on site.
Quantum confinement in 2D hexagonal crystals like graphene and TMDs produces discrete electronic and excitonic spectra with strongly amplified interactions that enable correlated quantum states.
Certain biomembrane shapes like cylinders, spheres, tori, biconcave discoids, and Delaunay surfaces form a geometric group independent of the specific biomembrane equation when pressure, tension, and bending moduli meet particular conditions.
Exciton polaritons in microcavities form synthetic photonic crystals with engineered band structures and interactions for exploring many-body physics from mean-field to quantum regimes.
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Liquid Crystal Theory of Biomembranes
Certain biomembrane shapes like cylinders, spheres, tori, biconcave discoids, and Delaunay surfaces form a geometric group independent of the specific biomembrane equation when pressure, tension, and bending moduli meet particular conditions.