Transconductance in multilayer WSe2 exhibits a valley-crossover signature quantified by valley susceptibility χ_v reaching ~0.20 V^{-1} in bilayer devices, absent in single-valley systems and bounded by the thermodynamic limit (4k_BT)^{-1}.
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Thermoelectric and non-reciprocal transport effects are predicted as accessible probes for spin- and valley-polarized states in hybrid Ising superconductor and van der Waals material junctions.
Theory demonstrates that reduced symmetry in TMD heterobilayers enables electric-dipole spin-flip transitions between conduction band subbands via spin-orbit mixing, with rates greatly exceeding magnetic-dipole transitions.
First-order transitions emerge in weak-ISOC superconductors under large exchange fields, with the gap equation yielding only the supercooling field and two in-gap coherence peaks appearing as weak-ISOC mirage-gap signatures.
citing papers explorer
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Transconductance as a Probe of Valley Thermodynamics in Multilayer WSe$_2$
Transconductance in multilayer WSe2 exhibits a valley-crossover signature quantified by valley susceptibility χ_v reaching ~0.20 V^{-1} in bilayer devices, absent in single-valley systems and bounded by the thermodynamic limit (4k_BT)^{-1}.
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Detection of spin- and valley-polarized states in van der Waals materials via thermoelectric and non-reciprocal transport
Thermoelectric and non-reciprocal transport effects are predicted as accessible probes for spin- and valley-polarized states in hybrid Ising superconductor and van der Waals material junctions.
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Intersubband electric dipole spin resonance in transition metal dichalcogenide heterobilayers
Theory demonstrates that reduced symmetry in TMD heterobilayers enables electric-dipole spin-flip transitions between conduction band subbands via spin-orbit mixing, with rates greatly exceeding magnetic-dipole transitions.
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First-Order Transitions in Weak Ising Spin-Orbit-Coupled Superconductors
First-order transitions emerge in weak-ISOC superconductors under large exchange fields, with the gap equation yielding only the supercooling field and two in-gap coherence peaks appearing as weak-ISOC mirage-gap signatures.