Alterelectricity is introduced as switchable states with alternating band structures arising from sublattice-selective structural changes related by non-inversion symmetry, with realizations in bilayer sliding and ferroelectric materials plus a proposed tunnel junction application.
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8 Pith papers cite this work. Polarity classification is still indexing.
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Pith papers citing it
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Symmetry classification framework for unconventional magnetism identifies hybrid-parity and unconstrained-parity classes beyond altermagnets and odd-parity magnets, with computational example of combined spintronic effects.
Crystalline antiunitary symmetry in altermagnets selects pairing that produces robust nodal topological superconducting phases with Majorana flat bands and chiral edge states.
Static lattice distortions from adiabatic electron-phonon coupling act as a tuning knob that alters the magnitude, anisotropy, phase, and chirality of noncollinear RKKY couplings in Rashba d-wave altermagnets.
CrSb is a high-temperature metallic altermagnet with coherent magnons of group velocities 61 and 58 km/s that exhibit chiral momentum-space splitting, described by a minimal Heisenberg model with alternating exchange interactions.
Slow phonons suppress the spin Edelstein effect in strained Rashba d-wave altermagnets through energy renormalization that collapses the Fermi surface, producing tunable anisotropic depolarization.
Orbital altermagnetism is defined as a symmetry-protected order of orbital magnetic moments with d-wave-like momentum locking, shown via tight-binding models and DFT in materials such as CuBr2, VS2, MoO and CrO.
Theoretical proposal for magnetic-field-free deterministic Néel vector switching in d-wave altermagnets using octupole torque from current-induced multipole injection in bilayers.
citing papers explorer
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Alterelectricity: Electrical Analogue of Altermagnetism
Alterelectricity is introduced as switchable states with alternating band structures arising from sublattice-selective structural changes related by non-inversion symmetry, with realizations in bilayer sliding and ferroelectric materials plus a proposed tunnel junction application.
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Unconventional Magnetism: Symmetry Classification, Hybrid-parity and Unconstrained-parity Classes
Symmetry classification framework for unconventional magnetism identifies hybrid-parity and unconstrained-parity classes beyond altermagnets and odd-parity magnets, with computational example of combined spintronic effects.
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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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RKKY interaction in altermagnets with adiabatic electron-phonon coupling
Static lattice distortions from adiabatic electron-phonon coupling act as a tuning knob that alters the magnitude, anisotropy, phase, and chirality of noncollinear RKKY couplings in Rashba d-wave altermagnets.
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Coherent high-velocity chiral magnons in the metallic altermagnet CrSb
CrSb is a high-temperature metallic altermagnet with coherent magnons of group velocities 61 and 58 km/s that exhibit chiral momentum-space splitting, described by a minimal Heisenberg model with alternating exchange interactions.
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Slow-phonon control of spin Edelstein effect in Rashba $d$-wave altermagnets
Slow phonons suppress the spin Edelstein effect in strained Rashba d-wave altermagnets through energy renormalization that collapses the Fermi surface, producing tunable anisotropic depolarization.
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Orbital Altermagnetism
Orbital altermagnetism is defined as a symmetry-protected order of orbital magnetic moments with d-wave-like momentum locking, shown via tight-binding models and DFT in materials such as CuBr2, VS2, MoO and CrO.
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Deterministic N\'eel vector switching of altermagnets via magnetic octupole torque
Theoretical proposal for magnetic-field-free deterministic Néel vector switching in d-wave altermagnets using octupole torque from current-induced multipole injection in bilayers.