Cs1-δV2Te2O hosts hidden altermagnetism consisting of spatially alternating altermagnetic layers whose local spin polarizations are verified by spin-resolved ARPES.
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MnSb2 has been synthesized under high pressure and shows transport signatures of a flat band near the Fermi level consistent with DFT band structure.
CaSnN2 in the Pna21 structure has a direct bandgap of 2.59 eV at Gamma, corresponding to 478 nm blue light emission, with analyzed valence band symmetries, effective masses, and excitonic effects.
In noncentrosymmetric materials such as ferroelectric GeTe, charge current generation is dominated by the Rashba-Edelstein effect rather than spin or orbital Hall effects.
First-principles calculations with anharmonic corrections predict metastable metallic phases of RbH12 stable at pressures as low as 10 GPa exhibiting superconductivity with Tc between 46 and 111 K.
citing papers explorer
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Observation of hidden altermagnetism in Cs$_{1-\delta}$V$_2$Te$_2$O
Cs1-δV2Te2O hosts hidden altermagnetism consisting of spatially alternating altermagnetic layers whose local spin polarizations are verified by spin-resolved ARPES.
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Flat band in multiband-metal MnSb$_2$
MnSb2 has been synthesized under high pressure and shows transport signatures of a flat band near the Fermi level consistent with DFT band structure.
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Spin and orbital-to-charge conversion in noncentrosymmetric materials: Hall versus Rashba-Edelstein effects
In noncentrosymmetric materials such as ferroelectric GeTe, charge current generation is dominated by the Rashba-Edelstein effect rather than spin or orbital Hall effects.
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Superconductivity in RbH$_{12}$ at low pressures: an \emph{ab initio} study
First-principles calculations with anharmonic corrections predict metastable metallic phases of RbH12 stable at pressures as low as 10 GPa exhibiting superconductivity with Tc between 46 and 111 K.