P-wave orbital magnetism protected by combined translation and time-reversal symmetry is proposed to originate from loop-current-induced orbital textures in a 2D Dirac lattice model, measurable via orbital Hall conductivity.
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A universal analytic formula for the TMR ratio in X-wave magnet junctions is derived, proportional to |J|/(N_X Γ) for small Γ, in contrast to the J²/Γ² dependence for ferromagnets.
Second-order nonlinear response to a temperature gradient induces magnetization in d′, g′, and i′ altermagnets (and in d-wave for arbitrary gradient direction), but not in the corresponding unprimed g- and i-wave cases.
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$P$-wave Orbital Magnetism
P-wave orbital magnetism protected by combined translation and time-reversal symmetry is proposed to originate from loop-current-induced orbital textures in a 2D Dirac lattice model, measurable via orbital Hall conductivity.
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Tunneling magnetoresistance in a junction made of $X$-wave magnets with $X=p,d,f,g,i$
A universal analytic formula for the TMR ratio in X-wave magnet junctions is derived, proportional to |J|/(N_X Γ) for small Γ, in contrast to the J²/Γ² dependence for ferromagnets.
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Magnetization induced by a nonlinear response to temperature gradient in $d^{\prime }$, $g^{\prime }$ and $i^{\prime }$ altermagnets
Second-order nonlinear response to a temperature gradient induces magnetization in d′, g′, and i′ altermagnets (and in d-wave for arbitrary gradient direction), but not in the corresponding unprimed g- and i-wave cases.