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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Scattering and interference dominate circular-dichroic ARPES signals in graphene and WSe2, complicating extraction of initial-state orbital angular momentum.
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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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Scattering makes a difference in circular dichroic angle-resolved photoemission
Scattering and interference dominate circular-dichroic ARPES signals in graphene and WSe2, complicating extraction of initial-state orbital angular momentum.