Introduces spinor pairing orders with half-integer monopole charges from odd Chern number differences between paired Fermi surfaces, shown in tight-binding models with single gap nodes and fractional Mermin-Ho relations.
\ Turner , author Ashvin \ Vishwanath , \ and\ author Sergey Y
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AMTe4 (A=Ta,Nb; M=Ir,Rh) compounds host Weyl points within a few meV of the Fermi energy, including multiple types such as type-I, II, and III in NbRhTe4, substantially revising the topological electronic structure.
Floating-zone-grown RAlGe (R=Pr,Ce) crystals achieve 1:1:1 stoichiometry in I4₁md structure and display spin-glass and antiferromagnetic orders instead of the expected ferromagnetism.
citing papers explorer
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Berry Phase Enforced Spinor Pairing Order
Introduces spinor pairing orders with half-integer monopole charges from odd Chern number differences between paired Fermi surfaces, shown in tight-binding models with single gap nodes and fractional Mermin-Ho relations.
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Fermi energy Weyl nodes in $\mathbf{AM}$Te$_4$ ($\mathbf{A}$=Ta, Nb, $\mathbf{M}$=Ir, Rh)
AMTe4 (A=Ta,Nb; M=Ir,Rh) compounds host Weyl points within a few meV of the Fermi energy, including multiple types such as type-I, II, and III in NbRhTe4, substantially revising the topological electronic structure.
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Bulk single crystal growth of the theoretically predicted magnetic Weyl semimetals $R$AlGe ($R$ = Pr, Ce)
Floating-zone-grown RAlGe (R=Pr,Ce) crystals achieve 1:1:1 stoichiometry in I4₁md structure and display spin-glass and antiferromagnetic orders instead of the expected ferromagnetism.