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max ∼200 K eventually.
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32
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33744692389
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note
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(1/2)qi which is familiar from Chern-Simons transformations for the QHE problem.
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33744568196
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note
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Dirac. Thus the transformation ψ(x,y)→τψ*(-x,-y) leaves the crystal momentum unaffected, while changing the sign of the energy.
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-
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35
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33744646561
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note
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Strictly speaking, we just need to have an odd number of doublets at zero energy, which in the generic case will be just one doublet.
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-
-
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36
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33744587258
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note
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This is guaranteed at node 1, 1(2,2) if the vortex lattice is symmetric under the reflection x→-x (y→-y).
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-
-
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37
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33744614354
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note
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D for the opposite nodes may be proved more generally, and holds even in the absence of inversion symmetry. It derives from the intrinsic particle-hole symmetry present in the, Boguliubov-de Gennes equation, that relates the opposite nodes.
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39
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