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Implications of setting ds = 0 to remove Berry-phase ambiguity

Ascertain the mathematical and physical implications of the heuristic replacement ds = 0 that eliminates the Berry-phase–induced non-uniqueness in the spinor definition under coordinate rotation, specifically in the diagonalization of H(\mathrm{d}\boldsymbol{x}) and the construction of covariant spinor bases using V(\mathrm{d}\boldsymbol{x}) and (\mathrm{d}s^2)^{1/4}.

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Background

When diagonalizing the Weyl Hamiltonian H(\mathrm{d}\boldsymbol{x}) with differential-form parameters, coordinate rotations induce a Berry phase, leading to non-uniqueness in the spinor basis up to a phase. The authors show that by formally setting \mathrm{d}s → 0, the Berry phase tends to unity, thereby removing the ambiguity.

However, the authors explicitly note that the implication of this heuristic procedure is unclear, motivating a careful investigation into its justification and consequences for the proposed spinor framework based on differential forms.

References

We also discuss the ambiguity of the definition of the spinor under coordinate rotation originating from Berry's phase, and point out that if we heuristically set $ \mathrm{d}s=0 $, the ambiguity disappears, though its implication remains unclear.

Basis of spinors expressed by differential forms and calculating its norm (2403.13003 - Takahashi, 13 Mar 2024) in Abstract