Spin Rotatory Strength as the Equilibrium Observable for Chiral-Induced Spin Selectivity
Abstract
We identify the spin rotatory strength---a chirality-odd, finite-frequency spin--dipole cross response---as the equilibrium observable for chiral-induced spin selectivity. Time-reversal symmetry forces the static response to vanish, while nonzero SU(2) Wilson-loop flux is an independent necessary condition. Exact diagonalization of a Kane--Mele--Hubbard model ($N{=}4,6,8$) reveals that gapped molecules robustly suppress the response, whereas near-degenerate systems show amplification at small $N...
Description / Details
We identify the spin rotatory strength---a chirality-odd, finite-frequency spin--dipole cross response---as the equilibrium observable for chiral-induced spin selectivity. Time-reversal symmetry forces the static response to vanish, while nonzero SU(2) Wilson-loop flux is an independent necessary condition. Exact diagonalization of a Kane--Mele--Hubbard model () reveals that gapped molecules robustly suppress the response, whereas near-degenerate systems show amplification at small whose persistence at larger sizes remains open.
Source: arXiv:2608.10697v1 - http://arxiv.org/abs/2608.10697v1 PDF: https://arxiv.org/pdf/2608.10697v1 Original Link: http://arxiv.org/abs/2608.10697v1
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Aug 12, 2026
Chemistry
Chemistry
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