Vortexable Chern Bands Sit Exactly on the Topological Floor of Flat-Band Superfluid Stiffness

arXiv:2610.24877 · cond-mat.supr-con, cond-mat.mes-hall, cond-mat.quant-gas, cond-mat.str-el · Submitted 2026-10-17 · Read on arXiv

cond-mat.supr-con, cond-mat.mes-hall, cond-mat.quant-gas, cond-mat.str-el

Submitted: 2026-10-17

Updated: 2026-10-17

Comments: 32 pages, 5 figures

License: http://creativecommons.org/licenses/by/4.0/

The gist: Vortexable Chern bands host ideal fractional Chern insulators.

Abstract

Vortexable Chern bands host ideal fractional Chern insulators. Paired with time-reversed partners by orbital-diagonal on-site attraction, they are the least stiff flat-band superconductors at fixed Chern number C, filling, and pairing amplitude. For uniform pairing and a nondegenerate paired state, the exact T=0 stiffness determinant is the topological floor times 1+(/2πC) 2 1+(/2πC) squared, where and measure departures from vortexability. Enhancement costs vortexability, and the inequality is strict only if internal components share a site, as in heterostrained bilayers.

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