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On the nu-invariant of two-step nilmanifolds with closed G2-structure

Anna Fino, Gueo Grantcharov, Giovanni Russo

TL;DR

The paper computes the ν-invariant for specific left-invariant closed G2-structures on compact two-step nilmanifolds by combining spin geometry with Kirillov representation theory. It shows that the space of harmonic spinors is always even-dimensional and contains non-invariant spinors, and that η-invariants vanish via orientation-reversing isometries while the Mathai-Quillen current vanishes for the relevant harmonic spinors. For the h1 and h2 cases, the ν-invariant vanishes on the invariant harmonic spinors for the one- and two-parameter families φ_a and φ_{b1,b2}, respectively. The results provide explicit vanishing of ν in these non-integrable settings and illustrate a workflow to analyze ν on higher-step nilmanifolds using Kirillov theory and invariant geometric data.

Abstract

For every non-vanishing spinor field on a Riemannian spin seven-manifold, Crowley, Goette, and Nordström defined the so-called $ν$-invariant. This is an integer modulo $48$ that detects connected components of the moduli space of $\mathrm G_2$-structures on any seven-dimensional oriented spin manifold. The $ν$-invariant can be defined in terms of Mathai--Quillen currents, harmonic spinors, and $η$-invariants of spin Dirac and odd-signature operator. We compute these data for certain families of left-invariant closed $\mathrm G_2$-structures on compact two-step nilmanifolds with their natural spin structure. Specifically, we establish the existence of non-invariant harmonic spinors and determine the parity of the dimension of the space of harmonic spinors. We deduce the vanishing of $ν$ on invariant harmonic spinors.

On the nu-invariant of two-step nilmanifolds with closed G2-structure

TL;DR

The paper computes the ν-invariant for specific left-invariant closed G2-structures on compact two-step nilmanifolds by combining spin geometry with Kirillov representation theory. It shows that the space of harmonic spinors is always even-dimensional and contains non-invariant spinors, and that η-invariants vanish via orientation-reversing isometries while the Mathai-Quillen current vanishes for the relevant harmonic spinors. For the h1 and h2 cases, the ν-invariant vanishes on the invariant harmonic spinors for the one- and two-parameter families φ_a and φ_{b1,b2}, respectively. The results provide explicit vanishing of ν in these non-integrable settings and illustrate a workflow to analyze ν on higher-step nilmanifolds using Kirillov theory and invariant geometric data.

Abstract

For every non-vanishing spinor field on a Riemannian spin seven-manifold, Crowley, Goette, and Nordström defined the so-called -invariant. This is an integer modulo that detects connected components of the moduli space of -structures on any seven-dimensional oriented spin manifold. The -invariant can be defined in terms of Mathai--Quillen currents, harmonic spinors, and -invariants of spin Dirac and odd-signature operator. We compute these data for certain families of left-invariant closed -structures on compact two-step nilmanifolds with their natural spin structure. Specifically, we establish the existence of non-invariant harmonic spinors and determine the parity of the dimension of the space of harmonic spinors. We deduce the vanishing of on invariant harmonic spinors.
Paper Structure (8 sections, 10 theorems, 100 equations)

This paper contains 8 sections, 10 theorems, 100 equations.

Key Result

Theorem 1

Let $\mathfrak g$ be a two-step nilpotent seven-dimensional Lie algebra admitting a closed $\mathrm G_2$-structure. Let $G$ be the corresponding connected, simply connected Lie group, and let $M$ denote a quotient of $G$ by some cocompact lattice $\Gamma$. The following hold for the trivial spin str

Theorems & Definitions (19)

  • Theorem
  • Lemma 2.1
  • Lemma 2.2
  • proof
  • Lemma 2.3
  • proof
  • Proposition 2.4
  • proof
  • Proposition 2.5
  • proof
  • ...and 9 more