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Higher Willmore Energies from tractor coupled GJMS operators

Ben F. Allen, Rod Gover

TL;DR

This work extends the Willmore energy paradigm to higher-dimensional, higher-codimension submanifolds in conformally flat spaces by constructing a conformally invariant energy via coupling the ambient tractor connection to the submanifold's intrinsic GJMS operator. It presents two complementary energies: a GJMS energy defined by $\tilde{\mathcal{E}}=\int_{\Sigma}N^A{}_B P_m N^B{}_A\, dv^{\Sigma}_{\bar{\boldsymbol{g}}}$ and, in four dimensions, a $Q$-operator based energy derived from the tractor second fundamental form, with a precise density formula. The paper analyzes the relation between these energies, including an explicit comparison to the Graham–Reichert energy in dimension four, and proves that both energies are of Willmore-type by identifying their leading derivative terms. The development relies on a detailed tractor-calculus framework for conformal submanifolds, including tangent/normal tractor bundles, the tractor second fundamental form, and Gauss–Codazzi-type equations, providing direct, conformally invariant densities that generalize Willmore theory beyond hypersurfaces. Overall, the results offer new direct PDE- and invariant-theory tools for higher-dimensional Willmore-type variational problems with potential connections to holographic approaches.

Abstract

We define and construct a conformally invariant energy for closed smoothly immersed submanifolds of even dimension, but of arbitrary codimension, in conformally flat Riemannian manifolds. This is a higher dimensional analogue of the Willmore energy for immersed surfaces and is given directly via a coupling of the tractor connection to the (submanifold critical) GJMS operators. In the case where the submanifold is of dimension 4 we compare this to other energies, including one found using a second simple construction that uses $Q$-operators.

Higher Willmore Energies from tractor coupled GJMS operators

TL;DR

This work extends the Willmore energy paradigm to higher-dimensional, higher-codimension submanifolds in conformally flat spaces by constructing a conformally invariant energy via coupling the ambient tractor connection to the submanifold's intrinsic GJMS operator. It presents two complementary energies: a GJMS energy defined by and, in four dimensions, a -operator based energy derived from the tractor second fundamental form, with a precise density formula. The paper analyzes the relation between these energies, including an explicit comparison to the Graham–Reichert energy in dimension four, and proves that both energies are of Willmore-type by identifying their leading derivative terms. The development relies on a detailed tractor-calculus framework for conformal submanifolds, including tangent/normal tractor bundles, the tractor second fundamental form, and Gauss–Codazzi-type equations, providing direct, conformally invariant densities that generalize Willmore theory beyond hypersurfaces. Overall, the results offer new direct PDE- and invariant-theory tools for higher-dimensional Willmore-type variational problems with potential connections to holographic approaches.

Abstract

We define and construct a conformally invariant energy for closed smoothly immersed submanifolds of even dimension, but of arbitrary codimension, in conformally flat Riemannian manifolds. This is a higher dimensional analogue of the Willmore energy for immersed surfaces and is given directly via a coupling of the tractor connection to the (submanifold critical) GJMS operators. In the case where the submanifold is of dimension 4 we compare this to other energies, including one found using a second simple construction that uses -operators.

Paper Structure

This paper contains 19 sections, 13 theorems, 127 equations, 1 figure.

Key Result

Theorem 1.1

Let $\Sigma^m\rightarrow M$ be a closed submanifold of even dimension $m$ immersed in a conformally flat Riemannian manifold $M$ of arbitrary codimension. There is a conformally invariant energy $\Tilde{\mathcal{E}}$ on $\Sigma$ of Willmore-type defined by where $N^A_B$ is the normal tractor projector and $P^\nabla_m$ is the intrinsic critical GJMS operator coupled to the ambient tractor connecti

Figures (1)

  • Figure 1: Tractor inner product

Theorems & Definitions (23)

  • Theorem 1.1
  • Theorem 1.2
  • Lemma 2.1
  • proof
  • Proposition 3.1
  • proof
  • Corollary 3.2
  • proof
  • Proposition 3.3
  • Proposition 3.4
  • ...and 13 more