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Semiclassical trace formula for the Bochner-Schrödinger operator

Yuri A. Kordyukov

TL;DR

This work develops a semiclassical trace framework for the Bochner-Schrödinger operator $H_p=\frac{1}{p^2}\Delta^{L^p\otimes E}+V$ on manifolds of bounded geometry. By localizing to normal coordinates, rescaling, and applying Dynkin-Helffer-Sjöstrand functional calculus, the authors obtain a complete near-diagonal asymptotic expansion of the Schwartz kernel $K_{\varphi(H_p)}$ as $p\to\infty$, with diagonal coefficients $f_r(x_0)$ expressed as universal polynomials in derivatives of $V$ and the curvatures. In the compact case this yields a full trace expansion $\operatorname{tr}\varphi(H_p)\sim p^{d}\sum_{r=0}^{\infty}f_r(\varphi) p^{-r}$, where the coefficients are local and gauge-invariant. The approach avoids magnetic pseudodifferential calculus by adapting Bergman-kernel localization techniques and provides explicit formulas for $f_1$ and $f_2$ in the Euclidean gauge model, illustrating the structure of the coefficients. These results extend prior magnetic trace formulas to a broad geometric setting and offer a robust tool for semiclassical spectral analysis on manifolds with bounded geometry.

Abstract

We study the semiclassical Bochner-Schrödinger operator $H_{p}=\frac{1}{p^2}Δ^{L^p\otimes E}+V$ on tensor powers $L^p$ of a Hermitian line bundle $L$ twisted by a Hermitian vector bundle $E$ on a Riemannian manifold of bounded geometry. For any function $\varphi\in C^\infty_c(\mathbb R)$, we consider the bounded linear operator $\varphi(H_p)$ in $L^2(X,L^p\otimes E)$ defined by the spectral theorem. We prove that its smooth Schwartz kernel on the diagonal admits a complete asymptotic expansion in powers of $p^{-1}$ in the semiclassical limit $p\to \infty$. In particular, when the manifold is compact, we get a complete asymptotic expansion for the trace of $\varphi(H_p)$.

Semiclassical trace formula for the Bochner-Schrödinger operator

TL;DR

This work develops a semiclassical trace framework for the Bochner-Schrödinger operator on manifolds of bounded geometry. By localizing to normal coordinates, rescaling, and applying Dynkin-Helffer-Sjöstrand functional calculus, the authors obtain a complete near-diagonal asymptotic expansion of the Schwartz kernel as , with diagonal coefficients expressed as universal polynomials in derivatives of and the curvatures. In the compact case this yields a full trace expansion , where the coefficients are local and gauge-invariant. The approach avoids magnetic pseudodifferential calculus by adapting Bergman-kernel localization techniques and provides explicit formulas for and in the Euclidean gauge model, illustrating the structure of the coefficients. These results extend prior magnetic trace formulas to a broad geometric setting and offer a robust tool for semiclassical spectral analysis on manifolds with bounded geometry.

Abstract

We study the semiclassical Bochner-Schrödinger operator on tensor powers of a Hermitian line bundle twisted by a Hermitian vector bundle on a Riemannian manifold of bounded geometry. For any function , we consider the bounded linear operator in defined by the spectral theorem. We prove that its smooth Schwartz kernel on the diagonal admits a complete asymptotic expansion in powers of in the semiclassical limit . In particular, when the manifold is compact, we get a complete asymptotic expansion for the trace of .

Paper Structure

This paper contains 8 sections, 9 theorems, 138 equations.

Key Result

Theorem 1.2

The following asymptotic expansion holds true uniformly in $x_0\in X$: where $f_{r},$$r=0,1,\ldots$, is a smooth section of the vector bundle $\operatorname{End}(E)$ on $X$. The leading coefficient of this expansion is given by The next coefficients have the form where $P_{r, \ell,x_0}(\xi)$ is a universal polynomial depending on a finite number of derivatives of $V$ and the curvatures $R^{TX}$

Theorems & Definitions (15)

  • Example 1.1
  • Theorem 1.2
  • Theorem 1.3
  • Theorem 1.4
  • Proposition 2.1
  • Example 2.2
  • Example 3.1
  • Theorem 4.1
  • proof
  • Proposition 4.2
  • ...and 5 more