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1122 · Apr 202419922001200920172026
13 results for eigensections

We derive a bound on the LL^{\infty}-norm of the covariant derivative of Laplace eigensections on general Riemannian vector bundles depending on the diameter, the dimension, the Ricci curvature of the underlying manifold, and the curvature of the Riemannian vector bundle. Our result implies that eigensections with sma…

2015-11-25abs ↗pdf ↗

Study on eigenfunctions on sphere configurations, proving non-existence and construction of critical eigensections.

problem Existence and rigidity of critical Z2 eigenvalues on sphere configurations.
method Algebraic identities and finite group representation theory.
result Construction of infinitely many configurations admitting critical eigensections and proof of deformation rigidity of Taubes-Wu tetrahedral eigensections.

Exponential localization of eigensections for Bochner-Schrödinger operator.

problem Understanding spectral properties of Bochner-Schrödinger operator on high tensor powers of Hermitian line bundles.
method Approximation of operator by model Schrödinger operator with constant magnetic field, analysis of spectrum.
result Spectrum of Bochner-Schrödinger operator in gaps is discrete and eigensections decay exponentially.

The paper studies spectral analysis on complex spaces and finds explicit formulas for eigensections.

problem Understanding eigensections on complex projective spaces and Grassmannians.
method Using creation and annihilation operators, converting higher energy eigensections to lower energy holomorphic sections.
result Explicit formulas for the dimension of higher-level eigensections on Pn\mathbb{P}^{n}.

Let YY be a compact, oriented 3-manifold with a contact form aa and a metric ds2ds^2. Suppose that FYF\to Y is a principal bundle with structure group U(2)=SU(2)×±1S1U(2) = SU(2)\times_{\pm1}S^1 such that F/S1F/S^1 is the principal SO(3) bundle of orthonormal frames for TYTY. A unitary connection A0A_0 on the Hermitian line bundle $…

2013-07-17abs ↗pdf ↗

We introduce and study new spectral invariant of two elliptic partial differential operators of Laplace and Dirac type on compact smooth manifolds without boundary that depends on both the eigenvalues and the eigensections of the operators, which is a equal to the regularized number of created particles from the vacuum…

2019-09-20abs ↗pdf ↗

We introduce and study {\it new} relative spectral invariants of {\it two} elliptic partial differential operators of Laplace and Dirac type on compact smooth manifolds without boundary that depend on both the eigenvalues and the eigensections of these operators and contain much more information about geometry. We prov…

2019-08-04abs ↗pdf ↗

It is known that a compact symplectic manifold endowed with a prequantum line bundle can be embedded in the projective space generated by the eigensections of low energy of the Bochner Laplacian acting on high pp-tensor powers of the prequantum line bundle. We show that the Fubini-Study forms induced by these embeddin…

2017-02-03abs ↗pdf ↗

Bounds on spectral gaps of hyperbolic 3-manifolds and orbifolds.

problem Constraining the spectra of Laplace operators on hyperbolic manifolds and orbifolds.
method Linear programming and spectral identities derived from the conformal bootstrap and Selberg trace formula.
result Upper bounds on the first and second Laplacian eigenvalues, and spectral gaps of hyperbolic 3-manifolds and orbifolds.

Study on G2G_{2}-instantons and Hermitian Yang-Mills connections, focusing on spectrum analysis.

problem Analyzing the spectrum of operators associated with G2G_{2}-instantons and Hermitian Yang-Mills connections.
method Using quaternion structure in Sasakian geometry, the paper describes the spectrum of a self-adjoint operator derived from these connections.
result The spectrum of the operator consists of both finitely many integers and infinitely many real numbers, with explicit descriptions of multiplicities and eigensections.

Generalizing work of W. Müller we investigate the spectral theory for the Dirac operator D on a noncompact manifold X with generalized fibred cusps C(M)=M×[A,[r,g=dr2+φgY+e2crgZ, C(M)=M\times [A,\infty[_r, g= d r^2+ φ^*g_Y+ e^{-2cr}g_Z, at infinity. Here φ:Mh+vYhφ:M^{h+v}\to Y^h is a compact fibre bundle with fibre Z and a distinguished horizontal s…

2001-02-08abs ↗pdf ↗