In this paper we show that, for a sub-Laplacian Δ on a 3-dimensional manifold M, no point interaction centered at a point q0∈M exists. When M is complete w.r.t. the associated sub-Riemannian structure, this means that Δ acting on C0∞(M∖{q0}) is essentially self-adjoint in L2(M). A particular example is the standard sub-Laplacian on the Heisenberg group. This is in stark contrast with what happens in a Riemannian manifold N, whose associated Laplace-Beltrami operator acting on C0∞(N∖{q0}) is never essentially self-adjoint in L2(N), if dimN≤3. We then apply this result to the Schrödinger evolution of a thin molecule, i.e., with a vanishing moment of inertia, rotating around its center of mass.
Point interactions for 3D sub-Laplacians / Adami, R.; Boscain, U.; Franceschi, V.; Prandi, D.. - In: ANNALES DE L INSTITUT HENRI POINCARÉ. ANALYSE NON LINÉAIRE. - ISSN 0294-1449. - 38:4(2021), pp. 1095-1113. [10.1016/j.anihpc.2020.10.007]
Point interactions for 3D sub-Laplacians
Adami R.;
2021
Abstract
In this paper we show that, for a sub-Laplacian Δ on a 3-dimensional manifold M, no point interaction centered at a point q0∈M exists. When M is complete w.r.t. the associated sub-Riemannian structure, this means that Δ acting on C0∞(M∖{q0}) is essentially self-adjoint in L2(M). A particular example is the standard sub-Laplacian on the Heisenberg group. This is in stark contrast with what happens in a Riemannian manifold N, whose associated Laplace-Beltrami operator acting on C0∞(N∖{q0}) is never essentially self-adjoint in L2(N), if dimN≤3. We then apply this result to the Schrödinger evolution of a thin molecule, i.e., with a vanishing moment of inertia, rotating around its center of mass.| File | Dimensione | Formato | |
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https://hdl.handle.net/11583/2875552
			
		
	
	
	
			      	