Extensions of Schrödinger operators that generate $C_0$ contraction semigroups
- URL: http://arxiv.org/abs/2506.00231v1
- Date: Fri, 30 May 2025 21:08:15 GMT
- Title: Extensions of Schrödinger operators that generate $C_0$ contraction semigroups
- Authors: Lawrence Frolov,
- Abstract summary: Tumulka argued that the dynamics of $psi$ must be governed by a $C_0$ contraction semigroup.<n>We show that all such evolutions are generated by the placement of (potentially nonlocal) absorbing boundary conditions on $psi$ along $partial Omega$.
- Score: 0.0
- License: http://creativecommons.org/licenses/by/4.0/
- Abstract: Consider a non-relativistic quantum particle with wave function $\psi$ in a bounded $C^2$ region $\Omega \subset \mathbb{R}^n$, and suppose detectors are placed along the boundary $\partial \Omega$. Assume the detection process is irreversible, its mechanism is time independent and also hard, i.e., detections occur only along the boundary $\partial \Omega$. Under these conditions Tumulka argued that the dynamics of $\psi$ must be governed by a $C_0$ contraction semigroup that weakly solves the Schr\"odinger equation and proposed modeling the detector by a time-independent local absorbing boundary condition at $\partial \Omega$. In this paper, we apply the newly discovered theory of boundary quadruples to parameterize all $C_0$ contraction semigroups whose generators extend the Schr\"odinger Hamiltonian, and prove a variant of Tumulka's claim: all such evolutions are generated by the placement of (potentially nonlocal) absorbing boundary conditions on $\psi$ along $\partial \Omega$. We combine this result with the work of Werner to show that each $C_0$ contraction semigroup naturally admits a probability distribution for the time of detection along $\partial \Omega$, and we prove for a wide class of absorbing boundary conditions that the probability of the particle being ever detected is equal to $1$.
Related papers
- Practical Criteria for Entanglement and Nonlocality in Systems with Additive Observables [44.99833362998488]
For general bipartite mixed states, a sufficient and necessary mathematical condition for certifying entanglement and/or (Bell) non-locality remains unknown.<n>We derive very simple, handy criteria for detecting entanglement or non-locality in many cases.<n>We illustrate these results by analyzing the potential detection of entanglement and nonlocality in Higgs to ZZ decays at the LHC.
arXiv Detail & Related papers (2025-03-21T16:48:04Z) - Geometric bound on structure factor [44.99833362998488]
We show that a quadratic form of quantum geometric tensor in $k$-space sets a bound on the $q4$ term in the static structure factor $S(q)$ at small $vecq$.<n> Bands that saturate this bound satisfy a condition similar to Laplace's equation, leading us to refer to them as $textitharmonic bands$.
arXiv Detail & Related papers (2024-12-03T18:30:36Z) - Hamiltonians for Quantum Systems with Contact Interactions [49.1574468325115]
We show that in the limit one obtains the one-body Hamiltonian for the light particle subject to $N$ (non-local) point interactions placed at fixed positions.
We will verify that such non-local point interactions do not exhibit the ultraviolet pathologies that are present in the case of standard local point interactions.
arXiv Detail & Related papers (2024-07-09T14:04:11Z) - Convergence rates for the Trotter-Kato splitting [1.3624495460189865]
We study convergence rates of the Trotter-Kato splitting $eA+L = lim_n to infty (eL/n eA/n)n$ in the strong operator topology.
arXiv Detail & Related papers (2024-07-04T16:37:54Z) - A Unified Framework for Uniform Signal Recovery in Nonlinear Generative
Compressed Sensing [68.80803866919123]
Under nonlinear measurements, most prior results are non-uniform, i.e., they hold with high probability for a fixed $mathbfx*$ rather than for all $mathbfx*$ simultaneously.
Our framework accommodates GCS with 1-bit/uniformly quantized observations and single index models as canonical examples.
We also develop a concentration inequality that produces tighter bounds for product processes whose index sets have low metric entropy.
arXiv Detail & Related papers (2023-09-25T17:54:19Z) - Rigorous derivation of the Efimov effect in a simple model [68.8204255655161]
We consider a system of three identical bosons in $mathbbR3$ with two-body zero-range interactions and a three-body hard-core repulsion of a given radius $a>0$.
arXiv Detail & Related papers (2023-06-21T10:11:28Z) - A Law of Robustness beyond Isoperimetry [84.33752026418045]
We prove a Lipschitzness lower bound $Omega(sqrtn/p)$ of robustness of interpolating neural network parameters on arbitrary distributions.
We then show the potential benefit of overparametrization for smooth data when $n=mathrmpoly(d)$.
We disprove the potential existence of an $O(1)$-Lipschitz robust interpolating function when $n=exp(omega(d))$.
arXiv Detail & Related papers (2022-02-23T16:10:23Z) - Conditions for realizing one-point interactions from a multi-layer
structure model [77.34726150561087]
A heterostructure composed of $N$ parallel homogeneous layers is studied in the limit as their widths shrink to zero.
The problem is investigated in one dimension and the piecewise constant potential in the Schr"odinger equation is given.
arXiv Detail & Related papers (2021-12-15T22:30:39Z) - The Schr\"odinger particle on the half-line with an attractive
$\delta$-interaction: bound states and resonances [0.0]
We describe a self-adjoint Hamiltonian operator representing the negative Laplacian on the positive half-line with a Dirichlet (resp. Neuman)
We show that both systems exhibit resonances as poles of the analytic continuation of the resolvent.
arXiv Detail & Related papers (2021-04-14T09:53:31Z) - Scattering data and bound states of a squeezed double-layer structure [77.34726150561087]
A structure composed of two parallel homogeneous layers is studied in the limit as their widths $l_j$ and $l_j$, and the distance between them $r$ shrinks to zero simultaneously.
The existence of non-trivial bound states is proven in the squeezing limit, including the particular example of the squeezed potential in the form of the derivative of Dirac's delta function.
The scenario how a single bound state survives in the squeezed system from a finite number of bound states in the finite system is described in detail.
arXiv Detail & Related papers (2020-11-23T14:40:27Z) - Energy-Time Uncertainty Relation for Absorbing Boundaries [0.0]
We prove the uncertainty relation $sigma_T, sigma_E geq hbar/2$ between the time $T$ of detection of a quantum particle on the surface.
arXiv Detail & Related papers (2020-05-29T12:04:57Z) - Existence of Schrodinger Evolution with Absorbing Boundary Condition [0.0]
Consider a non-relativistic quantum particle with wave function inside a region $Omegasubset mathbbR3$.
The question how to compute the probability distribution of the time at which the detector surface registers the particle boils down to finding a reasonable mathematical definition of an ideal detecting surface.
A particularly convincing definition, called the absorbing boundary rule, involves a time evolution for the particle's wave function $psi$ expressed by a Schrodinger equation in $Omega$ together with an "absorbing" boundary condition on $partial Omega$ first considered by Werner in
arXiv Detail & Related papers (2019-12-27T10:53:31Z) - Detection Time Distribution for Several Quantum Particles [0.0]
We address the question of how to compute the probability distribution of the time at which a detector clicks.
A key element of this extension is that, upon a detection event, the wave function gets collapsed by inserting the detected position.
We also describe an extension of the absorbing boundary rule to the case of moving detectors.
arXiv Detail & Related papers (2016-01-15T10:56:51Z)
This list is automatically generated from the titles and abstracts of the papers in this site.
This site does not guarantee the quality of this site (including all information) and is not responsible for any consequences.