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Rate of Convergence towards Hartree Dynamics with Singular Interaction Potential
Mathematical Physics · Submitted 24 Aug 2017
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We show that, with $H^1(\mathbb{R}^3)$ initial data, the difference between the many-body Schr\"odinger evolution in the mean-field regime and the corresponding Hartree dynamics is of order $1/N$, for any fixed time.
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The abstract, sentence by sentence
We consider a system of $N$-Bosons with a two-body interaction potential $V \in L^2(\mathbb{R}^3)+L^\infty(\mathbb{R}^3)$, possibly singular than the Coulomb interaction. We show that, with $H^1(\mathbb{R}^3)$ initial data, the difference between the many-body Schr\"odinger evolution in the mean-field regime and the corresponding Hartree dynamics is of order $1/N$, for any fixed time. The $N$-dependence of the bound is optimal.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We consider a system of $N$-Bosons with a two-body interaction potential $V \in L^2(\mathbb{R}^3)+L^\infty(\mathbb{R}^3)$, possibly singular than the Coulomb interaction. | background 0.84 | 0.24 | 0.03 | asserted 0.74 |
| s1 | We show that, with $H^1(\mathbb{R}^3)$ initial data, the difference between the many-body Schr\"odinger evolution in the mean-field regime and the corresponding Hartree dynamics is of order $1/N$, for any fixed time. | result 0.99 | 0.96 | 0.92 | asserted 1.00 |
| s2 | The $N$-dependence of the bound is optimal. | interpretation 0.61 | 0.79 | 0.12 | asserted 1.00 |
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The paper
Original abstract
We consider a system of $N$-Bosons with a two-body interaction potential $V \in L^2(\mathbb{R}^3)+L^\infty(\mathbb{R}^3)$, possibly singular than the Coulomb interaction. We show that, with $H^1(\mathbb{R}^3)$ initial data, the difference between the many-body Schr\"odinger evolution in the mean-field regime and the corresponding Hartree dynamics is of order $1/N$, for any fixed time. The $N$-dependence of the bound is optimal.
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1 arXiv paper cite this in 4 sentences
Papers whose main result relates to this one's
States the same result 1 paper
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We show that the difference between the many-body Schr\"odinger evolution in the mean-field regime and the effective nonlinear Hartree dynamics is at most of the order 1/N, for any fixed time.
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Compares with it 1 paper
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In particular, the above mentioned integral can be bounded via [equation] Whereas [ref] use the above decomposition of the interaction potential together with Strichartz estimates to control more singular potentials, we want to employ the fact that $|·|^-γ∈L^3/γ_w(^3)$ together with Strichartz estimates both for considering more singular potentials and lowering the required regularity on the initial datum $_0$.
Convergence rate towards the fractional Hartree-equation with singular potentials in higher Sobolev norms · Preliminary tools and notations · 0.80
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