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Wave Operators for Schr\"odinger Operators with Threshold Singuralities, Revisited

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abstract

The continuity property in the Sobolev space $W^{k,p}({\bf R}^m)$ of wave operators of scattering theory for $m$-dimensional single-body Schr\"odinger operator is considered when the resolvent of the operator has singularities at the bottom of the continuous spectrum. It is shown that they are continuous in $W^{k,p}({\bf R}^m)$, $0\leq k \leq 2$, for $1<p<3$ but not for $p>3$ if $m=3$ and, for $1<p<m/2$ but not for $p>m/2$ if $m\geq 5$. This extends the previously known interval of $p$ for the continuity, $3/2<p<3$ for $m=3$ and $m/(m-2)<p<m/2$ for $m\geq 5$. The formula which represents the integral kernel of the resolvent of the even dimensional free Sch\"odinger operator as the superposition of exponential-polynomial like functions substantially simplifies the proof of the previous paper when $m \geq 6$ is even.

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math.AP 1

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2024 1

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representative citing papers

Intertwining operators beyond the Stark Effect

math.AP · 2024-12-05 · conditional · novelty 6.0

In two dimensions, for scaling-critical electromagnetic Schrödinger operators with mean flux outside 1/2 Z (or with symmetric electric potential in the resonant case), the newly defined intertwining operators are L^p-bounded and transfer key estimates from the magnetic-only operator.

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  • Intertwining operators beyond the Stark Effect math.AP · 2024-12-05 · conditional · none · ref 44 · internal anchor

    In two dimensions, for scaling-critical electromagnetic Schrödinger operators with mean flux outside 1/2 Z (or with symmetric electric potential in the resonant case), the newly defined intertwining operators are L^p-bounded and transfer key estimates from the magnetic-only operator.