Žurnal matematičeskoj fiziki, analiza, geometrii, Tome 8 (2012) no. 2, pp. 158-176
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V. Katsnelson; R. Machluf. The truncated Fourier operator. General results. Žurnal matematičeskoj fiziki, analiza, geometrii, Tome 8 (2012) no. 2, pp. 158-176. http://geodesic.mathdoc.fr/item/JMAG_2012_8_2_a3/
@article{JMAG_2012_8_2_a3,
author = {V. Katsnelson and R. Machluf},
title = {The truncated {Fourier} operator. {General} results},
journal = {\v{Z}urnal matemati\v{c}eskoj fiziki, analiza, geometrii},
pages = {158--176},
year = {2012},
volume = {8},
number = {2},
language = {en},
url = {http://geodesic.mathdoc.fr/item/JMAG_2012_8_2_a3/}
}
TY - JOUR
AU - V. Katsnelson
AU - R. Machluf
TI - The truncated Fourier operator. General results
JO - Žurnal matematičeskoj fiziki, analiza, geometrii
PY - 2012
SP - 158
EP - 176
VL - 8
IS - 2
UR - http://geodesic.mathdoc.fr/item/JMAG_2012_8_2_a3/
LA - en
ID - JMAG_2012_8_2_a3
ER -
%0 Journal Article
%A V. Katsnelson
%A R. Machluf
%T The truncated Fourier operator. General results
%J Žurnal matematičeskoj fiziki, analiza, geometrii
%D 2012
%P 158-176
%V 8
%N 2
%U http://geodesic.mathdoc.fr/item/JMAG_2012_8_2_a3/
%G en
%F JMAG_2012_8_2_a3
Let $\mathcal F$ be the one dimensional Fourier–Plancherel operator and $E$ be a subset of the real axis. The truncated Fourier operator is the operator $\mathcal F_E$ of the form $\mathcal F_E=P_E\mathcal FP_E$, where $(P_Ex)(t)=\mathbf 1_E(t)x(t)$, and $\mathbf 1_E(t)$ is the indicator function of the set $E$. In the presented work, the basic properties of the operator $\mathcal F_E$ according to the set $E$ are discussed. Among these properties there are the following ones: 1) the operator $\mathcal F_E$ has a nontrivial null-space; 2) $\mathcal F_E$ is strictly contractive; 3) $\mathcal F_E$ is a normal operator; 4) $\mathcal F_E$ is a Hilbert–Schmidt operator; 5) $\mathcal F_E$ is a trace class operator.
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