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Let <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/h/h110/h110190/h1101901.png" /> be an [[Integral operator|integral operator]] from <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/h/h110/h110190/h1101902.png" /> into <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/h/h110/h110190/h1101903.png" />, i.e., there exists a <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/h/h110/h110190/h1101904.png" />-measurable function <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/h/h110/h110190/h1101905.png" /> on <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/h/h110/h110190/h1101906.png" /> such that <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/h/h110/h110190/h1101907.png" /> a.e. on <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/h/h110/h110190/h1101908.png" />. Then <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/h/h110/h110190/h1101909.png" /> is called a Hille–Tamarkin operator if
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<table class="eq" style="width:100%;"> <tr><td valign="top" style="width:94%;text-align:center;"><img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/h/h110/h110190/h11019010.png" /></td> </tr></table>
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where <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/h/h110/h110190/h11019011.png" />. By taking <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/h/h110/h110190/h11019012.png" /> one obtains the class of Hilbert–Schmidt operators (cf. [[Hilbert–Schmidt operator|Hilbert–Schmidt operator]]). Replacing <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/h/h110/h110190/h11019013.png" />, respectively <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/h/h110/h110190/h11019014.png" />, by arbitrary Banach function norms <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/h/h110/h110190/h11019015.png" />, respectively <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/h/h110/h110190/h11019016.png" />, one obtains the class of Hille–Tamarkin operators between Banach function spaces (sometimes called integral operators of finite double norm, see [[#References|[a1]]]). Under some mild hypotheses on the norms, one can show that Hille–Tamarkin operators have rather strong compactness properties (see [[#References|[a2]]]).
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Let 
 +
be an [[Integral operator|integral operator]] from    L _ {p} ( Y, \nu )
 +
into    L _ {q} ( X, \mu ) ,
 +
i.e., there exists a    ( \mu \times \nu ) -
 +
measurable function    T ( x,y )
 +
on    X \times Y
 +
such that  $  Tf ( x ) = \int {T ( x,y ) }  {d \nu ( y ) } $
 +
a.e. on    X .  
 +
Then    T
 +
is called a Hille–Tamarkin operator if
 +
 
 +
$$
 +
\int\limits {\left ( \int\limits {\left | {T ( x,y ) } \right | ^ {p  ^  \prime  } }  {d \nu ( y ) } \right ) ^ { {q / {p  ^  \prime  } } } }  {d \mu ( x ) } < \infty,
 +
$$
 +
 
 +
where  $  {1 / p } + {1 / { {p  ^  \prime  } } } = 1 $.  
 +
By taking $  p = q = 2 $
 +
one obtains the class of Hilbert–Schmidt operators (cf. [[Hilbert–Schmidt operator|Hilbert–Schmidt operator]]). Replacing   \| \cdot \| _ {p} ,  
 +
respectively   \| \cdot \| _ {q} ,  
 +
by arbitrary Banach function norms   \rho _ {2} ,  
 +
respectively   \rho _ {1} ,  
 +
one obtains the class of Hille–Tamarkin operators between Banach function spaces (sometimes called integral operators of finite double norm, see [[#References|[a1]]]). Under some mild hypotheses on the norms, one can show that Hille–Tamarkin operators have rather strong compactness properties (see [[#References|[a2]]]).
  
 
====References====
 
====References====
 
<table><TR><TD valign="top">[a1]</TD> <TD valign="top">  A.C. Zaanen,  "Riesz spaces" , '''II''' , North-Holland  (1983)</TD></TR><TR><TD valign="top">[a2]</TD> <TD valign="top">  A.R. Schep,  "Compactness properties of Carleman and Hille–Tamarkin operators"  ''Canad. J. Math.'' , '''37'''  (1985)  pp. 921–933</TD></TR></table>
 
<table><TR><TD valign="top">[a1]</TD> <TD valign="top">  A.C. Zaanen,  "Riesz spaces" , '''II''' , North-Holland  (1983)</TD></TR><TR><TD valign="top">[a2]</TD> <TD valign="top">  A.R. Schep,  "Compactness properties of Carleman and Hille–Tamarkin operators"  ''Canad. J. Math.'' , '''37'''  (1985)  pp. 921–933</TD></TR></table>

Latest revision as of 22:10, 5 June 2020


Let T be an integral operator from L _ {p} ( Y, \nu ) into L _ {q} ( X, \mu ) , i.e., there exists a ( \mu \times \nu ) - measurable function T ( x,y ) on X \times Y such that Tf ( x ) = \int {T ( x,y ) } {d \nu ( y ) } a.e. on X . Then T is called a Hille–Tamarkin operator if

\int\limits {\left ( \int\limits {\left | {T ( x,y ) } \right | ^ {p ^ \prime } } {d \nu ( y ) } \right ) ^ { {q / {p ^ \prime } } } } {d \mu ( x ) } < \infty,

where {1 / p } + {1 / { {p ^ \prime } } } = 1 . By taking p = q = 2 one obtains the class of Hilbert–Schmidt operators (cf. Hilbert–Schmidt operator). Replacing \| \cdot \| _ {p} , respectively \| \cdot \| _ {q} , by arbitrary Banach function norms \rho _ {2} , respectively \rho _ {1} , one obtains the class of Hille–Tamarkin operators between Banach function spaces (sometimes called integral operators of finite double norm, see [a1]). Under some mild hypotheses on the norms, one can show that Hille–Tamarkin operators have rather strong compactness properties (see [a2]).

References

[a1] A.C. Zaanen, "Riesz spaces" , II , North-Holland (1983)
[a2] A.R. Schep, "Compactness properties of Carleman and Hille–Tamarkin operators" Canad. J. Math. , 37 (1985) pp. 921–933
How to Cite This Entry:
Hille-Tamarkin operator. Encyclopedia of Mathematics. URL: http://encyclopediaofmath.org/index.php?title=Hille-Tamarkin_operator&oldid=22579
This article was adapted from an original article by A.R. Schep (originator), which appeared in Encyclopedia of Mathematics - ISBN 1402006098. See original article