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	<title>Comments on: Fefferman&#8217;s ball multiplier counterexample</title>
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	<link>http://lewko.wordpress.com/2009/08/04/feffermans-ball-multiplier-counterexample/</link>
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		<title>By: Hormander-Minlin &#124; Being simple</title>
		<link>http://lewko.wordpress.com/2009/08/04/feffermans-ball-multiplier-counterexample/#comment-189</link>
		<dc:creator><![CDATA[Hormander-Minlin &#124; Being simple]]></dc:creator>
		<pubDate>Sun, 03 Feb 2013 03:05:32 +0000</pubDate>
		<guid isPermaLink="false">http://lewko.wordpress.com/?p=221#comment-189</guid>
		<description><![CDATA[[...] for  be a Fourier multiplier on  (see e.g., [1]). However, Fefferman (see [2],[3]) gave an intricate proof which show us that this condition is not sufficient, that is, he showed that the operator  does [...]]]></description>
		<content:encoded><![CDATA[<p>[...] for  be a Fourier multiplier on  (see e.g., [1]). However, Fefferman (see [2],[3]) gave an intricate proof which show us that this condition is not sufficient, that is, he showed that the operator  does [...]</p>
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		<title>By: Thomas</title>
		<link>http://lewko.wordpress.com/2009/08/04/feffermans-ball-multiplier-counterexample/#comment-91</link>
		<dc:creator><![CDATA[Thomas]]></dc:creator>
		<pubDate>Fri, 22 Oct 2010 09:35:03 +0000</pubDate>
		<guid isPermaLink="false">http://lewko.wordpress.com/?p=221#comment-91</guid>
		<description><![CDATA[Of course, that makes a lot of sense. Thank you very much.]]></description>
		<content:encoded><![CDATA[<p>Of course, that makes a lot of sense. Thank you very much.</p>
]]></content:encoded>
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		<title>By: Mark Lewko</title>
		<link>http://lewko.wordpress.com/2009/08/04/feffermans-ball-multiplier-counterexample/#comment-90</link>
		<dc:creator><![CDATA[Mark Lewko]]></dc:creator>
		<pubDate>Wed, 20 Oct 2010 22:33:28 +0000</pubDate>
		<guid isPermaLink="false">http://lewko.wordpress.com/?p=221#comment-90</guid>
		<description><![CDATA[Thomas,

Thanks for reading! You&#039;re right that this follows from self-adjointness. By Parseval&#039;s identity we have

$latex  (S_{1}f,g) =\int_{\mathbb{R}^2} \widehat{S_{1} f}(\xi)\overline{\widehat{g}(\xi)}d\xi=\int_{B}\widehat{f}(\xi) \overline{\widehat{g}(\xi)}d\xi$.

The last equality follows from the definition of $latex S_{1}$ where $latex B$ denotes the unit ball.  Now the last expression is also equal to (by essentially the same argument just given) $latex \int_{\mathbb{R}^2} \widehat{f}(\xi) \widehat{S_{1}g}(\xi)d\xi=(f,S_{1}g)$.
]]></description>
		<content:encoded><![CDATA[<p>Thomas,</p>
<p>Thanks for reading! You&#8217;re right that this follows from self-adjointness. By Parseval&#8217;s identity we have</p>
<p><img src='http://s0.wp.com/latex.php?latex=%28S_%7B1%7Df%2Cg%29+%3D%5Cint_%7B%5Cmathbb%7BR%7D%5E2%7D+%5Cwidehat%7BS_%7B1%7D+f%7D%28%5Cxi%29%5Coverline%7B%5Cwidehat%7Bg%7D%28%5Cxi%29%7Dd%5Cxi%3D%5Cint_%7BB%7D%5Cwidehat%7Bf%7D%28%5Cxi%29+%5Coverline%7B%5Cwidehat%7Bg%7D%28%5Cxi%29%7Dd%5Cxi&amp;bg=fff&amp;fg=222&amp;s=0' alt='(S_{1}f,g) =&#92;int_{&#92;mathbb{R}^2} &#92;widehat{S_{1} f}(&#92;xi)&#92;overline{&#92;widehat{g}(&#92;xi)}d&#92;xi=&#92;int_{B}&#92;widehat{f}(&#92;xi) &#92;overline{&#92;widehat{g}(&#92;xi)}d&#92;xi' title='(S_{1}f,g) =&#92;int_{&#92;mathbb{R}^2} &#92;widehat{S_{1} f}(&#92;xi)&#92;overline{&#92;widehat{g}(&#92;xi)}d&#92;xi=&#92;int_{B}&#92;widehat{f}(&#92;xi) &#92;overline{&#92;widehat{g}(&#92;xi)}d&#92;xi' class='latex' />.</p>
<p>The last equality follows from the definition of <img src='http://s0.wp.com/latex.php?latex=S_%7B1%7D&amp;bg=fff&amp;fg=222&amp;s=0' alt='S_{1}' title='S_{1}' class='latex' /> where <img src='http://s0.wp.com/latex.php?latex=B&amp;bg=fff&amp;fg=222&amp;s=0' alt='B' title='B' class='latex' /> denotes the unit ball.  Now the last expression is also equal to (by essentially the same argument just given) <img src='http://s0.wp.com/latex.php?latex=%5Cint_%7B%5Cmathbb%7BR%7D%5E2%7D+%5Cwidehat%7Bf%7D%28%5Cxi%29+%5Cwidehat%7BS_%7B1%7Dg%7D%28%5Cxi%29d%5Cxi%3D%28f%2CS_%7B1%7Dg%29&amp;bg=fff&amp;fg=222&amp;s=0' alt='&#92;int_{&#92;mathbb{R}^2} &#92;widehat{f}(&#92;xi) &#92;widehat{S_{1}g}(&#92;xi)d&#92;xi=(f,S_{1}g)' title='&#92;int_{&#92;mathbb{R}^2} &#92;widehat{f}(&#92;xi) &#92;widehat{S_{1}g}(&#92;xi)d&#92;xi=(f,S_{1}g)' class='latex' />.</p>
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	<item>
		<title>By: Thomas</title>
		<link>http://lewko.wordpress.com/2009/08/04/feffermans-ball-multiplier-counterexample/#comment-89</link>
		<dc:creator><![CDATA[Thomas]]></dc:creator>
		<pubDate>Wed, 20 Oct 2010 17:36:32 +0000</pubDate>
		<guid isPermaLink="false">http://lewko.wordpress.com/?p=221#comment-89</guid>
		<description><![CDATA[I really like this post, I&#039;m doing a paper on Kakeya sets and their applications and this (and its prequel) helped me a lot. I hope you have time to answer a (probably simple) question about the very last line of the post: why is 

sup sup [S_1 f, g] 

equal to

sup sup [f, S_1 g]

It looks like some kind of self-adjointness, do we know that the operator is its own adjoint?

Thanks,
Thomas]]></description>
		<content:encoded><![CDATA[<p>I really like this post, I&#8217;m doing a paper on Kakeya sets and their applications and this (and its prequel) helped me a lot. I hope you have time to answer a (probably simple) question about the very last line of the post: why is </p>
<p>sup sup [S_1 f, g] </p>
<p>equal to</p>
<p>sup sup [f, S_1 g]</p>
<p>It looks like some kind of self-adjointness, do we know that the operator is its own adjoint?</p>
<p>Thanks,<br />
Thomas</p>
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		<title>By: L^{p} Convergence of Fourier Transforms &#171; Lewko&#39;s Blog</title>
		<link>http://lewko.wordpress.com/2009/08/04/feffermans-ball-multiplier-counterexample/#comment-6</link>
		<dc:creator><![CDATA[L^{p} Convergence of Fourier Transforms &#171; Lewko&#39;s Blog]]></dc:creator>
		<pubDate>Wed, 05 Aug 2009 01:32:33 +0000</pubDate>
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		<description><![CDATA[[...] Fourier Multipliers, Marcel Riesz   leave a comment    &#171; Lattice Points in l^{1}&#160;Balls Fefferman&#8217;s Ball Multiplier&#160;Counterexample [...]]]></description>
		<content:encoded><![CDATA[<p>[...] Fourier Multipliers, Marcel Riesz   leave a comment    &laquo; Lattice Points in l^{1}&nbsp;Balls Fefferman&#8217;s Ball Multiplier&nbsp;Counterexample [...]</p>
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