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	    2019</a> | <a href="http://www.inria.fr/en/teams/modal">Presentation of the Project-Team MODAL</a></small>
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        <h2>Section: 
      New Results</h2>
        <h3 class="titre3">Axis 2: Multi-kernel unmixing and super-resolution using the Modified Matrix Pencil method</h3>
        <p><b>Participant:</b> Hemant Tyagi.</p>
        <p>Consider <span class="math"><math xmlns="http://www.w3.org/1998/Math/MathML"><mi>L</mi></math></span> groups of point sources or spike trains, with the <span class="math"><math xmlns="http://www.w3.org/1998/Math/MathML"><msup><mi>l</mi><mrow><mi>t</mi><mi>h</mi></mrow></msup></math></span> group represented by <span class="math"><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msub><mi>x</mi><mi>l</mi></msub><mrow><mo>(</mo><mi>t</mi><mo>)</mo></mrow></mrow></math></span>.
For a function <span class="math"><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>g</mi><mo>:</mo><mi>R</mi><mo>→</mo><mi>R</mi></mrow></math></span>, let <span class="math"><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msub><mi>g</mi><mi>l</mi></msub><mrow><mo>(</mo><mi>t</mi><mo>)</mo></mrow><mo>=</mo><mi>g</mi><mrow><mo>(</mo><mi>t</mi><mo>/</mo><msub><mi>μ</mi><mi>l</mi></msub><mo>)</mo></mrow></mrow></math></span> denote a point spread function with scale <span class="math"><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msub><mi>μ</mi><mi>l</mi></msub><mo>&gt;</mo><mn>0</mn></mrow></math></span>, and with <span class="math"><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><msub><mi>μ</mi><mn>1</mn></msub><mo>&lt;</mo><mo>⋯</mo><mo>&lt;</mo><msub><mi>μ</mi><mi>L</mi></msub></mrow></math></span>.
With <span class="math"><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>y</mi><mrow><mo>(</mo><mi>t</mi><mo>)</mo></mrow><mo>=</mo><msubsup><mo>∑</mo><mrow><mi>l</mi><mo>=</mo><mn>1</mn></mrow><mi>L</mi></msubsup><mrow><mo>(</mo><msub><mi>g</mi><mi>l</mi></msub><mo>☆</mo><msub><mi>x</mi><mi>l</mi></msub><mo>)</mo></mrow><mrow><mo>(</mo><mi>t</mi><mo>)</mo></mrow></mrow></math></span>, our goal is to recover the
source parameters given samples of <span class="math"><math xmlns="http://www.w3.org/1998/Math/MathML"><mi>y</mi></math></span>, or given the Fourier samples of <span class="math"><math xmlns="http://www.w3.org/1998/Math/MathML"><mi>y</mi></math></span>. This problem is a generalization of
the usual super-resolution setup wherein <span class="math"><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mi>L</mi><mo>=</mo><mn>1</mn></mrow></math></span>; we call this the multi-kernel unmixing super-resolution problem.
Assuming access to Fourier samples of <span class="math"><math xmlns="http://www.w3.org/1998/Math/MathML"><mi>y</mi></math></span>, we derive an algorithm for this problem for estimating the source parameters
of each group, along with precise non-asymptotic guarantees. Our approach involves estimating the group parameters sequentially
in the order of increasing scale parameters, i.e., from group 1 to <span class="math"><math xmlns="http://www.w3.org/1998/Math/MathML"><mi>L</mi></math></span>. In particular, the estimation process at stage
<span class="math"><math xmlns="http://www.w3.org/1998/Math/MathML"><mrow><mn>1</mn><mo>≤</mo><mi>l</mi><mo>≤</mo><mi>L</mi></mrow></math></span> involves (i) carefully sampling the tail of the Fourier transform of <span class="math"><math xmlns="http://www.w3.org/1998/Math/MathML"><mi>y</mi></math></span>,
(ii) a <i>deflation</i> step wherein we subtract the contribution of the groups processed thus far from the obtained Fourier samples,
and (iii) applying Moitra's modified Matrix Pencil method on a deconvolved version of the samples in (ii).</p>
        <p>This is joint work with Stephane Chretien (National Physical Laboratory, UK &amp; Alan Turing Institute, London) and was mostly done while Hemant Tyagi was affiliated to the Alan Turing Institute. It is currently under revision in an international journal and is available as a preprint <a href="./bibliography.html#modal-2019-bid15">[56]</a>.
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