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	<title>MTL Annual Research Report 2011 &#187; Priya Jadhav</title>
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		<title>Anomalous Singlet Exciton Fission Magnetic Field Effect in Diphenyltetracene-C60 Solar Cells</title>
		<link>http://www-mtl.mit.edu/wpmu/ar2011/anomalous-singlet-exciton-fission-magnetic-field-effect-in-diphenyltetracene-c60-solar-cells/</link>
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		<pubDate>Thu, 23 Jun 2011 14:49:54 +0000</pubDate>
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				<category><![CDATA[Energy]]></category>
		<category><![CDATA[Optics & Photonics]]></category>
		<category><![CDATA[Marc Baldo]]></category>
		<category><![CDATA[Priya Jadhav]]></category>

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		<description><![CDATA[Singlet exciton fission may find application in more efficient solar cells. Fission can reduce thermalization losses because by splitting the...]]></description>
				<content:encoded><![CDATA[<div class="page-restrict-output"><p>Singlet exciton fission may find application in more efficient solar cells. Fission can reduce thermalization losses because by splitting the exciton, a high energy photon can produce two charge carrier pairs instead of one. The two device implementations to date that exploit singlet exciton fission, a pentacene photodetector and a tetracene solar cell, produce more current by multiplying the number of excitons in the visible part of the spectrum<sup> [<a href="http://www-mtl.mit.edu/wpmu/ar2011/anomalous-singlet-exciton-fission-magnetic-field-effect-in-diphenyltetracene-c60-solar-cells/#footnote_0_2737" id="identifier_0_2737" class="footnote-link footnote-identifier-link" title="J. Lee, P. Jadhav, and M. A. Baldo, &ldquo;High efficiency organic multilayer photodetectors based on singlet exciton fission,&rdquo; Applied Physics Letters, vol. 95, pp. 033301-033303, July 2009">1</a>] </sup><sup> [<a href="http://www-mtl.mit.edu/wpmu/ar2011/anomalous-singlet-exciton-fission-magnetic-field-effect-in-diphenyltetracene-c60-solar-cells/#footnote_1_2737" id="identifier_1_2737" class="footnote-link footnote-identifier-link" title="P. J. Jadhav, A. Mohanty, J. Sussman, and M. A. Baldo, &ldquo;Singlet exciton fission in nanostructured organic solar cells,&rdquo; Nano Letters, DOI: 10.1021/nl104202j.">2</a>] </sup>. In this work we show that diphenyltetracene (DPT) also exhibits singlet exciton fission; in Figure 1 we present a DPT-C<sub>60</sub> device in which singlet exciton fission contributes negatively to the current, which is opposite behavior to the previous two implementations.</p>
<p>DPT differs from previous implementations of singlet exciton fission in that its triplet <em>E<sub>t</sub></em> = 1.2eV<sup> [<a href="http://www-mtl.mit.edu/wpmu/ar2011/anomalous-singlet-exciton-fission-magnetic-field-effect-in-diphenyltetracene-c60-solar-cells/#footnote_2_2737" id="identifier_2_2737" class="footnote-link footnote-identifier-link" title="C. Burgdorff, T. Kircher, and H. G. L&ouml;hmannsr&ouml;ben, &ldquo;Photophysical properties of tetracene derivatives in solution,&rdquo; Spectrochimica Acta Part A: Molecular Spectroscopy vol. 44, pp. 1137-1141, Apr. 1988.">3</a>] </sup> is less than the energy of the DPT-C<sub>60 </sub>charge transfer state (CT) <em>E<sub>CT</sub></em> = 1.25eV. Hence the triplets cannot break up to form charge carriers. This effect is seen in the positive magnetic field effect shown in Figure 2. The application of a magnetic field results in reduced singlet fission and hence an increase in the number of singlet excitons and thereby increased current. In contrast, a similar measurement with a lower CT energy yields the usual negative magnetic field dependence. For example, below we demonstrate a negative magnetic field effect in DPT-F<sub>16</sub>CuPC, where F<sub>16</sub>CuPC is fluorinated copper phthalocyanine.</p>
<p>The amorphous nature of the DPT film in the device results in an isotropic magnetic field effect. Consequently, the large magnetic field effect shown by the device, 5% at .45T, may be used in an isotropic magnetic field detector.</p>

<a href='http://www-mtl.mit.edu/wpmu/ar2011/anomalous-singlet-exciton-fission-magnetic-field-effect-in-diphenyltetracene-c60-solar-cells/jadhav_singlet-fission_01/' title='Figure 1'><img width="130" height="130" src="http://www-mtl.mit.edu/wpmu/ar2011/files/2011/06/jadhav_singlet-fission_01-150x150.jpg" class="attachment-thumbnail" alt="Figure 1: Device structures for the DPT-C60 and the DPT- F16CuPC devices." /></a>
<a href='http://www-mtl.mit.edu/wpmu/ar2011/anomalous-singlet-exciton-fission-magnetic-field-effect-in-diphenyltetracene-c60-solar-cells/jadhav_singlet-fission_02/' title='Figure 2'><img width="130" height="130" src="http://www-mtl.mit.edu/wpmu/ar2011/files/2011/06/jadhav_singlet-fission_02-150x150.jpg" class="attachment-thumbnail" alt="Figure 2" /></a>

<ol class="footnotes"><li id="footnote_0_2737" class="footnote">J. Lee, P. Jadhav, and M. A. Baldo, “High efficiency organic multilayer photodetectors based on singlet exciton fission,” <em>Applied Physics Letters</em>, vol. 95, pp. 033301-033303, July 2009</li><li id="footnote_1_2737" class="footnote">P. J. Jadhav, A. Mohanty, J. Sussman, and M. A. Baldo, “Singlet exciton fission in nanostructured organic solar cells,” <em>Nano Letters</em>, <strong>DOI: </strong>10.1021/nl104202j.</li><li id="footnote_2_2737" class="footnote">C. Burgdorff, T. Kircher, and H. G. Löhmannsröben, &#8220;Photophysical properties of tetracene derivatives in solution,” <em>Spectrochimica Acta Part A: Molecular Spectroscopy</em> vol. 44, pp. 1137-1141, Apr. 1988.</li></ol></div>]]></content:encoded>
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