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	<title>MTL Annual Research Report 2012 &#187; evelina polyzoeva</title>
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		<title>Gate-last Process for Strained-Ge p-MOSFETs with a High-k/Metal Gate Stack</title>
		<link>http://www-mtl.mit.edu/wpmu/ar2012/gate-last-process-for-strained-ge-p-mosfets-with-a-high-kmetal-gate-stack/</link>
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		<pubDate>Wed, 18 Jul 2012 22:29:05 +0000</pubDate>
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				<category><![CDATA[Electronic Devices]]></category>
		<category><![CDATA[dimitri antoniadis]]></category>
		<category><![CDATA[evelina polyzoeva]]></category>
		<category><![CDATA[judy l. hoyt]]></category>

		<guid isPermaLink="false">http://www-mtl.mit.edu/wpmu/ar2012/?p=5191</guid>
		<description><![CDATA[Strained-Ge MOSFETs with significantly enhanced mobility compared to Si/SiO2 hole mobility have previously been reported by our group (see Figure...]]></description>
				<content:encoded><![CDATA[<div class="page-restrict-output"><p>Strained-Ge MOSFETs with significantly enhanced mobility compared to Si/SiO<sub>2</sub> hole mobility have previously been reported by our group (see Figure 1).  To enable use of these enhanced channel materials in future nanoscale gate-length FETs, the equivalent oxide thickness (EOT) must be scaled, and improved dielectric/semiconductor interface properties are required. In the search for  suitable gate dielectrics for use with Ge, bilayer dielectric systems have been investigated.  The bottom layer in these systems is expected to provide a high-quality interface to the semiconductor while the top layer is a high-k dielectric used to reduce the overall EOT and gate leakage of the structure.  An Al<sub>2</sub>O<sub>3</sub>/TiO<sub>2 </sub>dielectric system with a sub-nm EOT and low density of interface states on bulk Ge wafers has been demonstrated<sup> [<a href="http://www-mtl.mit.edu/wpmu/ar2012/gate-last-process-for-strained-ge-p-mosfets-with-a-high-kmetal-gate-stack/#footnote_0_5191" id="identifier_0_5191" class="footnote-link footnote-identifier-link" title="S. Swaminathan. M.&nbsp; Shandalov, Y.&nbsp; Oshima, and P. C.&nbsp; McIntyre, &ldquo;Bilayer metal oxide gate insulators for scaled Ge-channel metal-oxide-semiconductor devices,&rdquo; Applied Physics Letters, vol. 96, no. 8, pp. 082904-082904-3, Feb. 2010.">1</a>] </sup>, and its implementation with strained-Ge devices is the aim of this work. Due to the limited thermal budget associated with the bilayer dielectric/metal gate stack, a gate-last process is developed.</p>
<p>In the gate-last process, the source and drain regions are activated before the gate dielectric and gate metal are deposited.  This is done to improve device reliability and mobility at scaled EOT, which can be significantly degraded when the high-k dielectric has gone through the high-temperature steps. Figure 2 shows the schematic gate-last process flow as well as the mask layout of the designed MOSFET structure. The preliminary experiments on gate-last Si MOSFETs show a superior interface quality compared to gate-first devices, a promising result in favor of gate-last strained-Ge MOSFETs, at least as a means of studying the dielectric/semiconductor interface.</p>

<a href='http://www-mtl.mit.edu/wpmu/ar2012/gate-last-process-for-strained-ge-p-mosfets-with-a-high-kmetal-gate-stack/polyzoeva_mosfets_01/' title='polyzoeva_mosfets_01'><img width="300" height="225" src="http://www-mtl.mit.edu/wpmu/ar2012/files/2012/07/polyzoeva_mosfets_01-300x225.png" class="attachment-medium" alt="Figure 1" /></a>
<a href='http://www-mtl.mit.edu/wpmu/ar2012/gate-last-process-for-strained-ge-p-mosfets-with-a-high-kmetal-gate-stack/polyzoeva_mosfets_02/' title='polyzoeva_mosfets_02'><img width="300" height="225" src="http://www-mtl.mit.edu/wpmu/ar2012/files/2012/06/polyzoeva_mosfets_02-300x225.png" class="attachment-medium" alt="Figure 2" /></a>

<ol class="footnotes"><li id="footnote_0_5191" class="footnote">S. Swaminathan. M.  Shandalov, Y.  Oshima, and P. C.  McIntyre, &#8220;Bilayer metal oxide gate insulators for scaled Ge-channel metal-oxide-semiconductor devices,&#8221; <em>Applied Physics Letters</em>, vol. 96, no. 8, pp. 082904-082904-3, Feb. 2010.</li></ol></div>]]></content:encoded>
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