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	<journal>
		<journal_title>eEarth</journal_title>
		<journal_url>www.electronic-earth.net</journal_url>
		<issn>1815-381X</issn>
		<eissn>1815-3828</eissn>
		<volume_number>2</volume_number>
		<issue_number>1</issue_number>
		<publication_year>2007</publication_year>
	</journal>
	<doi>10.5194/ee-2-7-2007</doi>
	<article_url>http://www.electronic-earth.net/2/7/2007/</article_url>
	<abstract_html>http://www.electronic-earth.net/2/7/2007/ee-2-7-2007.html</abstract_html>
	<fulltext_pdf>http://www.electronic-earth.net/2/7/2007/ee-2-7-2007.pdf</fulltext_pdf>
	<start_page>7</start_page>
	<end_page>16</end_page>
	<publication_date>2007-01-10</publication_date>
	<article_title content_type="html">Stimulated infrared emission from rocks: assessing a stress indicator</article_title>
	<authors>
		<author numeration="1" affiliations="1,2">
			<name>F. T. Freund</name>
			<email>ffreund@mail.arc.nasa.gov</email>
		</author>
		<author numeration="2" affiliations="2,3">
			<name>A. Takeuchi</name>
		</author>
		<author numeration="3" affiliations="2">
			<name>B. W. S. Lau</name>
		</author>
		<author numeration="4" affiliations="4">
			<name>A. Al-Manaseer</name>
		</author>
		<author numeration="5" affiliations="5">
			<name>C. C. Fu</name>
		</author>
		<author numeration="6" affiliations="6">
			<name>N. A. Bryant</name>
		</author>
		<author numeration="7" affiliations="7">
			<name>D. Ouzounov</name>
		</author>
	</authors>
	<affiliations>
		<affiliation numeration="1" content_type="html">Ecosystems Science and Technology Branch, Code SGE, NASA Ames Research Center, Moffett Field, CA 94035-1000, USA</affiliation>
		<affiliation numeration="2" content_type="html">Department of Physics, San Jose State University, San Jose, CA 95192-0106, USA</affiliation>
		<affiliation numeration="3" content_type="html">Department of Chemistry, Niigata University, Ikarashi-ninotyo, Niigata 950-2181, Japan</affiliation>
		<affiliation numeration="4" content_type="html">Department of Civil Engineering, San Jose State University, San Jose, CA 95192-0083, USA</affiliation>
		<affiliation numeration="5" content_type="html">Department of Civil Engineering, University of Maryland, College Park, MD 20742, USA</affiliation>
		<affiliation numeration="6" content_type="html">Jet Propulsion Laboratory, Org. 3880, Pasadena, CA 91109-8099, USA</affiliation>
		<affiliation numeration="7" content_type="html">CEORS, George Mason University, Fairfax, VA 22030-4444, USA</affiliation>
	</affiliations>
	<abstract content_type="html">To study the effect of stress-activated positive hole (p-hole) charge
carriers on the infrared (IR) emission from rocks, we subjected a portion
(~10 vol.%) of a large (30&amp;times;60&amp;times;7.5 cm&lt;sup&gt;3&lt;/sup&gt;) block of
anorthosite, a nearly monomineralic (Ca-rich feldspar) igneous rock, to
uniaxial deviatory stress up to failure. We measured the IR emission from a
flat surface &amp;asymp;40 cm from the stressed rock volume over the 800&amp;ndash;1300 cm&lt;sup&gt;&amp;minus;1&lt;/sup&gt; (7.7&amp;ndash;12.5 μm)
range. Instantly, upon loading, the emission
spectrum and intensity change. At first narrow bands appear at 930 cm&lt;sup&gt;&amp;minus;1&lt;/sup&gt;
(10.75 μm), 880 cm&lt;sup&gt;&amp;minus;1&lt;/sup&gt; (11.36 μm), 820 cm&lt;sup&gt;&amp;minus;1&lt;/sup&gt; (12.4 μm)
plus additional narrow bands in the 1000&amp;ndash;1300 cm&lt;sup&gt;&amp;minus;1&lt;/sup&gt; (7.7&amp;ndash;10.0 μm)
range. The 10.75&amp;ndash;12.4 μm bands are thought to arise from vibrationally
excited O-O stretching modes, which form when p-hole charge carriers, which
spread from the stressed rock volume into the unstressed rock, recombine at
the surface. They radiatively decay, giving rise to &quot;hot&quot; bands due to
transitions between excited states. Before failure the broad emission bands
at 1170 cm&lt;sup&gt;&amp;minus;1&lt;/sup&gt; and 1030 cm&lt;sup&gt;&amp;minus;1&lt;/sup&gt; (8.7 and 9.7 μm) also
increase slightly in intensity, suggesting a small increase in temperature
due to thermalization of the energy deposited into the surface through
p-hole recombination. Stimulated IR emission due to hole-hole recombination
and its follow-on effects may help understand the enhanced IR emission seen
in night-time satellite images of the land surface before major earthquakes
known as &quot;thermal anomalies&quot;.</abstract>
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</article>

