<?xml version="1.0" encoding="UTF-8"?><?xml-stylesheet type="text/xsl" href="static/style.xsl"?><OAI-PMH xmlns="http://www.openarchives.org/OAI/2.0/" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/ http://www.openarchives.org/OAI/2.0/OAI-PMH.xsd"><responseDate>2026-10-01T00:29:22Z</responseDate><request verb="GetRecord" identifier="oai:docta.ucm.es:20.500.14352/59307" metadataPrefix="marc">https://docta.ucm.es/rest/oai/request</request><GetRecord><record><header><identifier>oai:docta.ucm.es:20.500.14352/59307</identifier><datestamp>2024-08-27T14:11:10Z</datestamp><setSpec>com_20.500.14352_14</setSpec><setSpec>col_20.500.14352_15</setSpec></header><metadata><record xmlns="http://www.loc.gov/MARC21/slim" xmlns:dcterms="http://purl.org/dc/terms/" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xmlns:doc="http://www.lyncode.com/xoai" xsi:schemaLocation="http://www.loc.gov/MARC21/slim http://www.loc.gov/standards/marcxml/schema/MARC21slim.xsd">
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      <subfield code="a">Martil De La Plaza, Ignacio</subfield>
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      <subfield code="a">González Díaz, Germán</subfield>
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      <subfield code="a">García, S.</subfield>
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      <subfield code="a">Martín Pacheco, Jaime Miguel</subfield>
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      <subfield code="a">Castán, E.</subfield>
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      <subfield code="a">Dueñas, S.</subfield>
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      <subfield code="c">1995-11-01</subfield>
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      <subfield code="a">Current-voltage, small-signal measurements, and deep-level transient spectroscopy (DLTS) spectra of p-n junctions made by Mg implantation into undoped InP are described. The I-V characteristics show that the dominant conduction mechanism at forward bias is recombination in the space-charge zone, whereas a thermally activated tunneling mechanism involving a trap at 0.32 eV dominates at reverse bias. Five deep levels located in the upper-half of the band gap were detected in the junctions by DLTS measurements, three of which (at 0.6, 0.45, and 0.425 eV) were found to appear due to rapid thermal annealing. The origin of the other two levels, at 0.31 and 0.285 eV, can be ascribed to implantation damage. Admittance spectroscopy measurements showed the presence of three levels at 0.44, 0.415, and 0.30 eV, all in agreement with those found by DLTS. The DLTS measurements showed that the concentration of deep levels decreased after longer annealing times, and that the concentration of deep levels due to the implantation increased after additional P or Si implantations. This explains the influence of annealing time and additional implantations on the I-V characteristics of the junctions.</subfield>
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      <subfield code="a">0021-8979</subfield>
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      <subfield code="a">10.1063/1.359710</subfield>
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      <subfield code="a">https://hdl.handle.net/20.500.14352/59307</subfield>
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      <subfield code="a">http://dx.doi.org/10.1063/1.359710</subfield>
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      <subfield code="a">http://scitation.aip.org/</subfield>
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      <subfield code="a">Deep-level transient spectroscopy and electrical characterization  of ion-implanted p-n junctions into undoped InP</subfield>
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