<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">JCPT</journal-id><journal-title-group><journal-title>Journal of Crystallization Process and Technology</journal-title></journal-title-group><issn pub-type="epub">2161-7678</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/jcpt.2013.32009</article-id><article-id pub-id-type="publisher-id">JCPT-30881</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Chemistry&amp;Materials Science</subject></subj-group></article-categories><title-group><article-title>
 
 
  Optical Methods in Orientation of High-Purity Germanium Crystal
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>uojian</surname><given-names>Wang</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Yongchen</surname><given-names>Sun</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Yutong</surname><given-names>Guan</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Dongming</surname><given-names>Mei</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Gang</surname><given-names>Yang</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Angela</surname><given-names>Alanson Chiller</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Bruce</surname><given-names>Gray</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Department of Physics, University of South Dakota, Vermillion, USA</addr-line></aff><aff id="aff2"><addr-line>Department of Chemistry, University of South Dakota, Vermillion, USA.</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>Guojian.Wang@usd.edu(UW)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>30</day><month>04</month><year>2013</year></pub-date><volume>03</volume><issue>02</issue><fpage>60</fpage><lpage>63</lpage><history><date date-type="received"><day>February</day>	<month>2nd,</month>	<year>2013</year></date><date date-type="rev-recd"><day>March</day>	<month>5th,</month>	<year>2013</year>	</date><date date-type="accepted"><day>March</day>	<month>15th,</month>	<year>2013</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
   Two optical methods, namely crystal facet reflection and etching pits reflection, were used to orient &lt;100&gt; and &lt;111&gt; high-purity germanium crystals. The X-ray diffraction patterns of three slices that were cut from the oriented &lt;100&gt; and &lt;111&gt; crystals were measured by X-ray diffraction. The experimental errors of crystal facet reflection method and etching pits reflection method are in the range of 0.05&#176; - 0.12&#176;. The crystal facet reflection method and etching pits reflection method are extremely simple and cheap and their accuracies are acceptable for characterizing high purity detector-grade germanium crystals.
     
 
</p></abstract><kwd-group><kwd>Reflection Method; High-Purity Germanium Crystal</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Recently, there has been a great deal of interest in searching for dark matter and neutrinoless double-beta decay that are so called rare event physics beyond Standard Model using ton-scale high-purity germanium (HPGe) detectors with ultra-low internal radioactive backgrounds [1-8]. The high purity germanium crystal (net concentration range below 10<sup>10</sup>/cm<sup>3</sup>) was grown in pure hydrogen atmosphere. The divacancy-hydrogen center (V<sub>2</sub>H) in the crystal will cause trapping of holes which will degrade the performance of nuclear radiation detectors. In order to reduce the impact of V<sub>2</sub>H center, the dislocation density must be everywhere between 10<sup>2</sup> and 10<sup>4</sup> cm<sup>−2</sup> [<xref ref-type="bibr" rid="scirp.30881-ref9">9</xref>]. For fabricating detectors, the orientation of the Ge crystal is important. High-Purity germanium crystals used for fabricating detectors are usually oriented along &lt;100&gt; direction [10,11]. Although an accurately oriented seed is used for growing a crystal, the grown crystal will deviate from the &lt;100&gt; direction because the seed rod is slightly off-center in the crucible. Therefore, the grown crystals should be oriented before fabricating detectors. X-ray diffraction is an accurate technique to orient crystals [12,13]. However, the equipment and operation of X-ray diffraction is complex.</p><p>Based on the structure and crystal growth behavior of Ge, the optical method that has been used in Si crystals [<xref ref-type="bibr" rid="scirp.30881-ref14">14</xref>] is used to orient Ge crystals for cutting since it is extremely simple and effective. <xref ref-type="fig" rid="fig1">Figure 1</xref> shows the morphology of Ge crystal, which is from the structure data of Ge crystal [<xref ref-type="bibr" rid="scirp.30881-ref15">15</xref>]. The interfacial angle between (111) and (100) is 54.72 degrees. The angle between the normal line of (111) facet and another normal line of (100) facet is 54.72 degrees. These normal lines are parallel to &lt;111&gt; and &lt;100&gt; directions, respectively. The interfacial angle between (111) and (11ī) ((1ī1) or (ī11) is 70.53 degrees.</p><p>For Ge crystals, because the atom density of (111) facet is the largest, the growth speed of (111) is the slowest one. Therefore, Ge crystals tend to develop (111) facets. If the axial thermal gradient is lower, three {111} facets will be formed in the enlarging process after the dash process. For crystals along &lt;100&gt;, there are four {111} facets and four crystal edges [<xref ref-type="bibr" rid="scirp.30881-ref110">110</xref>]. For Ge crystals along &lt;111&gt;, there are three facets and three crystal edges [<xref ref-type="bibr" rid="scirp.30881-ref110">110</xref>]. Therefore, the reflection of crystal facets can be used to orient the Ge crystals. On the other hand, because of the dissolution speed difference in (111) and (100) facets the etching pits reflection can also be used to orient Ge crystals. In this paper, both crystal facets reflection and etching pits reflection in the orientation of high-purity germanium crystals are discussed.</p></sec><sec id="s2"><title>2. Experimental</title><sec id="s2_1"><title>2.1. Crystal Facet Reflection Method in Orientation of &lt;100&gt; Crystal</title><p><xref ref-type="fig" rid="fig2">Figure 2</xref> shows the geometry of orienting a &lt;100&gt; crystal with four {111} facets. Two Metrologic neon (He-Ne) lasers (632.8 nm) are mounted perpendicularly to a screen and pass through the holes in the screen. The two lasers and a graphite plate are then adjusted using a bubble level until paralleling with the optical table. The angle between the lasers and the long edge of the graphite plate is set to 54.72 degrees. The crystal is mounted on the graphite plate by placing one facet vertical to the lasers until the reflected lasers pass back through the two holes. The &lt;100&gt; orientation is thus parallel to long edge of graphite plate.</p></sec></sec></body><back><ref-list><title>References</title><ref id="scirp.30881-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">F. T. Avignone, S. R. Elliott and J. 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