{"id":{"repo_id":"uiuc","oai_identifier":"oai:www.ideals.illinois.edu:2142/82923"},"canonical_url":"https://search.dev.ndltd.org/etd/uiuc/oai:www.ideals.illinois.edu:2142/82923","repository":{"repo_id":"uiuc","name":"University of Illinois - Urbana-Champaign","base_url":"https://www.ideals.illinois.edu/oai-pmh"},"display":{"title":"Ultra-High B Doping During Si(1-X)ge(x)(001) Gas-Source Molecular-Beam Epitaxy: A Mechanistic Study of Layer Growth Kinetics, Dopant Incorporation, Electrical Activation, and Carrier Transport","abstract":"CB in Si1-xGex(001) increases with precursor flux ratio and B is incorporated into active sites at concentrations to C*B (Ts) = 2.5 x 1020 and 4.6 x 1020 cm-3 for x = 0 and 0.18 at Ts = 600 and 500°C, respectively. At higher B concentrations, there is a large decrease in the activated fraction of incorporated B. The total acceptor concentration continues to increase. No B precipitates or misfit dislocations were detected by HR-XRD or TEM. The out-of-plane lattice constant a⊥ decreases linearly with increasing C*B and non-linearly, for CB > C*B . Electrical properties are in good agreement with theoretical values to C*B . When thetaB > thetaB,sat, B accumulates in the upper layer, and a parallel incorporation channel becomes available in which B is incorporated as B-pairs which are electrically inactive.","abstract_html":"CB in Si1-xGex(001) increases with precursor flux ratio and B is incorporated into active sites at concentrations to C*B (Ts) = 2.5 x 1020 and 4.6 x 1020 cm-3 for x = 0 and 0.18 at Ts = 600 and 500°C, respectively. At higher B concentrations, there is a large decrease in the activated fraction of incorporated B. The total acceptor concentration continues to increase. No B precipitates or misfit dislocations were detected by HR-XRD or TEM. The out-of-plane lattice constant a⊥ decreases linearly with increasing C*B and non-linearly, for CB > C*B . Electrical properties are in good agreement with theoretical values to C*B . When thetaB > thetaB,sat, B accumulates in the upper layer, and a parallel incorporation channel becomes available in which B is incorporated as B-pairs which are electrically inactive.","abstract_has_math":false,"creators":["Glass, Glenn Aaron"],"institution":"University of Illinois at Urbana-Champaign","degree_name":"Ph.D.","degree_level":"Dissertation","degree_discipline":"Materials Science and Engineering","degree_department":null,"school":null,"contributors":["Greene, Joseph E."],"advisors":[],"committee_chairs":[],"committee_members":[],"year":2015,"date_issued":"2015-09-25T20:53:39Z","date_published":"2015-09-25T20:53:39Z","updated_at":"2026-07-22T22:26:20Z","subjects":["Engineering, Electronics and Electrical"],"languages":["eng"],"rights":[],"rights_urls":[],"identifier_entries":[{"key":"dc:identifier","label":"Identifier","values":["(MiAaPQ)AAI9953025"],"render_values":[{"text":"(MiAaPQ)AAI9953025","href":null,"code":true}]}]},"links":{"outbound_url":"http://hdl.handle.net/2142/82923","outbound_label":"Handle","outbound_source":"dc:identifier"},"metadata_groups":[{"id":"people","label":"People","entries":[{"key":"dc:contributor","label":"Contributor","values":["Greene, Joseph E."]},{"key":"dc:creator","label":"Author","values":["Glass, Glenn Aaron"]}]},{"id":"academic_context","label":"Academic Context","entries":[{"key":"dc:date","label":"Dc Date","values":["2015-09-25T20:53:39Z","1999"]},{"key":"dc:type","label":"Dc Type","values":["text"]},{"key":"thesis:degree_discipline","label":"Discipline","values":["Materials Science and Engineering"]},{"key":"thesis:degree_level","label":"Degree Level","values":["Dissertation"]},{"key":"thesis:degree_name","label":"Degree Name","values":["Ph.D."]},{"key":"thesis:institution_name","label":"Thesis Institution Name","values":["University of Illinois at Urbana-Champaign"]}]},{"id":"subjects_keywords","label":"Subjects and Keywords","entries":[{"key":"dc:subject","label":"Dc Subject","values":["Engineering, Electronics and Electrical"]}]},{"id":"language_rights","label":"Language and Rights","entries":[{"key":"dc:language","label":"Dc Language","values":["eng"]}]},{"id":"identifiers","label":"Identifiers","entries":[{"key":"dc:identifier","label":"Identifier","values":["http://hdl.handle.net/2142/82923","(MiAaPQ)AAI9953025"]}]},{"id":"additional","label":"Additional Metadata","entries":[{"key":"dc:description","label":"Description","values":["CB in Si1-xGex(001) increases with precursor flux ratio and B is incorporated into active sites at concentrations to C*B (Ts) = 2.5 x 1020 and 4.6 x 1020 cm-3 for x = 0 and 0.18 at Ts = 600 and 500°C, respectively. At higher B concentrations, there is a large decrease in the activated fraction of incorporated B. The total acceptor concentration continues to increase. No B precipitates or misfit dislocations were detected by HR-XRD or TEM. The out-of-plane lattice constant a⊥ decreases linearly with increasing C*B and non-linearly, for CB > C*B . Electrical properties are in good agreement with theoretical values to C*B . When thetaB > thetaB,sat, B accumulates in the upper layer, and a parallel incorporation channel becomes available in which B is incorporated as B-pairs which are electrically inactive.","Made available in DSpace on 2015-09-25T20:53:39Z (GMT). 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At higher B concentrations, there is a large decrease in the activated fraction of incorporated B. The total acceptor concentration continues to increase. No B precipitates or misfit dislocations were detected by HR-XRD or TEM. The out-of-plane lattice constant a⊥ decreases linearly with increasing C*B and non-linearly, for CB > C*B . Electrical properties are in good agreement with theoretical values to C*B . When thetaB > thetaB,sat, B accumulates in the upper layer, and a parallel incorporation channel becomes available in which B is incorporated as B-pairs which are electrically inactive.","Made available in DSpace on 2015-09-25T20:53:39Z (GMT). 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