Electron- and photon-induced conductivity in chalcogenide glasses
A comprehensive study of the effects of electron and photon beams on the electrical properties of rf-sputtered chalcogenide-glass films of composition Te40As35Si15Ge7P3 has been carried out. Optical results indicate that the material has a gap near 1.1 eV. Four major conclusions follow from a detail...
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Veröffentlicht in: | Journal of applied physics 1976, Vol.47 (4), p.1560-1573 |
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creator | Reinhard, D. K. Adler, D. Arntz, F. O. |
description | A comprehensive study of the effects of electron and photon beams on the electrical properties of rf-sputtered chalcogenide-glass films of composition Te40As35Si15Ge7P3 has been carried out. Optical results indicate that the material has a gap near 1.1 eV. Four major conclusions follow from a detailed investigation of the field and polarity dependence of the photocurrent: (1) the exponential increase of dark conductivity with electric field intensity is a carrier concentration rather than a mobility effect; (2) internal fields exist at molybdenum-chalcogenide junctions; (3) hole conduction dominates electron conduction at room temperature; (4) the chalcogenide bands bend up at the interface with molybdenum electrodes. Electron-beam-induced conductivity (EBIC) resulting from bombardment by 5–20-keV electrons has also been studied as a function of applied voltage on these films. A threshold energy of about 7 keV is necessary to obtain an EBIC signal, resulting from a schubweg of the order of 1000 Å and a film thickness of 1 μm. The photoconductivity and EBIC results are consistent and indicate that the product of mobility and lifetime for the carriers in these materials is approximately 2×10−10 cm2/V. This corresponds to carrier lifetimes of the order of 2×10−11 sec. The drift mobility is trap controlled and of the order of 2×10−5 cm2/V sec. |
doi_str_mv | 10.1063/1.322771 |
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K. ; Adler, D. ; Arntz, F. O.</creator><creatorcontrib>Reinhard, D. K. ; Adler, D. ; Arntz, F. O.</creatorcontrib><description>A comprehensive study of the effects of electron and photon beams on the electrical properties of rf-sputtered chalcogenide-glass films of composition Te40As35Si15Ge7P3 has been carried out. Optical results indicate that the material has a gap near 1.1 eV. Four major conclusions follow from a detailed investigation of the field and polarity dependence of the photocurrent: (1) the exponential increase of dark conductivity with electric field intensity is a carrier concentration rather than a mobility effect; (2) internal fields exist at molybdenum-chalcogenide junctions; (3) hole conduction dominates electron conduction at room temperature; (4) the chalcogenide bands bend up at the interface with molybdenum electrodes. Electron-beam-induced conductivity (EBIC) resulting from bombardment by 5–20-keV electrons has also been studied as a function of applied voltage on these films. A threshold energy of about 7 keV is necessary to obtain an EBIC signal, resulting from a schubweg of the order of 1000 Å and a film thickness of 1 μm. The photoconductivity and EBIC results are consistent and indicate that the product of mobility and lifetime for the carriers in these materials is approximately 2×10−10 cm2/V. This corresponds to carrier lifetimes of the order of 2×10−11 sec. 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O.</creatorcontrib><title>Electron- and photon-induced conductivity in chalcogenide glasses</title><title>Journal of applied physics</title><description>A comprehensive study of the effects of electron and photon beams on the electrical properties of rf-sputtered chalcogenide-glass films of composition Te40As35Si15Ge7P3 has been carried out. Optical results indicate that the material has a gap near 1.1 eV. Four major conclusions follow from a detailed investigation of the field and polarity dependence of the photocurrent: (1) the exponential increase of dark conductivity with electric field intensity is a carrier concentration rather than a mobility effect; (2) internal fields exist at molybdenum-chalcogenide junctions; (3) hole conduction dominates electron conduction at room temperature; (4) the chalcogenide bands bend up at the interface with molybdenum electrodes. Electron-beam-induced conductivity (EBIC) resulting from bombardment by 5–20-keV electrons has also been studied as a function of applied voltage on these films. A threshold energy of about 7 keV is necessary to obtain an EBIC signal, resulting from a schubweg of the order of 1000 Å and a film thickness of 1 μm. The photoconductivity and EBIC results are consistent and indicate that the product of mobility and lifetime for the carriers in these materials is approximately 2×10−10 cm2/V. This corresponds to carrier lifetimes of the order of 2×10−11 sec. 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O.</creator><scope>AAYXX</scope><scope>CITATION</scope><scope>7QQ</scope><scope>8FD</scope><scope>JG9</scope></search><sort><creationdate>1976</creationdate><title>Electron- and photon-induced conductivity in chalcogenide glasses</title><author>Reinhard, D. K. ; Adler, D. ; Arntz, F. O.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c171t-4778bb8947e3da84a49836f9f8caa369430aa57d3c8a58e88f730cb20a6081b73</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>1976</creationdate><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Reinhard, D. K.</creatorcontrib><creatorcontrib>Adler, D.</creatorcontrib><creatorcontrib>Arntz, F. O.</creatorcontrib><collection>CrossRef</collection><collection>Ceramic Abstracts</collection><collection>Technology Research Database</collection><collection>Materials Research Database</collection><jtitle>Journal of applied physics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Reinhard, D. K.</au><au>Adler, D.</au><au>Arntz, F. O.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Electron- and photon-induced conductivity in chalcogenide glasses</atitle><jtitle>Journal of applied physics</jtitle><date>1976</date><risdate>1976</risdate><volume>47</volume><issue>4</issue><spage>1560</spage><epage>1573</epage><pages>1560-1573</pages><issn>0021-8979</issn><eissn>1089-7550</eissn><abstract>A comprehensive study of the effects of electron and photon beams on the electrical properties of rf-sputtered chalcogenide-glass films of composition Te40As35Si15Ge7P3 has been carried out. Optical results indicate that the material has a gap near 1.1 eV. Four major conclusions follow from a detailed investigation of the field and polarity dependence of the photocurrent: (1) the exponential increase of dark conductivity with electric field intensity is a carrier concentration rather than a mobility effect; (2) internal fields exist at molybdenum-chalcogenide junctions; (3) hole conduction dominates electron conduction at room temperature; (4) the chalcogenide bands bend up at the interface with molybdenum electrodes. Electron-beam-induced conductivity (EBIC) resulting from bombardment by 5–20-keV electrons has also been studied as a function of applied voltage on these films. A threshold energy of about 7 keV is necessary to obtain an EBIC signal, resulting from a schubweg of the order of 1000 Å and a film thickness of 1 μm. The photoconductivity and EBIC results are consistent and indicate that the product of mobility and lifetime for the carriers in these materials is approximately 2×10−10 cm2/V. This corresponds to carrier lifetimes of the order of 2×10−11 sec. The drift mobility is trap controlled and of the order of 2×10−5 cm2/V sec.</abstract><doi>10.1063/1.322771</doi><tpages>14</tpages></addata></record> |
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title | Electron- and photon-induced conductivity in chalcogenide glasses |
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