Third order nonlinear optical susceptibility for transparent tin oxide thin films
Third order nonlinear optical susceptibilities for transparent SnO2 thin films were examined by a combined study on both the experimental evaluation of X(3)(-3ω:ω, ω, ω) and theoretical analysis of the electronic structure. The X(3) of SnO2 thin film was evaluated to be about 10-12 esu from the meas...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Watanabe, Yuichi [verfasserIn] Sakai, Mitsuhiro [verfasserIn] Takata, Masauke [verfasserIn] Ueda, Naoyuki [verfasserIn] Kawazoe, Hiroshi [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2011 |
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| Übergeordnetes Werk: |
Enthalten in: Ferroelectrics - London [u.a.] : Taylor & Francis, 1970, 131(1992), 1 vom: 01. Juni, Seite 111-117 |
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| Übergeordnetes Werk: |
number:1 ; volume:131 ; year:1992 ; month:06 ; day:01 ; pages:111-117 |
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10.1080/00150199208223400 |
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| 520 | |a Third order nonlinear optical susceptibilities for transparent SnO2 thin films were examined by a combined study on both the experimental evaluation of X(3)(-3ω:ω, ω, ω) and theoretical analysis of the electronic structure. The X(3) of SnO2 thin film was evaluated to be about 10-12 esu from the measurement of the third harmonic generation. The origin of a large X(3) for SnO2 was interpreted as follows: the large mobility of optically excited electrons at the conduction band, which consists of spherically symmetric 5s orbital of Sn atoms, must contribute to the enlargement of dipole moment induced by optical excitation. | ||
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10.1080/00150199208223400 doi (DE-627)NLEJ252062914 (TFO)751940385 DE-627 ger DE-627 rda eng Watanabe, Yuichi verfasserin aut Third order nonlinear optical susceptibility for transparent tin oxide thin films 2011 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Third order nonlinear optical susceptibilities for transparent SnO2 thin films were examined by a combined study on both the experimental evaluation of X(3)(-3ω:ω, ω, ω) and theoretical analysis of the electronic structure. The X(3) of SnO2 thin film was evaluated to be about 10-12 esu from the measurement of the third harmonic generation. The origin of a large X(3) for SnO2 was interpreted as follows: the large mobility of optically excited electrons at the conduction band, which consists of spherically symmetric 5s orbital of Sn atoms, must contribute to the enlargement of dipole moment induced by optical excitation. Sakai, Mitsuhiro verfasserin aut Takata, Masauke verfasserin aut Ueda, Naoyuki verfasserin aut Kawazoe, Hiroshi verfasserin aut Enthalten in Ferroelectrics London [u.a.] : Taylor & Francis, 1970 131(1992), 1 vom: 01. Juni, Seite 111-117 Online-Ressource (DE-627)NLEJ252047974 (DE-600)2042895-9 (DE-576)263253996 1563-5112 nnns number:1 volume:131 year:1992 month:06 day:01 pages:111-117 https://www.tib.eu/de/suchen/id/tandf%3Aeb74b7e1fe5730894a43230b1296d212de32ea64 Digitalisierung Deutschlandweit zugänglich ZDB-1-TFO GBV_NL_ARTICLE AR 1 131 1992 6 01 111-117 |
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10.1080/00150199208223400 doi (DE-627)NLEJ252062914 (TFO)751940385 DE-627 ger DE-627 rda eng Watanabe, Yuichi verfasserin aut Third order nonlinear optical susceptibility for transparent tin oxide thin films 2011 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Third order nonlinear optical susceptibilities for transparent SnO2 thin films were examined by a combined study on both the experimental evaluation of X(3)(-3ω:ω, ω, ω) and theoretical analysis of the electronic structure. The X(3) of SnO2 thin film was evaluated to be about 10-12 esu from the measurement of the third harmonic generation. The origin of a large X(3) for SnO2 was interpreted as follows: the large mobility of optically excited electrons at the conduction band, which consists of spherically symmetric 5s orbital of Sn atoms, must contribute to the enlargement of dipole moment induced by optical excitation. Sakai, Mitsuhiro verfasserin aut Takata, Masauke verfasserin aut Ueda, Naoyuki verfasserin aut Kawazoe, Hiroshi verfasserin aut Enthalten in Ferroelectrics London [u.a.] : Taylor & Francis, 1970 131(1992), 1 vom: 01. Juni, Seite 111-117 Online-Ressource (DE-627)NLEJ252047974 (DE-600)2042895-9 (DE-576)263253996 1563-5112 nnns number:1 volume:131 year:1992 month:06 day:01 pages:111-117 https://www.tib.eu/de/suchen/id/tandf%3Aeb74b7e1fe5730894a43230b1296d212de32ea64 Digitalisierung Deutschlandweit zugänglich ZDB-1-TFO GBV_NL_ARTICLE AR 1 131 1992 6 01 111-117 |
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10.1080/00150199208223400 doi (DE-627)NLEJ252062914 (TFO)751940385 DE-627 ger DE-627 rda eng Watanabe, Yuichi verfasserin aut Third order nonlinear optical susceptibility for transparent tin oxide thin films 2011 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Third order nonlinear optical susceptibilities for transparent SnO2 thin films were examined by a combined study on both the experimental evaluation of X(3)(-3ω:ω, ω, ω) and theoretical analysis of the electronic structure. The X(3) of SnO2 thin film was evaluated to be about 10-12 esu from the measurement of the third harmonic generation. The origin of a large X(3) for SnO2 was interpreted as follows: the large mobility of optically excited electrons at the conduction band, which consists of spherically symmetric 5s orbital of Sn atoms, must contribute to the enlargement of dipole moment induced by optical excitation. Sakai, Mitsuhiro verfasserin aut Takata, Masauke verfasserin aut Ueda, Naoyuki verfasserin aut Kawazoe, Hiroshi verfasserin aut Enthalten in Ferroelectrics London [u.a.] : Taylor & Francis, 1970 131(1992), 1 vom: 01. Juni, Seite 111-117 Online-Ressource (DE-627)NLEJ252047974 (DE-600)2042895-9 (DE-576)263253996 1563-5112 nnns number:1 volume:131 year:1992 month:06 day:01 pages:111-117 https://www.tib.eu/de/suchen/id/tandf%3Aeb74b7e1fe5730894a43230b1296d212de32ea64 Digitalisierung Deutschlandweit zugänglich ZDB-1-TFO GBV_NL_ARTICLE AR 1 131 1992 6 01 111-117 |
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10.1080/00150199208223400 doi (DE-627)NLEJ252062914 (TFO)751940385 DE-627 ger DE-627 rda eng Watanabe, Yuichi verfasserin aut Third order nonlinear optical susceptibility for transparent tin oxide thin films 2011 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Third order nonlinear optical susceptibilities for transparent SnO2 thin films were examined by a combined study on both the experimental evaluation of X(3)(-3ω:ω, ω, ω) and theoretical analysis of the electronic structure. The X(3) of SnO2 thin film was evaluated to be about 10-12 esu from the measurement of the third harmonic generation. The origin of a large X(3) for SnO2 was interpreted as follows: the large mobility of optically excited electrons at the conduction band, which consists of spherically symmetric 5s orbital of Sn atoms, must contribute to the enlargement of dipole moment induced by optical excitation. Sakai, Mitsuhiro verfasserin aut Takata, Masauke verfasserin aut Ueda, Naoyuki verfasserin aut Kawazoe, Hiroshi verfasserin aut Enthalten in Ferroelectrics London [u.a.] : Taylor & Francis, 1970 131(1992), 1 vom: 01. Juni, Seite 111-117 Online-Ressource (DE-627)NLEJ252047974 (DE-600)2042895-9 (DE-576)263253996 1563-5112 nnns number:1 volume:131 year:1992 month:06 day:01 pages:111-117 https://www.tib.eu/de/suchen/id/tandf%3Aeb74b7e1fe5730894a43230b1296d212de32ea64 Digitalisierung Deutschlandweit zugänglich ZDB-1-TFO GBV_NL_ARTICLE AR 1 131 1992 6 01 111-117 |
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10.1080/00150199208223400 doi (DE-627)NLEJ252062914 (TFO)751940385 DE-627 ger DE-627 rda eng Watanabe, Yuichi verfasserin aut Third order nonlinear optical susceptibility for transparent tin oxide thin films 2011 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Third order nonlinear optical susceptibilities for transparent SnO2 thin films were examined by a combined study on both the experimental evaluation of X(3)(-3ω:ω, ω, ω) and theoretical analysis of the electronic structure. The X(3) of SnO2 thin film was evaluated to be about 10-12 esu from the measurement of the third harmonic generation. The origin of a large X(3) for SnO2 was interpreted as follows: the large mobility of optically excited electrons at the conduction band, which consists of spherically symmetric 5s orbital of Sn atoms, must contribute to the enlargement of dipole moment induced by optical excitation. Sakai, Mitsuhiro verfasserin aut Takata, Masauke verfasserin aut Ueda, Naoyuki verfasserin aut Kawazoe, Hiroshi verfasserin aut Enthalten in Ferroelectrics London [u.a.] : Taylor & Francis, 1970 131(1992), 1 vom: 01. Juni, Seite 111-117 Online-Ressource (DE-627)NLEJ252047974 (DE-600)2042895-9 (DE-576)263253996 1563-5112 nnns number:1 volume:131 year:1992 month:06 day:01 pages:111-117 https://www.tib.eu/de/suchen/id/tandf%3Aeb74b7e1fe5730894a43230b1296d212de32ea64 Digitalisierung Deutschlandweit zugänglich ZDB-1-TFO GBV_NL_ARTICLE AR 1 131 1992 6 01 111-117 |
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Enthalten in Ferroelectrics 131(1992), 1 vom: 01. Juni, Seite 111-117 number:1 volume:131 year:1992 month:06 day:01 pages:111-117 |
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Third order nonlinear optical susceptibility for transparent tin oxide thin films |
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Third order nonlinear optical susceptibilities for transparent SnO2 thin films were examined by a combined study on both the experimental evaluation of X(3)(-3ω:ω, ω, ω) and theoretical analysis of the electronic structure. The X(3) of SnO2 thin film was evaluated to be about 10-12 esu from the measurement of the third harmonic generation. The origin of a large X(3) for SnO2 was interpreted as follows: the large mobility of optically excited electrons at the conduction band, which consists of spherically symmetric 5s orbital of Sn atoms, must contribute to the enlargement of dipole moment induced by optical excitation. |
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Third order nonlinear optical susceptibilities for transparent SnO2 thin films were examined by a combined study on both the experimental evaluation of X(3)(-3ω:ω, ω, ω) and theoretical analysis of the electronic structure. The X(3) of SnO2 thin film was evaluated to be about 10-12 esu from the measurement of the third harmonic generation. The origin of a large X(3) for SnO2 was interpreted as follows: the large mobility of optically excited electrons at the conduction band, which consists of spherically symmetric 5s orbital of Sn atoms, must contribute to the enlargement of dipole moment induced by optical excitation. |
| abstract_unstemmed |
Third order nonlinear optical susceptibilities for transparent SnO2 thin films were examined by a combined study on both the experimental evaluation of X(3)(-3ω:ω, ω, ω) and theoretical analysis of the electronic structure. The X(3) of SnO2 thin film was evaluated to be about 10-12 esu from the measurement of the third harmonic generation. The origin of a large X(3) for SnO2 was interpreted as follows: the large mobility of optically excited electrons at the conduction band, which consists of spherically symmetric 5s orbital of Sn atoms, must contribute to the enlargement of dipole moment induced by optical excitation. |
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<?xml version="1.0" encoding="UTF-8"?><collection xmlns="http://www.loc.gov/MARC21/slim"><record><leader>01000naa a22002652 4500</leader><controlfield tag="001">NLEJ252062914</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20231206141239.0</controlfield><controlfield tag="007">cr uuu---uuuuu</controlfield><controlfield tag="008">231206s2011 xx |||||o 00| ||eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1080/00150199208223400</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)NLEJ252062914</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(TFO)751940385</subfield></datafield><datafield tag="040" ind1=" " ind2=" "><subfield code="a">DE-627</subfield><subfield code="b">ger</subfield><subfield code="c">DE-627</subfield><subfield code="e">rda</subfield></datafield><datafield tag="041" ind1=" " ind2=" "><subfield code="a">eng</subfield></datafield><datafield tag="100" ind1="1" ind2=" "><subfield code="a">Watanabe, Yuichi</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Third order nonlinear optical susceptibility for transparent tin oxide thin films</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2011</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">Text</subfield><subfield code="b">txt</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">Computermedien</subfield><subfield code="b">c</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Online-Ressource</subfield><subfield code="b">cr</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Third order nonlinear optical susceptibilities for transparent SnO2 thin films were examined by a combined study on both the experimental evaluation of X(3)(-3ω:ω, ω, ω) and theoretical analysis of the electronic structure. The X(3) of SnO2 thin film was evaluated to be about 10-12 esu from the measurement of the third harmonic generation. The origin of a large X(3) for SnO2 was interpreted as follows: the large mobility of optically excited electrons at the conduction band, which consists of spherically symmetric 5s orbital of Sn atoms, must contribute to the enlargement of dipole moment induced by optical excitation.</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Sakai, Mitsuhiro</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Takata, Masauke</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Ueda, Naoyuki</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Kawazoe, Hiroshi</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">Enthalten in</subfield><subfield code="t">Ferroelectrics</subfield><subfield code="d">London [u.a.] : Taylor & Francis, 1970</subfield><subfield code="g">131(1992), 1 vom: 01. Juni, Seite 111-117</subfield><subfield code="h">Online-Ressource</subfield><subfield code="w">(DE-627)NLEJ252047974</subfield><subfield code="w">(DE-600)2042895-9</subfield><subfield code="w">(DE-576)263253996</subfield><subfield code="x">1563-5112</subfield><subfield code="7">nnns</subfield></datafield><datafield tag="773" ind1="1" ind2="8"><subfield code="g">number:1</subfield><subfield code="g">volume:131</subfield><subfield code="g">year:1992</subfield><subfield code="g">month:06</subfield><subfield code="g">day:01</subfield><subfield code="g">pages:111-117</subfield></datafield><datafield tag="856" ind1="4" ind2="0"><subfield code="u">https://www.tib.eu/de/suchen/id/tandf%3Aeb74b7e1fe5730894a43230b1296d212de32ea64</subfield><subfield code="x">Digitalisierung</subfield><subfield code="z">Deutschlandweit zugänglich</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">ZDB-1-TFO</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_NL_ARTICLE</subfield></datafield><datafield tag="951" ind1=" " ind2=" "><subfield code="a">AR</subfield></datafield><datafield tag="952" ind1=" " ind2=" "><subfield code="e">1</subfield><subfield code="d">131</subfield><subfield code="j">1992</subfield><subfield code="c">6</subfield><subfield code="b">01</subfield><subfield code="h">111-117</subfield></datafield></record></collection>
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