Angular anisotropy and dichroism in molecular Auger spectroscopy following photo-absorption
Abstract This paper shows that angular distribution of spin-unresolved Auger electrons emitted in the decay of a vacancy created by the absorption of a photon in a certain class of free, unpolarized and gaseous non-linear molecules is completely characterized by three, rather than by two well-known...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Chakraborty, M. [verfasserIn] |
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| Format: |
Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
1999 |
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| Schlagwörter: |
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| Anmerkung: |
© Indian Academy of Sciences 1999 |
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| Übergeordnetes Werk: |
Enthalten in: Pramāna - Springer India, 1973, 52(1999), 5 vom: Mai, Seite 479-491 |
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| Übergeordnetes Werk: |
volume:52 ; year:1999 ; number:5 ; month:05 ; pages:479-491 |
| Links: |
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| DOI / URN: |
10.1007/BF02830094 |
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OLC2076030956 |
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| 520 | |a Abstract This paper shows that angular distribution of spin-unresolved Auger electrons emitted in the decay of a vacancy created by the absorption of a photon in a certain class of free, unpolarized and gaseous non-linear molecules is completely characterized by three, rather than by two well-known parameters. The presence of this additional third parameter gives rise to circular dichroic effect which varies as cosine of the angle made by the departing Auger electron with the direction of incidence of the circularly polarized radiation. Linear dichroic effect varies as the square of sine of the angle made by the direction of emission of Auger electron and the polar axis of the space frame. Linear and circular dichroism in the angular correlation between theE1 photoelectron and Auger electron emitted sequentially from a molecule belonging to one of the 32 point groups has also been investigated. | ||
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| 650 | 4 | |a Auger electron | |
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| 650 | 4 | |a correlation between photo- and Auger-electron | |
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10.1007/BF02830094 doi (DE-627)OLC2076030956 (DE-He213)BF02830094-p DE-627 ger DE-627 rakwb eng 530 VZ Chakraborty, M. verfasserin aut Angular anisotropy and dichroism in molecular Auger spectroscopy following photo-absorption 1999 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Indian Academy of Sciences 1999 Abstract This paper shows that angular distribution of spin-unresolved Auger electrons emitted in the decay of a vacancy created by the absorption of a photon in a certain class of free, unpolarized and gaseous non-linear molecules is completely characterized by three, rather than by two well-known parameters. The presence of this additional third parameter gives rise to circular dichroic effect which varies as cosine of the angle made by the departing Auger electron with the direction of incidence of the circularly polarized radiation. Linear dichroic effect varies as the square of sine of the angle made by the direction of emission of Auger electron and the polar axis of the space frame. Linear and circular dichroism in the angular correlation between theE1 photoelectron and Auger electron emitted sequentially from a molecule belonging to one of the 32 point groups has also been investigated. Circular dichroism linear dichroism Auger electron photoelectron correlation between photo- and Auger-electron Enthalten in Pramāna Springer India, 1973 52(1999), 5 vom: Mai, Seite 479-491 (DE-627)129403342 (DE-600)186949-8 (DE-576)014785102 0304-4289 nnns volume:52 year:1999 number:5 month:05 pages:479-491 https://doi.org/10.1007/BF02830094 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_11 GBV_ILN_70 GBV_ILN_4012 AR 52 1999 5 05 479-491 |
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10.1007/BF02830094 doi (DE-627)OLC2076030956 (DE-He213)BF02830094-p DE-627 ger DE-627 rakwb eng 530 VZ Chakraborty, M. verfasserin aut Angular anisotropy and dichroism in molecular Auger spectroscopy following photo-absorption 1999 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Indian Academy of Sciences 1999 Abstract This paper shows that angular distribution of spin-unresolved Auger electrons emitted in the decay of a vacancy created by the absorption of a photon in a certain class of free, unpolarized and gaseous non-linear molecules is completely characterized by three, rather than by two well-known parameters. The presence of this additional third parameter gives rise to circular dichroic effect which varies as cosine of the angle made by the departing Auger electron with the direction of incidence of the circularly polarized radiation. Linear dichroic effect varies as the square of sine of the angle made by the direction of emission of Auger electron and the polar axis of the space frame. Linear and circular dichroism in the angular correlation between theE1 photoelectron and Auger electron emitted sequentially from a molecule belonging to one of the 32 point groups has also been investigated. Circular dichroism linear dichroism Auger electron photoelectron correlation between photo- and Auger-electron Enthalten in Pramāna Springer India, 1973 52(1999), 5 vom: Mai, Seite 479-491 (DE-627)129403342 (DE-600)186949-8 (DE-576)014785102 0304-4289 nnns volume:52 year:1999 number:5 month:05 pages:479-491 https://doi.org/10.1007/BF02830094 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_11 GBV_ILN_70 GBV_ILN_4012 AR 52 1999 5 05 479-491 |
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10.1007/BF02830094 doi (DE-627)OLC2076030956 (DE-He213)BF02830094-p DE-627 ger DE-627 rakwb eng 530 VZ Chakraborty, M. verfasserin aut Angular anisotropy and dichroism in molecular Auger spectroscopy following photo-absorption 1999 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Indian Academy of Sciences 1999 Abstract This paper shows that angular distribution of spin-unresolved Auger electrons emitted in the decay of a vacancy created by the absorption of a photon in a certain class of free, unpolarized and gaseous non-linear molecules is completely characterized by three, rather than by two well-known parameters. The presence of this additional third parameter gives rise to circular dichroic effect which varies as cosine of the angle made by the departing Auger electron with the direction of incidence of the circularly polarized radiation. Linear dichroic effect varies as the square of sine of the angle made by the direction of emission of Auger electron and the polar axis of the space frame. Linear and circular dichroism in the angular correlation between theE1 photoelectron and Auger electron emitted sequentially from a molecule belonging to one of the 32 point groups has also been investigated. Circular dichroism linear dichroism Auger electron photoelectron correlation between photo- and Auger-electron Enthalten in Pramāna Springer India, 1973 52(1999), 5 vom: Mai, Seite 479-491 (DE-627)129403342 (DE-600)186949-8 (DE-576)014785102 0304-4289 nnns volume:52 year:1999 number:5 month:05 pages:479-491 https://doi.org/10.1007/BF02830094 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_11 GBV_ILN_70 GBV_ILN_4012 AR 52 1999 5 05 479-491 |
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10.1007/BF02830094 doi (DE-627)OLC2076030956 (DE-He213)BF02830094-p DE-627 ger DE-627 rakwb eng 530 VZ Chakraborty, M. verfasserin aut Angular anisotropy and dichroism in molecular Auger spectroscopy following photo-absorption 1999 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Indian Academy of Sciences 1999 Abstract This paper shows that angular distribution of spin-unresolved Auger electrons emitted in the decay of a vacancy created by the absorption of a photon in a certain class of free, unpolarized and gaseous non-linear molecules is completely characterized by three, rather than by two well-known parameters. The presence of this additional third parameter gives rise to circular dichroic effect which varies as cosine of the angle made by the departing Auger electron with the direction of incidence of the circularly polarized radiation. Linear dichroic effect varies as the square of sine of the angle made by the direction of emission of Auger electron and the polar axis of the space frame. Linear and circular dichroism in the angular correlation between theE1 photoelectron and Auger electron emitted sequentially from a molecule belonging to one of the 32 point groups has also been investigated. Circular dichroism linear dichroism Auger electron photoelectron correlation between photo- and Auger-electron Enthalten in Pramāna Springer India, 1973 52(1999), 5 vom: Mai, Seite 479-491 (DE-627)129403342 (DE-600)186949-8 (DE-576)014785102 0304-4289 nnns volume:52 year:1999 number:5 month:05 pages:479-491 https://doi.org/10.1007/BF02830094 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_11 GBV_ILN_70 GBV_ILN_4012 AR 52 1999 5 05 479-491 |
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10.1007/BF02830094 doi (DE-627)OLC2076030956 (DE-He213)BF02830094-p DE-627 ger DE-627 rakwb eng 530 VZ Chakraborty, M. verfasserin aut Angular anisotropy and dichroism in molecular Auger spectroscopy following photo-absorption 1999 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Indian Academy of Sciences 1999 Abstract This paper shows that angular distribution of spin-unresolved Auger electrons emitted in the decay of a vacancy created by the absorption of a photon in a certain class of free, unpolarized and gaseous non-linear molecules is completely characterized by three, rather than by two well-known parameters. The presence of this additional third parameter gives rise to circular dichroic effect which varies as cosine of the angle made by the departing Auger electron with the direction of incidence of the circularly polarized radiation. Linear dichroic effect varies as the square of sine of the angle made by the direction of emission of Auger electron and the polar axis of the space frame. Linear and circular dichroism in the angular correlation between theE1 photoelectron and Auger electron emitted sequentially from a molecule belonging to one of the 32 point groups has also been investigated. Circular dichroism linear dichroism Auger electron photoelectron correlation between photo- and Auger-electron Enthalten in Pramāna Springer India, 1973 52(1999), 5 vom: Mai, Seite 479-491 (DE-627)129403342 (DE-600)186949-8 (DE-576)014785102 0304-4289 nnns volume:52 year:1999 number:5 month:05 pages:479-491 https://doi.org/10.1007/BF02830094 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_11 GBV_ILN_70 GBV_ILN_4012 AR 52 1999 5 05 479-491 |
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Abstract This paper shows that angular distribution of spin-unresolved Auger electrons emitted in the decay of a vacancy created by the absorption of a photon in a certain class of free, unpolarized and gaseous non-linear molecules is completely characterized by three, rather than by two well-known parameters. The presence of this additional third parameter gives rise to circular dichroic effect which varies as cosine of the angle made by the departing Auger electron with the direction of incidence of the circularly polarized radiation. Linear dichroic effect varies as the square of sine of the angle made by the direction of emission of Auger electron and the polar axis of the space frame. Linear and circular dichroism in the angular correlation between theE1 photoelectron and Auger electron emitted sequentially from a molecule belonging to one of the 32 point groups has also been investigated. © Indian Academy of Sciences 1999 |
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Abstract This paper shows that angular distribution of spin-unresolved Auger electrons emitted in the decay of a vacancy created by the absorption of a photon in a certain class of free, unpolarized and gaseous non-linear molecules is completely characterized by three, rather than by two well-known parameters. The presence of this additional third parameter gives rise to circular dichroic effect which varies as cosine of the angle made by the departing Auger electron with the direction of incidence of the circularly polarized radiation. Linear dichroic effect varies as the square of sine of the angle made by the direction of emission of Auger electron and the polar axis of the space frame. Linear and circular dichroism in the angular correlation between theE1 photoelectron and Auger electron emitted sequentially from a molecule belonging to one of the 32 point groups has also been investigated. © Indian Academy of Sciences 1999 |
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Abstract This paper shows that angular distribution of spin-unresolved Auger electrons emitted in the decay of a vacancy created by the absorption of a photon in a certain class of free, unpolarized and gaseous non-linear molecules is completely characterized by three, rather than by two well-known parameters. The presence of this additional third parameter gives rise to circular dichroic effect which varies as cosine of the angle made by the departing Auger electron with the direction of incidence of the circularly polarized radiation. Linear dichroic effect varies as the square of sine of the angle made by the direction of emission of Auger electron and the polar axis of the space frame. Linear and circular dichroism in the angular correlation between theE1 photoelectron and Auger electron emitted sequentially from a molecule belonging to one of the 32 point groups has also been investigated. © Indian Academy of Sciences 1999 |
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<?xml version="1.0" encoding="UTF-8"?><collection xmlns="http://www.loc.gov/MARC21/slim"><record><leader>01000caa a22002652 4500</leader><controlfield tag="001">OLC2076030956</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20230402042537.0</controlfield><controlfield tag="007">tu</controlfield><controlfield tag="008">200820s1999 xx ||||| 00| ||eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1007/BF02830094</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)OLC2076030956</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-He213)BF02830094-p</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">rakwb</subfield></datafield><datafield tag="041" ind1=" " ind2=" "><subfield code="a">eng</subfield></datafield><datafield tag="082" ind1="0" ind2="4"><subfield code="a">530</subfield><subfield code="q">VZ</subfield></datafield><datafield tag="100" ind1="1" ind2=" "><subfield code="a">Chakraborty, M.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Angular anisotropy and dichroism in molecular Auger spectroscopy following photo-absorption</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">1999</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">ohne Hilfsmittel zu benutzen</subfield><subfield code="b">n</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Band</subfield><subfield code="b">nc</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="500" ind1=" " ind2=" "><subfield code="a">© Indian Academy of Sciences 1999</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract This paper shows that angular distribution of spin-unresolved Auger electrons emitted in the decay of a vacancy created by the absorption of a photon in a certain class of free, unpolarized and gaseous non-linear molecules is completely characterized by three, rather than by two well-known parameters. The presence of this additional third parameter gives rise to circular dichroic effect which varies as cosine of the angle made by the departing Auger electron with the direction of incidence of the circularly polarized radiation. Linear dichroic effect varies as the square of sine of the angle made by the direction of emission of Auger electron and the polar axis of the space frame. Linear and circular dichroism in the angular correlation between theE1 photoelectron and Auger electron emitted sequentially from a molecule belonging to one of the 32 point groups has also been investigated.</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Circular dichroism</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">linear dichroism</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Auger electron</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">photoelectron</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">correlation between photo- and Auger-electron</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">Enthalten in</subfield><subfield code="t">Pramāna</subfield><subfield code="d">Springer India, 1973</subfield><subfield code="g">52(1999), 5 vom: Mai, Seite 479-491</subfield><subfield code="w">(DE-627)129403342</subfield><subfield code="w">(DE-600)186949-8</subfield><subfield code="w">(DE-576)014785102</subfield><subfield code="x">0304-4289</subfield><subfield code="7">nnns</subfield></datafield><datafield tag="773" ind1="1" ind2="8"><subfield code="g">volume:52</subfield><subfield code="g">year:1999</subfield><subfield code="g">number:5</subfield><subfield code="g">month:05</subfield><subfield code="g">pages:479-491</subfield></datafield><datafield tag="856" ind1="4" ind2="1"><subfield code="u">https://doi.org/10.1007/BF02830094</subfield><subfield code="z">lizenzpflichtig</subfield><subfield code="3">Volltext</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_USEFLAG_A</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SYSFLAG_A</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_OLC</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SSG-OLC-PHY</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_11</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_70</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4012</subfield></datafield><datafield tag="951" ind1=" " ind2=" "><subfield code="a">AR</subfield></datafield><datafield tag="952" ind1=" " ind2=" "><subfield code="d">52</subfield><subfield code="j">1999</subfield><subfield code="e">5</subfield><subfield code="c">05</subfield><subfield code="h">479-491</subfield></datafield></record></collection>
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