M1 and E2 transitions in the ground-state configuration of atomic manganese
Abstract Using the multiconfiguration Hartree–Fock approximation within the framework of the Breit–Pauli Hamiltonian (MCHF+BP) and the relativistic Hartree–Fock (HFR) approximation, we have calculated the forbidden transition (M1 and E2) parameters such as transition energies, logarithmic weighted o...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
KABAKÇI, S [verfasserIn] |
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| Format: |
Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2015 |
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| Schlagwörter: |
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| Anmerkung: |
© Indian Academy of Sciences 2015 |
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| Übergeordnetes Werk: |
Enthalten in: Pramāna - Springer India, 1973, 85(2015), 4 vom: 13. Juni, Seite 691-699 |
|---|---|
| Übergeordnetes Werk: |
volume:85 ; year:2015 ; number:4 ; day:13 ; month:06 ; pages:691-699 |
| Links: |
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| DOI / URN: |
10.1007/s12043-014-0911-6 |
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OLC2076066160 |
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| 520 | |a Abstract Using the multiconfiguration Hartree–Fock approximation within the framework of the Breit–Pauli Hamiltonian (MCHF+BP) and the relativistic Hartree–Fock (HFR) approximation, we have calculated the forbidden transition (M1 and E2) parameters such as transition energies, logarithmic weighted oscillator strengths and transition probabilities between the fine-structure levels in the ground-state configuration of $ 3d^{5} $$ 4s^{2} $ for atomic manganese (Mn I, Z = 25). A discussion of these calculations for manganese using MCHF+BP and HFR methods is given here. | ||
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10.1007/s12043-014-0911-6 doi (DE-627)OLC2076066160 (DE-He213)s12043-014-0911-6-p DE-627 ger DE-627 rakwb eng 530 VZ KABAKÇI, S verfasserin aut M1 and E2 transitions in the ground-state configuration of atomic manganese 2015 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Indian Academy of Sciences 2015 Abstract Using the multiconfiguration Hartree–Fock approximation within the framework of the Breit–Pauli Hamiltonian (MCHF+BP) and the relativistic Hartree–Fock (HFR) approximation, we have calculated the forbidden transition (M1 and E2) parameters such as transition energies, logarithmic weighted oscillator strengths and transition probabilities between the fine-structure levels in the ground-state configuration of $ 3d^{5} $$ 4s^{2} $ for atomic manganese (Mn I, Z = 25). A discussion of these calculations for manganese using MCHF+BP and HFR methods is given here. Forbidden transitions transition energies logarithmic weighted oscillator strengths transition probabilities. USTA, B KARAÇOBAN aut ÖZDEMİR, L aut Enthalten in Pramāna Springer India, 1973 85(2015), 4 vom: 13. Juni, Seite 691-699 (DE-627)129403342 (DE-600)186949-8 (DE-576)014785102 0304-4289 nnns volume:85 year:2015 number:4 day:13 month:06 pages:691-699 https://doi.org/10.1007/s12043-014-0911-6 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_70 AR 85 2015 4 13 06 691-699 |
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10.1007/s12043-014-0911-6 doi (DE-627)OLC2076066160 (DE-He213)s12043-014-0911-6-p DE-627 ger DE-627 rakwb eng 530 VZ KABAKÇI, S verfasserin aut M1 and E2 transitions in the ground-state configuration of atomic manganese 2015 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Indian Academy of Sciences 2015 Abstract Using the multiconfiguration Hartree–Fock approximation within the framework of the Breit–Pauli Hamiltonian (MCHF+BP) and the relativistic Hartree–Fock (HFR) approximation, we have calculated the forbidden transition (M1 and E2) parameters such as transition energies, logarithmic weighted oscillator strengths and transition probabilities between the fine-structure levels in the ground-state configuration of $ 3d^{5} $$ 4s^{2} $ for atomic manganese (Mn I, Z = 25). A discussion of these calculations for manganese using MCHF+BP and HFR methods is given here. Forbidden transitions transition energies logarithmic weighted oscillator strengths transition probabilities. USTA, B KARAÇOBAN aut ÖZDEMİR, L aut Enthalten in Pramāna Springer India, 1973 85(2015), 4 vom: 13. Juni, Seite 691-699 (DE-627)129403342 (DE-600)186949-8 (DE-576)014785102 0304-4289 nnns volume:85 year:2015 number:4 day:13 month:06 pages:691-699 https://doi.org/10.1007/s12043-014-0911-6 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_70 AR 85 2015 4 13 06 691-699 |
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10.1007/s12043-014-0911-6 doi (DE-627)OLC2076066160 (DE-He213)s12043-014-0911-6-p DE-627 ger DE-627 rakwb eng 530 VZ KABAKÇI, S verfasserin aut M1 and E2 transitions in the ground-state configuration of atomic manganese 2015 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Indian Academy of Sciences 2015 Abstract Using the multiconfiguration Hartree–Fock approximation within the framework of the Breit–Pauli Hamiltonian (MCHF+BP) and the relativistic Hartree–Fock (HFR) approximation, we have calculated the forbidden transition (M1 and E2) parameters such as transition energies, logarithmic weighted oscillator strengths and transition probabilities between the fine-structure levels in the ground-state configuration of $ 3d^{5} $$ 4s^{2} $ for atomic manganese (Mn I, Z = 25). A discussion of these calculations for manganese using MCHF+BP and HFR methods is given here. Forbidden transitions transition energies logarithmic weighted oscillator strengths transition probabilities. USTA, B KARAÇOBAN aut ÖZDEMİR, L aut Enthalten in Pramāna Springer India, 1973 85(2015), 4 vom: 13. Juni, Seite 691-699 (DE-627)129403342 (DE-600)186949-8 (DE-576)014785102 0304-4289 nnns volume:85 year:2015 number:4 day:13 month:06 pages:691-699 https://doi.org/10.1007/s12043-014-0911-6 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_70 AR 85 2015 4 13 06 691-699 |
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10.1007/s12043-014-0911-6 doi (DE-627)OLC2076066160 (DE-He213)s12043-014-0911-6-p DE-627 ger DE-627 rakwb eng 530 VZ KABAKÇI, S verfasserin aut M1 and E2 transitions in the ground-state configuration of atomic manganese 2015 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Indian Academy of Sciences 2015 Abstract Using the multiconfiguration Hartree–Fock approximation within the framework of the Breit–Pauli Hamiltonian (MCHF+BP) and the relativistic Hartree–Fock (HFR) approximation, we have calculated the forbidden transition (M1 and E2) parameters such as transition energies, logarithmic weighted oscillator strengths and transition probabilities between the fine-structure levels in the ground-state configuration of $ 3d^{5} $$ 4s^{2} $ for atomic manganese (Mn I, Z = 25). A discussion of these calculations for manganese using MCHF+BP and HFR methods is given here. Forbidden transitions transition energies logarithmic weighted oscillator strengths transition probabilities. USTA, B KARAÇOBAN aut ÖZDEMİR, L aut Enthalten in Pramāna Springer India, 1973 85(2015), 4 vom: 13. Juni, Seite 691-699 (DE-627)129403342 (DE-600)186949-8 (DE-576)014785102 0304-4289 nnns volume:85 year:2015 number:4 day:13 month:06 pages:691-699 https://doi.org/10.1007/s12043-014-0911-6 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_70 AR 85 2015 4 13 06 691-699 |
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Abstract Using the multiconfiguration Hartree–Fock approximation within the framework of the Breit–Pauli Hamiltonian (MCHF+BP) and the relativistic Hartree–Fock (HFR) approximation, we have calculated the forbidden transition (M1 and E2) parameters such as transition energies, logarithmic weighted oscillator strengths and transition probabilities between the fine-structure levels in the ground-state configuration of $ 3d^{5} $$ 4s^{2} $ for atomic manganese (Mn I, Z = 25). A discussion of these calculations for manganese using MCHF+BP and HFR methods is given here. © Indian Academy of Sciences 2015 |
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Abstract Using the multiconfiguration Hartree–Fock approximation within the framework of the Breit–Pauli Hamiltonian (MCHF+BP) and the relativistic Hartree–Fock (HFR) approximation, we have calculated the forbidden transition (M1 and E2) parameters such as transition energies, logarithmic weighted oscillator strengths and transition probabilities between the fine-structure levels in the ground-state configuration of $ 3d^{5} $$ 4s^{2} $ for atomic manganese (Mn I, Z = 25). A discussion of these calculations for manganese using MCHF+BP and HFR methods is given here. © Indian Academy of Sciences 2015 |
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Abstract Using the multiconfiguration Hartree–Fock approximation within the framework of the Breit–Pauli Hamiltonian (MCHF+BP) and the relativistic Hartree–Fock (HFR) approximation, we have calculated the forbidden transition (M1 and E2) parameters such as transition energies, logarithmic weighted oscillator strengths and transition probabilities between the fine-structure levels in the ground-state configuration of $ 3d^{5} $$ 4s^{2} $ for atomic manganese (Mn I, Z = 25). A discussion of these calculations for manganese using MCHF+BP and HFR methods is given here. © Indian Academy of Sciences 2015 |
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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">OLC2076066160</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20230402043102.0</controlfield><controlfield tag="007">tu</controlfield><controlfield tag="008">200820s2015 xx ||||| 00| ||eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1007/s12043-014-0911-6</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)OLC2076066160</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-He213)s12043-014-0911-6-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">KABAKÇI, S</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">M1 and E2 transitions in the ground-state configuration of atomic manganese</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2015</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 2015</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract Using the multiconfiguration Hartree–Fock approximation within the framework of the Breit–Pauli Hamiltonian (MCHF+BP) and the relativistic Hartree–Fock (HFR) approximation, we have calculated the forbidden transition (M1 and E2) parameters such as transition energies, logarithmic weighted oscillator strengths and transition probabilities between the fine-structure levels in the ground-state configuration of $ 3d^{5} $$ 4s^{2} $ for atomic manganese (Mn I, Z = 25). A discussion of these calculations for manganese using MCHF+BP and HFR methods is given here.</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Forbidden transitions</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">transition energies</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">logarithmic weighted oscillator strengths</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">transition probabilities.</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">USTA, B KARAÇOBAN</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">ÖZDEMİR, L</subfield><subfield code="4">aut</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">85(2015), 4 vom: 13. Juni, Seite 691-699</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:85</subfield><subfield code="g">year:2015</subfield><subfield code="g">number:4</subfield><subfield code="g">day:13</subfield><subfield code="g">month:06</subfield><subfield code="g">pages:691-699</subfield></datafield><datafield tag="856" ind1="4" ind2="1"><subfield code="u">https://doi.org/10.1007/s12043-014-0911-6</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_70</subfield></datafield><datafield tag="951" ind1=" " ind2=" "><subfield code="a">AR</subfield></datafield><datafield tag="952" ind1=" " ind2=" "><subfield code="d">85</subfield><subfield code="j">2015</subfield><subfield code="e">4</subfield><subfield code="b">13</subfield><subfield code="c">06</subfield><subfield code="h">691-699</subfield></datafield></record></collection>
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