Molecular effects in light muonic atoms
Abstract Muonic X-ray cascades in B, C, N, O and Ne following muonic atom formation in $ B_{2} $$ H_{6} $, $ CH_{4} $, $ C_{2} $$ H_{6} $, $ C_{4} $$ H_{10} $, $ N_{2} $, $ O_{2} $ and Ne were investigated. The densities of the different target gases were low enough to prevent any contact of the ato...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Kirch, K. [verfasserIn] |
|---|
| Format: |
Artikel |
|---|---|
| Sprache: |
Englisch |
| Erschienen: |
1999 |
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| Anmerkung: |
© Kluwer Academic Publishers 1999 |
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| Übergeordnetes Werk: |
Enthalten in: Hyperfine interactions - Kluwer Academic Publishers, 1975, 119(1999), 1-4 vom: Juni, Seite 83-88 |
|---|---|
| Übergeordnetes Werk: |
volume:119 ; year:1999 ; number:1-4 ; month:06 ; pages:83-88 |
| Links: |
|---|
| DOI / URN: |
10.1023/A:1012658619364 |
|---|
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OLC2076392963 |
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| 520 | |a Abstract Muonic X-ray cascades in B, C, N, O and Ne following muonic atom formation in $ B_{2} $$ H_{6} $, $ CH_{4} $, $ C_{2} $$ H_{6} $, $ C_{4} $$ H_{10} $, $ N_{2} $, $ O_{2} $ and Ne were investigated. The densities of the different target gases were low enough to prevent any contact of the atom or molecule on which the formation takes place with surrounding atoms or molecules during the cascade. Molecular effects of the capturing molecule are clearly seen. The observed transition yields could be reproduced by variation of only two parameters in a cascade calculation: the number of initially available electrons and the muon angular momentum distribution at the starting point of the calculation. By varying the number of electrons, the molecular effects could be described. | ||
| 700 | 1 | |a Hauser, P. |4 aut | |
| 700 | 1 | |a Kottmann, F. |4 aut | |
| 700 | 1 | |a Simons, L.M. |4 aut | |
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10.1023/A:1012658619364 doi (DE-627)OLC2076392963 (DE-He213)A:1012658619364-p DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Kirch, K. verfasserin aut Molecular effects in light muonic atoms 1999 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Kluwer Academic Publishers 1999 Abstract Muonic X-ray cascades in B, C, N, O and Ne following muonic atom formation in $ B_{2} $$ H_{6} $, $ CH_{4} $, $ C_{2} $$ H_{6} $, $ C_{4} $$ H_{10} $, $ N_{2} $, $ O_{2} $ and Ne were investigated. The densities of the different target gases were low enough to prevent any contact of the atom or molecule on which the formation takes place with surrounding atoms or molecules during the cascade. Molecular effects of the capturing molecule are clearly seen. The observed transition yields could be reproduced by variation of only two parameters in a cascade calculation: the number of initially available electrons and the muon angular momentum distribution at the starting point of the calculation. By varying the number of electrons, the molecular effects could be described. Hauser, P. aut Kottmann, F. aut Simons, L.M. aut Enthalten in Hyperfine interactions Kluwer Academic Publishers, 1975 119(1999), 1-4 vom: Juni, Seite 83-88 (DE-627)129438685 (DE-600)194471-X (DE-576)014809028 0304-3843 nnns volume:119 year:1999 number:1-4 month:06 pages:83-88 https://doi.org/10.1023/A:1012658619364 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_20 GBV_ILN_22 GBV_ILN_40 GBV_ILN_70 GBV_ILN_2279 GBV_ILN_4307 33.00 VZ AR 119 1999 1-4 06 83-88 |
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10.1023/A:1012658619364 doi (DE-627)OLC2076392963 (DE-He213)A:1012658619364-p DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Kirch, K. verfasserin aut Molecular effects in light muonic atoms 1999 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Kluwer Academic Publishers 1999 Abstract Muonic X-ray cascades in B, C, N, O and Ne following muonic atom formation in $ B_{2} $$ H_{6} $, $ CH_{4} $, $ C_{2} $$ H_{6} $, $ C_{4} $$ H_{10} $, $ N_{2} $, $ O_{2} $ and Ne were investigated. The densities of the different target gases were low enough to prevent any contact of the atom or molecule on which the formation takes place with surrounding atoms or molecules during the cascade. Molecular effects of the capturing molecule are clearly seen. The observed transition yields could be reproduced by variation of only two parameters in a cascade calculation: the number of initially available electrons and the muon angular momentum distribution at the starting point of the calculation. By varying the number of electrons, the molecular effects could be described. Hauser, P. aut Kottmann, F. aut Simons, L.M. aut Enthalten in Hyperfine interactions Kluwer Academic Publishers, 1975 119(1999), 1-4 vom: Juni, Seite 83-88 (DE-627)129438685 (DE-600)194471-X (DE-576)014809028 0304-3843 nnns volume:119 year:1999 number:1-4 month:06 pages:83-88 https://doi.org/10.1023/A:1012658619364 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_20 GBV_ILN_22 GBV_ILN_40 GBV_ILN_70 GBV_ILN_2279 GBV_ILN_4307 33.00 VZ AR 119 1999 1-4 06 83-88 |
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10.1023/A:1012658619364 doi (DE-627)OLC2076392963 (DE-He213)A:1012658619364-p DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Kirch, K. verfasserin aut Molecular effects in light muonic atoms 1999 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Kluwer Academic Publishers 1999 Abstract Muonic X-ray cascades in B, C, N, O and Ne following muonic atom formation in $ B_{2} $$ H_{6} $, $ CH_{4} $, $ C_{2} $$ H_{6} $, $ C_{4} $$ H_{10} $, $ N_{2} $, $ O_{2} $ and Ne were investigated. The densities of the different target gases were low enough to prevent any contact of the atom or molecule on which the formation takes place with surrounding atoms or molecules during the cascade. Molecular effects of the capturing molecule are clearly seen. The observed transition yields could be reproduced by variation of only two parameters in a cascade calculation: the number of initially available electrons and the muon angular momentum distribution at the starting point of the calculation. By varying the number of electrons, the molecular effects could be described. Hauser, P. aut Kottmann, F. aut Simons, L.M. aut Enthalten in Hyperfine interactions Kluwer Academic Publishers, 1975 119(1999), 1-4 vom: Juni, Seite 83-88 (DE-627)129438685 (DE-600)194471-X (DE-576)014809028 0304-3843 nnns volume:119 year:1999 number:1-4 month:06 pages:83-88 https://doi.org/10.1023/A:1012658619364 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_20 GBV_ILN_22 GBV_ILN_40 GBV_ILN_70 GBV_ILN_2279 GBV_ILN_4307 33.00 VZ AR 119 1999 1-4 06 83-88 |
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10.1023/A:1012658619364 doi (DE-627)OLC2076392963 (DE-He213)A:1012658619364-p DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Kirch, K. verfasserin aut Molecular effects in light muonic atoms 1999 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Kluwer Academic Publishers 1999 Abstract Muonic X-ray cascades in B, C, N, O and Ne following muonic atom formation in $ B_{2} $$ H_{6} $, $ CH_{4} $, $ C_{2} $$ H_{6} $, $ C_{4} $$ H_{10} $, $ N_{2} $, $ O_{2} $ and Ne were investigated. The densities of the different target gases were low enough to prevent any contact of the atom or molecule on which the formation takes place with surrounding atoms or molecules during the cascade. Molecular effects of the capturing molecule are clearly seen. The observed transition yields could be reproduced by variation of only two parameters in a cascade calculation: the number of initially available electrons and the muon angular momentum distribution at the starting point of the calculation. By varying the number of electrons, the molecular effects could be described. Hauser, P. aut Kottmann, F. aut Simons, L.M. aut Enthalten in Hyperfine interactions Kluwer Academic Publishers, 1975 119(1999), 1-4 vom: Juni, Seite 83-88 (DE-627)129438685 (DE-600)194471-X (DE-576)014809028 0304-3843 nnns volume:119 year:1999 number:1-4 month:06 pages:83-88 https://doi.org/10.1023/A:1012658619364 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_20 GBV_ILN_22 GBV_ILN_40 GBV_ILN_70 GBV_ILN_2279 GBV_ILN_4307 33.00 VZ AR 119 1999 1-4 06 83-88 |
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10.1023/A:1012658619364 doi (DE-627)OLC2076392963 (DE-He213)A:1012658619364-p DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Kirch, K. verfasserin aut Molecular effects in light muonic atoms 1999 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Kluwer Academic Publishers 1999 Abstract Muonic X-ray cascades in B, C, N, O and Ne following muonic atom formation in $ B_{2} $$ H_{6} $, $ CH_{4} $, $ C_{2} $$ H_{6} $, $ C_{4} $$ H_{10} $, $ N_{2} $, $ O_{2} $ and Ne were investigated. The densities of the different target gases were low enough to prevent any contact of the atom or molecule on which the formation takes place with surrounding atoms or molecules during the cascade. Molecular effects of the capturing molecule are clearly seen. The observed transition yields could be reproduced by variation of only two parameters in a cascade calculation: the number of initially available electrons and the muon angular momentum distribution at the starting point of the calculation. By varying the number of electrons, the molecular effects could be described. Hauser, P. aut Kottmann, F. aut Simons, L.M. aut Enthalten in Hyperfine interactions Kluwer Academic Publishers, 1975 119(1999), 1-4 vom: Juni, Seite 83-88 (DE-627)129438685 (DE-600)194471-X (DE-576)014809028 0304-3843 nnns volume:119 year:1999 number:1-4 month:06 pages:83-88 https://doi.org/10.1023/A:1012658619364 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_20 GBV_ILN_22 GBV_ILN_40 GBV_ILN_70 GBV_ILN_2279 GBV_ILN_4307 33.00 VZ AR 119 1999 1-4 06 83-88 |
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Abstract Muonic X-ray cascades in B, C, N, O and Ne following muonic atom formation in $ B_{2} $$ H_{6} $, $ CH_{4} $, $ C_{2} $$ H_{6} $, $ C_{4} $$ H_{10} $, $ N_{2} $, $ O_{2} $ and Ne were investigated. The densities of the different target gases were low enough to prevent any contact of the atom or molecule on which the formation takes place with surrounding atoms or molecules during the cascade. Molecular effects of the capturing molecule are clearly seen. The observed transition yields could be reproduced by variation of only two parameters in a cascade calculation: the number of initially available electrons and the muon angular momentum distribution at the starting point of the calculation. By varying the number of electrons, the molecular effects could be described. © Kluwer Academic Publishers 1999 |
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Abstract Muonic X-ray cascades in B, C, N, O and Ne following muonic atom formation in $ B_{2} $$ H_{6} $, $ CH_{4} $, $ C_{2} $$ H_{6} $, $ C_{4} $$ H_{10} $, $ N_{2} $, $ O_{2} $ and Ne were investigated. The densities of the different target gases were low enough to prevent any contact of the atom or molecule on which the formation takes place with surrounding atoms or molecules during the cascade. Molecular effects of the capturing molecule are clearly seen. The observed transition yields could be reproduced by variation of only two parameters in a cascade calculation: the number of initially available electrons and the muon angular momentum distribution at the starting point of the calculation. By varying the number of electrons, the molecular effects could be described. © Kluwer Academic Publishers 1999 |
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Abstract Muonic X-ray cascades in B, C, N, O and Ne following muonic atom formation in $ B_{2} $$ H_{6} $, $ CH_{4} $, $ C_{2} $$ H_{6} $, $ C_{4} $$ H_{10} $, $ N_{2} $, $ O_{2} $ and Ne were investigated. The densities of the different target gases were low enough to prevent any contact of the atom or molecule on which the formation takes place with surrounding atoms or molecules during the cascade. Molecular effects of the capturing molecule are clearly seen. The observed transition yields could be reproduced by variation of only two parameters in a cascade calculation: the number of initially available electrons and the muon angular momentum distribution at the starting point of the calculation. By varying the number of electrons, the molecular effects could be described. © Kluwer Academic Publishers 1999 |
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