Negative muon capture in carbon leading to specific final states
The yields of γ rays from specific final nuclear states excited following negative muon capture in ^1^2C have been measured. Using the values for the capture rates to excited states in ^1^2B and the result of an earlier experiment for the total capture to all bound states in ^1^2B, we obtain for the...
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
1972 |
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| Reproduktion: |
Elsevier Journal Backfiles on ScienceDirect 1907 - 2002 |
|---|---|
| Übergeordnetes Werk: |
in: Physics Letters B - Amsterdam : Elsevier, 41(1972), 1, Seite 50-52 |
| Übergeordnetes Werk: |
volume:41 ; year:1972 ; number:1 ; pages:50-52 |
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NLEJ181172798 |
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| 245 | 1 | 0 | |a Negative muon capture in carbon leading to specific final states |
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| 520 | |a The yields of γ rays from specific final nuclear states excited following negative muon capture in ^1^2C have been measured. Using the values for the capture rates to excited states in ^1^2B and the result of an earlier experiment for the total capture to all bound states in ^1^2B, we obtain for the durect capture rate to the ground state of ^1^2B, λ(^1^2B"g"s) = (6.0 +/- 0.4) x 10^3 s^-^1. This value is in agreement with theoretical predictions, but the theoretical and experimental uncertainties permit extraction of only a rather imprecise value for the weak-magnetism coupling constant in the muon capture Hamiltonian. | ||
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| 700 | 1 | |a Miller, G.H. |4 oth | |
| 700 | 1 | |a Eckhause, M. |4 oth | |
| 700 | 1 | |a Kane, F.R. |4 oth | |
| 700 | 1 | |a Martin, P. |4 oth | |
| 700 | 1 | |a Welsh, R.E. |4 oth | |
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(DE-627)NLEJ181172798 (DE-599)GBVNLZ181172798 DE-627 ger DE-627 rakwb eng Negative muon capture in carbon leading to specific final states 1972 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier The yields of γ rays from specific final nuclear states excited following negative muon capture in ^1^2C have been measured. Using the values for the capture rates to excited states in ^1^2B and the result of an earlier experiment for the total capture to all bound states in ^1^2B, we obtain for the durect capture rate to the ground state of ^1^2B, λ(^1^2B"g"s) = (6.0 +/- 0.4) x 10^3 s^-^1. This value is in agreement with theoretical predictions, but the theoretical and experimental uncertainties permit extraction of only a rather imprecise value for the weak-magnetism coupling constant in the muon capture Hamiltonian. Elsevier Journal Backfiles on ScienceDirect 1907 - 2002 Miller, G.H. oth Eckhause, M. oth Kane, F.R. oth Martin, P. oth Welsh, R.E. oth in Physics Letters B Amsterdam : Elsevier 41(1972), 1, Seite 50-52 (DE-627)NLEJ177212217 (DE-600)1466612-1 0370-2693 nnns volume:41 year:1972 number:1 pages:50-52 http://linkinghub.elsevier.com/retrieve/pii/0370-2693(72)90365-6 GBV_USEFLAG_H ZDB-1-SDJ GBV_NL_ARTICLE AR 41 1972 1 50-52 |
| spelling |
(DE-627)NLEJ181172798 (DE-599)GBVNLZ181172798 DE-627 ger DE-627 rakwb eng Negative muon capture in carbon leading to specific final states 1972 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier The yields of γ rays from specific final nuclear states excited following negative muon capture in ^1^2C have been measured. Using the values for the capture rates to excited states in ^1^2B and the result of an earlier experiment for the total capture to all bound states in ^1^2B, we obtain for the durect capture rate to the ground state of ^1^2B, λ(^1^2B"g"s) = (6.0 +/- 0.4) x 10^3 s^-^1. This value is in agreement with theoretical predictions, but the theoretical and experimental uncertainties permit extraction of only a rather imprecise value for the weak-magnetism coupling constant in the muon capture Hamiltonian. Elsevier Journal Backfiles on ScienceDirect 1907 - 2002 Miller, G.H. oth Eckhause, M. oth Kane, F.R. oth Martin, P. oth Welsh, R.E. oth in Physics Letters B Amsterdam : Elsevier 41(1972), 1, Seite 50-52 (DE-627)NLEJ177212217 (DE-600)1466612-1 0370-2693 nnns volume:41 year:1972 number:1 pages:50-52 http://linkinghub.elsevier.com/retrieve/pii/0370-2693(72)90365-6 GBV_USEFLAG_H ZDB-1-SDJ GBV_NL_ARTICLE AR 41 1972 1 50-52 |
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(DE-627)NLEJ181172798 (DE-599)GBVNLZ181172798 DE-627 ger DE-627 rakwb eng Negative muon capture in carbon leading to specific final states 1972 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier The yields of γ rays from specific final nuclear states excited following negative muon capture in ^1^2C have been measured. Using the values for the capture rates to excited states in ^1^2B and the result of an earlier experiment for the total capture to all bound states in ^1^2B, we obtain for the durect capture rate to the ground state of ^1^2B, λ(^1^2B"g"s) = (6.0 +/- 0.4) x 10^3 s^-^1. This value is in agreement with theoretical predictions, but the theoretical and experimental uncertainties permit extraction of only a rather imprecise value for the weak-magnetism coupling constant in the muon capture Hamiltonian. Elsevier Journal Backfiles on ScienceDirect 1907 - 2002 Miller, G.H. oth Eckhause, M. oth Kane, F.R. oth Martin, P. oth Welsh, R.E. oth in Physics Letters B Amsterdam : Elsevier 41(1972), 1, Seite 50-52 (DE-627)NLEJ177212217 (DE-600)1466612-1 0370-2693 nnns volume:41 year:1972 number:1 pages:50-52 http://linkinghub.elsevier.com/retrieve/pii/0370-2693(72)90365-6 GBV_USEFLAG_H ZDB-1-SDJ GBV_NL_ARTICLE AR 41 1972 1 50-52 |
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(DE-627)NLEJ181172798 (DE-599)GBVNLZ181172798 DE-627 ger DE-627 rakwb eng Negative muon capture in carbon leading to specific final states 1972 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier The yields of γ rays from specific final nuclear states excited following negative muon capture in ^1^2C have been measured. Using the values for the capture rates to excited states in ^1^2B and the result of an earlier experiment for the total capture to all bound states in ^1^2B, we obtain for the durect capture rate to the ground state of ^1^2B, λ(^1^2B"g"s) = (6.0 +/- 0.4) x 10^3 s^-^1. This value is in agreement with theoretical predictions, but the theoretical and experimental uncertainties permit extraction of only a rather imprecise value for the weak-magnetism coupling constant in the muon capture Hamiltonian. Elsevier Journal Backfiles on ScienceDirect 1907 - 2002 Miller, G.H. oth Eckhause, M. oth Kane, F.R. oth Martin, P. oth Welsh, R.E. oth in Physics Letters B Amsterdam : Elsevier 41(1972), 1, Seite 50-52 (DE-627)NLEJ177212217 (DE-600)1466612-1 0370-2693 nnns volume:41 year:1972 number:1 pages:50-52 http://linkinghub.elsevier.com/retrieve/pii/0370-2693(72)90365-6 GBV_USEFLAG_H ZDB-1-SDJ GBV_NL_ARTICLE AR 41 1972 1 50-52 |
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(DE-627)NLEJ181172798 (DE-599)GBVNLZ181172798 DE-627 ger DE-627 rakwb eng Negative muon capture in carbon leading to specific final states 1972 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier The yields of γ rays from specific final nuclear states excited following negative muon capture in ^1^2C have been measured. Using the values for the capture rates to excited states in ^1^2B and the result of an earlier experiment for the total capture to all bound states in ^1^2B, we obtain for the durect capture rate to the ground state of ^1^2B, λ(^1^2B"g"s) = (6.0 +/- 0.4) x 10^3 s^-^1. This value is in agreement with theoretical predictions, but the theoretical and experimental uncertainties permit extraction of only a rather imprecise value for the weak-magnetism coupling constant in the muon capture Hamiltonian. Elsevier Journal Backfiles on ScienceDirect 1907 - 2002 Miller, G.H. oth Eckhause, M. oth Kane, F.R. oth Martin, P. oth Welsh, R.E. oth in Physics Letters B Amsterdam : Elsevier 41(1972), 1, Seite 50-52 (DE-627)NLEJ177212217 (DE-600)1466612-1 0370-2693 nnns volume:41 year:1972 number:1 pages:50-52 http://linkinghub.elsevier.com/retrieve/pii/0370-2693(72)90365-6 GBV_USEFLAG_H ZDB-1-SDJ GBV_NL_ARTICLE AR 41 1972 1 50-52 |
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Negative muon capture in carbon leading to specific final states |
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The yields of γ rays from specific final nuclear states excited following negative muon capture in ^1^2C have been measured. Using the values for the capture rates to excited states in ^1^2B and the result of an earlier experiment for the total capture to all bound states in ^1^2B, we obtain for the durect capture rate to the ground state of ^1^2B, λ(^1^2B"g"s) = (6.0 +/- 0.4) x 10^3 s^-^1. This value is in agreement with theoretical predictions, but the theoretical and experimental uncertainties permit extraction of only a rather imprecise value for the weak-magnetism coupling constant in the muon capture Hamiltonian. |
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The yields of γ rays from specific final nuclear states excited following negative muon capture in ^1^2C have been measured. Using the values for the capture rates to excited states in ^1^2B and the result of an earlier experiment for the total capture to all bound states in ^1^2B, we obtain for the durect capture rate to the ground state of ^1^2B, λ(^1^2B"g"s) = (6.0 +/- 0.4) x 10^3 s^-^1. This value is in agreement with theoretical predictions, but the theoretical and experimental uncertainties permit extraction of only a rather imprecise value for the weak-magnetism coupling constant in the muon capture Hamiltonian. |
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The yields of γ rays from specific final nuclear states excited following negative muon capture in ^1^2C have been measured. Using the values for the capture rates to excited states in ^1^2B and the result of an earlier experiment for the total capture to all bound states in ^1^2B, we obtain for the durect capture rate to the ground state of ^1^2B, λ(^1^2B"g"s) = (6.0 +/- 0.4) x 10^3 s^-^1. This value is in agreement with theoretical predictions, but the theoretical and experimental uncertainties permit extraction of only a rather imprecise value for the weak-magnetism coupling constant in the muon capture Hamiltonian. |
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