A Measurement of the Branching Ratio of Pi[superscript 0] -> E[superscript+] E[superscript-] Using K[subscript L] -> 3pi[superscript 0] Decays in Flight PDF Download
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Author: Eric D. Zimmerman
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Category : Branching ratios (Nuclear physics)
Languages : en
Pages : 344
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![A Measurement of the Branching Ratio of Pi[superscript 0] -> E[superscript+] E[superscript-] Using K[subscript L] -> 3pi[superscript 0] Decays in Flight PDF](https://books.google.com/books/content/images/frontcover/sUZ0IAAACAAJ?fife=w80-h100)
Author: Eric D. Zimmerman
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Category : Branching ratios (Nuclear physics)
Languages : en
Pages : 344
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Author: William Parker Oliver
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Languages : en
Pages : 114
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![A Measurement of the Branching Ratio of the Mode K[subscript L] [arrow Pointing Right] Mu+mu-. PDF](https://books.google.com/books/content/images/frontcover/8mWpHAAACAAJ?fife=w80-h100)
Author: Paul Stanley Linsay
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Category : Branching ratios (Nuclear physics)
Languages : en
Pages : 196
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Author: H. Faissner
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Languages : en
Pages : 20
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![A Measurement of the Branching Ratio KL° -> 2[pi]°/KL° -> 3[pi]° PDF](https://books.google.com/books/content/images/frontcover/5InjoQEACAAJ?fife=w80-h100)
Author: William P. Oliver
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Languages : en
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Author: David Page Coupal
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Category : Kaons
Languages : en
Pages : 306
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Languages : en
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The authors have measured a preliminary value for the branching ratio (Gamma)(D*[sup +][sub s] --> D[sup +][sub s][pi][sup 0])/[Gamma](D*[sup +][sub s] --> D[sup +][sub s][gamma]) = 0.0621 [+-] 0.0049(stat) [+-] 0.0063(syst), which is consistent with the previous measurement, but has higher precision. They have also measured [Gamma](D*[sup 0] --> D[sup 0][pi][sup 0])/[Gamma](D*[sup 0] --> D[sup 0][gamma]) = 1.740 [+-] 0.020(stat) [+-] 0.125(syst), which is more precise than, and in agreement with, the world average. The branching fraction B(D*[sup +][sub s] --> D[sup +][sub s][pi][sup 0]) = 0.0585 [+-] 0.0043(stat) [+-] 0.0056(syst) is larger than the theoretical prediction, which is in the 1-3% range. However, it should be noted that the theory predicts a strong correlation between B(D*[sup +][sub s] --> D[sup +][sub s][pi][sup 0]) and B(D*[sup +] --> D[sup +][gamma]); for B(D*[sup +] --> D[sup +][gamma]) [approx]1%, B(D*[sup +][sub s] -- D[sup +][sub s][pi][sup 0]) is expected to be greatly enhanced.
