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Measurement of negative chi baryon p...
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Huang, Melin.
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Measurement of negative chi baryon polarization and decay parameters in negative chi baryon decays to lambda baryon and negative pion.
紀錄類型:
書目-語言資料,印刷品 : Monograph/item
正題名/作者:
Measurement of negative chi baryon polarization and decay parameters in negative chi baryon decays to lambda baryon and negative pion./
作者:
Huang, Melin.
面頁冊數:
216 p.
附註:
Adviser: Kenneth S. Nelson.
Contained By:
Dissertation Abstracts International64-03B.
標題:
Physics, Elementary Particles and High Energy. -
電子資源:
http://pqdd.sinica.edu.tw/twdaoapp/servlet/advanced?query=3083116
Measurement of negative chi baryon polarization and decay parameters in negative chi baryon decays to lambda baryon and negative pion.
Huang, Melin.
Measurement of negative chi baryon polarization and decay parameters in negative chi baryon decays to lambda baryon and negative pion.
- 216 p.
Adviser: Kenneth S. Nelson.
Thesis (Ph.D.)--University of Virginia, 2003.
This work describes an experimental study of the decay parameters, β<sub> Ξ</sub> and γ<sub>Ξ</sub>, and the polarization of Ξ<super> −</super> in Ξ<super>−</super> → Λπ<super>− </super> decay. An 800 GeV/<italic>c</italic> proton beam was used to produce Ξ<super> −</super> through the inclusive reaction <italic>p</italic> + <italic> Cu</italic> → Ξ<super>−</super> + <italic>X</italic>. Based on a total sample of 132 million polarized Ξ<super>−</super> after all event selection criteria, the polarization and the decays parameters of the Ξ<super>−</super> were measured. The Ξ<super>−</super> polarization showed an increase in magnitude with both Feynman <italic>x</italic> (<italic>x<sub>f</sub></italic>) and transverse momentum (<italic>p<sub>t </sub></italic>) with an average of −0.0360 ± 0.0005(<italic> stat</italic>.)<math> <f> <hsp sp="0.167"><sup>+0.0005</sup><inf>-0.0002</inf></f> </math> (<italic>sys</italic>.) at a mean <italic>x<sub>f</sub></italic> = 0.20 and <italic>p<sub>t</sub></italic> = 0.46 GeV/<italic>c</italic>. With the direction and the magnitude, of the Ξ<super>−</super> polarization, the <sub>Ξ</sub><super>−</super> decay parameters were measured to be β<sub>Ξ</sub> = −0.080 ± 0.011<math> <f> <hsp sp="0.167"><sup>+0.016</sup><inf>-0.004</inf></f> </math> and γ<sub>Ξ</sub> = 0.893 ± 0.010<math> <f> <hsp sp="0.167"><sup>+0.010</sup><inf>-0.005</inf></f> </math>, yielding &phis;<sub>Ξ</sub> = tan<super>−1</super> (β<sub> Ξ</sub>/γ<sub>Ξ</sub>) = (−5.1 ± 0.7<math> <f> <hsp sp="0.167"><sup>+1.0</sup><inf>-0.3</inf></f> </math>)° and the final-state Λπ strong phase shift difference δ<italic><sub> p</sub></italic><sub>3</sub> − δ<italic><sub>s</sub></italic><sub> 3</sub> = tan<super>−1</super> (β<sub>Ξ</sub>/α<sub>Ξ </sub>) = (9.9 ± 1.3<math> <f> <hsp sp="0.167"><sup>-2.0</sup><inf>+0.5</inf></f> </math>)°, where the first (second) error is the statistical (systematic) error.Subjects--Topical Terms:
1019488
Physics, Elementary Particles and High Energy.
Measurement of negative chi baryon polarization and decay parameters in negative chi baryon decays to lambda baryon and negative pion.
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This work describes an experimental study of the decay parameters, β<sub> Ξ</sub> and γ<sub>Ξ</sub>, and the polarization of Ξ<super> −</super> in Ξ<super>−</super> → Λπ<super>− </super> decay. An 800 GeV/<italic>c</italic> proton beam was used to produce Ξ<super> −</super> through the inclusive reaction <italic>p</italic> + <italic> Cu</italic> → Ξ<super>−</super> + <italic>X</italic>. Based on a total sample of 132 million polarized Ξ<super>−</super> after all event selection criteria, the polarization and the decays parameters of the Ξ<super>−</super> were measured. The Ξ<super>−</super> polarization showed an increase in magnitude with both Feynman <italic>x</italic> (<italic>x<sub>f</sub></italic>) and transverse momentum (<italic>p<sub>t </sub></italic>) with an average of −0.0360 ± 0.0005(<italic> stat</italic>.)<math> <f> <hsp sp="0.167"><sup>+0.0005</sup><inf>-0.0002</inf></f> </math> (<italic>sys</italic>.) at a mean <italic>x<sub>f</sub></italic> = 0.20 and <italic>p<sub>t</sub></italic> = 0.46 GeV/<italic>c</italic>. With the direction and the magnitude, of the Ξ<super>−</super> polarization, the <sub>Ξ</sub><super>−</super> decay parameters were measured to be β<sub>Ξ</sub> = −0.080 ± 0.011<math> <f> <hsp sp="0.167"><sup>+0.016</sup><inf>-0.004</inf></f> </math> and γ<sub>Ξ</sub> = 0.893 ± 0.010<math> <f> <hsp sp="0.167"><sup>+0.010</sup><inf>-0.005</inf></f> </math>, yielding &phis;<sub>Ξ</sub> = tan<super>−1</super> (β<sub> Ξ</sub>/γ<sub>Ξ</sub>) = (−5.1 ± 0.7<math> <f> <hsp sp="0.167"><sup>+1.0</sup><inf>-0.3</inf></f> </math>)° and the final-state Λπ strong phase shift difference δ<italic><sub> p</sub></italic><sub>3</sub> − δ<italic><sub>s</sub></italic><sub> 3</sub> = tan<super>−1</super> (β<sub>Ξ</sub>/α<sub>Ξ </sub>) = (9.9 ± 1.3<math> <f> <hsp sp="0.167"><sup>-2.0</sup><inf>+0.5</inf></f> </math>)°, where the first (second) error is the statistical (systematic) error.
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http://pqdd.sinica.edu.tw/twdaoapp/servlet/advanced?query=3083116
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