Sign of φ-ω Mixing and the OZI Rule
碩士 === 國立臺灣大學 === 物理學系 === 85 === We try to understand the dynamical origin of OZI violation. The earlier works including gluonic annihilation and meson rescattering pictures are reviewed. With the rising value of the vector glueball(O) mas...
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ndltd-TW-085NTU001980182016-07-01T04:15:35Z http://ndltd.ncl.edu.tw/handle/46525501588047294921 Sign of φ-ω Mixing and the OZI Rule φ-ω介子混合的符號與OZI法則 Ko, Cheng-Ying 柯澄瑛 碩士 國立臺灣大學 物理學系 85 We try to understand the dynamical origin of OZI violation. The earlier works including gluonic annihilation and meson rescattering pictures are reviewed. With the rising value of the vector glueball(O) mass, we find that a new viewpoint could be taken: the smallness of $\phi-\omega$ mixing is related to the heaviness of O! A difficulty arises with the sign of the $\phi- \omega$ mixing fromthis model when comparing to experiments. This is solved by redefining the $\phi_0$ state from $s\bar s \rightarrow-s\bar s$ and modifying the mass matrix. We find that Nature chooses this relative sign of $-s\bar s$ for $\phi$ as compared to$\omega\cong(u\bar u+d\bar d)/\sqrt{2}$, if the O dominance pictureis correct. There is a leftover problem with $\rho-\omega$ mass difference, but no other mechanism seems to give any appropriate solution. Perhaps it could be explained by tuning of meson rescattering. Hou Wei-Shu 侯維恕 1997 學位論文 ; thesis 39 zh-TW |
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碩士 === 國立臺灣大學 === 物理學系 === 85 === We try to understand the dynamical origin of OZI violation. The
earlier works including gluonic annihilation and meson
rescattering pictures are reviewed. With the rising value of the
vector glueball(O) mass, we find that a new viewpoint could be
taken: the smallness of $\phi-\omega$ mixing is related to the
heaviness of O! A difficulty arises with the sign of the $\phi-
\omega$ mixing fromthis model when comparing to experiments.
This is solved by redefining the $\phi_0$ state from $s\bar s
\rightarrow-s\bar s$ and modifying the mass matrix. We find that
Nature chooses this relative sign of $-s\bar s$ for $\phi$ as
compared to$\omega\cong(u\bar u+d\bar d)/\sqrt{2}$, if the O
dominance pictureis correct. There is a leftover problem with
$\rho-\omega$ mass difference, but no other mechanism seems to
give any appropriate solution. Perhaps it could be explained by
tuning of meson rescattering.
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author2 |
Hou Wei-Shu |
author_facet |
Hou Wei-Shu Ko, Cheng-Ying 柯澄瑛 |
author |
Ko, Cheng-Ying 柯澄瑛 |
spellingShingle |
Ko, Cheng-Ying 柯澄瑛 Sign of φ-ω Mixing and the OZI Rule |
author_sort |
Ko, Cheng-Ying |
title |
Sign of φ-ω Mixing and the OZI Rule |
title_short |
Sign of φ-ω Mixing and the OZI Rule |
title_full |
Sign of φ-ω Mixing and the OZI Rule |
title_fullStr |
Sign of φ-ω Mixing and the OZI Rule |
title_full_unstemmed |
Sign of φ-ω Mixing and the OZI Rule |
title_sort |
sign of φ-ω mixing and the ozi rule |
publishDate |
1997 |
url |
http://ndltd.ncl.edu.tw/handle/46525501588047294921 |
work_keys_str_mv |
AT kochengying signofphōmixingandtheozirule AT kēchéngyīng signofphōmixingandtheozirule AT kochengying phōjièzihùnhédefúhàoyǔozifǎzé AT kēchéngyīng phōjièzihùnhédefúhàoyǔozifǎzé |
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