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In high energy physics, a vector meson is a meson with total spin 1 and odd parity (usually noted as JP = 1−). Vector mesons have been seen in experiments since the 1960s, and are well known for their spectroscopic pattern of masses.
Uniquely pure flavor states, Backbone of meson spectroscopy & Hypothetical
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mesons vector meson pure states also pseudovector parity spectroscopy quark nearly scalar total spin flavor fact processes high experiments since
| Subject | Predicate | Object | Confidence | Src |
|---|---|---|---|---|
| Vector meson | is a | meson with total spin 1 and odd parity | 0.90 | text |
| Vector meson | related to Backbone of meson spectroscopy | At | 0.60 | section |
| Vector meson | related to Backbone of meson spectroscopy | In | 0.60 | section |
| Vector meson | related to Backbone of meson spectroscopy | Pseudovector | 0.60 | section |
| Vector meson | related to Backbone of meson spectroscopy | Because | 0.60 | section |
| Vector meson | related to Backbone of meson spectroscopy | Some | 0.60 | section |
| Vector meson | related to Backbone of meson spectroscopy | This | 0.60 | section |
| Vector meson | related to Backbone of meson spectroscopy | JPC | 0.60 | section |
| Vector meson | related to Backbone of meson spectroscopy | Therefore | 0.60 | section |
| Vector meson | related to Backbone of meson spectroscopy | Vector | 0.60 | section |
| Vector meson | related to Uniquely pure flavor states | Since | 0.60 | section |
| Vector meson | related to Uniquely pure flavor states | Murray Gell-Mann | 0.60 | section |
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