CHARMED MESONS ($\mathit C$ = $\pm1$) ${{\mathit D}^{+}}$ = ${\mathit {\mathit c}}$ ${\mathit {\overline{\mathit d}}}$, ${{\mathit D}^{0}}$ = ${\mathit {\mathit c}}$ ${\mathit {\overline{\mathit u}}}$, ${{\overline{\mathit D}}^{0}}$ = ${\mathit {\overline{\mathit c}}}$ ${\mathit {\mathit u}}$, ${{\mathit D}^{-}}$ = ${\mathit {\overline{\mathit c}}}$ ${\mathit {\mathit d}}$, similarly for ${{\mathit D}^{*}}$'s |
INSPIRE
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PDGID: S032
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${{\mathit D}^{0}}$ |
See related review: | |
${{\mathit D}^{0}}$ $-$ ${{\overline{\mathit D}}^{0}}$ Mixing |
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${{\mathit D}^{0}}$ $\mathit CP$-VIOLATING ASYMMETRY DIFFERENCES | |||
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${{\mathit D}^{0}}$ $\mathit CPT$-VIOLATING DECAY-RATE ASYMMETRIES | |||
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Amplitude analyses | |||
${{\mathit D}^{0}}$ DECAY MODES ▸ Expand all decays | ||||||||||
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Most decay modes (other than the semileptonic modes) that involve a neutral ${{\mathit K}}$ meson are now given as ${{\mathit K}_S^0}$ modes, not as ${{\overline{\mathit K}}^{0}}$ modes. Nearly always it is a ${{\mathit K}_S^0}$ that is measured, and interference between Cabibbo-allowed and doubly Cabibbo-suppressed modes can invalidate the assumption that 2$~\Gamma ({{\mathit K}_S^0}$ ) = $\Gamma ({{\overline{\mathit K}}^{0}}$).
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Constrained Fit information |
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