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BOTTOM, STRANGE MESONS
($\mathit B$ = $\pm1$, $\mathit S$ = $\mp{}$1)
${{\mathit B}_{{s}}^{0}}$ = ${\mathit {\mathit s}}$ ${\mathit {\overline{\mathit b}}}$, ${{\overline{\mathit B}}_{{s}}^{0}}$ = ${\mathit {\overline{\mathit s}}}$ ${\mathit {\mathit b}}$,
similarly for ${{\mathit B}_{{s}}^{*}}$'s

INSPIRE JSON (beta) PDGID:

${{\mathit B}_{{s}}^{0}}$

$I(J^P)$ = $0(0^{-})$

$\mathit I$, $\mathit J$, ${}^{P}$ need confirmation. Quantum numbers shown are quark-model predictions.

${{\mathit B}_{{s}}^{0}}$ MASS

$5366.92 \pm0.10$ MeV

${\mathit m}_{{{\mathit B}_{{s}}^{0}}}–{\mathit m}_{{{\mathit B}}}$

$87.42 \pm0.14$ MeV

$\Gamma _{{{\mathit B}_{{s}}^{0}}}$

$(65.73 \pm0.23) \times 10^{10}$ s${}^{-1}$ (S = 2.6)

$\Delta \Gamma _{{{\mathit B}_{{s}}^{0}}}/\Gamma _{{{\mathit B}_{{s}}^{0}}}$

$0.126 \pm0.007$

${{\mathit B}_{{sH}}^{0}}$ MEAN LIFE

$(1.624 \pm0.009) \times 10^{-12}$ s

${{\mathit B}_{{sL}}^{0}}$ MEAN LIFE

$(1.431 \pm0.007) \times 10^{-12}$ s

${{\mathit B}_{{s}}^{0}}$ MEAN LIFE (Flavor specific)

$(1.527 \pm0.011) \times 10^{-12}$ s

▸	POLARIZATION IN ${{\mathit B}_{{s}}^{0}}$ DECAY

▸	${{\mathit B}_{{s}}^{0}}-{{\overline{\mathit B}}_{{s}}^{0}}$ MIXING

▸	$\mathit CP$ VIOLATION PARAMETERS in ${{\mathit B}_{{s}}^{0}}$

▸	$\mathit CPT$ VIOLATION PARAMETERS

▸	PARTIAL BRANCHING FRACTIONS IN ${{\mathit B}_{{s}}}$ $\rightarrow$ ${{\mathit \phi}}{{\mathit \ell}^{+}}{{\mathit \ell}^{-}}$

PRODUCTION ASYMMETRIES

A$_{P}({{\mathit B}_{{s}}^{0}}$)

$0.012 \pm0.016$

${{\mathit B}_{{s}}^{0}}$ $\rightarrow$ ${{\mathit D}_{{s}}^{*-}}{{\mathit \ell}^{+}}{{\mathit \nu}_{{{{\mathit \ell}}}}}$ FORM FACTORS

$\rho {}^{2}$ (form factor slope)

${{\mathit B}_{{s}}^{0}}$ DECAY MODES ▸ Expand all decays

These branching fractions all scale with B( ${{\overline{\mathit b}}}$ $\rightarrow$ ${{\mathit B}_{{s}}^{0}}$ ).
The branching fraction B( ${{\mathit B}_{{s}}^{0}}$ $\rightarrow$ ${{\mathit D}_{{s}}^{-}}{{\mathit \ell}^{+}}{{\mathit \nu}_{{{{\mathit \ell}}}}}$ anything) is not a pure measurement since the measured product branching fraction B( ${{\overline{\mathit b}}}$ $\rightarrow$ ${{\mathit B}_{{s}}^{0}}$ ) ${\times }$ B( ${{\mathit B}_{{s}}^{0}}$ $\rightarrow$ ${{\mathit D}_{{s}}^{-}}{{\mathit \ell}^{+}}{{\mathit \nu}_{{{{\mathit \ell}}}}}$ anything) was used to determine B( ${{\overline{\mathit b}}}$ $\rightarrow$ ${{\mathit B}_{{s}}^{0}}$ ), as described in the note on ``${{\mathit B}^{0}}-{{\overline{\mathit B}}^{0}}$ Mixing''
For inclusive branching fractions, $\mathit e.g.,$ ${{\mathit B}}$ $\rightarrow$ ${{\mathit D}^{\pm}}$ anything, the values usually are multiplicities, not branching fractions. They can be greater than one.

${{\mathit D}_{{s}}^{-}}$ anything

${{\mathit \ell}}{{\mathit \nu}_{{{{\mathit \ell}}}}}{{\mathit X}}$

$(9.6\pm{0.8})\%$

${{\mathit e}^{+}}{{\mathit \nu}}{{\mathit X}^{-}}$

$(9.1\pm{0.8})\%$

${{\mathit \mu}^{+}}{{\mathit \nu}}{{\mathit X}^{-}}$

$(10.2\pm{1.0})\%$

${{\mathit D}_{{s}}^{-}}{{\mathit \ell}^{+}}{{\mathit \nu}_{{{{\mathit \ell}}}}}$ anything

$(8.1\pm{1.3})\%$

${{\mathit D}_{{s}}^{*-}}{{\mathit \ell}^{+}}{{\mathit \nu}_{{{{\mathit \ell}}}}}$ anything

$(5.4\pm{1.1})\%$

${{\mathit D}_{{s}}^{-}}{{\mathit \mu}^{+}}{{\mathit \nu}_{{\mu}}}$

$(2.44\pm{0.23})\%$

${{\mathit D}_{{s}}^{*-}}{{\mathit \mu}^{+}}{{\mathit \nu}_{{\mu}}}$

$(5.3\pm{0.5})\%$

${{\mathit D}_{{s1}}{(2536)}^{-}}{{\mathit \mu}^{+}}{{\mathit \nu}_{{\mu}}}$ , ${{\mathit D}_{{s1}}^{-}}$ $\rightarrow$ ${{\mathit D}^{*-}}{{\mathit K}_S^0}$

$(2.7\pm{0.7})\times 10^{-3}$

${{\mathit D}_{{s1}}{(2536)}^{-}}{{\mathit X}}{{\mathit \mu}^{+}}{{\mathit \nu}}$ , ${{\mathit D}_{{s1}}^{-}}$ $\rightarrow$ ${{\overline{\mathit D}}^{0}}{{\mathit K}^{+}}$

$(4.4\pm{1.3})\times 10^{-3}$

${{\mathit D}_{{s2}}{(2573)}^{-}}{{\mathit X}}{{\mathit \mu}^{+}}{{\mathit \nu}}$ , ${{\mathit D}_{{s2}}^{-}}$ $\rightarrow$ ${{\overline{\mathit D}}^{0}}{{\mathit K}^{+}}$

$(2.7\pm{1.0})\times 10^{-3}$

${{\mathit K}^{-}}{{\mathit \mu}^{+}}{{\mathit \nu}_{{\mu}}}$

$(1.06\pm{0.09})\times 10^{-4}$

${{\mathit D}_{{s}}^{-}}{{\mathit \pi}^{+}}$

$(2.98\pm{0.14})\times 10^{-3}$

${{\mathit D}_{{s}}^{-}}{{\mathit \rho}^{+}}$

$(6.8\pm{1.4})\times 10^{-3}$

${{\mathit D}_{{s}}^{-}}{{\mathit \pi}^{+}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$

$(6.1\pm{1.0})\times 10^{-3}$

${{\mathit D}_{{s1}}{(2536)}^{-}}{{\mathit \pi}^{+}}$ , ${{\mathit D}_{{s1}}^{-}}$ $\rightarrow$ ${{\mathit D}_{{s}}^{-}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$

$(2.4\pm{0.8})\times 10^{-5}$

${{\mathit D}_{{s}}^{\mp}}{{\mathit K}^{\pm}}$

$(2.25\pm{0.12})\times 10^{-4}$

${{\mathit D}_{{s}}^{-}}{{\mathit K}^{+}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$

$(3.2\pm{0.6})\times 10^{-4}$

${{\mathit D}_{{s}}^{+}}{{\mathit D}_{{s}}^{-}}$

$(4.4\pm{0.5})\times 10^{-3}$

${{\mathit D}_{{s}}^{-}}{{\mathit D}^{+}}$

$(2.8\pm{0.5})\times 10^{-4}$

${{\mathit D}^{+}}{{\mathit D}^{-}}$

$(2.2\pm{0.6})\times 10^{-4}$

${{\mathit D}^{*+}}{{\mathit D}^{-}}$

${{\mathit D}^{*-}}{{\mathit D}^{+}}$

${{\mathit D}^{0}}{{\overline{\mathit D}}^{0}}$

$(1.9\pm{0.5})\times 10^{-4}$

${{\mathit D}_{{s}}^{*-}}{{\mathit \pi}^{+}}$

$(1.9^{+0.5}_{-0.4})\times 10^{-3}$

${{\mathit D}_{{s}}^{*\mp}}{{\mathit K}^{\pm}}$

$(1.32^{+0.40}_{-0.32})\times 10^{-4}$

${{\mathit D}_{{s}}^{*-}}{{\mathit \rho}^{+}}$

$(9.5\pm{2.0})\times 10^{-3}$

${{\mathit D}_{{s}}^{*+}}{{\mathit D}_{{s}}^{-}}{+}$ ${{\mathit D}_{{s}}^{*-}}{{\mathit D}_{{s}}^{+}}$

$(1.39\pm{0.17})\%$

${{\mathit D}_{{s}}^{*+}}{{\mathit D}_{{s}}^{*-}}$

$(1.44\pm{0.21})\%$

${{\mathit D}_{{s}}^{(*)+}}{{\mathit D}_{{s}}^{(*)-}}$

$(4.5\pm{1.4})\%$

${{\mathit D}^{*-}}{{\mathit D}_{{s}}^{+}}$

$(3.9\pm{0.8})\times 10^{-4}$

${{\overline{\mathit D}}^{*0}}{{\overline{\mathit K}}^{0}}$

$(2.8\pm{1.1})\times 10^{-4}$

${{\overline{\mathit D}}^{0}}{{\overline{\mathit K}}^{0}}$

$(4.3\pm{0.9})\times 10^{-4}$

${{\overline{\mathit D}}^{0}}{{\mathit K}^{-}}{{\mathit \pi}^{+}}$

$(1.04\pm{0.13})\times 10^{-3}$

${{\overline{\mathit D}}^{*}{(2007)}^{0}}{{\mathit K}^{-}}{{\mathit \pi}^{+}}$

$(7.3\pm{2.6})\times 10^{-4}$

${{\overline{\mathit D}}^{0}}{{\overline{\mathit K}}^{*}{(892)}^{0}}$

$(4.4\pm{0.6})\times 10^{-4}$

${{\overline{\mathit D}}^{0}}{{\overline{\mathit K}}^{*}{(1410)}}$

$(3.9\pm{3.5})\times 10^{-4}$

${{\overline{\mathit D}}^{0}}{{\overline{\mathit K}}_{{0}}^{*}{(1430)}}$

$(3.0\pm{0.7})\times 10^{-4}$

${{\overline{\mathit D}}^{0}}{{\overline{\mathit K}}_{{2}}^{*}{(1430)}}$

$(1.1\pm{0.4})\times 10^{-4}$

${{\overline{\mathit D}}^{0}}{{\overline{\mathit K}}^{*}{(1680)}}$

$<7.8\times 10^{-5}$

${{\overline{\mathit D}}^{0}}{{\overline{\mathit K}}_{{0}}^{*}{(1950)}}$

$<1.1\times 10^{-4}$

${{\overline{\mathit D}}^{0}}{{\overline{\mathit K}}_{{3}}^{*}{(1780)}}$

$<2.6\times 10^{-5}$

${{\overline{\mathit D}}^{0}}{{\overline{\mathit K}}_{{4}}^{*}{(2045)}}$

$<3.1\times 10^{-5}$

${{\overline{\mathit D}}^{0}}{{\mathit K}^{-}}{{\mathit \pi}^{+}}$ (non-resonant)

$(2.1\pm{0.8})\times 10^{-4}$

${{\mathit D}_{{s2}}^{*}{(2573)}^{-}}{{\mathit \pi}^{+}}$ , ${{\mathit D}_{{s2}}^{*}}$ $\rightarrow$ ${{\overline{\mathit D}}^{0}}{{\mathit K}^{-}}$

$(2.6\pm{0.4})\times 10^{-4}$

${{\mathit D}_{{s1}}^{*}{(2700)}^{-}}{{\mathit \pi}^{+}}$ , ${{\mathit D}_{{s1}}^{*}}$ $\rightarrow$ ${{\overline{\mathit D}}^{0}}{{\mathit K}^{-}}$

$(1.6\pm{0.8})\times 10^{-5}$

${{\mathit D}_{{s1}}^{*}{(2860)}^{-}}{{\mathit \pi}^{+}}$ , ${{\mathit D}_{{s1}}^{*}}$ $\rightarrow$ ${{\overline{\mathit D}}^{0}}{{\mathit K}^{-}}$

$(5\pm{4})\times 10^{-5}$

${{\mathit D}_{{s3}}^{*}{(2860)}^{-}}{{\mathit \pi}^{+}}$ , ${{\mathit D}_{{s3}}^{*}}$ $\rightarrow$ ${{\overline{\mathit D}}^{0}}{{\mathit K}^{-}}$

$(2.2\pm{0.6})\times 10^{-5}$

${{\overline{\mathit D}}^{0}}{{\mathit K}^{+}}{{\mathit K}^{-}}$

$(5.6\pm{0.9})\times 10^{-5}$

${{\overline{\mathit D}}^{0}}{{\mathit f}_{{0}}{(980)}}$

$<3.1\times 10^{-6}$

${{\overline{\mathit D}}^{0}}{{\mathit \phi}}$

$(3.0\pm{0.5})\times 10^{-5}$

${{\overline{\mathit D}}^{*0}}{{\mathit \phi}}$

$(3.7\pm{0.6})\times 10^{-5}$

${{\mathit D}^{*\mp}}{{\mathit \pi}^{\pm}}$

$<6.1\times 10^{-6}$

${{\mathit \eta}_{{c}}}{{\mathit \phi}}$

$(5.0\pm{0.9})\times 10^{-4}$

${{\mathit \eta}^{\,'}}{{\mathit X}}$ $_{ {{\mathit s}} {{\overline{\mathit s}}} }$

${{\mathit \eta}_{{c}}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$

$(1.8\pm{0.7})\times 10^{-4}$

${{\mathit J / \psi}{(1S)}}{{\mathit \phi}}$

$(1.04\pm{0.04})\times 10^{-3}$

${{\mathit J / \psi}{(1S)}}{{\mathit \phi}}{{\mathit \phi}}$

$(1.20^{+0.14}_{-0.16})\times 10^{-5}$

${{\mathit J / \psi}{(1S)}}{{\mathit \pi}^{0}}$

$<1.2\times 10^{-3}$

${{\mathit J / \psi}{(1S)}}{{\mathit \eta}}$

$(4.0\pm{0.7})\times 10^{-4}$

${{\mathit J / \psi}{(1S)}}{{\mathit K}_S^0}$

$(1.92\pm{0.14})\times 10^{-5}$

${{\mathit J / \psi}{(1S)}}{{\overline{\mathit K}}^{*}{(892)}^{0}}$

$(4.1\pm{0.4})\times 10^{-5}$

${{\mathit J / \psi}{(1S)}}{{\mathit \eta}^{\,'}}$

$(3.3\pm{0.4})\times 10^{-4}$

${{\mathit J / \psi}{(1S)}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$

$(2.02\pm{0.17})\times 10^{-4}$

${{\mathit J / \psi}{(1S)}}{{\mathit f}_{{0}}{(500)}}$ , ${{\mathit f}_{{0}}}$ $\rightarrow$ ${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$

$<4\times 10^{-6}$

${{\mathit J / \psi}{(1S)}}{{\mathit \rho}}$ , ${{\mathit \rho}}$ $\rightarrow$ ${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$

$<3.4\times 10^{-6}$

${{\mathit J / \psi}{(1S)}}{{\mathit f}_{{0}}{(980)}}$ , ${{\mathit f}_{{0}}}$ $\rightarrow$ ${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$

$(1.24\pm{0.15})\times 10^{-4}$

${{\mathit J / \psi}{(1S)}}{{\mathit f}_{{2}}{(1270)}}$ , ${{\mathit f}_{{2}}}$ $\rightarrow$ ${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$

$(1.0\pm{0.4})\times 10^{-6}$

${{\mathit J / \psi}{(1S)}}{{\mathit f}_{{2}}{(1270)}}$ $_{0}$ , ${{\mathit f}_{{2}}}$ $\rightarrow$ ${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$

$(7.3\pm{1.7})\times 10^{-7}$

${{\mathit J / \psi}{(1S)}}{{\mathit f}_{{2}}{(1270)}}$ $_{\parallel}$ , ${{\mathit f}_{{2}}}$ $\rightarrow$ ${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$

$(1.05\pm{0.33})\times 10^{-6}$

${{\mathit J / \psi}{(1S)}}{{\mathit f}_{{2}}{(1270)}}$ $_{\perp}$ , ${{\mathit f}_{{2}}}$ $\rightarrow$ ${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$

$(1.3\pm{0.7})\times 10^{-6}$

${{\mathit J / \psi}{(1S)}}{{\mathit f}_{{0}}{(1370)}}$ , ${{\mathit f}_{{0}}}$ $\rightarrow$ ${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$

$(4.4^{+0.6}_{-4.0})\times 10^{-5}$

${{\mathit J / \psi}{(1S)}}{{\mathit f}_{{0}}{(1500)}}$ , ${{\mathit f}_{{0}}}$ $\rightarrow$ ${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$

$(2.04^{+0.32}_{-0.24})\times 10^{-5}$

${{\mathit J / \psi}{(1S)}}{{\mathit f}_{{2}}^{\,'}{(1525)}}$ $_{0}$ , ${{\mathit f}_{{2}}^{\,'}}$ $\rightarrow$ ${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$

$(1.03\pm{0.22})\times 10^{-6}$

${{\mathit J / \psi}{(1S)}}{{\mathit f}_{{2}}^{\,'}{(1525)}}$ $_{\parallel}$ , ${{\mathit f}_{{2}}^{\,'}}$ $\rightarrow$ ${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$

$(1.2^{+2.6}_{-0.8})\times 10^{-7}$

${{\mathit J / \psi}{(1S)}}{{\mathit f}_{{2}}^{\,'}{(1525)}}$ $_{\perp}$ , ${{\mathit f}_{{2}}^{\,'}}$ $\rightarrow$ ${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$

$(5\pm{4})\times 10^{-7}$

${{\mathit J / \psi}{(1S)}}{{\mathit f}_{{0}}{(1790)}}$ , ${{\mathit f}_{{0}}}$ $\rightarrow$ ${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$

$(4.9^{+10.0}_{-1.0})\times 10^{-6}$

${{\mathit J / \psi}{(1S)}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$ (nonresonant)

$(1.74^{+1.10}_{-0.34})\times 10^{-5}$

${{\mathit J / \psi}{(1S)}}{{\overline{\mathit K}}^{0}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$

$<4.4\times 10^{-5}$

${{\mathit J / \psi}{(1S)}}{{\mathit K}^{+}}{{\mathit K}^{-}}$

$(7.9\pm{0.7})\times 10^{-4}$

${{\mathit J / \psi}{(1S)}}{{\mathit K}^{0}}{{\mathit K}^{-}}{{\mathit \pi}^{+}}$ + c.c.

$(9.5\pm{1.3})\times 10^{-4}$

${{\mathit J / \psi}{(1S)}}{{\overline{\mathit K}}^{0}}{{\mathit K}^{+}}{{\mathit K}^{-}}$

$<1.2\times 10^{-5}$

${{\mathit J / \psi}}{{\mathit K}^{*}{(892)}^{0}}{{\overline{\mathit K}}^{*}{(892)}^{0}}$

$(1.10\pm{0.09})\times 10^{-4}$

${{\mathit J / \psi}{(1S)}}{{\mathit f}_{{2}}^{\,'}{(1525)}}$

$(2.6\pm{0.6})\times 10^{-4}$

${{\mathit J / \psi}{(1S)}}{{\mathit p}}{{\overline{\mathit p}}}$

$(3.6\pm{0.4})\times 10^{-6}$

${{\mathit J / \psi}{(1S)}}{{\mathit \gamma}}$

$<7.3\times 10^{-6}$

${{\mathit J / \psi}}{{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$ , ${{\mathit J / \psi}}$ $\rightarrow$ ${{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$

$<2.6\times 10^{-9}$

${{\mathit J / \psi}{(1S)}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$

$(7.5\pm{0.8})\times 10^{-5}$

${{\mathit J / \psi}{(1S)}}{{\mathit f}_{{1}}{(1285)}}$

$(7.2\pm{1.4})\times 10^{-5}$

${{\mathit \psi}{(2S)}}{{\mathit \eta}}$

$(3.3\pm{0.9})\times 10^{-4}$

${{\mathit \psi}{(2S)}}{{\mathit \eta}^{\,'}}$

$(1.29\pm{0.35})\times 10^{-4}$

${{\mathit \psi}{(2S)}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$

$(6.9\pm{1.2})\times 10^{-5}$

${{\mathit \psi}{(2S)}}{{\mathit \phi}}$

$(5.2\pm{0.4})\times 10^{-4}$

${{\mathit \psi}{(2S)}}{{\mathit K}^{0}}$

$(1.9\pm{0.5})\times 10^{-5}$

${{\mathit \psi}{(2S)}}{{\mathit K}^{-}}{{\mathit \pi}^{+}}$

$(3.1\pm{0.4})\times 10^{-5}$

${{\mathit \psi}{(2S)}}{{\overline{\mathit K}}^{*}{(892)}^{0}}$

$(3.3\pm{0.5})\times 10^{-5}$

${{\mathit \chi}_{{c1}}}{{\mathit \phi}}$

$(1.97\pm{0.25})\times 10^{-4}$

${{\mathit \chi}_{{c1}}}{{\mathit K}^{+}}{{\mathit K}^{-}}$

${{\mathit \chi}_{{c2}}}{{\mathit K}^{+}}{{\mathit K}^{-}}$

${{\mathit \chi}_{{c1}}{(3872)}}{{\mathit \phi}}$

$(1.1\pm{0.4})\times 10^{-4}$

${{\mathit \chi}_{{c1}}{(3872)}}$( ${{\mathit K}^{+}}{{\mathit K}^{-}}$) $_{non-{{\mathit \phi}}}$

$(8.6\pm{3.5})\times 10^{-5}$

${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$

$(7.0\pm{1.0})\times 10^{-7}$

${{\mathit \pi}^{0}}{{\mathit \pi}^{0}}$

$<2.1\times 10^{-4}$

${{\mathit \eta}}{{\mathit \pi}^{0}}$

$<1.0\times 10^{-3}$

${{\mathit \eta}}{{\mathit \eta}}$

$<1.43\times 10^{-4}$

${{\mathit \rho}^{0}}{{\mathit \rho}^{0}}$

$<3.20\times 10^{-4}$

${{\mathit \eta}^{\,'}}{{\mathit K}_S^0}$

$<8.16\times 10^{-6}$

${{\mathit \eta}^{\,'}}{{\mathit \eta}}$

$<6.5\times 10^{-5}$

${{\mathit \eta}^{\,'}}{{\mathit \eta}^{\,'}}$

$(3.3\pm{0.7})\times 10^{-5}$

${{\mathit \eta}^{\,'}}{{\mathit \phi}}$

$<8.2\times 10^{-7}$

${{\mathit \phi}}{{\mathit f}_{{0}}{(980)}}$ , ${{\mathit f}_{{0}}{(980)}}$ $\rightarrow$ ${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$

$(1.12\pm{0.21})\times 10^{-6}$

${{\mathit \phi}}{{\mathit f}_{{2}}{(1270)}}$ , ${{\mathit f}_{{2}}{(1270)}}$ $\rightarrow$ ${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$

$(6.1^{+1.8}_{-1.5})\times 10^{-7}$

${{\mathit \phi}}{{\mathit \rho}^{0}}$

$(2.7\pm{0.8})\times 10^{-7}$

${{\mathit \phi}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$

$(3.5\pm{0.5})\times 10^{-6}$

${{\mathit \phi}}{{\mathit \phi}}$

$(1.85\pm{0.14})\times 10^{-5}$

${{\mathit \phi}}{{\mathit \phi}}{{\mathit \phi}}$

$(2.2\pm{0.6})\times 10^{-6}$

${{\mathit \pi}^{+}}{{\mathit K}^{-}}$

$(5.8\pm{0.7})\times 10^{-6}$

${{\mathit K}^{+}}{{\mathit K}^{-}}$

$(2.66\pm{0.22})\times 10^{-5}$

${{\mathit K}^{0}}{{\overline{\mathit K}}^{0}}$

$(1.76\pm{0.31})\times 10^{-5}$

${{\mathit K}^{0}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$

$(9.5\pm{2.1})\times 10^{-6}$

${{\mathit K}^{0}}{{\mathit K}^{\pm}}{{\mathit \pi}^{\mp}}$

$(8.4\pm{0.9})\times 10^{-5}$

${{\mathit K}^{*}{(892)}^{-}}{{\mathit \pi}^{+}}$

$(2.9\pm{1.1})\times 10^{-6}$

${{\mathit K}^{*}{(892)}^{\pm}}{{\mathit K}^{\mp}}$

$(1.9\pm{0.5})\times 10^{-5}$

${{\mathit K}_{{0}}^{*}{(1430)}^{\pm}}{{\mathit K}^{\mp}}$

$(3.1\pm{2.5})\times 10^{-5}$

${{\mathit K}_{{2}}^{*}{(1430)}^{\pm}}{{\mathit K}^{\mp}}$

$(1.0\pm{1.7})\times 10^{-5}$

${{\mathit K}^{*}{(892)}^{0}}{{\overline{\mathit K}}^{0}}$ + c.c.

$(2.0\pm{0.6})\times 10^{-5}$

${{\mathit K}_{{0}}^{*}{(1430)}}{{\overline{\mathit K}}^{0}}$ + c.c.

$(3.3\pm{1.0})\times 10^{-5}$

${{\mathit K}_{{2}}^{*}{(1430)}^{0}}{{\overline{\mathit K}}^{0}}$ + c.c.

$(1.7\pm{2.2})\times 10^{-5}$

${{\mathit K}_S^0}$ ${{\overline{\mathit K}}^{*}{(892)}^{0}}$ + c.c.

$(1.6\pm{0.4})\times 10^{-5}$

${{\mathit K}^{0}}{{\mathit K}^{+}}{{\mathit K}^{-}}$

$(1.3\pm{0.6})\times 10^{-6}$

${{\overline{\mathit K}}^{*}{(892)}^{0}}{{\mathit \rho}^{0}}$

$<7.67\times 10^{-4}$

${{\overline{\mathit K}}^{*}{(892)}^{0}}{{\mathit K}^{*}{(892)}^{0}}$

$(1.11\pm{0.27})\times 10^{-5}$

${{\mathit K}^{*}{(892)}^{0}}{{\overline{\mathit K}}_{{2}}^{*}{(1430)}^{0}}$

${{\mathit K}_{{2}}^{*}{(1430)}^{0}}{{\overline{\mathit K}}^{*}{(892)}^{0}}$

${{\mathit K}_{{2}}^{*}{(1430)}^{0}}{{\overline{\mathit K}}_{{2}}^{*}{(1430)}^{0}}$

${{\mathit \phi}}{{\mathit K}^{*}{(892)}^{0}}$

$(1.14\pm{0.30})\times 10^{-6}$

${{\mathit p}}{{\overline{\mathit p}}}$

$<1.5\times 10^{-8}$

${{\mathit p}}{{\overline{\mathit p}}}{{\mathit K}^{+}}{{\mathit K}^{-}}$

$(4.5\pm{0.5})\times 10^{-6}$

${{\mathit p}}{{\overline{\mathit p}}}{{\mathit K}^{+}}{{\mathit \pi}^{-}}$

$(1.39\pm{0.26})\times 10^{-6}$

${{\mathit p}}{{\overline{\mathit p}}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$

$(4.3\pm{2.0})\times 10^{-7}$

${{\mathit p}}{{\overline{\mathit \Lambda}}}{{\mathit K}^{-}}$ + c.c.

$(5.5\pm{1.0})\times 10^{-6}$

${{\mathit \Lambda}_{{c}}^{-}}{{\mathit \Lambda}}{{\mathit \pi}^{+}}$

$(3.6\pm{1.6})\times 10^{-4}$

${{\mathit \Lambda}_{{c}}^{-}}{{\mathit \Lambda}_{{c}}^{+}}$

$<8.0\times 10^{-5}$

▸	Lepton Family number ($\mathit LF$) violating modes or $\Delta \mathit B$ = 1 weak neutral current ($\mathit B1$) modes

FOOTNOTES

Constrained Fit information

Except where otherwise noted, content of the 2023 Review of Particle Physics is licensed under a Creative Commons Attribution-NonCommercial 4.0 International (CC BY-NC 4.0) license. The publication of the Review of Particle Physics is supported by US DOE, MEXT (Japan), INFN (Italy), JPS and CERN. Individual collaborators receive support for their PDG activities from their respective institutes or funding agencies. © 2023. See LBNL disclaimers.