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BOTTOM, STRANGE MESONS
($\boldsymbol B$ = $\pm1$, $\boldsymbol S$ = $\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

${{\boldsymbol B}_{{s}}^{0}}$ $I(J^P)$ = $0(0^{-})$

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

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

$5366.88 \pm0.14$ MeV

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

$87.38 \pm0.16$ MeV

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

$(66.00 \pm0.16) \times 10^{10}$ s${}^{-1}$

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

$0.129 \pm0.006$

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

$(1.620 \pm0.007) \times 10^{-12}$ s

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

$(1.423 \pm0.005) \times 10^{-12}$ s

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

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

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

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

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

▸	$\boldsymbol CPT$ VIOLATION PARAMETERS

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

PRODUCTION ASYMMETRIES

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

$0.012 \pm0.016$

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

$(93\pm{25})\%$

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

$(3.00\pm{0.23})\times 10^{-3}$

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

$(6.9\pm{1.4})\times 10^{-3}$

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

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

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

$(2.5\pm{0.8})\times 10^{-5}$

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

$(2.27\pm{0.19})\times 10^{-4}$

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

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

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

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

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

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

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

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

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

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

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

$(2.0\pm{0.5})\times 10^{-3}$

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

$(1.33\pm{0.35})\times 10^{-4}$

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

$(9.6\pm{2.1})\times 10^{-3}$

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

$(5.5\pm{0.8})\times 10^{-5}$

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

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

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

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

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

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

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

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

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

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

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

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

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

$(1.08\pm{0.08})\times 10^{-3}$

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

$(1.24^{+0.17}_{-0.19})\times 10^{-5}$

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

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

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

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

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

$(1.88\pm{0.15})\times 10^{-5}$

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

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

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

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

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

$(2.09\pm{0.23})\times 10^{-4}$

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

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

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

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

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

$(1.28\pm{0.18})\times 10^{-4}$

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

$(1.1\pm{0.4})\times 10^{-6}$

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

$(7.5\pm{1.8})\times 10^{-7}$

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

$(1.09\pm{0.34})\times 10^{-6}$

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

$(1.3\pm{0.8})\times 10^{-6}$

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

$(4.5^{+0.7}_{-4.0})\times 10^{-5}$

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

$(2.11^{+0.40}_{-0.29})\times 10^{-5}$

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

$(1.07\pm{0.24})\times 10^{-6}$

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

$(1.3^{+2.7}_{-0.9})\times 10^{-7}$

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

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

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

$(5.0^{+11.0}_{-1.1})\times 10^{-6}$

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

$(1.8^{+1.1}_{-0.4})\times 10^{-5}$

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

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

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

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

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

$(9.2\pm{1.3})\times 10^{-4}$

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

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

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

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

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

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

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

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

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

$(7.8\pm{1.0})\times 10^{-5}$

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

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

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

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

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

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

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

$(7.1\pm{1.3})\times 10^{-5}$

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

$(5.4\pm{0.6})\times 10^{-4}$

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

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

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

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

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

$(2.04\pm{0.30})\times 10^{-4}$

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

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

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

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

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

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

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

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

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

$<1.5\times 10^{-3}$

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

$(1.87\pm{0.15})\times 10^{-5}$

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

$(2.2\pm{0.7})\times 10^{-6}$

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

constrained fit information