BOTTOM BARYONS
($\mathit B$ = $-1$)
${{\mathit \Lambda}_{{{b}}}^{0}}$ = ${{\mathit u}}{{\mathit d}}{{\mathit b}}$, ${{\mathit \Sigma}_{{{b}}}^{0}}$ = ${{\mathit u}}{{\mathit d}}{{\mathit b}}$, ${{\mathit \Sigma}_{{{b}}}^{+}}$ = ${{\mathit u}}{{\mathit u}}{{\mathit b}}$, ${{\mathit \Sigma}_{{{b}}}^{-}}$ = ${{\mathit d}}{{\mathit d}}{{\mathit b}}$
${{\mathit \Xi}_{{{b}}}^{0}}$ = ${{\mathit u}}{{\mathit s}}{{\mathit b}}$, ${{\mathit \Xi}_{{{b}}}^{-}}$ = ${{\mathit d}}{{\mathit s}}{{\mathit b}}$, ${{\mathit \Omega}_{{{b}}}^{-}}$ = ${{\mathit s}}{{\mathit s}}{{\mathit b}}$ 		INSPIRE   JSON PDGID:
S070

${{\mathit \Xi}_{{{b}}}^{0}}$

$I(J^P)$ = $1/2(1/2^{+})$ I, J, P need confirmation.
In the quark model, ${{\mathit \Xi}_{{{b}}}^{0}}$ and ${{\mathit \Xi}_{{{b}}}^{-}}$ are an isodoublet ($\mathit usb$, $\mathit dsb$) state; the lowest ${{\mathit \Xi}_{{{b}}}^{0}}$ and ${{\mathit \Xi}_{{{b}}}^{-}}$ ought to have $\mathit J{}^{P} = 1/2{}^{+}$. None of $\mathit I$, $\mathit J$, or ${}^{P}$ have actually been measured.
Expand/Collapse All
▸  ${{\mathit \Xi}_{{{b}}}^{0}}$ MASS
▸  ${{\mathit \Xi}_{{{b}}}^{0}}$ MEAN LIFE
▸  $\mathit P$ AND $\mathit CP$ VIOLATION ASYMMETRIES
Mode  
Fraction ($\Gamma_i$ / $\Gamma$) Scale Factor/
Conf. Level		 P(MeV/c)  
$\Gamma_{1}$ ${{\mathit p}}{{\mathit D}^{0}}{{\mathit K}^{-}}$ ${\times }$ B(${{\mathit b}}$ $\rightarrow$ ${{\mathit \Xi}_{{{b}}}^{0}}$) ($1.7$ $\pm0.6$) $ \times 10^{-6}$ 2374
 
$\Gamma_{2}$ ${{\mathit p}}{{\overline{\mathit K}}^{0}}{{\mathit \pi}^{-}}$ ${\times }$ B(${{\mathit b}}$ $\rightarrow$ ${{\mathit \Xi}_{{{b}}}^{0}})/B({{\overline{\mathit b}}}$ $\rightarrow$ ${{\mathit B}^{0}}$ ) $<1.6$ $\times 10^{-6}$ CL=90% 2783
 
$\Gamma_{3}$ ${{\mathit p}}{{\mathit K}^{0}}{{\mathit K}^{-}}$ ${\times }$ B(${{\mathit b}}$ $\rightarrow$ ${{\mathit \Xi}_{{{b}}}^{0}})/B({{\overline{\mathit b}}}$ $\rightarrow$ ${{\mathit B}^{0}}$ ) $<1.1$ $\times 10^{-6}$ CL=90% 2730
 
$\Gamma_{4}$ ${{\mathit \Lambda}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$ ${\times }$ B(${{\mathit b}}$ $\rightarrow$ ${{\mathit \Xi}_{{{b}}}^{0}})/B({{\mathit b}}$ $\rightarrow$ ${{\mathit \Lambda}_{{{b}}}^{0}}$ ) $<1.7$ $\times 10^{-6}$ CL=90% 2781
 
$\Gamma_{5}$ ${{\mathit \Lambda}}{{\mathit K}^{-}}{{\mathit \pi}^{+}}$ ${\times }$ B(${{\mathit b}}$ $\rightarrow$ ${{\mathit \Xi}_{{{b}}}^{0}})/B({{\mathit b}}$ $\rightarrow$ ${{\mathit \Lambda}_{{{b}}}^{0}}$ ) $<8$ $\times 10^{-7}$ CL=90% 2751
 
$\Gamma_{6}$ ${{\mathit \Lambda}}{{\mathit K}^{+}}{{\mathit K}^{-}}$ ${\times }$ B(${{\mathit b}}$ $\rightarrow$ ${{\mathit \Xi}_{{{b}}}^{0}})/B({{\mathit b}}$ $\rightarrow$ ${{\mathit \Lambda}_{{{b}}}^{0}}$ ) $<3$ $\times 10^{-7}$ CL=90% 2698
 
$\Gamma_{7}$ ${{\mathit J / \psi}}{{\mathit \Lambda}}$ seen 1868
 
$\Gamma_{8}$ ${{\mathit J / \psi}}{{\mathit \Xi}^{0}}$ seen 1785
 
$\Gamma_{9}$ ${{\mathit \Xi}_{{{c}}}^{+}}{{\mathit D}_{{{s}}}^{-}}{\times }$ B(${{\mathit b}}$ $\rightarrow$ ${{\mathit \Xi}_{{{b}}}^{0}}$ )/B(${{\mathit b}}$ $\rightarrow$ ${{\mathit \Lambda}_{{{b}}}^{0}}$ ) ($1.7$ $\pm0.9$) $ \times 10^{-3}$  
 
$\Gamma_{10}$ ${{\mathit \Lambda}_{{{c}}}^{+}}{{\mathit K}^{-}}{\times }$ B(${{\mathit b}}$ $\rightarrow$ ${{\mathit \Xi}_{{{b}}}^{0}}$) ($6$ $\pm4$) $ \times 10^{-7}$ 2416
 
$\Gamma_{11}$ ${{\mathit p}}{{\mathit K}^{-}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$ ${\times }$ B(${{\mathit b}}$ $\rightarrow$ ${{\mathit \Xi}_{{{b}}}^{0}})/B({{\mathit b}}$ $\rightarrow$ ${{\mathit \Lambda}_{{{b}}}^{0}}$ ) ($1.9$ $\pm0.4$) $ \times 10^{-6}$ 2766
 
$\Gamma_{12}$ ${{\mathit p}}{{\mathit K}^{-}}{{\mathit K}^{-}}{{\mathit \pi}^{+}}$ ${\times }$ B(${{\mathit b}}$ $\rightarrow$ ${{\mathit \Xi}_{{{b}}}^{0}})/B({{\mathit b}}$ $\rightarrow$ ${{\mathit \Lambda}_{{{b}}}^{0}}$ ) ($1.73$ $\pm0.31$) $ \times 10^{-6}$ 2704
 
$\Gamma_{13}$ ${{\mathit p}}{{\mathit K}^{-}}{{\mathit K}^{+}}{{\mathit K}^{-}}$ ${\times }$ B(${{\mathit b}}$ $\rightarrow$ ${{\mathit \Xi}_{{{b}}}^{0}})/B({{\mathit b}}$ $\rightarrow$ ${{\mathit \Lambda}_{{{b}}}^{0}}$ ) ($1.8$ $\pm1.0$) $ \times 10^{-7}$ 2620