in ${{\mathit \Lambda}_{{{b}}}^{0}}$ $\rightarrow$ ${{\mathit D}^{0}}{{\mathit p}}{{\mathit \pi}^{-}}$
$2939.8$ $\pm1.3$ $\pm1.0$
2.2k
AUBERT
2007
BABR
in ${{\mathit p}}{{\mathit D}^{0}}$
$2938.0$ $\pm1.3$ ${}^{+2.0}_{-4.0}$
220
MIZUK
2007
BELL
in ${{\mathit \Sigma}_{{{c}}}{(2455)}^{0}}{}^{,++}$ ${{\mathit \pi}^{\pm}}$
1
The third AAIJ 2017S uncertainty comes from modeling the resonant shape of the nearby ${{\mathit \Lambda}_{{{c}}}{(2880)}^{+}}$ and the background (non-resonant) amplitudes.
References:
AAIJ
2017S
JHEP 1705 030
Study of the ${{\mathit D}^{0}}{{\mathit p}}$ Amplitude in ${{\mathit \Lambda}_{{{b}}}^{0}}$ $\rightarrow$ ${{\mathit D}^{0}}{{\mathit p}}{{\mathit \pi}^{-}}$ Decays
AUBERT
2007
PRL 98 012001
Observation of a Charmed Baryon Decaying to ${{\mathit D}^{0}}{{\mathit p}}$ at a Mass Near 2.94 GeV/$\mathit c{}^{2}$
MIZUK
2007
PRL 98 262001
Experimental Constraints on the Spin and Parity of the ${{\mathit \Lambda}_{{{c}}}{(2880)}^{+}}$
