${{\mathit \rho}_{{{3}}}{(2250)}}$ MASS

${{\overline{\mathit p}}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit \pi}}{{\mathit \pi}}$ or ${{\mathit K}}{{\overline{\mathit K}}}$

INSPIRE   PDGID:
M044M1
VALUE (MeV) EVTS DOCUMENT ID TECN CHG  COMMENT
• • We do not use the following data for averages, fits, limits, etc. • •
$2248$ $\pm17$ ${}^{+59}_{-5}$ 1.8k 1
ABLIKIM
2020F
BES3 ${{\mathit \psi}{(2S)}}$ $\rightarrow$ ${{\mathit K}^{+}}{{\mathit K}^{-}}{{\mathit \eta}}$
$\sim$$2232$
HASAN
1994
RVUE ${{\overline{\mathit p}}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit \pi}}{{\mathit \pi}}$
$\sim$$2090$ 2
OAKDEN
1994
RVUE $0.36 - 1.55$ ${{\overline{\mathit p}}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit \pi}}{{\mathit \pi}}$
$\sim$$2250$ 3
MARTIN
1980B
RVUE
$\sim$$2300$ 3
MARTIN
1980C
RVUE
$\sim$$2140$ 4
CARTER
1978B
CNTR 0 0.7$-$2.4 ${{\overline{\mathit p}}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit K}^{-}}{{\mathit K}^{+}}$
$\sim$$2150$ 5
CARTER
1977
CNTR 0 0.7$-$2.4 ${{\overline{\mathit p}}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit \pi}}{{\mathit \pi}}$
1  Seen in ${{\mathit \psi}{(2S)}}$ decay with branching ratio ${{\mathit \psi}{(2S)}}$ $\rightarrow$ ${{\mathit X}}{{\mathit \eta}}$ $\rightarrow$ ${{\mathit K}^{+}}{{\mathit K}^{-}}{{\mathit \eta}}$ = ($1.9$ $\pm0.4$ ${}^{+0.5}_{-1.3}$) $ \times 10^{-6}$.
2  See however KLOET 1996 who fit ${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$ only and find waves only up to $\mathit J = 3$ to be important but not significantly resonant.
3  $\mathit I(\mathit J{}^{P}) = 1(3{}^{-})$ from simultaneous analysis of ${{\mathit p}}$ ${{\overline{\mathit p}}}$ $\rightarrow$ ${{\mathit \pi}^{-}}{{\mathit \pi}^{+}}$ and ${{\mathit \pi}^{0}}{{\mathit \pi}^{0}}$.
4  $\mathit I = 0$, $1{}^{}{}^{}$. $\mathit J{}^{P} = 3{}^{-}$ from Barrelet-zero analysis.
5  $\mathit I(\mathit J{}^{P}) = 1(3{}^{-})$ from amplitude analysis.
References