${{\mathit \rho}{(1700)}}$ MASS

${{\mathit K}}{{\overline{\mathit K}}}$ MODE

INSPIRE   PDGID:
M065M2
VALUE (MeV) EVTS DOCUMENT ID TECN CHG  COMMENT
• • We do not use the following data for averages, fits, limits, etc. • •
$1688.7$ $\pm3.1$ ${}^{+141.1}_{-1.3}$ 1
ALBRECHT
2020
RVUE 0.9 ${{\overline{\mathit p}}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit K}^{+}}{{\mathit K}^{-}}{{\mathit \pi}^{0}}$
$1541$ $\pm12$ $\pm33$ 190k 2
AAIJ
2016N
 LHCB ${{\mathit D}^{0}}$ $\rightarrow$ ${{\mathit K}_S^0}$ ${{\mathit K}^{\pm}}{{\mathit \pi}^{\mp}}$
$1740.8$ $\pm22.2$ 27k 3
ABELE
1999D
 CBAR $\pm{}$ 0.0 ${{\overline{\mathit p}}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit K}^{+}}{{\mathit K}^{-}}{{\mathit \pi}^{0}}$
$1582$ $\pm36$ 1600
CLELAND
1982B
 SPEC $\pm{}$ 50 ${{\mathit \pi}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit K}_S^0}$ ${{\mathit K}^{\pm}}{{\mathit p}}$
1  T-matrix pole, 2 poles, 3 channels, including ${{\mathit \pi}}{{\mathit \pi}}$ scattering data from HYAMS 1975 .
2  Using the GOUNARIS 1968 parameterization with a fixed width. Value is average using different ${{\mathit K}}{{\mathit \pi}}$ ${\mathit S}{\mathrm -wave}$ parametrizations in fit.
3  K-matrix pole. Isospin not determined, could be ${{\mathit \omega}{(1650)}}$ or ${{\mathit \phi}{(1680)}}$.
References:
ALBRECHT 2020
EPJ C80 453 Coupled channel analysis of ${\bar{p}p}\,\rightarrow \,\pi ^0\pi ^0\eta $, ${\pi ^0\eta \eta }$ and ${K^+K^-\pi ^0}$ at 900 MeV/c and of ${\pi \pi }$-scattering data
AAIJ 2016N
PR D93 052018 Studies of the Resonance Structure in ${{\mathit D}^{0}}$ $\rightarrow$ ${{\mathit K}_S^0}$ ${{\mathit K}^{\pm}}{{\mathit \pi}^{\mp}}$ Decays
ABELE 1999D
PL B468 178 Antiproton Proton Annihilation at Rest into ${{\mathit K}_L^0}{{\mathit K}^{+}}{{\mathit K}^{-}}{{\mathit \pi}^{0}}$
CLELAND 1982B
NP B208 228 Resonance Production in the Reaction ${{\mathit \pi}^{\pm}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit K}_S^0}$ ${{\mathit K}^{\pm}}{{\mathit p}}$ at 30 and 50 ${\mathrm {GeV/}}\mathit c$