$\bf{
1815 \pm12}$
|
OUR AVERAGE
Error includes scale factor of 1.4.
|
$1822$ ${}^{+29}_{-24}$ ${}^{+66}_{-57}$ |
5.5k |
1 |
|
BES3 |
$1737$ $\pm9$ ${}^{+198}_{-65}$ |
|
2 |
|
BELL |
$1800$ $\pm30$ |
40 |
|
|
GAM4 |
$1806$ $\pm10$ |
1600 |
|
|
GAM4 |
$1870$ $\pm40$ |
|
3 |
|
GAM4 |
$1857$ ${}^{+35}_{-24}$ |
|
4 |
|
OMEG |
• • • We do not use the following data for averages, fits, limits, etc. • • • |
$1858$ ${}^{+18}_{-71}$ |
|
5 |
|
RVUE |
$1799$ $\pm15$ |
|
6 |
|
STRC |
1
From partial wave analysis including all possible combinations of 0${}^{++}$, 2${}^{++}$, and 4${}^{++}$ resonances.
|
2
Breit-Wigner mass. Could also be the ${{\mathit f}_{{2}}{(1910)}}$.
|
3
Seen in only one solution.
|
4
Error increased by spread of two solutions. Included in LONGACRE 1986 global analysis.
|
5
From a partial-wave analysis of data using a K-matrix formalism with 5 poles. Includes compilation of several other experiments.
|
6
From an amplitude analysis of the reaction ${{\mathit \pi}^{+}}$ ${{\mathit \pi}^{-}}$ $\rightarrow$ 2 ${{\mathit \pi}^{0}}$ . The resonance in the 2${{\mathit \pi}^{0}}$ final state is not confirmed by PROKOSHKIN 1997 .
|