${{\mathit f}_{{{2}}}{(2300)}}$ MASS INSPIRE search

M107M
VALUE (MeV) DOCUMENT ID TECN  COMMENT
$2297$ $\pm28$ 1
ETKIN
1988
MPS 22 ${{\mathit \pi}^{-}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit \phi}}{{\mathit \phi}}{{\mathit n}}$
• • • We do not use the following data for averages, fits, limits, etc. • • •
$2262$ $\pm4$ $\pm28$ 2
ABLIKIM
2021AI
 BES3 $3.51 - 4.60$ ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit \phi}}{{\mathit \Lambda}}{{\overline{\mathit \Lambda}}}$
$2243$ ${}^{+7}_{-6}$ ${}^{+3}_{-29}$ 3
UEHARA
2013
BELL ${{\mathit \gamma}}$ ${{\mathit \gamma}}$ $\rightarrow$ ${{\mathit K}_S^0}$ ${{\mathit K}_S^0}$
$2270$ $\pm12$
VLADIMIRSKY
2006
SPEC 40 ${{\mathit \pi}^{-}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit K}_S^0}$ ${{\mathit K}_S^0}$ ${{\mathit n}}$
$2327$ $\pm9$ $\pm6$
ABE
2004
BELL 10.6 ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit e}^{+}}{{\mathit e}^{-}}{{\mathit K}^{+}}{{\mathit K}^{-}}$
$2340$ $\pm13$ 4
LONGACRE
2004
RVUE 22 ${{\mathit \pi}^{-}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit \phi}}{{\mathit \phi}}{{\mathit n}}$, 450 ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit p}_{{{f}}}}$4 ${{\mathit \pi}}{{\mathit p}_{{{s}}}}$
$2231$ $\pm10$
BOOTH
1986
OMEG 85 ${{\mathit \pi}^{-}}$ ${}^{}\mathrm {Be}$ $\rightarrow$ 2 ${{\mathit \phi}}{}^{}\mathrm {Be}$
$2220$ ${}^{+90}_{-20}$
LINDENBAUM
1984
RVUE
$2320$ $\pm40$
ETKIN
1982
MPS 22 ${{\mathit \pi}^{-}}$ ${{\mathit p}}$ $\rightarrow$ 2 ${{\mathit \phi}}{{\mathit n}}$
1  Includes data of ETKIN 1985. The percentage of the resonance going into ${{\mathit \phi}}{{\mathit \phi}}{}^{}2{}^{++}$ $\mathit S_{2}$, $\mathit D_{2}$, and $\mathit D_{0}$ is $6$ ${}^{+15}_{-5}$, $25$ ${}^{+18}_{-14}$, and $69$ ${}^{+16}_{-27}$, respectively.
2  Threshold enhancement in ${{\mathit \Lambda}}{{\overline{\mathit \Lambda}}}$, preferred $\mathit J{}^{PC}$ are ${}^{}2{}^{++}$, ${}^{}2{}^{-+}$, or ${}^{}1{}^{++}$. Could be another state.
3  Spin 2 preferred, tentatively assigned to $f_2(2300)$.
4  From a four pole K-matrix reanalysis of ETKIN 1988 and BARBERIS 2000C data.
  References:
ABLIKIM 2021AI
PR D104 052006 Observation of a near-threshold enhancement in the $\Lambda\bar{\Lambda}$ mass spectrum from $e^+e^-\to\phi\Lambda\bar{\Lambda}$ at $\sqrt{s}$ from 3.51 to 4.60 GeV
UEHARA 2013
PTEP 2013 123C01 High-Statistics Study of ${{\mathit K}_S^0}$ Pair Production in Two-Photon Collisions
VLADIMIRSKY 2006
PAN 69 493 Analysis of the ${{\mathit K}_S^0}$ ${{\mathit K}_S^0}$ System from the Reaction ${{\mathit \pi}^{-}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit K}_S^0}$ ${{\mathit K}_S^0}$ ${{\mathit n}}$ at 40 GeV
ABE 2004
EPJ C32 323 Measurement of ${{\mathit K}^{+}}{{\mathit K}^{-}}$ Production in Two Photon Collisions in the Resonant Mass Region
LONGACRE 2004
PR D70 094041 Evidence for a Fourth State Related to the three $\mathit J{}^{PC} = 2{}^{++}$, ${{\mathit \pi}^{-}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit \phi}}{{\mathit \phi}}{{\mathit n}}$ States Explainable by 2${}^{++}$ Gluebal Production
ETKIN 1988
PL B201 568 Increased Statistics and Observation of $\mathit g_{{{\mathit T}}}$, $\mathit g_{{{\mathit T}^{\,'}}}$ and $\mathit g_{{{\mathit T}^{"}}}$ $2+{}^{+}{}^{}$ Resonances in Glueball Enhanced Channel ${{\mathit \pi}^{-}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit \phi}}{{\mathit \phi}}{{\mathit n}}$
BOOTH 1986
NP B273 677 A High Statistics Study of the ${{\mathit \phi}}{{\mathit \phi}}$ Mass Spectrum
LINDENBAUM 1984
CNPP 13 285 Production of Glueballs
ETKIN 1982
PRL 49 1620 Reaction ${{\mathit \pi}^{-}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit \phi}}{{\mathit \phi}}{{\mathit n}}$ and Evidence for Glueballs
Also
Brighton Conf. 351 Hadronic Production of Glueballs