${{\mathit \chi}_{{{c1}}}{(1P)}}$ MASS

INSPIRE   PDGID:
M055M
VALUE (MeV) EVTS DOCUMENT ID TECN  COMMENT
$\bf{ 3510.67 \pm0.05}$ OUR AVERAGE  Error includes scale factor of 1.2.
$3509.84$ $\pm0.69$ $\pm0.64$ 2.8k
AAIJ
2023AH
LHCB ${{\mathit B}^{+}}$ $\rightarrow$ ${{\mathit K}^{+}}$( ${{\mathit K}_S^0}$ ${{\mathit K}}{{\mathit \pi}}$)
$3508.4$ $\pm1.9$ $\pm0.7$ 460 1
AAIJ
2017BB
LHCB ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}{{\mathit X}}$ $\rightarrow$ 2( ${{\mathit K}^{+}}{{\mathit K}^{-}}$) ${{\mathit X}}$
$3510.71$ $\pm0.04$ $\pm0.09$ 4.8k 2
AAIJ
2017BI
LHCB ${{\mathit \chi}_{{{c1}}}}$ $\rightarrow$ ${{\mathit J / \psi}}{{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$
$3510.30$ $\pm0.14$ $\pm0.16$
ABLIKIM
2005G
BES2 ${{\mathit \psi}{(2S)}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \chi}_{{{c1}}}}$
$3510.719$ $\pm0.051$ $\pm0.019$
ANDREOTTI
2005A
E835 ${{\mathit p}}$ ${{\overline{\mathit p}}}$ $\rightarrow$ ${{\mathit e}^{+}}{{\mathit e}^{-}}{{\mathit \gamma}}$
$3509.4$ $\pm0.9$
BAI
1999B
BES ${{\mathit \psi}{(2S)}}$ $\rightarrow$ ${{\mathit \gamma}}$ X
$3510.60$ $\pm0.087$ $\pm0.019$ 513 3
ARMSTRONG
1992
E760 ${{\overline{\mathit p}}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit e}^{+}}{{\mathit e}^{-}}{{\mathit \gamma}}$
$3511.3$ $\pm0.4$ $\pm0.4$ 30
BAGLIN
1986B
SPEC ${{\overline{\mathit p}}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit e}^{+}}{{\mathit e}^{-}}$ X
$3512.3$ $\pm0.3$ $\pm4.0$ 4
GAISER
1986
CBAL ${{\mathit \psi}{(2S)}}$ $\rightarrow$ ${{\mathit \gamma}}$ X
$3507.4$ $\pm1.7$ 91 5
LEMOIGNE
1982
GOLI 185 ${{\mathit \pi}^{-}}$ ${}^{}\mathrm {Be}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \mu}^{+}}{{\mathit \mu}^{-}}{}^{}\mathrm {A}$
$3510.4$ $\pm0.6$
OREGLIA
1982
CBAL ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit J / \psi}}$2 ${{\mathit \gamma}}$
$3510.1$ $\pm1.1$ 254 6
HIMEL
1980
MRK2 ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit J / \psi}}$2 ${{\mathit \gamma}}$
$3509$ $\pm11$ 21
BRANDELIK
1979B
DASP ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit J / \psi}}$2 ${{\mathit \gamma}}$
$3507$ $\pm3$ 6
BARTEL
1978B
CNTR ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit J / \psi}}$2 ${{\mathit \gamma}}$
$3505.0$ $\pm4$ $\pm4$ 6, 7
TANENBAUM
1978
MRK1 ${{\mathit e}^{+}}{{\mathit e}^{-}}$
$3513$ $\pm7$ 367 6
BIDDICK
1977
CNTR ${{\mathit \psi}{(2S)}}$ $\rightarrow$ ${{\mathit \gamma}}$ X
• • We do not use the following data for averages, fits, limits, etc. • •
$3500$ $\pm10$ 40
TANENBAUM
1975
MRK1 Hadrons ${{\mathit \gamma}}$
1  From a fit of the ${{\mathit \phi}}{{\mathit \phi}}$ invariant mass with the width of ${{\mathit \chi}_{{{c1}}}{(1P)}}$ fixed to the PDG 2016 value.
2  AAIJ 2017BI reports also m(${{\mathit \chi}_{{{c2}}}}$) $−$ m(${{\mathit \chi}_{{{c1}}}}$) = $45.39$ $\pm0.07$ $\pm0.03$ MeV.
3  Recalculated by ANDREOTTI 2005A, using the value of ${{\mathit \psi}{(2S)}}$ mass from AULCHENKO 2003.
4  Using mass of ${{\mathit \psi}{(2S)}}$ = 3686.0 MeV.
5  ${{\mathit J / \psi}{(1S)}}$ mass constrained to 3097 MeV.
6  Mass value shifted by us by amount appropriate for ${{\mathit \psi}{(2S)}}$ mass = 3686 MeV and ${{\mathit J / \psi}{(1S)}}$ mass = 3097 MeV.
7  From a simultaneous fit to radiative and hadronic decay channels.
References