${{\mathit h}_{{{c}}}{(1P)}}$ MASS INSPIRE search

M144M
VALUE (MeV) EVTS DOCUMENT ID TECN  COMMENT
$\bf{ 3525.37 \pm0.14}$ OUR AVERAGE  Error includes scale factor of 1.2.
$3525.32$ $\pm0.06$ $\pm0.15$ 23k
ABLIKIM
2022AQ
 BES3 ${{\mathit \psi}{(2S)}}$ $\rightarrow$ ${{\mathit \pi}^{0}}$ hadrons; ${{\mathit \pi}^{0}}{{\mathit \gamma}}$( ${{\mathit \eta}_{{{c}}}}$)
$3525.20$ $\pm0.18$ $\pm0.12$ 1282 1
DOBBS
2008A
 CLEO ${{\mathit \psi}{(2S)}}$ $\rightarrow$ ${{\mathit \pi}^{0}}{{\mathit \eta}_{{{c}}}}{{\mathit \gamma}}$
$3525.8$ $\pm0.2$ $\pm0.2$ 13
ANDREOTTI
2005B
 E835 ${{\overline{\mathit p}}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit \eta}_{{{c}}}}{{\mathit \gamma}}$
• • • We do not use the following data for averages, fits, limits, etc. • • •
$3525.31$ $\pm0.11$ $\pm0.14$ 832 2, 3
ABLIKIM
2012N
 BES3 ${{\mathit \psi}{(2S)}}$ $\rightarrow$ ${{\mathit \pi}^{0}}{{\mathit \gamma}}$ hadrons
$3525.40$ $\pm0.13$ $\pm0.18$ 3679 2
ABLIKIM
2010B
 BES3 ${{\mathit \psi}{(2S)}}$ $\rightarrow$ ${{\mathit \pi}^{0}}{{\mathit \gamma}}{{\mathit \eta}_{{{c}}}}$
$3525.6$ $\pm0.5$ 92
ADAMS
2009
CLEO ${{\mathit \psi}{(2S)}}$ $\rightarrow$ 2 ( ${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}{{\mathit \pi}^{0}}$)
$3524.4$ $\pm0.6$ $\pm0.4$ 168 4
ROSNER
2005
CLEO ${{\mathit \psi}{(2S)}}$ $\rightarrow$ ${{\mathit \pi}^{0}}{{\mathit \eta}_{{{c}}}}{{\mathit \gamma}}$
$3527$ $\pm8$ 42
ANTONIAZZI
1994
E705 300 ${{\mathit \pi}^{\pm}}$, ${{\mathit p}}$ ${}^{}\mathrm {Li}$ $\rightarrow$ ${{\mathit J / \psi}}{{\mathit \pi}^{0}}$ X
$3526.28$ $\pm0.18$ $\pm0.19$ 59 5
ARMSTRONG
1992D
 E760 ${{\overline{\mathit p}}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit J / \psi}}{{\mathit \pi}^{0}}$
$3525.4$ $\pm0.8$ $\pm0.4$ 5
BAGLIN
1986
SPEC ${{\overline{\mathit p}}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit J / \psi}}$ X
1  Combination of exclusive and inclusive analyses for the reaction ${{\mathit \psi}{(2S)}}$ $\rightarrow$ ${{\mathit \pi}^{0}}{{\mathit h}_{{{c}}}}$ $\rightarrow$ ${{\mathit \pi}^{0}}{{\mathit \eta}_{{{c}}}}{{\mathit \gamma}}$. This result is the average of DOBBS 2008A and ROSNER 2005.
2  Superseded by ABLIKIM 2022AQ
3  With floating width.
4  Superseded by DOBBS 2008A.
5  Mass central value and systematic error recalculated by us according to Eq.$~$(16) in ARMSTRONG 1993B, using the value for the ${{\mathit \psi}{(2S)}}$ mass from AULCHENKO 2003.
  References:
ABLIKIM 2022AQ
PR D106 072007 Study of the $h_c$($1^1P_1$) meson via $\psi(2S) \rightarrow \pi^0 h_c$ decays at BESIII
ABLIKIM 2012N
PR D86 092009 Study of ${{\mathit \psi}{(3686)}}$ $\rightarrow$ ${{\mathit \pi}^{0}}{{\mathit h}_{{{c}}}}$, ${{\mathit h}_{{{c}}}}$ $\rightarrow$ ${{\mathit \gamma}}{{\mathit \eta}_{{{c}}}}$ via ${{\mathit \eta}_{{{c}}}}$ Exclusive Decays
ABLIKIM 2010B
PRL 104 132002 Measurements of ${{\mathit h}_{{{c}}}}({}^{1}\!{\mathit P}_{1}$) in ${{\mathit \psi}^{\,'}}$ Decays
ADAMS 2009
PR D80 051106 Evidence for Decays of ${{\mathit h}_{{{c}}}}$ to Multipion Final States
DOBBS 2008A
PRL 101 182003 Precision Measurement of the Mass of the ${{\mathit h}_{{{c}}}}({}^{1}\mathit P_{1}$) State of Charmonium
ANDREOTTI 2005B
PR D72 032001 Results of a Search for the ${{\mathit h}_{{{c}}}}({}^{1}{{\mathit P}_{{{1}}}}$) State of Charmonium in the ${{\mathit \eta}_{{{c}}}}{{\mathit \gamma}}$ and ${{\mathit J / \psi}}{{\mathit \pi}^{0}}$ Decay Modes
ROSNER 2005
PRL 95 102003 Observation of the ${{\mathit h}_{{{c}}}}({}^{1}P_{1}$) State of Charmonium
ANTONIAZZI 1994
PR D50 4258 Search for Hidden Charm Resonance States Decaying into ${{\mathit J / \psi}}$ or ${{\mathit \psi}^{\,'}}$ Plus Pions
ARMSTRONG 1992D
PRL 69 2337 Observation of the ${}^{1}\mathit P_{1}$ State of Charmonium
BAGLIN 1986
PL B171 135 Search for the ${}^{1}P_{1}$ Charmonium State in ${{\overline{\mathit p}}}{{\mathit p}}$ Annihilations at the CERN Intersecting Storage Rings