# ${{\boldsymbol \Upsilon}{(10860)}}$ MASS INSPIRE search

VALUE (MeV) DOCUMENT ID TECN  COMMENT
$\bf{ 10885.2 {}^{+2.6}_{-1.6}}$ OUR AVERAGE
$10885.3$ $\pm1.5$ ${}^{+2.2}_{-0.9}$ 1
 2019
BELL ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit \Upsilon}{(nS)}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$
$10884.7$ ${}^{+3.6}_{-3.4}$ ${}^{+8.9}_{-1.0}$ 2
 2016
BELL ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit h}_{{b}}{(1P,2P)}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$
• • • We do not use the following data for averages, fits, limits, etc. • • •
$10881.8$ ${}^{+1.0}_{-1.1}$ $\pm1.2$ 3, 4
 2016
BELL ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ hadrons
$10891.1$ $\pm3.2$ ${}^{+1.2}_{-2.0}$ 5, 6
 2016
BELL ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit \Upsilon}{(1S,2S,3S)}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$
$10879$ $\pm3$ 7, 8
 2010
BELL ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ hadrons
$10888.4$ ${}^{+2.7}_{-2.6}$ $\pm1.2$ 9
 2010
BELL ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit \Upsilon}{(1S,2S,3S)}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$
$10876$ $\pm2$ 7
 2009 E
BABR ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ hadrons
$10869$ $\pm2$ 10
 2009 E
BABR ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ hadrons
$10868$ $\pm6$ $\pm5$ 11
 1985
CLEO ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ hadrons
$10845$ $\pm20$ 12
 1985
CUSB ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ hadrons
1  From a simultaneous fit to the ${{\mathit \Upsilon}{(nS)}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$ , $\mathit n$ = 1, 2, 3, cross sections at 28 energy points within $\sqrt {s }$ = $10.6 - 11.05$ GeV, including the initial-state radiation at ${{\mathit \Upsilon}{(10860)}}$.
2  From a simultaneous fit to the ${{\mathit h}_{{b}}{(nP)}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$ , $\mathit n$ = 1, 2 cross sections at 22 energy points within $\sqrt {s }$ = $10.77 - 11.02$ GeV to a pair of interfering Breit-Wigner amplitudes modified by phase space factors, with eight resonance parameters (a mass and width for each of ${{\mathit \Upsilon}{(10860)}}$ and ${{\mathit \Upsilon}{(11020)}}$, a single relative phase, a single relative amplitude, and two overall normalization factors, one for each $\mathit n$). The systematic error estimate is dominated by possible interference with a small nonresonant continuum amplitude.
3  From a fit to the total hadronic cross sections measured at 60 energy points within $\sqrt {s }$ = $10.82 - 11.05$ GeV to a pair of interfering Breit-Wigner amplitudes and two floating continuum amplitudes with 1/$\sqrt {s }$ dependence, one coherent with the resonances and one incoherent, with six resonance parameters (a mass, width, and an amplitude for each of ${{\mathit \Upsilon}{(10860)}}$ and ${{\mathit \Upsilon}{(11020)}}$, one relative phase, and one decoherence coefficient).
4  Not including uncertain and potentially large systematic errors due to assumed continuum amplitude 1/$\sqrt {s }$ dependence and related interference contributions.
5  From a simultaneous fit to the ${{\mathit \Upsilon}{(nS)}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$ , $\mathit n$ = 1, 2, 3, cross sections at 25energy points within $\sqrt {s }$ = $10.6 - 11.05$ GeV to a pair of interfering Breit-Wigner amplitudesmodified by phase space factors, with fourteen resonance parameters (a mass, width, and threeamplitudes for each of ${{\mathit \Upsilon}{(10860)}}$ and ${{\mathit \Upsilon}{(11020)}}$, a single universal relativephase, and three decoherence coefficients, one for each $\mathit n$). Continuum contributions weremeasured (and therefore fixed) to be zero.
6  Superseded by MIZUK 2019 .
7  In a model where a flat non-resonant ${{\mathit b}}{{\overline{\mathit b}}}$ -continuum is incoherently added to a second flat component interfering with two Breit-Wigner resonances. Systematic uncertainties not estimated.
8  The parameters of the ${{\mathit \Upsilon}{(11020)}}$ are fixed to those in AUBERT 2009E.
9  In a model where a flat nonresonant ${{\mathit \Upsilon}{(1S,2S,3S)}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$ continuum interferes with a single Breit-Wigner resonance.
10  In a model where a non-resonant ${{\mathit b}}{{\overline{\mathit b}}}$ -continuum represented by a threshold function at $\sqrt {s }=2{\mathit m}_{{{\mathit B}}}$ is incoherently added to a flat component interfering with two Breit-Wigner resonances. Not independent of other AUBERT 2009E results. Systematic uncertainties not estimated.
11  Assuming four Gaussians with radiative tails and a single step in $\mathit R$.
12  In a coupled-channel model with three resonances and a smooth step in $\mathit R$.
References:
 MIZUK 2019
JHEP 1910 220 Observation of a new structure near 10.75 GeV in the energy dependence of the e$^{+}$e$^{?}$? ? (nS)?$^{+}$?$^{?}$ (n = 1, 2, 3) cross sections
 MIZUK 2016
PRL 117 142001 Energy Scan of the ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit h}_{{b}}}$( ${{\mathit n}}{{\mathit P}}$) ${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$ (n=1,2) Cross Sections and Evidence for ${{\mathit \Upsilon}{(11020)}}$ Decays into Charged Bottomonium-like States
 SANTEL 2016
PR D93 011101 Measurements of the ${{\mathit \Upsilon}{(10860)}}$ and ${{\mathit \Upsilon}{(11020)}}$ Resonances via $\sigma\mathrm {( {{\mathit e}^{+}} {{\mathit e}^{-}} \rightarrow {{\mathit \Upsilon}{(nS)}} {{\mathit \pi}^{+}} {{\mathit \pi}^{-}} )}$
 CHEN 2010
PR D82 091106 Observation of an Enhancement in ${{\mathit e}^{+}}{{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit \Upsilon}{(1S)}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$, ${{\mathit \Upsilon}{(2S)}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$, and ${{\mathit \Upsilon}{(3S)}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$ Production near $\sqrt {s }$ = 10.89 GeV
 AUBERT 2009E
PRL 102 012001 Measurement of the ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit b}}{{\overline{\mathit b}}}$ Cross Section between $\sqrt {s }$ = 10.54 and 11.20 GeV
 BESSON 1985
PRL 54 381 Observation of New Structure in the ${{\mathit e}^{+}}{{\mathit e}^{-}}$ Cross Section above the ${{\mathit \Upsilon}{(4S)}}$
 LOVELOCK 1985
PRL 54 377 Masses, Widths and Leptonic Widths of the Higher ${{\mathit \Upsilon}}$ Resonances