herwig
is hosted by
Hepforge
,
IPPP Durham
Comparisions of Herwig7 and Hadronic Decay Data
Meson
Light, Unflavoured
π
0
Mode:
π
0
→
γ
e
+
e
−
Monte Carlo
⚓
⌘
MC_Meson_Meson_Leptons_Decay/h2_111p_22p_11_mVf
⚓
⌘
MC_Meson_Meson_Leptons_Decay/h2_111p_22p_11_mVfbar
⚓
⌘
MC_Meson_Meson_Leptons_Decay/h2_111p_22p_11_mff
η
Mode:
η
→
π
+
π
−
π
0
Data
⚓
⌘
KLOE2_2016_I1416990/d01-x01-y01
⚓
⌘
KLOE2_2016_I1416990/d01-x01-y01_EE
⚓
⌘
KLOE2_2016_I1416990/d02-x01-y01
⚓
⌘
KLOE2_2016_I1416990/d02-x01-y02
⚓
⌘
KLOE2_2016_I1416990/d02-x01-y03
⚓
⌘
KLOE2_2016_I1416990/d02-x01-y04
⚓
⌘
KLOE2_2016_I1416990/d02-x01-y05
⚓
⌘
KLOE2_2016_I1416990/d02-x01-y06
⚓
⌘
KLOE2_2016_I1416990/d02-x01-y07
⚓
⌘
KLOE2_2016_I1416990/d02-x01-y08
⚓
⌘
KLOE2_2016_I1416990/d02-x01-y09
⚓
⌘
KLOE2_2016_I1416990/d02-x01-y10
⚓
⌘
KLOE2_2016_I1416990/d02-x01-y11
⚓
⌘
KLOE2_2016_I1416990/d02-x01-y12
⚓
⌘
KLOE2_2016_I1416990/d02-x01-y13
⚓
⌘
KLOE2_2016_I1416990/d02-x01-y14
⚓
⌘
KLOE2_2016_I1416990/d02-x01-y15
⚓
⌘
KLOE2_2016_I1416990/d02-x01-y16
⚓
⌘
KLOE2_2016_I1416990/d02-x01-y17
Monte Carlo
⚓
⌘
MC_Eta_Decay/dpi0pim_0
⚓
⌘
MC_Eta_Decay/dpi0pip_0
⚓
⌘
MC_Eta_Decay/dpippim_0
Mode:
η
→
γ
e
+
e
−
Data
⚓
⌘
A2_2017_I1486671/d01-x01-y01
Monte Carlo
⚓
⌘
MC_Meson_Meson_Leptons_Decay/h2_221p_22p_11_mVf
⚓
⌘
MC_Meson_Meson_Leptons_Decay/h2_221p_22p_11_mVfbar
⚓
⌘
MC_Meson_Meson_Leptons_Decay/h2_221p_22p_11_mff
Mode:
η
→
π
0
π
0
π
0
Monte Carlo
⚓
⌘
MC_Eta_Decay/dpi0pi0_0
Mode:
η
→
γ
π
+
π
−
Monte Carlo
⚓
⌘
MC_Eta_Decay/mpimgamma_0
⚓
⌘
MC_Eta_Decay/mpipgamma_0
⚓
⌘
MC_Eta_Decay/mpippim_0
⚓
⌘
MC_Eta_Decay/photonenergy_0
Mode:
η
→
γ
γ
π
0
Monte Carlo
⚓
⌘
MC_Eta_Decay/mgammagamma_0
⚓
⌘
MC_Eta_Decay/mpi0gamma_0
η
′
Mode:
η
′
→
γ
μ
+
μ
−
Monte Carlo
⚓
⌘
MC_Meson_Meson_Leptons_Decay/h2_331p_22p_13_mVf
⚓
⌘
MC_Meson_Meson_Leptons_Decay/h2_331p_22p_13_mVfbar
⚓
⌘
MC_Meson_Meson_Leptons_Decay/h2_331p_22p_13_mff
Mode:
η
′
→
η
π
0
π
0
Monte Carlo
⚓
⌘
MC_Eta_Decay/dpi0eta
⚓
⌘
MC_Eta_Decay/dpi0pi0_2
Mode:
η
′
→
γ
e
+
e
−
Data
⚓
⌘
BESIII_2015_I1364494/d01-x01-y03
Monte Carlo
Mode:
η
′
→
η
π
+
π
−
Monte Carlo
⚓
⌘
MC_Eta_Decay/dpimeta
⚓
⌘
MC_Eta_Decay/dpipeta
⚓
⌘
MC_Eta_Decay/dpippim_2
Mode:
η
′
→
π
0
π
0
π
0
Monte Carlo
⚓
⌘
MC_Eta_Decay/dpi0pi0_1
Mode:
η
′
→
π
+
π
−
π
0
Monte Carlo
⚓
⌘
MC_Eta_Decay/dpi0pim_1
⚓
⌘
MC_Eta_Decay/dpi0pip_1
⚓
⌘
MC_Eta_Decay/dpippim_1
Mode:
η
′
→
γ
π
+
π
−
Data
⚓
⌘
BESIII_2018_I1641075/d01-x01-y05
Monte Carlo
⚓
⌘
MC_Eta_Decay/mpimgamma_1
⚓
⌘
MC_Eta_Decay/mpipgamma_1
⚓
⌘
MC_Eta_Decay/mpippim_1
⚓
⌘
MC_Eta_Decay/photonenergy_1
Mode:
η
′
→
γ
γ
π
0
Monte Carlo
⚓
⌘
MC_Eta_Decay/mgammagamma_1
⚓
⌘
MC_Eta_Decay/mpi0gamma_1
ω
Mode:
ω
→
π
+
π
−
π
0
Monte Carlo
⚓
⌘
MC_OmegaPhia1_3Pion_Decay/dalitz_1_EE
⚓
⌘
MC_OmegaPhia1_3Pion_Decay/m0_1
⚓
⌘
MC_OmegaPhia1_3Pion_Decay/mminus_1
⚓
⌘
MC_OmegaPhia1_3Pion_Decay/mplus_1
⚓
⌘
MC_OmegaPhia1_3Pion_Decay/xhist_1
⚓
⌘
MC_OmegaPhia1_3Pion_Decay/yhist_1
Mode:
ω
→
e
+
e
−
π
0
Data
⚓
⌘
A2_2017_I1486671/d02-x01-y01
Monte Carlo
⚓
⌘
MC_Meson_Meson_Leptons_Decay/h_223p_111p_11_mPf
⚓
⌘
MC_Meson_Meson_Leptons_Decay/h_223p_111p_11_mPfbar
⚓
⌘
MC_Meson_Meson_Leptons_Decay/h_223p_111p_11_mff
Mode:
ω
→
μ
+
μ
−
π
0
Monte Carlo
⚓
⌘
MC_Meson_Meson_Leptons_Decay/h_223p_111p_13_mPf
⚓
⌘
MC_Meson_Meson_Leptons_Decay/h_223p_111p_13_mPfbar
⚓
⌘
MC_Meson_Meson_Leptons_Decay/h_223p_111p_13_mff
ϕ
Mode:
ϕ
→
η
π
0
γ
Data
⚓
⌘
KLOE_2009_I818106/d01-x01-y01
⚓
⌘
SND_2000_I527094/d01-x01-y01
Mode:
ϕ
→
e
+
e
−
η
Data
⚓
⌘
KLOE2_2014_I1317236/d01-x01-y01
Monte Carlo
⚓
⌘
MC_Meson_Meson_Leptons_Decay/h_333p_221p_11_mPf
⚓
⌘
MC_Meson_Meson_Leptons_Decay/h_333p_221p_11_mPfbar
⚓
⌘
MC_Meson_Meson_Leptons_Decay/h_333p_221p_11_mff
Mode:
ϕ
→
π
+
π
−
π
0
Data
⚓
⌘
SND_2001_I558279/d01-x01-y01
⚓
⌘
SND_2001_I558279/d02-x01-y01
Monte Carlo
⚓
⌘
MC_OmegaPhia1_3Pion_Decay/dalitz_2_EE
⚓
⌘
MC_OmegaPhia1_3Pion_Decay/m0_2
⚓
⌘
MC_OmegaPhia1_3Pion_Decay/mminus_2
⚓
⌘
MC_OmegaPhia1_3Pion_Decay/mplus_2
⚓
⌘
MC_OmegaPhia1_3Pion_Decay/xhist_2
⚓
⌘
MC_OmegaPhia1_3Pion_Decay/yhist_2
Mode:
ϕ
→
μ
+
μ
−
γ
Monte Carlo
⚓
⌘
MC_Meson_Meson_Leptons_Decay/h2_333p_22p_13_mVf
⚓
⌘
MC_Meson_Meson_Leptons_Decay/h2_333p_22p_13_mVfbar
⚓
⌘
MC_Meson_Meson_Leptons_Decay/h2_333p_22p_13_mff
Mode:
ϕ
→
e
+
e
−
π
0
Data
⚓
⌘
KLOE2_2016_I1416825/d01-x01-y01
Monte Carlo
⚓
⌘
MC_Meson_Meson_Leptons_Decay/h_333p_111p_11_mPf
⚓
⌘
MC_Meson_Meson_Leptons_Decay/h_333p_111p_11_mPfbar
⚓
⌘
MC_Meson_Meson_Leptons_Decay/h_333p_111p_11_mff
Mode:
ϕ
→
π
0
π
0
γ
Data
⚓
⌘
KLOE_2002_I585183/d01-x01-y01
⚓
⌘
SND_2000_I525398/d01-x01-y01
a
±
1
Mode:
a
+
1
→
π
+
π
−
π
+
Monte Carlo
Mode:
a
+
1
→
π
+
π
0
π
0
Monte Carlo
a
0
1
Mode:
a
0
1
→
π
+
π
−
π
0
Monte Carlo
Mode:
a
0
1
→
π
0
π
0
π
0
Monte Carlo
Charm Mesons
D
±
Mode:
D
+
→
ˉ
K
1
(
1270
)
0
e
+
ν
e
Monte Carlo
⚓
⌘
MC_Semi_Leptonic_Decay/h_411p_10313m_11m_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_411p_10313m_11m_scale
Mode:
D
+
→
ˉ
K
0
π
+
π
0
Monte Carlo
⚓
⌘
MC_D_Dalitz/dalitz4_EE
⚓
⌘
MC_D_Dalitz/h_Kpi04
⚓
⌘
MC_D_Dalitz/h_Kpip4
⚓
⌘
MC_D_Dalitz/h_pipi4
Mode:
D
+
→
ˉ
K
∗
0
e
+
ν
e
Monte Carlo
⚓
⌘
MC_Semi_Leptonic_Decay/h_411p_313m_11m_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_411p_313m_11m_scale
Mode:
D
+
→
ˉ
K
0
e
+
ν
e
Data
⚓
⌘
BESIII_2017_I1519425/d01-x01-y01
Monte Carlo
⚓
⌘
MC_Semi_Leptonic_Decay/h_411p_311m_11m_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_411p_311m_11m_scale
Mode:
D
+
→
K
−
π
+
π
+
Monte Carlo
⚓
⌘
MC_D_Dalitz/dalitz3_EE
⚓
⌘
MC_D_Dalitz/h_Kpiall3
⚓
⌘
MC_D_Dalitz/h_Kpihigh3
⚓
⌘
MC_D_Dalitz/h_Kpilow3
⚓
⌘
MC_D_Dalitz/h_pipi3
Mode:
D
+
→
ρ
0
e
+
ν
e
Monte Carlo
⚓
⌘
MC_Semi_Leptonic_Decay/h_411p_113p_11m_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_411p_113p_11m_scale
Mode:
D
+
→
η
μ
+
ν
μ
Monte Carlo
⚓
⌘
MC_Semi_Leptonic_Decay/h_411m_221p_13p_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_411m_221p_13p_scale
Mode:
D
+
→
ˉ
K
∗
0
2
μ
+
ν
μ
Monte Carlo
⚓
⌘
MC_Semi_Leptonic_Decay/h_411m_315p_13p_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_411m_315p_13p_scale
Mode:
D
+
→
η
′
μ
+
ν
μ
Monte Carlo
⚓
⌘
MC_Semi_Leptonic_Decay/h_411m_331p_13p_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_411m_331p_13p_scale
Mode:
D
+
→
ˉ
K
1
(
1270
)
0
μ
+
ν
μ
Monte Carlo
⚓
⌘
MC_Semi_Leptonic_Decay/h_411m_10313p_13p_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_411m_10313p_13p_scale
Mode:
D
+
→
π
0
μ
+
ν
μ
Monte Carlo
⚓
⌘
MC_Semi_Leptonic_Decay/h_411m_111p_13p_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_411m_111p_13p_scale
Mode:
D
+
→
η
′
e
+
ν
e
Monte Carlo
⚓
⌘
MC_Semi_Leptonic_Decay/h_411p_331p_11m_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_411p_331p_11m_scale
Mode:
D
+
→
ˉ
K
∗
0
2
e
+
ν
e
Monte Carlo
⚓
⌘
MC_Semi_Leptonic_Decay/h_411p_315m_11m_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_411p_315m_11m_scale
Mode:
D
+
→
ˉ
K
∗
0
μ
+
ν
μ
Monte Carlo
⚓
⌘
MC_Semi_Leptonic_Decay/h_411m_313p_13p_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_411m_313p_13p_scale
Mode:
D
+
→
ρ
0
μ
+
ν
μ
Monte Carlo
⚓
⌘
MC_Semi_Leptonic_Decay/h_411m_113p_13p_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_411m_113p_13p_scale
Mode:
D
+
→
ˉ
K
0
μ
+
ν
μ
Monte Carlo
⚓
⌘
MC_Semi_Leptonic_Decay/h_411m_311p_13p_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_411m_311p_13p_scale
Mode:
D
+
→
ω
e
+
ν
e
Monte Carlo
⚓
⌘
MC_Semi_Leptonic_Decay/h_411p_223p_11m_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_411p_223p_11m_scale
Mode:
D
+
→
η
e
+
ν
e
Monte Carlo
⚓
⌘
MC_Semi_Leptonic_Decay/h_411p_221p_11m_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_411p_221p_11m_scale
Mode:
D
+
→
π
0
e
+
ν
e
Data
⚓
⌘
BESIII_2017_I1519425/d02-x01-y01
Monte Carlo
⚓
⌘
MC_Semi_Leptonic_Decay/h_411p_111p_11m_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_411p_111p_11m_scale
Mode:
D
+
→
ω
μ
+
ν
μ
Monte Carlo
⚓
⌘
MC_Semi_Leptonic_Decay/h_411m_223p_13p_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_411m_223p_13p_scale
Mode:
D
+
→
K
+
π
−
π
+
Monte Carlo
⚓
⌘
MC_D_Dalitz/dalitz5_EE
⚓
⌘
MC_D_Dalitz/h_kppim5
⚓
⌘
MC_D_Dalitz/h_kppip5
⚓
⌘
MC_D_Dalitz/h_pippim5
D
0
,
ˉ
D
0
Mode:
D
0
→
π
−
e
+
ν
e
Data
⚓
⌘
BABAR_2015_I1334693/d01-x01-y01
⚓
⌘
BESIII_2015_I1391138/d02-x01-y03
Monte Carlo
⚓
⌘
MC_Semi_Leptonic_Decay/h_421p_211m_11m_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_421p_211m_11m_scale
Mode:
D
0
→
K
∗
−
2
e
+
ν
e
Monte Carlo
⚓
⌘
MC_Semi_Leptonic_Decay/h_421p_325m_11m_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_421p_325m_11m_scale
Mode:
D
0
→
K
−
μ
+
ν
μ
Monte Carlo
⚓
⌘
MC_Semi_Leptonic_Decay/h_421m_321p_13p_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_421m_321p_13p_scale
Mode:
D
0
→
K
∗
−
e
+
ν
e
Monte Carlo
⚓
⌘
MC_Semi_Leptonic_Decay/h_421p_323m_11m_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_421p_323m_11m_scale
Mode:
D
0
→
K
∗
−
2
μ
+
ν
μ
Monte Carlo
⚓
⌘
MC_Semi_Leptonic_Decay/h_421m_325p_13p_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_421m_325p_13p_scale
Mode:
D
0
→
ˉ
K
0
π
+
π
−
Monte Carlo
⚓
⌘
MC_D_Dalitz/dalitz1_EE
⚓
⌘
MC_D_Dalitz/h_minus1
⚓
⌘
MC_D_Dalitz/h_pipi1
⚓
⌘
MC_D_Dalitz/h_plus1
Mode:
D
0
→
K
1
(
1270
)
−
e
+
ν
e
Monte Carlo
⚓
⌘
MC_Semi_Leptonic_Decay/h_421p_10323m_11m_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_421p_10323m_11m_scale
Mode:
D
0
→
ρ
−
e
+
ν
e
Monte Carlo
⚓
⌘
MC_Semi_Leptonic_Decay/h_421p_213m_11m_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_421p_213m_11m_scale
Mode:
D
0
→
K
−
e
+
ν
e
Data
⚓
⌘
BESIII_2015_I1391138/d01-x01-y03
Monte Carlo
⚓
⌘
MC_Semi_Leptonic_Decay/h_421p_321m_11m_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_421p_321m_11m_scale
Mode:
D
0
→
K
∗
−
μ
+
ν
μ
Monte Carlo
⚓
⌘
MC_Semi_Leptonic_Decay/h_421m_323p_13p_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_421m_323p_13p_scale
Mode:
D
0
→
K
−
π
+
π
0
Monte Carlo
⚓
⌘
MC_D_Dalitz/dalitz2_EE
⚓
⌘
MC_D_Dalitz/h_minus2
⚓
⌘
MC_D_Dalitz/h_neutral2
⚓
⌘
MC_D_Dalitz/h_pipi2
Mode:
D
0
→
π
−
μ
+
ν
μ
Monte Carlo
⚓
⌘
MC_Semi_Leptonic_Decay/h_421m_211p_13p_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_421m_211p_13p_scale
Mode:
D
0
→
ρ
−
μ
+
ν
μ
Monte Carlo
⚓
⌘
MC_Semi_Leptonic_Decay/h_421m_213p_13p_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_421m_213p_13p_scale
Mode:
D
0
→
K
1
(
1270
)
−
μ
+
ν
μ
Monte Carlo
⚓
⌘
MC_Semi_Leptonic_Decay/h_421m_10323p_13p_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_421m_10323p_13p_scale
D
±
s
Mode:
D
+
s
→
η
′
μ
+
ν
μ
Monte Carlo
⚓
⌘
MC_Semi_Leptonic_Decay/h_431m_331p_13p_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_431m_331p_13p_scale
Mode:
D
+
s
→
K
0
μ
+
ν
μ
Monte Carlo
⚓
⌘
MC_Semi_Leptonic_Decay/h_431m_311p_13p_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_431m_311p_13p_scale
Mode:
D
+
s
→
η
′
e
+
ν
e
Monte Carlo
⚓
⌘
MC_Semi_Leptonic_Decay/h_431p_331p_11m_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_431p_331p_11m_scale
Mode:
D
+
s
→
η
e
+
ν
e
Monte Carlo
⚓
⌘
MC_Semi_Leptonic_Decay/h_431p_221p_11m_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_431p_221p_11m_scale
Mode:
D
+
s
→
ϕ
μ
+
ν
μ
Monte Carlo
⚓
⌘
MC_Semi_Leptonic_Decay/h_431m_333p_13p_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_431m_333p_13p_scale
Mode:
D
+
s
→
K
∗
0
μ
+
ν
μ
Monte Carlo
⚓
⌘
MC_Semi_Leptonic_Decay/h_431m_313p_13p_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_431m_313p_13p_scale
Mode:
D
+
s
→
ϕ
e
+
ν
e
Monte Carlo
⚓
⌘
MC_Semi_Leptonic_Decay/h_431p_333p_11m_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_431p_333p_11m_scale
Mode:
D
+
s
→
η
μ
+
ν
μ
Monte Carlo
⚓
⌘
MC_Semi_Leptonic_Decay/h_431m_221p_13p_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_431m_221p_13p_scale
Mode:
D
+
s
→
K
∗
0
e
+
ν
e
Monte Carlo
⚓
⌘
MC_Semi_Leptonic_Decay/h_431p_313m_11m_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_431p_313m_11m_scale
⚓
⌘
MC_Semi_Leptonic_Decay/h_431p_313p_11m_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_431p_313p_11m_scale
Mode:
D
+
s
→
K
0
e
+
ν
e
Monte Carlo
⚓
⌘
MC_Semi_Leptonic_Decay/h_431p_311m_11m_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_431p_311m_11m_scale
⚓
⌘
MC_Semi_Leptonic_Decay/h_431p_311p_11m_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_431p_311p_11m_scale
Mode:
D
+
s
→
K
+
π
−
π
+
Monte Carlo
⚓
⌘
MC_D_Dalitz/dalitz6_EE
⚓
⌘
MC_D_Dalitz/h_kppim6
⚓
⌘
MC_D_Dalitz/h_kppip6
⚓
⌘
MC_D_Dalitz/h_pippim6
Bottom Mesons
B
0
,
ˉ
B
0
Mode:
B
0
→
π
−
e
+
ν
e
Data
⚓
⌘
BELLE_2011_I878990/d01-x01-y01
⚓
⌘
BELLE_2013_I1238273/d01-x01-y01
Monte Carlo
⚓
⌘
MC_Semi_Leptonic_Decay/h_511p_211m_11m_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_511p_211m_11m_scale
Mode:
B
0
→
K
0
μ
+
μ
−
Monte Carlo
⚓
⌘
MC_Meson_Meson_Leptons_Decay/h_511m_311m_13_mPf
⚓
⌘
MC_Meson_Meson_Leptons_Decay/h_511m_311m_13_mPfbar
⚓
⌘
MC_Meson_Meson_Leptons_Decay/h_511m_311m_13_mff
Mode:
B
0
→
D
∗
−
2
e
+
ν
e
Monte Carlo
⚓
⌘
MC_Semi_Leptonic_Decay/h_511p_415m_11m_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_511p_415m_11m_scale
Mode:
B
0
→
K
∗
0
μ
+
μ
−
Monte Carlo
⚓
⌘
MC_Meson_Meson_Leptons_Decay/h2_511p_313p_13_mVf
⚓
⌘
MC_Meson_Meson_Leptons_Decay/h2_511p_313p_13_mVfbar
⚓
⌘
MC_Meson_Meson_Leptons_Decay/h2_511p_313p_13_mff
Mode:
B
0
→
π
−
μ
+
ν
μ
Monte Carlo
⚓
⌘
MC_Semi_Leptonic_Decay/h_511m_211p_13p_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_511m_211p_13p_scale
Mode:
B
→
X
s
γ
Data
⚓
⌘
BELLE_2015_I1330289/d01-x01-y02
Mode:
B
0
→
D
∗
−
μ
+
ν
μ
Monte Carlo
⚓
⌘
MC_Semi_Leptonic_Decay/h_511m_413p_13p_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_511m_413p_13p_scale
Mode:
B
0
→
D
−
1
(
2430
)
e
+
ν
e
Monte Carlo
⚓
⌘
MC_Semi_Leptonic_Decay/h_511p_20413m_11m_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_511p_20413m_11m_scale
Mode:
B
0
→
D
∗
−
0
(
2400
)
μ
+
ν
μ
Monte Carlo
⚓
⌘
MC_Semi_Leptonic_Decay/h_511m_10411p_13p_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_511m_10411p_13p_scale
Mode:
B
0
→
K
∗
0
e
+
e
−
Monte Carlo
⚓
⌘
MC_Meson_Meson_Leptons_Decay/h2_511p_313p_11_mVf
⚓
⌘
MC_Meson_Meson_Leptons_Decay/h2_511p_313p_11_mVfbar
⚓
⌘
MC_Meson_Meson_Leptons_Decay/h2_511p_313p_11_mff
Mode:
B
0
→
D
−
μ
+
ν
μ
Data
⚓
⌘
BELLE_2015_I1397632/d01-x01-y02
Monte Carlo
⚓
⌘
MC_Semi_Leptonic_Decay/h_511m_411p_13p_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_511m_411p_13p_scale
Mode:
B
0
→
ρ
−
e
+
ν
e
Data
⚓
⌘
BELLE_2013_I1238273/d03-x01-y01
Monte Carlo
⚓
⌘
MC_Semi_Leptonic_Decay/h_511p_213m_11m_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_511p_213m_11m_scale
Mode:
B
0
→
D
∗
−
2
μ
+
ν
μ
Monte Carlo
⚓
⌘
MC_Semi_Leptonic_Decay/h_511m_415p_13p_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_511m_415p_13p_scale
Mode:
B
0
→
D
−
1
(
2420
)
μ
+
ν
μ
Monte Carlo
⚓
⌘
MC_Semi_Leptonic_Decay/h_511m_10413p_13p_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_511m_10413p_13p_scale
Mode:
B
0
→
D
∗
−
e
+
ν
e
Data
⚓
⌘
BELLE_2017_I1512299/d01-x01-y01
⚓
⌘
BELLE_2017_I1512299/d02-x01-y01
⚓
⌘
BELLE_2017_I1512299/d03-x01-y01
⚓
⌘
BELLE_2017_I1512299/d04-x01-y01
Monte Carlo
⚓
⌘
MC_Semi_Leptonic_Decay/h_511p_413m_11m_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_511p_413m_11m_scale
Mode:
B
0
→
D
−
e
+
ν
e
Data
⚓
⌘
BELLE_2015_I1397632/d01-x01-y01
Monte Carlo
⚓
⌘
MC_Semi_Leptonic_Decay/h_511p_411m_11m_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_511p_411m_11m_scale
Mode:
B
0
→
D
∗
−
0
(
2400
)
e
+
ν
e
Monte Carlo
⚓
⌘
MC_Semi_Leptonic_Decay/h_511p_10411m_11m_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_511p_10411m_11m_scale
Mode:
B
0
→
D
−
1
(
2430
)
μ
+
ν
μ
Monte Carlo
⚓
⌘
MC_Semi_Leptonic_Decay/h_511m_20413p_13p_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_511m_20413p_13p_scale
Mode:
B
0
→
ρ
−
μ
+
ν
μ
Monte Carlo
⚓
⌘
MC_Semi_Leptonic_Decay/h_511m_213p_13p_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_511m_213p_13p_scale
Mode:
B
0
→
K
0
e
+
e
−
Monte Carlo
Mode:
B
0
→
D
−
1
(
2420
)
e
+
ν
e
Monte Carlo
⚓
⌘
MC_Semi_Leptonic_Decay/h_511p_10413m_11m_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_511p_10413m_11m_scale
Spectrum of
K
0
,
ˉ
K
0
⚓
⌘
ARGUS_1994_I354224/d01-x01-y01
B
±
Mode:
B
+
→
π
0
e
+
ν
e
Data
⚓
⌘
BELLE_2013_I1238273/d02-x01-y01
Monte Carlo
⚓
⌘
MC_Semi_Leptonic_Decay/h_521p_111p_11m_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_521p_111p_11m_scale
Mode:
B
+
→
ˉ
D
∗
0
0
(
2400
)
μ
+
ν
μ
Monte Carlo
⚓
⌘
MC_Semi_Leptonic_Decay/h_521m_10421p_13p_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_521m_10421p_13p_scale
Mode:
B
+
→
ˉ
D
0
1
(
2430
)
e
+
ν
e
Monte Carlo
⚓
⌘
MC_Semi_Leptonic_Decay/h_521p_20423m_11m_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_521p_20423m_11m_scale
Mode:
B
+
→
K
−
μ
+
μ
−
Monte Carlo
⚓
⌘
MC_Meson_Meson_Leptons_Decay/h_521m_321m_13_mPf
⚓
⌘
MC_Meson_Meson_Leptons_Decay/h_521m_321m_13_mPfbar
⚓
⌘
MC_Meson_Meson_Leptons_Decay/h_521m_321m_13_mff
Mode:
B
+
→
η
′
e
+
ν
e
Monte Carlo
⚓
⌘
MC_Semi_Leptonic_Decay/h_521p_331p_11m_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_521p_331p_11m_scale
Mode:
B
+
→
π
0
μ
+
ν
μ
Monte Carlo
⚓
⌘
MC_Semi_Leptonic_Decay/h_521m_111p_13p_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_521m_111p_13p_scale
Mode:
B
+
→
ˉ
D
0
e
+
ν
e
Data
⚓
⌘
BELLE_2015_I1397632/d02-x01-y01
Monte Carlo
⚓
⌘
MC_Semi_Leptonic_Decay/h_521p_421m_11m_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_521p_421m_11m_scale
Mode:
B
+
→
ρ
0
e
+
ν
e
Data
⚓
⌘
BELLE_2013_I1238273/d04-x01-y01
Monte Carlo
⚓
⌘
MC_Semi_Leptonic_Decay/h_521p_113p_11m_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_521p_113p_11m_scale
Mode:
B
+
→
ˉ
D
∗
0
μ
+
ν
μ
Monte Carlo
⚓
⌘
MC_Semi_Leptonic_Decay/h_521m_423p_13p_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_521m_423p_13p_scale
Mode:
B
+
→
ω
μ
+
ν
μ
Monte Carlo
⚓
⌘
MC_Semi_Leptonic_Decay/h_521p_223p_11m_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_521p_223p_11m_scale
Mode:
B
+
→
ω
e
+
ν
e
Data
⚓
⌘
BABAR_2013_I1116411/d01-x01-y01
⚓
⌘
BELLE_2013_I1238273/d05-x01-y01
Monte Carlo
⚓
⌘
MC_Semi_Leptonic_Decay/h_521m_223p_13p_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_521m_223p_13p_scale
Mode:
B
+
→
ˉ
D
∗
0
e
+
ν
e
Monte Carlo
⚓
⌘
MC_Semi_Leptonic_Decay/h_521p_423m_11m_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_521p_423m_11m_scale
Mode:
B
+
→
η
μ
+
ν
μ
Monte Carlo
⚓
⌘
MC_Semi_Leptonic_Decay/h_521m_221p_13p_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_521m_221p_13p_scale
Mode:
B
+
→
ρ
0
μ
+
ν
μ
Monte Carlo
⚓
⌘
MC_Semi_Leptonic_Decay/h_521m_113p_13p_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_521m_113p_13p_scale
Mode:
B
+
→
ˉ
D
∗
0
2
e
+
ν
e
Monte Carlo
⚓
⌘
MC_Semi_Leptonic_Decay/h_521p_425m_11m_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_521p_425m_11m_scale
Mode:
B
+
→
η
′
μ
+
ν
μ
Monte Carlo
⚓
⌘
MC_Semi_Leptonic_Decay/h_521m_331p_13p_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_521m_331p_13p_scale
Mode:
B
+
→
ˉ
D
0
1
(
2420
)
μ
+
ν
μ
Monte Carlo
⚓
⌘
MC_Semi_Leptonic_Decay/h_521m_10423p_13p_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_521m_10423p_13p_scale
Mode:
B
+
→
K
∗
+
μ
+
μ
−
Monte Carlo
Mode:
B
+
→
ˉ
D
0
1
(
2420
)
e
+
ν
e
Monte Carlo
⚓
⌘
MC_Semi_Leptonic_Decay/h_521p_10423m_11m_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_521p_10423m_11m_scale
Mode:
B
+
→
η
e
+
ν
e
Monte Carlo
⚓
⌘
MC_Semi_Leptonic_Decay/h_521p_221p_11m_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_521p_221p_11m_scale
Mode:
B
+
→
ˉ
D
∗
0
2
μ
+
ν
μ
Monte Carlo
⚓
⌘
MC_Semi_Leptonic_Decay/h_521m_425p_13p_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_521m_425p_13p_scale
Mode:
B
+
→
K
−
e
+
e
−
Monte Carlo
Mode:
B
+
→
ˉ
D
∗
0
0
(
2400
)
e
+
ν
e
Monte Carlo
⚓
⌘
MC_Semi_Leptonic_Decay/h_521p_10421m_11m_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_521p_10421m_11m_scale
Mode:
B
+
→
ˉ
D
0
1
(
2430
)
μ
+
ν
μ
Monte Carlo
⚓
⌘
MC_Semi_Leptonic_Decay/h_521m_20423p_13p_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_521m_20423p_13p_scale
Mode:
B
+
→
ˉ
D
0
μ
+
ν
μ
Data
⚓
⌘
BELLE_2015_I1397632/d02-x01-y02
Monte Carlo
⚓
⌘
MC_Semi_Leptonic_Decay/h_521m_421p_13p_energy
⚓
⌘
MC_Semi_Leptonic_Decay/h_521m_421p_13p_scale
Mode:
B
+
→
K
∗
+
e
+
e
−
Monte Carlo
⚓
⌘
MC_Meson_Meson_Leptons_Decay/h2_521m_323m_11_mVf
⚓
⌘
MC_Meson_Meson_Leptons_Decay/h2_521m_323m_11_mVfbar
⚓
⌘
MC_Meson_Meson_Leptons_Decay/h2_521m_323m_11_mff
Charmonium
η
c
Charged Particle Multplicity Distribution
Data
⚓
⌘
BESIII_2019_I1724880/d01-x01-y01
J
/
ψ
Mode:
J
/
ψ
→
p
ˉ
p
Data
⚓
⌘
BESIII_2012_I1113599/d01-x01-y01
Monte Carlo
⚓
⌘
BESIII_2012_I1113599/ctheta_p
Mode:
J
/
ψ
→
Ξ
0
ˉ
Ξ
0
Data
⚓
⌘
BESIII_2017_I1506414/d01-x01-y02
⚓
⌘
BESIII_2017_I1506414/d02-x02-y01
Mode:
J
/
ψ
→
Σ
0
ˉ
Σ
0
Data
⚓
⌘
BESIII_2017_I1510563/d01-x01-y03
⚓
⌘
BESIII_2017_I1510563/d02-x02-y01
Mode:
J
/
ψ
→
Σ
∗
−
ˉ
Σ
∗
+
Data
⚓
⌘
BESIII_2016_I1422780/d01-x01-y03
⚓
⌘
BESIII_2016_I1422780/d02-x01-y02
Mode:
J
/
ψ
→
Σ
∗
+
ˉ
Σ
∗
−
Data
⚓
⌘
BESIII_2016_I1422780/d01-x01-y03
⚓
⌘
BESIII_2016_I1422780/d02-x01-y03
Mode:
J
/
ψ
→
η
e
+
e
−
Data
⚓
⌘
BESIII_2018_I1697377/d01-x01-y01
Mode:
J
/
ψ
→
γ
e
+
e
−
Monte Carlo
⚓
⌘
MC_Meson_Meson_Leptons_Decay/h2_443p_22p_11_mVf
⚓
⌘
MC_Meson_Meson_Leptons_Decay/h2_443p_22p_11_mVfbar
⚓
⌘
MC_Meson_Meson_Leptons_Decay/h2_443p_22p_11_mff
Mode:
J
/
ψ
→
Λ
0
ˉ
Λ
0
Data
⚓
⌘
BESIII_2017_I1510563/d01-x01-y01
⚓
⌘
BESIII_2017_I1510563/d02-x01-y01
⚓
⌘
BESIII_2019_I1691850/d01-x01-y01
⚓
⌘
BESIII_2019_I1691850/d01-x02-y01
⚓
⌘
BESIII_2019_I1691850/d01-x03-y01
⚓
⌘
BESIII_2019_I1691850/d01-x04-y01
⚓
⌘
BESIII_2019_I1691850/d01-x05-y01
Monte Carlo
⚓
⌘
BESIII_2019_I1691850/T1_n
⚓
⌘
BESIII_2019_I1691850/T1_p
⚓
⌘
BESIII_2019_I1691850/T2_n
⚓
⌘
BESIII_2019_I1691850/T2_p
⚓
⌘
BESIII_2019_I1691850/T3_n
⚓
⌘
BESIII_2019_I1691850/T3_p
⚓
⌘
BESIII_2019_I1691850/T4_n
⚓
⌘
BESIII_2019_I1691850/T4_p
⚓
⌘
BESIII_2019_I1691850/T5_n
⚓
⌘
BESIII_2019_I1691850/T5_p
⚓
⌘
BESIII_2019_I1691850/cThetaL
⚓
⌘
BESIII_2019_I1691850/mu_n
⚓
⌘
BESIII_2019_I1691850/mu_p
Mode:
J
/
ψ
→
Ξ
−
ˉ
Ξ
+
Data
⚓
⌘
BESIII_2016_I1422780/d01-x01-y03
⚓
⌘
BESIII_2016_I1422780/d02-x01-y01
Mode:
J
/
ψ
→
n
ˉ
n
Data
⚓
⌘
BESIII_2012_I1113599/d01-x01-y02
Monte Carlo
⚓
⌘
BESIII_2012_I1113599/ctheta_n
Mode:
J
/
ψ
→
Σ
∗
0
ˉ
Σ
∗
0
Data
⚓
⌘
BESIII_2017_I1506414/d01-x01-y01
⚓
⌘
BESIII_2017_I1506414/d02-x01-y01
ψ
(
2
S
)
Mode:
ψ
(
2
S
)
→
Σ
∗
−
ˉ
Σ
∗
+
Data
⚓
⌘
BESIII_2016_I1422780/d01-x01-y03
⚓
⌘
BESIII_2016_I1422780/d02-x01-y05
Mode:
ψ
(
2
S
)
→
Ξ
0
ˉ
Ξ
0
Data
⚓
⌘
BESIII_2017_I1506414/d01-x01-y04
⚓
⌘
BESIII_2017_I1506414/d02-x04-y01
Mode:
ψ
(
2
S
)
→
Λ
0
ˉ
Λ
0
Data
⚓
⌘
BESIII_2017_I1510563/d01-x01-y02
⚓
⌘
BESIII_2017_I1510563/d02-x03-y01
Mode:
ψ
(
2
S
)
→
Σ
0
ˉ
Σ
0
Data
⚓
⌘
BESIII_2017_I1510563/d01-x01-y04
⚓
⌘
BESIII_2017_I1510563/d02-x04-y01
Mode:
ψ
(
2
S
)
→
Σ
∗
+
ˉ
Σ
∗
−
Data
⚓
⌘
BESIII_2016_I1422780/d01-x01-y03
⚓
⌘
BESIII_2016_I1422780/d02-x01-y06
Mode:
ψ
(
2
S
)
→
Ξ
−
ˉ
Ξ
+
Data
⚓
⌘
BESIII_2016_I1422780/d01-x01-y03
⚓
⌘
BESIII_2016_I1422780/d02-x01-y04
Mode:
ψ
(
2
S
)
→
p
ˉ
p
Data
⚓
⌘
BESIII_2018_I1658762/d01-x01-y01
Monte Carlo
⚓
⌘
BESIII_2018_I1658762/ctheta_p
Mode:
ψ
(
2
S
)
→
Σ
∗
0
ˉ
Σ
∗
0
Data
⚓
⌘
BESIII_2017_I1506414/d01-x01-y03
⚓
⌘
BESIII_2017_I1506414/d02-x03-y01
Mode:
ψ
(
2
S
)
→
n
ˉ
n
Data
⚓
⌘
BESIII_2018_I1658762/d01-x01-y02
Monte Carlo
⚓
⌘
BESIII_2018_I1658762/ctheta_n
ψ
(
3770
)
Mode:
ψ
(
3770
)
→
J
/
ψ
π
+
π
−
Monte Carlo
⚓
⌘
MC_Onium_PiPi_Decay/h_30443_443_hpippim
⚓
⌘
MC_Onium_PiPi_Decay/h_30443_443_mpippim
Mode:
ψ
(
3770
)
→
J
/
ψ
π
0
π
0
Monte Carlo
⚓
⌘
MC_Onium_PiPi_Decay/h_30443_443_hpi0pi0
⚓
⌘
MC_Onium_PiPi_Decay/h_30443_443_mpi0pi0
Bottomonium
Υ
(
1
S
)
Multiplicity of
π
0
⚓
⌘
ARGUS_1990_I278933/d01-x01-y02
Multiplicity of
ρ
0
⚓
⌘
ARGUS_1993_S2789213/d02-x01-y02
Multiplicity of
π
±
⚓
⌘
ARGUS_1989_I276860/d01-x01-y01
⚓
⌘
ARGUS_1989_I276860/d01-x01-y02
Multiplicity of
η
⚓
⌘
ARGUS_1990_I278933/d02-x01-y02
Multiplicity of
ω
⚓
⌘
ARGUS_1993_S2789213/d02-x01-y01
Multiplicity of
K
0
,
ˉ
K
0
⚓
⌘
ARGUS_1989_I276860/d02-x01-y01
Multiplicity of
K
∗
0
,
ˉ
K
∗
0
⚓
⌘
ARGUS_1993_S2789213/d02-x01-y03
Multiplicity of
K
±
⚓
⌘
ARGUS_1989_I276860/d03-x01-y01
Multiplicity of
K
∗
±
⚓
⌘
ARGUS_1993_S2789213/d02-x01-y04
Multiplicity of
η
′
⚓
⌘
ARGUS_1993_S2669951/d01-x01-y01
⚓
⌘
ARGUS_1993_S2669951/d01-x01-y02
Multiplicity of
ϕ
⚓
⌘
ARGUS_1989_I262551/d03-x01-y01
⚓
⌘
ARGUS_1993_S2789213/d02-x01-y05
Multiplicity of
p
,
ˉ
p
⚓
⌘
ARGUS_1989_I276860/d04-x01-y01
⚓
⌘
ARGUS_1989_I276860/d04-x01-y02
Multiplicity of
Σ
∗
−
,
ˉ
Σ
∗
+
⚓
⌘
ARGUS_1988_I251097/d01-x01-y04
Multiplicity of
Λ
0
,
ˉ
Λ
0
⚓
⌘
ARGUS_1988_I251097/d01-x01-y01
Multiplicity of
Σ
0
,
ˉ
Σ
0
⚓
⌘
ARGUS_1988_I251097/d01-x01-y03
Multiplicity of
Σ
∗
+
,
ˉ
Σ
∗
−
⚓
⌘
ARGUS_1988_I251097/d01-x01-y05
Multiplicity of
Ξ
−
,
ˉ
Ξ
+
⚓
⌘
ARGUS_1988_I251097/d01-x01-y02
Multiplicity of
Ξ
∗
0
,
ˉ
Ξ
∗
0
⚓
⌘
ARGUS_1988_I251097/d01-x01-y06
Multiplicity of
Ω
−
,
ˉ
Ω
+
⚓
⌘
ARGUS_1988_I251097/d01-x01-y07
Multiplicity of
f
0
(
980
)
⚓
⌘
ARGUS_1993_S2669951/d05-x01-y01
Spectrum of
π
0
⚓
⌘
ARGUS_1990_I278933/d04-x01-y01
Spectrum of
ρ
0
⚓
⌘
ARGUS_1993_S2789213/d11-x01-y01
Spectrum of
π
±
⚓
⌘
ARGUS_1989_I276860/d05-x01-y01
⚓
⌘
ARGUS_1989_I276860/d09-x01-y01
Spectrum of
η
⚓
⌘
ARGUS_1990_I278933/d06-x01-y01
Spectrum of
ω
⚓
⌘
ARGUS_1993_S2789213/d14-x01-y01
Spectrum of
K
0
,
ˉ
K
0
⚓
⌘
ARGUS_1989_I276860/d07-x01-y01
⚓
⌘
ARGUS_1989_I276860/d11-x01-y01
⚓
⌘
PLUTO_1981_I165122/d06-x01-y01
Spectrum of
K
∗
0
,
ˉ
K
∗
0
⚓
⌘
ARGUS_1993_S2789213/d08-x01-y01
Spectrum of
K
±
⚓
⌘
ARGUS_1989_I276860/d06-x01-y01
⚓
⌘
ARGUS_1989_I276860/d10-x01-y01
Spectrum of
K
∗
±
⚓
⌘
ARGUS_1993_S2789213/d05-x01-y01
Spectrum of
ϕ
⚓
⌘
ARGUS_1989_I262551/d02-x01-y01
Spectrum of
p
,
ˉ
p
⚓
⌘
ARGUS_1989_I276860/d08-x01-y01
⚓
⌘
ARGUS_1989_I276860/d12-x01-y01
Spectrum of
Λ
0
,
ˉ
Λ
0
⚓
⌘
ARGUS_1988_I251097/d03-x01-y01
Spectrum of
Λ
0
(
1520
)
,
ˉ
Λ
0
(
1520
)
⚓
⌘
ARGUS_1989_I262415/d03-x01-y01
Spectrum of
Ξ
−
,
ˉ
Ξ
+
⚓
⌘
ARGUS_1988_I251097/d07-x01-y01
Spectrum of
f
0
(
980
)
⚓
⌘
ARGUS_1993_S2669951/d03-x01-y01
Υ
(
2
S
)
Mode:
Υ
(
2
S
)
→
Υ
(
1
S
)
π
+
π
−
Monte Carlo
⚓
⌘
MC_Onium_PiPi_Decay/h_100553_553_hpippim
⚓
⌘
MC_Onium_PiPi_Decay/h_100553_553_mpippim
Mode:
Υ
(
2
S
)
→
J
/
ψ
π
+
π
−
Monte Carlo
⚓
⌘
MC_Onium_PiPi_Decay/h_100443_443_hpippim
⚓
⌘
MC_Onium_PiPi_Decay/h_100443_443_mpippim
Mode:
Υ
(
2
S
)
→
Υ
(
1
S
)
)
π
0
π
0
Monte Carlo
⚓
⌘
MC_Onium_PiPi_Decay/h_100553_553_hpi0pi0
⚓
⌘
MC_Onium_PiPi_Decay/h_100553_553_mpi0pi0
Mode:
Υ
(
2
S
)
→
J
/
ψ
π
0
π
0
Monte Carlo
⚓
⌘
MC_Onium_PiPi_Decay/h_100443_443_hpi0pi0
⚓
⌘
MC_Onium_PiPi_Decay/h_100443_443_mpi0pi0
Multiplicity of
π
0
⚓
⌘
ARGUS_1990_I278933/d01-x01-y03
Multiplicity of
η
⚓
⌘
ARGUS_1990_I278933/d02-x01-y03
Multiplicity of
ϕ
⚓
⌘
ARGUS_1989_I262551/d04-x01-y01
Spectrum of
π
0
⚓
⌘
ARGUS_1990_I278933/d04-x01-y02
Spectrum of
η
⚓
⌘
ARGUS_1990_I278933/d06-x01-y02
Spectrum of
ϕ
⚓
⌘
ARGUS_1989_I262551/d02-x01-y02
Spectrum of
Λ
0
,
ˉ
Λ
0
⚓
⌘
ARGUS_1988_I251097/d04-x01-y01
Spectrum of
Ξ
−
,
ˉ
Ξ
+
⚓
⌘
ARGUS_1988_I251097/d08-x01-y01
Spectrum of
f
0
(
980
)
⚓
⌘
ARGUS_1993_S2669951/d04-x01-y01
Υ
(
4
S
)
Mode:
Υ
(
4
S
)
→
J
/
ψ
π
+
π
−
Monte Carlo
⚓
⌘
MC_Onium_PiPi_Decay/h_300553_553_hpippim
⚓
⌘
MC_Onium_PiPi_Decay/h_300553_553_mpippim
Mode:
Υ
(
4
S
)
→
Υ
(
1
S
)
π
+
π
−
Monte Carlo
⚓
⌘
MC_Onium_PiPi_Decay/h_300553_100553_hpippim
⚓
⌘
MC_Onium_PiPi_Decay/h_300553_100553_mpippim
Mode:
Υ
(
4
S
)
→
J
/
ψ
π
0
π
0
Monte Carlo
⚓
⌘
MC_Onium_PiPi_Decay/h_300553_553_hpi0pi0
⚓
⌘
MC_Onium_PiPi_Decay/h_300553_553_mpi0pi0
Mode:
Υ
(
4
S
)
→
Υ
(
1
S
)
π
0
π
0
Monte Carlo
⚓
⌘
MC_Onium_PiPi_Decay/h_300553_100553_hpi0pi0
⚓
⌘
MC_Onium_PiPi_Decay/h_300553_100553_mpi0pi0
Charged Particle Multplicity Distribution
Data
⚓
⌘
ARGUS_1992_I319102/d03-x01-y01
Multiplicity of
π
0
⚓
⌘
BELLE_2001_S4598261/d02-x01-y01
⚓
⌘
PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d88-x01-y01
Multiplicity of
ρ
0
⚓
⌘
ARGUS_1993_S2789213/d03-x01-y02
⚓
⌘
PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d90-x01-y01
Multiplicity of
π
±
⚓
⌘
ARGUS_1993_S2653028/d07-x01-y01
⚓
⌘
ARGUS_1993_S2653028/d08-x01-y01
⚓
⌘
PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d87-x01-y01
Multiplicity of
η
⚓
⌘
PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d89-x01-y01
Multiplicity of
ω
⚓
⌘
ARGUS_1993_S2789213/d03-x01-y01
Multiplicity of
K
0
,
ˉ
K
0
⚓
⌘
PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d63-x01-y01
Multiplicity of
K
∗
0
,
ˉ
K
∗
0
⚓
⌘
ARGUS_1993_S2789213/d03-x01-y03
⚓
⌘
PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d65-x01-y01
Multiplicity of
K
±
⚓
⌘
ARGUS_1993_S2653028/d09-x01-y01
⚓
⌘
PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d60-x01-y01
⚓
⌘
PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d61-x01-y01
⚓
⌘
PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d62-x01-y01
Multiplicity of
K
∗
±
⚓
⌘
ARGUS_1993_S2789213/d03-x01-y04
⚓
⌘
PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d64-x01-y01
Multiplicity of
ϕ
⚓
⌘
ARGUS_1993_S2789213/d03-x01-y05
⚓
⌘
PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d92-x01-y01
Multiplicity of
D
±
⚓
⌘
PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d29-x01-y01
Multiplicity of
D
∗
±
⚓
⌘
PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d31-x01-y01
Multiplicity of
D
0
,
ˉ
D
0
⚓
⌘
PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d30-x01-y01
Multiplicity of
D
∗
0
,
ˉ
D
∗
0
⚓
⌘
PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d32-x01-y01
Multiplicity of
D
±
s
⚓
⌘
PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d33-x01-y01
Multiplicity of
D
∗
±
s
⚓
⌘
PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d34-x01-y01
Multiplicity of
J
/
ψ
⚓
⌘
BABAR_2003_I593379/d01-x01-y01
⚓
⌘
BABAR_2003_I593379/d01-x01-y02
⚓
⌘
PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d48-x01-y01
Multiplicity of
χ
c
2
(
1
P
)
⚓
⌘
BABAR_2003_I593379/d01-x01-y05
⚓
⌘
BABAR_2003_I593379/d01-x01-y06
⚓
⌘
PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d53-x01-y01
Multiplicity of
p
,
ˉ
p
⚓
⌘
ARGUS_1993_S2653028/d10-x01-y01
⚓
⌘
ARGUS_1993_S2653028/d11-x01-y01
⚓
⌘
PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d110-x01-y01
Multiplicity of
Λ
0
,
ˉ
Λ
0
⚓
⌘
PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d113-x01-y01
Multiplicity of
Ξ
−
,
ˉ
Ξ
+
⚓
⌘
PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d116-x01-y01
Multiplicity of
Σ
0
c
,
ˉ
Σ
0
c
⚓
⌘
PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d106-x01-y01
Multiplicity of
Λ
+
c
,
ˉ
Λ
+
c
⚓
⌘
BABAR_2007_S6895344/d04-x01-y01
⚓
⌘
PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d96-x01-y01
Multiplicity of
Σ
+
+
c
,
Σ
0
c
,
ˉ
Σ
+
+
c
,
ˉ
Σ
0
c
⚓
⌘
PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d104-x01-y01
Multiplicity of
χ
c
1
(
1
P
)
⚓
⌘
BABAR_2003_I593379/d01-x01-y03
⚓
⌘
BABAR_2003_I593379/d01-x01-y04
⚓
⌘
PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d51-x01-y01
Multiplicity of
ψ
(
2
S
)
⚓
⌘
BABAR_2003_I593379/d01-x01-y07
⚓
⌘
PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d50-x01-y01
Spectrum of
π
0
⚓
⌘
BELLE_2001_S4598261/d01-x01-y01
Spectrum of
ρ
0
⚓
⌘
ARGUS_1993_S2789213/d12-x01-y01
Spectrum of
π
±
⚓
⌘
ARGUS_1993_S2653028/d01-x01-y01
⚓
⌘
ARGUS_1993_S2653028/d02-x01-y01
Spectrum of
K
∗
0
,
ˉ
K
∗
0
⚓
⌘
ARGUS_1993_S2789213/d09-x01-y01
Spectrum of
K
±
⚓
⌘
ARGUS_1993_S2653028/d03-x01-y01
⚓
⌘
ARGUS_1993_S2653028/d06-x01-y01
Spectrum of
K
∗
±
⚓
⌘
ARGUS_1993_S2789213/d06-x01-y01
Spectrum of
J
/
ψ
⚓
⌘
BABAR_2003_I593379/d06-x01-y01
⚓
⌘
BABAR_2003_I593379/d10-x01-y01
Spectrum of
χ
c
2
(
1
P
)
⚓
⌘
BABAR_2003_I593379/d07-x01-y02
Spectrum of
p
,
ˉ
p
⚓
⌘
ARGUS_1993_S2653028/d04-x01-y01
⚓
⌘
ARGUS_1993_S2653028/d05-x01-y01
Spectrum of
Λ
+
c
,
ˉ
Λ
+
c
⚓
⌘
BABAR_2007_S6895344/d03-x01-y01
Spectrum of
Ξ
0
c
,
ˉ
Ξ
0
c
⚓
⌘
BABAR_2005_S6181155/d01-x01-y01
⚓
⌘
BABAR_2005_S6181155/d02-x01-y01
Spectrum of
χ
c
1
(
1
P
)
⚓
⌘
BABAR_2003_I593379/d07-x01-y01
Spectrum of
ψ
(
2
S
)
⚓
⌘
BABAR_2003_I593379/d08-x01-y01
Hyperons
Ξ
−
,
ˉ
Ξ
+
Mode:
Ξ
−
→
Λ
0
π
−
Data
⚓
⌘
E756_2000_I530367/d01-x01-y01
⚓
⌘
E756_2000_I530367/d01-x01-y02
Monte Carlo
⚓
⌘
E756_2000_I530367/cthetaM
⚓
⌘
E756_2000_I530367/cthetaP
Ξ
0
,
ˉ
Ξ
0
Mode:
Ξ
0
→
Λ
0
π
0
Data
⚓
⌘
NA48_2010_I868871/d01-x01-y01
Monte Carlo
⚓
⌘
NA48_2010_I868871/ctheta_pi0
Mode:
Ξ
0
→
Σ
0
γ
Data
⚓
⌘
NA48_2010_I868871/d03-x01-y01
Monte Carlo
⚓
⌘
NA48_2010_I868871/ctheta_Sigma_0
⚓
⌘
NA48_2010_I868871/ctheta_Sigma_1
⚓
⌘
NA48_2010_I868871/ctheta_Sigma_10
⚓
⌘
NA48_2010_I868871/ctheta_Sigma_11
⚓
⌘
NA48_2010_I868871/ctheta_Sigma_12
⚓
⌘
NA48_2010_I868871/ctheta_Sigma_13
⚓
⌘
NA48_2010_I868871/ctheta_Sigma_14
⚓
⌘
NA48_2010_I868871/ctheta_Sigma_15
⚓
⌘
NA48_2010_I868871/ctheta_Sigma_16
⚓
⌘
NA48_2010_I868871/ctheta_Sigma_17
⚓
⌘
NA48_2010_I868871/ctheta_Sigma_18
⚓
⌘
NA48_2010_I868871/ctheta_Sigma_19
⚓
⌘
NA48_2010_I868871/ctheta_Sigma_2
⚓
⌘
NA48_2010_I868871/ctheta_Sigma_3
⚓
⌘
NA48_2010_I868871/ctheta_Sigma_4
⚓
⌘
NA48_2010_I868871/ctheta_Sigma_5
⚓
⌘
NA48_2010_I868871/ctheta_Sigma_6
⚓
⌘
NA48_2010_I868871/ctheta_Sigma_7
⚓
⌘
NA48_2010_I868871/ctheta_Sigma_8
⚓
⌘
NA48_2010_I868871/ctheta_Sigma_9
Mode:
Ξ
0
→
Λ
0
γ
Data
⚓
⌘
NA48_2010_I868871/d02-x01-y01
Monte Carlo
⚓
⌘
NA48_2010_I868871/ctheta_gamma
Ω
−
,
ˉ
Ω
+
Mode:
Ω
−
→
Λ
0
K
−
Data
⚓
⌘
HyperCP_2005_I677384/d01-x01-y01
⚓
⌘
HyperCP_2005_I677384/d01-x01-y02
⚓
⌘
HyperCP_2005_I677384/d01-x01-y03
Monte Carlo
⚓
⌘
HyperCP_2005_I677384/cthetaAll
⚓
⌘
HyperCP_2005_I677384/cthetaM
⚓
⌘
HyperCP_2005_I677384/cthetaP
Charm Baryons
Λ
+
c
,
ˉ
Λ
+
c
Mode:
Λ
+
c
→
Λ
0
π
+
Data
⚓
⌘
FOCUS_2006_I693639/d01-x01-y01
Monte Carlo
⚓
⌘
FOCUS_2006_I693639/ctheta
Ξ
0
c
,
ˉ
Ξ
0
c
Mode:
Ξ
0
c
→
Ξ
−
π
+
Data
⚓
⌘
CLEO_2000_I537236/d01-x01-y01
Monte Carlo
⚓
⌘
CLEO_2000_I537236/ctheta