new measurements of ψ(3770) resonance parameters & dd-bar ... · parameters & dd-bar cross...
TRANSCRIPT
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New Measurements of ψ(3770) Resonance Parameters & DD-bar Cross Section at
BES-II & CLEO-c
Gang RONG
Institute of High Energy Physics, Beijing 100039, P.R. China
3rd Workshop on QuarkoniumIHEP Beijing, China October 12—15, 2004
The review talk is based on the talks given at ICHEP’04 by Anders Ryd, Ian Shipsey, Gang Rong
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OutlineIntroduction
ψ(3770) resonance parameters
production at 3.773 GeVDDResult from BES-IIResult from CLEO-c
What indicate the new measurements ?
Summary
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Introduction Puzzle of ψ(3770)production and decays
Puzzle of ψ(3770) decay
It has long been a puzzle that the measured DD-bar cross section fail to fit the measured cross section for ψ(3770) production at 3.770 GeV in e+e- experiments.
nb 8.16.11))3770((122
)3770()3770( ±=→×= −+eeBF
Mprd ψπσ
ψψ
MeV 5.29.3769)3770( ±=ψM 51012.1))3770(( −−+ ×=→ eeBF ψMass and branching fraction (PDG02):
ψ(3770) production cross section at peak
For example:
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DD-bar cross sectionMARK-III measured the observed DD-bar cross section (at Ecm = 3.768 GeV)
nb 0.50.5)( ±=→−+ DDeeobsσproduction cross section
(Added all errors in quadrature)
70.0=ISRf
nb 7.01.7)( ±=→−+ DDeeprdσ
Potentail Models predict that ψ(3770) decay into DD-bar with branching fraction of  ̄100%.
Non-saturate decay ?
About 39% of ψ(3770) does not decay to DD-bar ?
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Are there non-DD-bar decay ?Theoretical prediction
There are theoretical arguments about ψ(3770) decays
Lipkin pointed out that ψ(3770) could decay to non-DD-bar final states with large branching fraction
)155PRD41(1990 Kuang, Y.P. keV, 200) /)3770(( <→Γ ππψψ J
Rosner) L. J. ,ph/0405196-(hep keV 620 ) )3770(( ≤→Γ cJχγψ
keV, 170) /)3770((37 <→Γ< ππψψ J (Y.P. Kuang, PRD65, (2002) 094024)
(1991)11 PLB267keV 160)( 13 =→Γ gggD
keV 950))3770(( ≤−→Γ DDnonψ
4.0%))3770(( ≤−→ DDnonBF ψ Added all above numbers up !
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Are there non-DD-bar decay ?About 35% of ψ(3770) missing ?
If all measurements are all right, these mean that 35%of ψ(3770) is missing
Lipkin proposed a rescattering model many years agoPL B179,278(1986)
Very recently Jonathan L. Rosner proposed a new model ---re-annihilation model to deal with that decays to charmless final states
ψ(3770)
arXiv:hep-ph/0405196 v2
To clarify this situation, it is important to more precisely measure both DD-bar cross section and ψ(3770) resonance parameters at same experiment simultaneously !
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The Beijing Electron Positron Collider(BEPC)
L ~ 1 ×1031 /cm2⋅s at ψ(3770) peak Ecm~2-5 GeV
One of the two e+e- machines in the world in the τ-charm energy region
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BESII Detector
VC: σxy = 100 µm TOF: σT = 180 ps µ counter: σrφ= 3 cm MDC: σxy = 220 µm BSC: ∆E/√E= 22 % σz = 5.5 cm
σdE/dx= 8.5 % σφ = 7.9 mr B field: 0.4 T∆p/p=1.7%√(1+p2) σz = 3.1 cm
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Muon identification can be done for the charged track with momentum of great than 0.52 GeV/c
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BES-II ψ(3770) data sample
~18 pb-1 of data taken at 3.773 GeV~7 pb-1 of data taken at the region from 3.768 GeV to 3.778 GeV
~8 pb-1 of data taken in the energy region from 3.665 to 3.878 GeV
about 33 pb-1 of data collected around 3.773 GeV in total.
CLEO-c ψ(3770) data sample
about 57 pb-1 of data taken at (around) 3.773 GeV
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World ψ(3770) Samples (pb-1)
Largest sample from CLEO-c by Spring, 2004
0
10
20
30
40
50
60
MARK-I DELCO MARK-II MARK-III BES-II CLEO-c
ψ(3770)
Energy [GeV] Lum [pb^-1] Exp. Note
3.60 –3.89 ~2 MARK-I parameters3.60 –3.89 ~2 DELCO parameters3.60 –3.89 ~2 MARK-IIparameters
3.768 9.6 MARK-III D decays
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ψ(3770) Resonance ParametersCross section scan experiment
The data were collected at 49 energy points from 3.66 to 3.89 GeV, which begin from off-resonance, cover ψ(2S), ψ(3770) and stop at DD* threshold .
Separated beam collision data at 3 energy points were collected to study beam associated background.
Some J/ψ, ψ(2S) data were also taken to calibrate BEPC energy and determine εtrg
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Integrated luminosities
Luminosities were measured by using large angleBhabha scattering
About 5.4 pb-1 of data were collected for the experiment
Monte Carlo
Developed a inclusive hadronic event generator with high order ISR corrections to simulate thehadronic event productions (including Lorentzboost due to initial state photon emission) in the full energy region
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ρ ωϕ
ψ/J'ψ
)3770(ψ
GeV 78.3energy c.m. Nominal =s
Monte Carlo productionhadronsee →−+
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Events Recorded by BESII
Primarycosmic rayNπ0
e+e-e+e-
µ+
νµ
π+µ-
e+
e-e-τ-
e+ µ+ τ+
e- e-
e+ e+
e+
e- γ
γ
Nhad
e- e-
e+ e+
l+l-
Primarycosmic rayNπ0
e+e-e+e-
µ+
νµ
π+
-e
e+
q-
q
Cosmic-ray and beam associated background
physics background could be estimated based on cross sections, luminosities and acceptances
bN
bN
bNhadn +)1( δ+= hadNhadn
Distributions of the vertex of events
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Hadron efficiency vs C.M. energy
[GeV] cmE
trgcmhadcm
hadcm
obshad EEL
nEεε
σ )( )(
)( =
∫ −=1
0
exp ))1(( ),( )( xssxfdxs Becthad σσ
)()()(12
)( 2222 sMMss
stot
feeB
Γ+−
ΓΓ=
πσ
(Kuraev and Fadin)
functionsampling issxf ),(
hadεObserved cross section
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'ψ
ψ/J
ψ(3770) productionTo get right resonance parameters, the two resonance productions and decays should be considered simultaneously. In this way the “correct” QED background ( )can be determined correctly !
udsR
quarks) s and du, (from QED
'ψ
)3770(ψ
)3770(ψ
BES-II Preliminary ![GeV] cmE [GeV] cmE
obshadσ obs
hadσ
0.142.24 ±=udsR
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Comparison of ψ(3770) Resonance Parameters
(preliminary !)BES-II
PDG02
MARK-II
DELCO
MARK-I
Experiment (MeV) Γ tot (eV) Γee
63772 ±
63770 ±
2.53769.9 ±
1.33772.8±
528±
524±
90370±
60180±
50276±
40260±
36225 ±
388±
286±
280±
(MeV) M∆
2.483.9 ±
524±
2.723.6±
53764 ±
4.025.5± 1.386.8±
(MeV) )3770(ψM
nb 99.011.9| MeV 8.3772)3770( ±==s
prdψσ
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Comparison of ψ(2s) Resonance Parameters
PDG2002
BES-II published(PLB550(2002)24)
This measurement(preliminary !)
experiment (keV) 'tot
ψΓ (keV) '
eeψ
Γ(MeV) M 'ψ
2860275 ±±
27264±
25300±
02.012.025.2 ±±3.01.07.3685 ±±
..AN 21.044.2 ±
09.096.3685 ± 15.019.2 ±
Using a constant for vacuum polarization correction
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DD-bar Cross Section at 3.773 GeV1pb 3.17 −=LBES-II: of data
@ 3.773 GeV
Using Kinematical fit method to improve momentum resolution and select the singly tagged D meson
D+
K-π+π+
Dtag
Single tag analysis e+ e-
D D-
−Xεσ
2 BrLN
tagDobsDD = From Monte
Carlo Xfit M=MRequiring
PDG02 Br
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+−→ πKD 0
−++−→ πππKD0
++−+ → ππKD
Observed cross sections for DD-bar production at 3.773 GeV
nb 0.310.093.58 00 ±±=obsDD
σ
nb 0.260.082.56 ±±=−+obs
DDσ
nb 0.500.126.14 ±±=obsDDσ
Preliminary !
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Radiative correctionAssuming that decay exclusively intoψ(3770) DD
2/41
0|))1((1|))1(( ),( )(
2−−
−Π−−= ∫ xsxssxfdxssM Bobs
DD
D σσ
024.0047.1)1(|))1((1| 2 ±=+=−Π− −vpxs δ PR D62
(2000)012002-1
)()()(12
)( 2222 sMMss
stot
feeB
Γ+−
ΓΓ=
πσ
B
obs
gσσ
=Initial State Radiation correction factor
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GeV 773.3At =s
MeV2.53769.9M ±=
MeV2.723.6" ±=Γtotψ
eV 40260" ±=Γeeψ
036.0779.0 ±== Tree
obs
gσσ
Obtained based on PDG02 ψ(3770) resonance parameters:
Radiative correction factor
Due to the uncertainties in resonance parameters and vaccum polarization )1( vpδ+
nb 0.370.103.29 ±±=−+tree
DDσ
nb 0.740.157.88 ±±=treeDDσ
nb 0.450.124.60 00 ±±=treeDD
σ
GeV 773.3@ =s
preliminary
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and
12.002.029.1 ±±==−+−+ → µµ
σσ
ee
treeDD
DDR
R
The contribution to R in the charm threshold region from the light quarks is estimated to be , which is obtained by fitting to the R values from 2.0 to 3.0 GeV measured by BES-II. The theoretical expectation is that is approximately independent of center of mass energy in this region.
14.026.2 ±=udsR
udsR
18.002.055.3 ±±=R
R DDR
The open square is charm counting method of R measurementAssuming that decays
exclusively into DD-bar
GeV) 3.773(at nb 709.6(GeV)
nb 8.8622 ==−+−+ →
cmee Eµµ
σ
Squares are the BES-II direct R measurements by counting inclusive hadronic events
(preliminary !)
ψ(3770)
0.142.24 ±=udsR which is obtained in measurement of ψ(3770) resonance parameters
udsDD RRR += udsDD RRR +=or
DDR
yielding
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1pb 2.57 −=L
DD-bar Cross Section at 3.773 GeVCLEO-c: of data @ 3.773 GeVUsing ‘double tag’ method, pioneered by MARK-III
Near DD-bar production threshold region
DK-π+tag
D+
π+
D D-
−X Doubly tagged D
e+ e- e-
DK-
tag
D0
π+
Singly tagged D sample
D D0
0X
e+
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44780)(
00 =DD
N
17360)(
=−+ DDN
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DDiii NBN ε2=2
2
4 i
ii
ii
iDD N
NNεε
=DDiiiii NBN 2ε=
510)03.004.098.1(00 ×±±=DD
N510)04.006.048.1( ×±±=−+DD
N
nb )150070473(00 ...obsDD
±±=σ
nb )110110592( ...obsDD
±±=−+σ
nb )22013006.6( ..obsDD ±±=σ
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What indicate the new measurements ?What information can we obtain from the new measurements at BES-II and CLEO-c ?
Based on the measured DD-bar cross sections from BES-II & CLEO-c, we obtain the averaged DD-bar cross section
nb )150493(00 ..obs
DD±=σ
nb )140582( ..obsDD
±=−+σnb )23008.6( .obs
DD ±=σ
averaged cross sections
Using the new ψ(3770) resonance parameters measured by BES-II, we obtain the ISR correction factor at 3.773 GeV
76.0=g
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Tree level cross sections
nb )200594(00 ..tree
DD±=σ
nb )180393( ..treeDD
±=−+σnb )30099.7( .tree
DD ±=σ
averaged cross sections from BES-IIand CLEO-c
From BES-II preliminary result of
nb 99.011.9| MeV 8.3772)3770( ±==s
prdψσ
We can obtain the tree level cross section for ψ(3770)production to be
nb )95.070.8()37770(
±=treeψσσ
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ψ(3770)Branching fractions of decays
Using the BES-II & CLEO-c preliminary results on and presented at ICHEP’04, we can obtain
DDσ)3770(ψ
σ
Branching fraction [%]
00(3770) DD→ψ 6.252.8 ±
−+→ DD(3770)ψ 4.739.0 ±
10.691.8 ±DD→(3770)ψ
10.68.2 ±DDnon −→(3770)ψ
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SUMMARYBES measured ψ(3770) resonance parameters .
PDG02
BES-II
Experiment (MeV) M )3770(ψ (MeV) Γ tot (eV) Γee
2.53769.9 ±
1.33772.8±
40260±
36225 ±
(MeV) M∆
2.723.6±
4.025.5± 1.386.9±(preliminary !)
2.483.9 ±
nb 0.999.11 )3770( ±=prdψσ (BES-II preliminary !)
0.142.24±=udsR From 3.66 to 3.87 GeV
BES measured the DD-bar Cross Section at 3.773 GeVto be.
( ISR based on PDG02 )nb 0.740.157.88 ±±=treeDDσ (BES-II preliminary !)
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SUMMARYMeasured the Observed cross section at 3.773 GeV .
CLEO-cBES-IIobs
DD00σ
obsDD −+σ
nb )31.009.058.3( ±±
nb )26.008.056.2( ±±
nb )50.012.014.6( ±±
nb )150070473( ... ±±
nb )110110592( ... ±±
nb )22013006.6( .. ±±
(preliminary !) (preliminary !)
Both the BES-II and the CLEO-c results were reported at ICHEP’04 as well
obsDDσ
.What is the non-DD-bar branching fraction of ψ(3770)
It is reduced to about from using the new measurements at BES-II and CLEO-c
)%118( ± %39
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谢 谢!
Thank You!