brian lang university of minnesota on behalf of the cleo collaboration charm 2007
DESCRIPTION
Charm – Production in e + e - Annihilation around 4 GeV. Brian Lang University of Minnesota on behalf of the CLEO Collaboration Charm 2007 Cornell University, August 5 th -8 th 2007. Region of Interest. The region which is being investigated. Fit to Continuum. - PowerPoint PPT PresentationTRANSCRIPT
Brian LangUniversity of Minnesota
on behalf of the CLEO Collaboration
Charm 2007
Cornell University, August 5th-8th 2007
Charm – Production in e+e-
Annihilation around 4 GeV
08/05/07- Charm 2007 Brian Lang University of Minnesota and the CLEO Collaboration
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Cross section as a function of Ecm from the 2005 PDG
Fit to Continuum
The region which is beinginvestigated.
Region of Interest
08/05/07- Charm 2007 Brian Lang University of Minnesota and the CLEO Collaboration
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Why investigate this region: The cross sections to DD, D*D, and D*D* are not well known
at the energies of interest.
The only previous measurements of Ds yields in this region: BES measured the production cross section times branching ratio
to at 4030 MeV as 11.2 pb, due to DsDs. Mark III measured the production cross section times branching
ratio to at 4140 MeV as 26 pb, production is largely DsDs*.
Optimal Ecm for Ds decay physics: balance of total production against event complexity.
Test of theoretical predictions from Eichten et al in 1980 Phys. Rev. D21 203
Coupling of open charm channels to cc states
08/05/07- Charm 2007 Brian Lang University of Minnesota and the CLEO Collaboration
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Data Sample from CLEO Scan Using the scan data which was collected between Aug. and Oct.
of 2005.
At each energy the data sample was sufficient to determine the cross sections for all expected charm states.
Total integrated Luminosity
Scan (12 energy points) ~ 60 pb-1
4170 MeV ~ 180 pb-1
08/05/07- Charm 2007 Brian Lang University of Minnesota and the CLEO Collaboration
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Cross Sections
Do not reconstruct D* since the momentum, in terms of Mbc, indicates event type
2||2Dp
beamE
bcM
beamD EEE MbcMD and E0 for DD
MC Simulation ECM=4160 MeV
08/05/07- Charm 2007 Brian Lang University of Minnesota and the CLEO Collaboration
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Multi-Body Production There is no reason why, for example, there can not exist multi-body
events like e+e-DD*or any other allowed combination of D-mesons and pions.
First, are there events outside our two-body D(s)(*)D(s)
(*) exclusive event categories? Yes!
■ Assuming only two body kinematics, NO D0 mesons with a momenta below ~350 MeV.
■ Data shows a clear D0 peak in the mass distribution for K- candidates with momenta below 250 MeV.
Ecm=4170 MeV
PD < 250 MeV
PRELIMINARY
08/05/07- Charm 2007 Brian Lang University of Minnesota and the CLEO Collaboration
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Momentum Spectrum of D0 at 4170 MeV
D0D*D*
D*D
DD
■ D0K- momentum spectrum after sideband subtraction
What populates this region?
PRELIMINARY
08/05/07- Charm 2007 Brian Lang University of Minnesota and the CLEO Collaboration
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Multi-Body Production
22)( * MMPPPDEvent
e-
X
D
D+*
e+
Ecm = 4170 MeV
e-
X
D0
e+
22)( MMPPP DEvent
Combining a D and a
Combining a D* and a
PD < 250 MeV
PD* < 400 MeV
PRELIMINARY
08/05/07- Charm 2007 Brian Lang University of Minnesota and the CLEO Collaboration
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Multi-Body Production
e-
D0*
X
D
D0*
e+
Ecm = 4260 MeV
22)( * MMPPPDEvent
PD* < 400 MeV
Combining a D* and a
PRELIMINARY
08/05/07- Charm 2007 Brian Lang University of Minnesota and the CLEO Collaboration
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How do we get a handle on the multi-body contribution?
It is possible to estimate the contribution of multibody events by fitting the observed D momentum spectrum with MC predictions for the two-body processes and some
representation of multi-body.
Momentum Fits using MC
08/05/07- Charm 2007 Brian Lang University of Minnesota and the CLEO Collaboration
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Momentum Fits using MC
Only assuming D*Dmulti-bodyis present.
D*D*
D*D
DD
D*D*
D*D
DD
D*D
D0K-Momentum Spectrum after sideband subtraction
D*D
D+K-Momentum Spectrum after sideband subtraction
Ecm = 4170 MeV~ 180 pb-1
D0 D+
PRELIMINARY
08/05/07- Charm 2007 Brian Lang University of Minnesota and the CLEO Collaboration
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Exclusive Cross Section Results
PRELIMINARY
No theoretical predictions for multi-body.
No evidence of DD in this region
08/05/07- Charm 2007 Brian Lang University of Minnesota and the CLEO Collaboration
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Check of the Total Charm Cross Section One can perform an inclusive measurement as a
cross check on the total charm cross section. The invariant mass used to extract the yields.
Only using D0K-, D+K-and the high yield mode of Ds
+K+K-.
Also, one can count the number of hadronic events above the uds continuum background as an additional check to the total charm cross section.
08/05/07- Charm 2007 Brian Lang University of Minnesota and the CLEO Collaboration
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Comparison: Exclusive from Momentum Fits vs. Inclusive
Exclusive: Sum of the two-body charmed mesons and multi-body
■ Inclusive charm: D0 + D+ + Ds
Inclusive Hadrons: Excess over uds
Includes multi-body
PRELIMINARY
08/05/07- Charm 2007 Brian Lang University of Minnesota and the CLEO Collaboration
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R
Radiative Corrections In order to compare the
observed cross sections to theory and previous experiments the cross sections need to be corrected for the effects of initial-state radiation.
Using theoretical treatment of Kuraev and Fadin (Sov. J. Nucl. Phys. 41 466) and Crystal Ball R measurement
Ruds=2.29 0.03
R = Ruds+Rcharm
PRELIMINARY
08/05/07- Charm 2007 Brian Lang University of Minnesota and the CLEO Collaboration
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These inclusive measurements can be compared to other experiments by the cross section times branching ratio for D0K- and
D+K-.
Inclusive Cross SectionPRELIMINARY
CLEO-c
CLEO-c
08/05/07- Charm 2007 Brian Lang University of Minnesota and the CLEO Collaboration
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Comparison with Updated Eichten et al.
Most noticeable difference in D*D* channel. Still reasonable qualitative agreement.
E. Eichten, International Workshop on Heavy Quarkonium (BNL 2006) and personal communication
PRELIMINARY
08/05/07- Charm 2007 Brian Lang University of Minnesota and the CLEO Collaboration
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Near D*D* Threshold R is proportion to the cross section.
Fit assumes only a single resonance.
Introduction of another narrow resonance can explain the ‘dip’ in DD at 4015 MeV
DD DsDs
D*D
D*D*
Updating S. Dubynskiy and M.B. Voloshin’s results hep-ph/0608179
R1 R2
R3R4
PRELIMINARY
NO DD
08/05/07- Charm 2007 Brian Lang University of Minnesota and the CLEO Collaboration
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Comparison with the Belle Collaboration
D*D
D*D*
Ph
ys. R
ev. L
ett.
98,
092
001
(200
7)
D*+D*-
D*+D-
DD
P.Pakhlov, EPS-HEP 2007
DD
PR
EL
IMIN
AR
Y
08/05/07- Charm 2007 Brian Lang University of Minnesota and the CLEO Collaboration
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Conclusions Exclusive charm production above threshold
have been measure. DsDs) peaks at 4010 MeV
Ds*Ds) peaks at 4170 MeV and is used by CLEO-c for Ds
decay studies
Interesting absence of DD at 4015 MeV (possibly a new resonance?)
These studies will lead to a better understanding of QCD
08/05/07- Charm 2007 Brian Lang University of Minnesota and the CLEO Collaboration
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Backup Slides
08/05/07- Charm 2007 Brian Lang University of Minnesota and the CLEO Collaboration
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Momentum Fits to Data
Ds+ momentum spectrum
after sideband subtraction
Ecm = 4170 MeV~ 180 pb-1
08/05/07- Charm 2007 Brian Lang University of Minnesota and the CLEO Collaboration
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Comparison with the BaBar Collaboration
DD
08/05/07- Charm 2007 Brian Lang University of Minnesota and the CLEO Collaboration
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Theoretical Predictions Determined partial widths at two ECM
energies.
Partial widths in units of MeV
hep-ph/0412057