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Hadron Spectroscopy at BABARBY
Usha Mallik (University of Iowa)
Representing
The BaBar Collaboration
The International Light-Cone WorkshopJuly 7, 2005
Cairns, Australia
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Topics:
Hadron Spectroscopy:– Ds (cs) States : Inclusive and Exclusive studies
– Double Charmonium Production; the X and the Y
– Pentaquarks– Charmed Baryon studies
Summary What can we learn from each other ?
3Plan to Double Dataset by Next Summer
The BABAR Detector at PEP-II and the Dataset
BBSee )4(
Ecm = 10.58 GeV
And Much More
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DSJ (cs) Spectroscopy
New States DSJ(2317)+ and DSJ(2460)+ – First Observed Inclusively in e+e- Collisions
Previously Established States with Likely JPC
DS (2112)+ 1-(+) S-Wave (c and s spins aligned)
Ds also DS 0
DS(2536)+ 1+(+) P-Wave (needs
confirmation)D*(2010)+K0
D*(2007)0K+
DS(2573)+ 2+(+) D-Wave (consistent
with)D0K+
Ground State DS(1969)+: JP=0-, c and s spins opposite, in S-
wave
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B(DsJ (2460) Ds
0)
B(DsJ (2460) Ds
* 0) 0.21 (90% CL)
Belle 87 fb-1
B(DsJ (2460) Ds
0)
B(DsJ (2460) Ds
0) 0.11 (95% CL)
BaBar 125 fb-1
Discovery
Ds* Ds
Discovery of DsJ Statese+e- cc DsJ + X
DsJ(2317)+ Ds+0 DsJ(2460)+ Ds
*+0
M(2460) – M(2112)
BABAR, BELLE, CLEO mutually confirm, also CDF (2317)
Caution: These Decays cross-feed
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• Decays violate isospin: mixing
• Look for radiative and dipion transitions
• If is , expect is forbidden
is forbidden
• If is , expect is allowed
is allowed
0 0
DsJ*(2317)
DsJ*(2317) Ds
0
DsJ*(2317) Ds
DsJ (2460) Ds
DsJ* (2460)
DsJ (2460) Ds
1
...3,2,1,0)2317( 0* PssJ JDD
1 )2460( 0* PssJ JwaveSDD
2,1,0PJwaveP(also D-Wave)
(for a conventional meson)
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DsJ(2460): 0± excluded
Search for DsJ→Ds
DsJ (2460)
B(DsJ (2460) Ds)
B(DsJ (2460) Ds 0)
0.3750.0540.057
B(DsJ (2317) Ds)
B(DsJ (2317) Ds 0)
0.17 (95% CL)
BaBar 125 fb-1
Excludes 0± if present
DsJ(2317): compatiblewith 0+
BABAR: PRD 69 (2004) 031101 (R) ; BELLE : PRL 92 (2004) 012002
BABAR
B(DsJ (2460) Ds)
B(DsJ (2460) Ds* 0)
0.550.130.08
B(DsJ (2317) Ds)
B(DsJ (2317) Ds 0)
0.05 (90% CL)
Belle 87 fb-1
)2317( No sJD
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DsJ(2460) → Ds0Kinematics
DsJ* (2317)reflection
Ds*
reflection
DsJ (2460)
high Ds* sideband
low Ds* sideband
DsJ(2460)
hep-ex/0408067
BABAR
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BELLE: PRL 91 (2003)262002
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Exclusive Production of D*SJ in B ->DSJ
(*)+ D(*)
Kinematic Constraints Help, Even though Lower Stats
Reduces Backgrounds
Measure Ratios of Branching Fractions
Measure Br
Well-defined Initial State
Test DSJ(*) Spin Assignments
Reconstruct one B: other is a B for Study
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B DsJ (*)+ D(*)
2*4/ BES psm
BABAR: PRL 93 (2004) 181801Data sample: 122 million B pairs
DDsJsJ**(2317)(2317)++
DDss00
DDsJsJ(2460(2460))++
DDss**00
DDsJsJ(2460(2460))++
DDss
mmESES mm((DDsJsJ)
Full reconstruction of the exclusive decay
Sum over charged and neutral B’s 112 ± 14 events
139 ± 17events
020.0045.0274.0
))2460(.(.
))2460(.(.0*
sDDFB
DDFB
sJ
ssJ
We measure:
2/* sEE B
mmESES mm((DDsJsJ)BABAR
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B DsJ (*)+D* Results
B.F. (10-3) DsJ*(2317)+ Ds0 DsJ(2460)+ Ds*0 DsJ(2460)+ Ds
B0 1.5 ± 0.4 ± 0.2(+0.5-0.3) 5.5 ± 1.2 ± 1.0(+1.9-1.2) 2.3 ± 0.3 ± 0.3(+0.8-0.5)
B+ 0.9 ± 0.6 ± 0.2(+0.3-0.2) 7.6 ± 1.7 ± 1.8(+2.6-1.6) 1.4 ± 0.4 ± 0.3(+0.5-0.3)
B.F. Productsfor BDsJ
(*)+D*
m(Ds+0) m(Ds
*+0) m(Ds)B0 B0 B0
B+B+ B+
DsJ(2317)DsJ(2460) DsJ(2460)
BABAR
BELLE: PRL 91 (2003) 262002 Data sample: ~124 million B pairs
in agreement with Belle results
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B DsJ (*)+D Results
B.F. (10-3) DsJ*(2317)+ Ds0 DsJ(2460)+ Ds*0 DsJ(2460)+ Ds
B0 1.8 ± 0.4 ± 0.3(+0.6-0.4) 2.8 ± 0.8 ± 0.5(+1.0-0.6)
0.8 ± 0.2 ± 0.1(+0.3-0.2)
B+ 1.0 ± 0.3 ± 0.1(+0.4-0.2) 2.7 ± 0.7 ± 0.5(+0.9-0.6)
0.6 ± 0.2 ± 0.1(+0.2-0.1)
B.F. Productsfor BDsJ
(*)+D
in agreement with Belle results
m(Ds+0) m(Ds
*+0) m(Ds)
B0 B0 B0
B+ B+ B+
DsJ(2460) DsJ(2460)DsJ(2317)
BABAR
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• Two body decay BDDSJ forces DSJ to populate helicity zero only
• Analyze angular distribution (cos h) of daughter of DSJ
• BELLE Finds from Angular Distribution – DSJ(2317)* J = 0 (Preliminary)
hB DsJ
D
0
Ds(*)
–
Spin Analysis of B DDSJ*
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BDsJ(2460)+D
DsJ+
(2460)
Ds
h
J=1 (2=4.0/4) preferred to J=2 (2=36.4/4)
Data points from m(Ds fits corrected for detector acceptance and efficiency
J=2J=1
confirms Belle measurement
BABAR
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e.g. Godfrey-Isgur model
S-wave P-wave
Ds+
Ds*+
Ds1(2536)+
DsJ (2573)+
Ds0(2317)
Ds1(2460)
DsJ*(2317)+, DsJ (2460)+
– Observed by BaBar, Belle and CLEO – Unexpectedly below threshold for DK and D*K, respectively – Consistent with P-wave cs states but other interpretations not ruled out– If cs, observed decays
• DsJ*(2317)+ Ds
+
• DsJ (2460)+ Ds*+
are isospin violating narrow
– DsJ (2460)+ Ds+
also observed (and used to
determine J)
Taking Stock of cs States
Several other explanations exist e.g. Molecules or Hybrids
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New Charmonium-like States
X(3872) J/π+π-
Average Mass 3871.9 ± 0.5 MeV
Narrow < 2.3 MeV @ 90% CL
(D0D*0 threshold at 3871.3 ± 1.0)
CDFPRL 93 072201 (2004)
BELLE PRL 92 262001 (2003)
BABARhep-ex/0406022
D0PRL 93 162002 (2004)
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B+ X(3872)0K+ Reconstruction
Recent Update:
BELLE (256 fb -1) hep-ex/0505038, BABAR hep-ex in preparation
Background from B decays to same final state J/K
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About X(3872)
• Search for a Charged Partner
From 212 fb -1 Data BABAR Observed No Signal for X-
Phys. Rev. D71 : 031501, 2005
B(B0 X-K+, X- J/ π-π0) < 5.4 X 10 -6 @ 90% CLB(B- X-KS, X- J/ π-π0) < 11 X 10 -6 @ 90% CL
• Charmonium State : no isospin partner expected (data)
• Molecule State (?) : highly suppressed B0 X(3872) predicted
• Diquark-antidiquark State : different masses of X(3872)
in B0 and B+ decays predicted, |M| > 5 MeV
E. Braten, M. Kusunoki hep-ph/0412268
L. Maiani, F. Piccini, A.D. Polosa, V. Riquer PRD 71(2005) 014028
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B0 X(3872)0KS Reconstruction
Background
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Other searches for X(3872)
Search for X(3872) in events with initial state radiation (if JPC = 1-- )
Search for X(3872) in B X(3872)K in the spectrum recoiling against K from the B decays (with the other B fully reconstructed):
B(X(3872) in B X(3872)K, X(3872) J/) < 3.2 X 10 -4 at 90% CL and so, BF(X(3872) J/+-) 4.3 %
mes of all the exclusively reconstructed B
mES : B mass using beam energy
Use BABAR-BELLE average BF(B+ X(3872)K+, X(3872)J/) = (13.2 2.2) x 10 -
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PRD 71 (2005) 052001
BABAR
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BELLE: 256 fb -14.0
C= +1 favored
hep-ex/0505037
X(3872) : +- Invariant Mass Distribution
BELLE: hep-ex/0505038BABAR: hep-ex in prep.
Di-pion mass consistent with 0+- , again C =+1 ; S-wave J/ favored: J++ favored over J-+
Isospin violating: predicted
D0D*0 molecule, Swanson PLB 588 (2004) 189, Törnqvist PLB 590 (2004) 209
Also X(3872) π+π-π0J/
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X(3872): BELLE Finds Data Disfavors 0++ and 2++, Leaving 1++
cc ? 1++ is c1’
X(3872) is too light
M[Ge
DDThreshold
3872
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}C=+1 }C=-1
c , c , c(2S)J/, (2S)
G. T. Bodwin, E. Braaten & J. Lee
PRD67, 054023 (2003)
Study double charmonium in e+e- annihilation
Double Charmonium Production
Theorists predict the cross sections of the two processes to be comparable
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Reconstruct J/ or (2S) and Look at Recoil MassBABAR: 124 fb -1, hep-ex/0506062
c
c(2S)
c0
BELLE: PRD 70 (2004) 071102
BABAR
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Double Charmonium Production from BELLE
From BELLE
Evidence of X(3940): 4.5
m = 3940 ± 12 MeV, < 96 MeV at 90% CL
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8 : 253 fb -1 with 59 ±11 Events
A Near-threshold J/ Mass Enhancement in B KJ/ at 3940 MeV/c2
BELLE: Phys. Rev. Lett. 94: 182002, 2005
Dominantly cc
BELLE
Is it the same as X(3940) ?
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A Broad Structure in J/π+π- Mass near 4.26 GeVe+e- ISRJ/+- in Initial State Radiation
BABAR: 211 fb-1 (preliminary)
(2S)125±23 excess events
Recoil Mass Consistent with zero
hep-ex/0506081, submitted to PRL
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•In addition to (2S) a Broad Structure is Observed in ISR Events
•JPC = 1-- ; Can be Characterized by a single Resonance at 4.26 GeV and Width ~ 0.09 GeV
•Too low Statistics to Discern if Multiple States together - (e.g. S and D waves can mix)
+ - mass distribution from Y(4260)
Y(4260) J/ S-wave phase space
Why no rise in R ?
4.26
D*D* threshold
3.77
BES, PRL 88 (2003), 101802
BABAR
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Pentaquark searchesPentaquark discovery in 2003, ( confirmed by 13 experiments)
(statistical significance of individual experiments is not high ~5-6 )Also many negative searches reported, especially a recent high statistics study by CLAS
Claims of exotic narrow baryons
LEPS, CLAS, …:
M=(1542±5)MeV/c2
<21MeV/c2
NA49:
M=(1862±2)MeV/c2
<18MeV/c2
H1:
M=(3099±6)MeV/c2
<28MeV/c2
S
I3
5(1540)+ [uudds]
5(1860)[ddssu]
5c(3100)[uuddc]
The anti-decuplet for Pentaquarks
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Inclusive and Exclusive Searches at BABAR
5+, 5
--, 50, 5c
0
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accepted by PRL
e+e- annihilation (~123 fb -1)hep-ex/0502004
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accepted by PRL
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Upper Limit
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No Signal Observed by CLAS in this Mode with ~40 times Statistics , now repeating other modes
BABAR studies electro- and hadro-production in interactions with the
material of the inner detector ; Observes no signal
•So far, evidence of 5 claimed in— real/virtual photoproduction— hadroproduction
• photoproduction
36Detector Tomography with pKS0 vertices
230 fb -1BABAR
e- e+
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pKs mass distribution
Mass resolution ~2 MeV
Clear Ks from Decays Selected
Protons Selected from Particle ID
BABAR
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Associate p Ks Vertex with ± and K±
BABAR
(1115)
39No Pentaquark Observed by BABARBABAR
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Charmed Baryon Studies
Precision Mass Measurement of C+ (cud)
Production Process and Ratio of Branching Fractions of C0 (csd)
cc or B C0 + X
Production Process and Ratio of Branching Fractions of C0 (css)
cc or B C0 + X C
0 - +
- + - +
-K- + +
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Mass Measurement of C
+
Using Low-Q-value Decay Modes of C+ KSK+ and C
+ 0KSK+
m(C+ KsK+ ) = 2286.501 ± 0.042 (stat.) ± 0.144 (sys.) MeV/c2
m(C+ 0KsK+ ) = 2286.303 ± 0.181 (stat.) ± 0.126 (sys.) MeV/c2
BABAR Result : m(C+ ) = 2286.46 ± 0.14 MeV/c2
PDG Value 2284.9 ± 0.6 MeV/c2
Cross-checks:
m(C+ pK+ ) = 2286.39 ± 0.12 (stat.) ± 0.45 (sys.) MeV/c2
m(C+ pKs) = 2286.36 ± 0.03 (stat.) ± 0.43 (sys.) MeV/c2
m() = 1115.68 ± 0.01 (stat.) ± 0.04 (sys.) MeV/c2 PDG Value = 1115.683 ± 0.006 MeV/c2 m(KS) = 497.56 ± 0.04 (stat.) ± 0.26 (sys.) MeV/c2 PDG Value = 497.648 ± 0.022 MeV/c2
BABAR
hep-ex/0507009, submitted to PRD
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116 fb -1
c0-π+
c0-K+
B(c0-K+)
B(c0-π+)
= 0.294 ± 0.018 ± 0.016
Goals: Measure Ratio of Decay BFs
: Study Production MechanismBABAR
hep-ex/0504014, submitted to PRL
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Study c0 Momentum (p*) in e+e- rest frame
c0 from B Decays
c0 peak from B’s absent in off-peak
B (B c0X) •B (c
0 -+) = 2.11 ± 0.19(stat.) ± 0.25(syst.) X 10 -
4
c0-π+
(e+e- C0X) •B (c
0 -+) = 388 ± 39(stat.) ± 41(syst.) fb
Results:
Efficiency Corrected
BABAR
116 fb -1
hep-ex/0504014, submitted to PRL
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Inclusive c0 Studies
Branching Fractions and Production Mechanism from p* Spectrum
Decay Modes of C0 Studied -+, -+- +, and -K- + +
C0-+
P* > 2.8 GeV/c
225 fb -1
Results:
BABAR
SLAC-PUB-11323, hep-ex/0507011
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The p* Spectrum from -π+ Mode
Off-peak onlyOn & Off-peak
Not Corrected for Efficiency
B C0 Production (First Observation)
Analysis in Progress
BABAR
SLAC-PUB-11323 hep-ex/0507011
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Summary & Conclusion
Unfolding cs spectroscopy
New States X(3872), Y(3940)… and Y(4260)?
Copious Double Charmonium Production
Pentaquark Fading ?
Exciting Charmed Baryon Spectroscopy
What can we Provide ?
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Kaon momentum spectrum
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Kinematics
DsJ* (2317)
Ds*
reflection
DsJ* (2317)
DsJ (2460) Ds*(Ds
) 0
DsJ* (2317)
reflection
• Mutual cross feed
•widths are consistentwith zero
• No evidence for
DsJ* (2317) DsJ (2460)
DsJ* (2317)
DsJ* (2317) and DsJ (2460)
DsJ (2460) Ds
0
B(DsJ (2460) Ds
0)
B(DsJ (2460) Ds
* 0) 0.21 (90% CL)
B(DsJ (2460) Ds
0)
B(DsJ (2460) Ds
0) 0.11 (95% CL)
Belle 87 fb-1
BaBar 125 fb-1
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DsJ(2460): 0± excluded
Search for DsJ→Ds
DsJ (2460)
B(DsJ (2460) Ds)
B(DsJ (2460) Ds 0)
0.3750.0540.057
B(DsJ (2317) Ds)
B(DsJ (2317) Ds 0)
0.17 (95% CL)
BaBar 125 fb-1
B(DsJ (2460) Ds)
B(DsJ (2460) Ds* 0)
0.550.130.08
B(DsJ (2317) Ds)
B(DsJ (2317) Ds 0)
0.05 (90% CL)
Belle 87 fb-1
Excludes 0± if present
DsJ(2317): compatiblewith 0+
BABAR: PRD 69 (2004) 031101 (R) ; BELLE : PRL 92 (2004) 012002
BABAR
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Search in Inclusive B XK Reconstruction
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Branching fractions from b xk study
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Ds+Results
• D* and selection analogous to inclusive analysis• Ds
+(K+K)fully reconstructed• measure branching fraction product:
Signal 212 ±19
2*4/ BES psm Dividing by our measurement of
B(B0 Ds*+D*-), we obtain
B(Ds++) = (3.6 ± 0.9)% (CLEO)
to be compared with
Readjustment of many results needed!Not used yet for other results in this talk
B (B0 Ds*+ D*) x B (Ds
++) = (8.71 0.78(stat)) x10-4
B(Ds++) = (4.71 ± 0.47(stat) ±0.35(syst))%
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Electroproduction in e-Be
BABAR