Research with Antiprotons - Hadron Spectroscopy and Hadronic Matter
Recent CLEO results on hadron spectroscopy
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Transcript of Recent CLEO results on hadron spectroscopy
Recent CLEO results on hadron spectroscopy
Tomasz SkwarnickiSyracuse University
Concentrate on the most recent results (mostly quarkonium spectroscopy).
Epiphany 2005, Krakow Tomasz Skwarnicki 2
Production of b-quark hadrons
SSS S,5S
s
Other states
b
b b
b
e
e
e
e
Soft g
Hard g
Long distance interactions
Short distance interactions
bb spectroscopy bq, (cq, cc) spectroscopy
W
3S ~ 24 keV
4S ~ 24 000 keV
s
c
q
Epiphany 2005, Krakow Tomasz Skwarnicki 3
• B physics runs ((4S)) at CLEO ended in mid 2001.
1
10
100
fb-1
/year
0.1
30.001
0.01
History of CLEO/CESR
(1S)(3S) (2S)
(3S) (2S)(1S)
BaBar
Belle
• CLEO-c phase 2003 – (2007)
CLEO-c
• Long runs at (5S) (3S), (2S),(1S) in 2001 – 2002.
(5S)
or #
of r
eson
ance
s
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CLEO-III data samples
• CLEO “owns” the field of spectroscopy
• Recently more than 10-fold increase in statistics for the narrow resonances over the previous generation of experiments
• Except for a few systematics limited measurements CLEO is no longer competitive in B physics
(1S)
(3S)
(2S)
(in millions of resonance decays)
(4S)
Continuum below (4S)
(in integrated luminosity fb-1)
• Large increase in statistics for 5S with much improved detector leads to a measurement of Bs production rate
(5S)
Epiphany 2005, Krakow Tomasz Skwarnicki 5
Superconducting CESR-cwiggler magnet (2.1 T)
Wigglers needed for low energy operations to increase radiation damping(to keep the size of the beams small)
e+e- collider
No.Of
rings
Instantaneous peak luminosity cm-2 s-1
Beauty Threshold Region
CESR(-b) 1 1.2 1033
PEP-II 2 9.2 1033
KEK-B 2 13.9 1033
Charm Threshold Region
SPEAR II 1 6 1029
BEPC 1 5 1030
CESR-c1 wiggler (fall 2002)
12 1031
6 wigglers (fall 2003) 5 1031
12 wigglers (fall 2004) projected
6 1031
Up to 3 1032
BEPC-II (2007) 2 1 1033
CESR-cCESR(-b)
CESR (single ring machine) PEP-II (double ring machine)
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CLEO-c data samples
• Proposed CLEO-c program:– 3 / 3 / 1 fb-1 at Ebeam=3770 / 4140 / 3100 MeV for DD / DsDs / J/– Would also like to take some(2S), c data and perform scan of R – Likely to be revised if CESR-c doesn’t reach its projected luminosity soon
• Advantages of threshold production of D(s) mesons:– Fully reconstruct one D(s) meson, then look at the other– No backgrounds (often limiting factor for D studies at B factories and fixed target
experiments)– Measurement of absolute branching fractions
~107 pb-1~6 pb-1We are continuingto run at (3770)
3640 3680 3720 3760 3800 3840
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CLEO-c data samples
• (2S) sample smaller (larger) than that of BES (Crystal Ball) with much better detector
(3770)
• (3770) sample much larger than those of Mark III and BES with much better detector
(2S)
(in millions of resonance decays)
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CLEO EM Calorimeter COIL (1.5T)
Detector Calorimetercrystals
E resolution at E=100 MeV
Number of inner segments (crystals)
Inner radius(cm)
CLEO-III CsI(Tl) 4.8 MeV 7800 100
CUSB-II BGO 4.2 MeV 72 8
Crystal Ball NaI(Tl) 4.8 MeV 672 25
BES-II Sampling 70 MeV
• Essential for photon spectroscopy– ~8000 CsI(Tl) crystals + photo-diodes– First crystal calorimeter in magnetic
field• In operation since 1990 (CLEO II)
Much better efficiencyin hadronic events
Narrower0 width
Epiphany 2005, Krakow Tomasz Skwarnicki 9
CLEO III Tracking• Large drift chamber in 1.5T field (lowered to 1.0T for
CLEO-c)
Stepped endplate toaccommodate newmicro- quadrupoles
Deconstruction of CLEO II DRCLEO III DR
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CLEO-c Inner Wire Chamber • CLEO-III Silicon Vertex Detector deteriorated due to radiation damage
and had to be replaced• “ZD Inner Chamber” commissioned Aug/Sep 2003 • The only new detector component of CLEO-c
6 stereo layers 53 to 105 mm radius
Detector Magnetic field
p /p resolution at p=1 GeV
dE/dXresolution
CLEO-c 1.0T 0.5% 6.0%
BES-II 0.4T 2.4% 8.5%
Mark-III 0.4T 2.1%
Tracking resolution
• Much improved momentum and dE/dX resolution compared to the previous charm-threshold experiments
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CLEO-III RICH• LiF – MWPC (Methane +
TEA) proximity focused RICH
RadiatorsLiF
PhotodetectorsMWPC
(Methane+TEA)
CLEO-c
B physics
Kaon efficiency = 0.80= 0.85= 0.90
First detector operating at charm threshold with excellent particle ID
In operation since 2000
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Measurement of fD
Calculate Missing-Massto separate
signal (MM=m=0)from backgrounds:
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Measurement of fD
D- KL -
D- -
8 events (1 background event expected)
Based on 6 wiggler data: 60 pb-1 (29k tagged events)
B(D- -) = (3.5±1.4±0.6) 10-4
fD- = (202±41±17) MeV
First statistically compelling evidence for this decay. (BES 2.7±1.7 events hep-ph/0400150)Need much larger statistics to constrain the theory (data taking in progress!)The same type of calculations used for fB needed for extraction of Vtd from B0B0 mixing
hep-ex/0411050 Accepted by PRD
Epiphany 2005, Krakow Tomasz Skwarnicki 14
D meson BRs
0.0380±0.0009
0.130±0.008
0.075±0.003
0.092±0.006
0.0141±0.0008
Using double-tag method (Preliminary)
PDG 2004
Future goal: reduce errors to 1-2% for the major modes
No surprises
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Heavy Quarkonia bb
S= 0 1 0 1 0 1 L= 0 1 2
?
cc
n 2S+1 L J
S= 0 1 0 1 0 1 0 1 L= 0 1 2 3
n=1
n=2
n=3
n=4
Hyperfine splitting: 1 2S S
Fine splitting:
1 2 1 2
,L S
S r S r S S
n=1
n=2
Hyperfine splitting
Fine splitting
J 1974
’’ 1974
c 1975
c 1980
c’’ 1982 hc
19861992
2002
1977
’’ 1977
’’’ 1979
b 1983
b’ 1982
2 2002’’’ 1977
’IV 1981
2004
CLEO-III
E835CLEO-c
Belle,BaBar,CLEO
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Fine and Hyperfine Structure
• nS states are special:– Have no fine structure (L=0 thus J=S)– The only states for which hyperfine structure is predicted to be significant– Observed in charmonium:
• M(J/) – M(c)= (116±2) MeV; M(’) – M(c’)= (48±4) MeV
• If long range spin-spin forces are negligible then for L>0:– MS=0 = M(c.o.g.) = J (2J+1) MJ
S=1 / J (2J+1)– M(hc)=(5 M(c2)+3 M(c1) + M(c0)) / 9 = (3525.3±0.1) MeV ???
n, L
c.o.g
L S
Spin-orbit
1 2 1 2r rS S S S
Tensor
J = L - 1
J = L + 1
J = L1 2S S
Spin-spin
J = L
S = 0 S = 1Fine structureHyperfine structure
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Inclusive search for hc
0
’
hc
c
• Require 0 recoil mass to be consistent with the c mass
• Plot 0 recoil mass (should reflect the hc mass)
hc
156 ± 48 events3.3significant
anything
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Exclusive search for hc
0
’
hc
c KsK,2K0,2K24,2
• Reconstruct c in one of the exclusive decay modes
• Then follow the same steps as in the inclusive analysis
hc15.0 ± 4.2 events5significant
c mass sidebandsData MC
Signal sample ’ 0 hc 0 c
Optimize c reconstruction on ’ cc
Epiphany 2005, Krakow Tomasz Skwarnicki 19
Preliminary CLEO results for hc mass
For comparison: hep-ex/040085Preliminary E835 results:
Disapprove E760 evidence for pp hc J ~13 pp c events in the peak~3.3 significance for hc
M(hc) = 3525.8±0.2±0.2 MeV
E835
• Inclusive analysis: M(hc)= (3524.8±0.7) MeV• Exclusive analysis: M(hc)= (3524.4±0.9) MeV• Together:
M(hc)= ( 3524.7 ± 0.6 ± 1.0 ) MeV M(c
cog) - M(hc) = ( 0.6 ±1.2 ) MeV• Consistent with zero• In any case small as expected
• The analysis is still in progress and numbers will change slightly before they are published
Epiphany 2005, Krakow Tomasz Skwarnicki 20
Search for X(3872) in fusion and ISR• Reconstruct exclusive J/, J/ events in CLEO-
III high energy data (15 fb-1)Untagged fusionJPC=0±+,2±+,…
Initial State RadiationJPC=1
_ _
No signal found
hep-ex/0410038Accepted by PRL
Epiphany 2005, Krakow Tomasz Skwarnicki 21
Search for X(3872) in fusion and ISRAssuming B(B± → K± X) ≈ B(B± → K± ψ’) → B(X → π+ π- J/ψ) ≈ 0.02our limits imply:
(2J+1)X(3872)) < 0.65 keV
• ¼ that for χc0 and χc2
• Ackleh &Barnes prediction for 11D2 state: (2J+1)(11D2) keVee(X(3872)) < 0.42 keV• comparable to ψ(3770)• ½ that of ψ(4040)
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Determination of B((nS) )Measure yields on and off the resonance peaks
• Much larger samples than previously available
• Much better detector than previously available (tracking, calorimeter, muon system)
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• Compared to the previous measurements:– Good agreement for (1S)– Substantial disagreement for (2S), (3S)
Determination of B((nS) )CLEO-III
hep-ex/0409027Accepted by PRL
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Determination of tot((nS))
B((nS) ) are important for determination of tot((nS))
and CLEO-III values for B and PDG values for B
• Important change for many comparisons of data (Bx) vs theory (x): Bx=x/tot
Epiphany 2005, Krakow Tomasz Skwarnicki 25
Photon transitions – E1
123
456
7891011
1213,14,15
16,1718
J=210
J=210
BR * tot E1
E M(n3PJ)
• Electric Dipole Transitions
g g gHadrons (…0..)
g g g
123
5,46
(2S)
21 3
65,4
(2S)87 9
65,4
1211,10
1514,13
16,1718
(3S)
22 3
E1 f f iQ iL r Le n n E
g g
cc
bb
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Photon transitions – E1
123
789
J=210
J=210
(2S)
(2S)
cc
bb(3S)
1
1 2
2
3
3 879
hep-ex/0408133 Accepted by PRD
hep-ex/0408133 Accepted by PRL
16,1718
(3S)
18
16,1733S1 13P0
Epiphany 2005, Krakow Tomasz Skwarnicki 27
Comparison to previous measurements - examples(2S) bJ(1P2) (3S) bJ(2P2)
Good agreementon Ei.e.mbJ
Disagreements on B((3S) bJ(2PJ))
Improvedprecision
Epiphany 2005, Krakow Tomasz Skwarnicki 28
Fine splitting of P-states• Tests of relativistic corrections to the mass spectrum
01
12
mmmm
r
r(1P) 0.570.010.01
r(2P) 0.580.010.01
r(1P) 0.4900.0020.003
bb
cc
Nearly equal, against most of theoretical predictions.}
The results favor confining potential of effective scalar type
(=0.8 for pure Coulomb potential)
Epiphany 2005, Krakow Tomasz Skwarnicki 29
Relativistic effects in transition rates• In non-relativistic approximation E1 matrix
elements are spin (J) independent2
E1 E13 3(2 1) (2 1)
( )f f i i JL L
Jr
B in n fE E
(J=2)/(J=1)b(2P): (J=0)/(J=1)
(J=0)/(J=2)
1.000.010.050.760.020.070.760.020.09
(J=2)/(J=1)b(1P): (J=0)/(J=1)
(J=0)/(J=2)
1.010.020.080.820.020.060.810.020.11
(J=2)/(J=1)c(1P): (J=0)/(J=1)
(J=0)/(J=2)
1.500.020.050.860.010.060.590.010.05
Ratio of 3(2 1)( ( 1) )J
JB nS n P
E
Consistent with the NRexpectations
Relativistic effects in J=0are expected to be the largest
Smaller c-quark massand substantial 2S-1D1
mixing}cc
bb
Epiphany 2005, Krakow Tomasz Skwarnicki 30
E1 matrix elements• Large relativistic
corrections (triangles) needed to describe E1 rates in charmonium.
• Corrections small in bottomonium.
• Small matrix element 33S1 13PJ difficult to predict (cancellations)
Date ofpublication 33S1 13PJ
33S1 23PJ
S.Godfrey
23S1 13PJ
-+
McC
lary
83
Gro
tch
84 23S1 13PJ
23S1 13PJ
33S1 23PJ
33S1 13P0
<1P 0|r
|3S>
“Spin averaged” matrix elements
bb
bb
cc
Epiphany 2005, Krakow Tomasz Skwarnicki 31
Photon transitions – M1
4
A way to reach singlet states
Crystal Ball claimed observation of all M1 transitions in charmonium ~20 years ago (Direct: “1”, “2”, Hindered: “4”)
1
2
365
• Magnetic Dipole Transitions
3
g g
2
4
(2S)
(2S)
4
2
(3S)
5
6
3
3
2 2
M3
1 2
DIRECT
1
tiny
HINDERED
l
0
arge
f i
f i
f i
i f
i f
Q
Q
n n
n
L L
n L n L
n L n
E
E
n
L
mE
en n
cc
bb
Epiphany 2005, Krakow Tomasz Skwarnicki 32
Search for b(11S0)
• No signal found for this or any other M1 transition in the Upsilon system
Hindered M1
E1
E1
E123PJ13S1 M1
33S111S0
M123S111S0(2S)
(3S)
cc
bb
4
6
(4)
(6)
Epiphany 2005, Krakow Tomasz Skwarnicki 33
M1 matrix elements
• Even recent calculations only marginally consistent with our upper limit on 33S1 11S0
13S1 11S0
23S1 11S0
23S1 11S0
33S1 21S0
33S1 11S0
allowed range
Lahd
e 03
Ebe
rt 0
3
Date ofpublication
Epiphany 2005, Krakow Tomasz Skwarnicki 34
Inclusive (2S) X J/(1S), J/(1S) +-
cut cutcut cut
MCLog
scal
e !
• Large statistics, good agreement with MC precision measurement of B((2S) X J/(1S))
Epiphany 2005, Krakow Tomasz Skwarnicki 35
Exclusive (2S) X J/(1S), J/(1S) +-
Epiphany 2005, Krakow Tomasz Skwarnicki 36
Exclusive (2S) X J/(1S), J/(1S) +-
Epiphany 2005, Krakow Tomasz Skwarnicki 37
(2S) X J/(1S), J/(1S) +-
• Preliminary results presented at QWG workshop Oct 2004
• Improved results are being prepared for publication.
Epiphany 2005, Krakow Tomasz Skwarnicki 38
Exclusive hadronic (2s) decays
Log scale!
• A lot of theoretical complications e.g.:
– Interference with continuum– s and relativistic
corrections• Happy with agreements
within a factor of ~2
Epiphany 2005, Krakow Tomasz Skwarnicki 39
Exclusive hadronic (2s) decays
• (2s) Dalitz plot distinctively different than continuum or J/(1S)
BESJ/
CLEO(2S)
Epiphany 2005, Krakow Tomasz Skwarnicki 40
Exclusive hadronic (2s) decays
Linear scale
Epiphany 2005, Krakow Tomasz Skwarnicki 41
Continuum production of PV at 3.67 GeVhep-ex/0407028
Epiphany 2005, Krakow Tomasz Skwarnicki 42Summary• First statistically compelling measurement of fD-
• Observe highly significant (2S)0hc,hc c signal with the hc mass consistent with the c.o.g. of the cJ states
• Non-observation of X(3872) and ee X(3872). • Precision measurements of B((nS) ). The results for
(2S),(3S) significantly different from the PDG values, impacting estimates of the total widths of these states.
• Precision measurements of photon transitions from (2S),(2S),(3S). More sensitive tests of relativistic corrections in the potential model calculations.
• Precision measurements of inclusive and exclusive transition rates for (2S) X J/(1S). Some significantly different from the previous measurements.
• Many new insights into B((2S)X)/B(J/(1S) X) for 2- and multi-body exclusive final states.
• First measurements of continuum productions of 2-body pseudo scalar-vector final states at 3.67 GeV. Ratios of cross-sections in rough agreement with SU(3) except for K*0K0