puzzle pieces: results on b and c spectroscopy and decay
DESCRIPTION
Puzzle Pieces: Results on b and c Spectroscopy and Decay. Hanna Mahlke-Krueger Cornell University. DAPHNE 2004. Heavy Quarkonia Puzzles. Selected. New / precision measurements. Key unanswered questions. experimental. results. BES (2S) results (XH. Mo). - PowerPoint PPT PresentationTRANSCRIPT
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Hanna Mahlke-KruegerCornell University
DAPHNE 2004
Puzzle Pieces:Results on b and c Spectroscopy and
Decay
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DAPHNE'04 06/08/04
Hanna Mahlke-Krueger, Cornell
2
Heavy Quarkonia Puzzles
New /
precision
measurements
Key
unanswere
d
questions
Selected
experimental
results
HQ @ TeV (M.Paulini)
BES (2S) results
(XH. Mo)
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DAPHNE'04 06/08/04
Hanna Mahlke-Krueger, Cornell
3
? Masses ? Widths ? Production and decay dynamics Partly discovery, partly precision measurements
Onia States
bb: 560MeV
cc: 589MeV
e+e-:510-
6MeV
L=0 L=1 L=2
Spin-spin interaction: 1S3S1, 1S0
Spin-Orbit splitting: 3PJ3P0,1,2
n=2 n
=3
Notation: n2S+1LJ J=L+S
– _
Q
,
hQ
Q
n=1
• Strongly bound qq states• Non-relativistic QM
applicable (Appelquist, Politzer)
– QCD analog to positronium– Provide insight into QCD
• Low Q2, non-perturbative
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DAPHNE'04 06/08/04
Hanna Mahlke-Krueger, Cornell
4
Two Theoretical Approaches
• Potential Model: Cf. hydrogen; Coulomb, VH(r)= - em/r
VhQ(r)= – (4/3) s/r + k r
• Lattice QCD (the only complete definition of QCD): recent breakthrough allows predictions at the % level; needs experimental data to verify that match this precision!
positronium energy levels, spacing and decay rates fine-tune QED parameters quarkonium QCD
Short distance,1g exch long distance
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DAPHNE'04 06/08/04
Hanna Mahlke-Krueger, Cornell
5
Why Investigate Heavy Quarkonia?
Excellent place to study an important region of the Standard Model
Simplest strongly interacting systems
Gain insight to underlying interaction, QCD
More convenient to handle experimentally than glueballs
Fairly non-relativistic
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DAPHNE'04 06/08/04
Hanna Mahlke-Krueger, Cornell
6
Data samples
C’
X(3872)
Transitions
,,,0,
(3770) non-DD decays
(1,2,3S) B
J/,(2S)pp,
(1S)J/X
2body hadronic (2S) decays
Experimental Data
_
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DAPHNE'04 06/08/04
Hanna Mahlke-Krueger, Cornell
7
Producing quarkonia
• e+e- colliders, e+e-*qq: can only directly produce states coupling to *, i.e. n3S1 (J/, ) with a tiny admixture of n3D1–
• two real photon collisions: J=0,2 ([b,c], [b,c][0,2])
• hadron colliders any energy, no quantum number restrictions, but not as clean
• transition from higher up, e.g. (2S)c0
n=1
n=2
n=3 n=4
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DAPHNE'04 06/08/04
Hanna Mahlke-Krueger, Cornell
8
0
5
10
15
20
25
30
CleoIII/c
CleoII
CUSB/CBAL
0
10
20
30
40
50
60
CLEOIII/cCUSB/CBALBESIBESIIDM2MKIII
J/
’’’10
(1S)
(2S)(3S
)
Datasets as of
spring 2004
• Cross section falls as n increases
• Additional data samples for special purposes
106
106
Data Samples
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DAPHNE'04 06/08/04
Hanna Mahlke-Krueger, Cornell
9
C’
X(3872)
Transitions
,,,0,
Spectroscopy
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DAPHNE'04 06/08/04
Hanna Mahlke-Krueger, Cornell
10
Recently observed in 3 different ways:
B K (KSK+-) Belle e+e- J/(X) (Belle) KSK (CLEO, BaBar)
Old result (c’X, m=3594) directly ruled out by CLEO.
KSK
Current Experimental
Information on c
c
0
Belle e+e-J/(X)
c’
c’
c
CB
AL P
RL4
8(1
98
2)7
0, B
aB
ar h
ep-e
x/0
31
10
38
, B
elle
PR
L89
(20
02
)10
20
01
, PR
L 89
(20
02
)14
20
01
, C
LEO
PR
L 92
(20
04
)14
20
01
m(’)-m(c’) (MeV)New 2S splitting about half as
big, ˜48MeV m(2S)/ m(1S)0.5. Theory needs to accommodate this!
m(
c ’)
3638 MeV
Hyperfine splitting
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DAPHNE'04 06/08/04
Hanna Mahlke-Krueger, Cornell
11
X(3872) – a cc state?
Peak in B± K±(+-J/), m = (3872.0 0.60.5) MeV, < 2.3 MeV (90%CL) Belle
Also in pp(+-J/)X: m = (3871.3 0.70.4) MeV CDF m = (3871.8 3.13.0) MeV D0
3872 MeV
Belle
Belle
PR
L91:2
620
01,2
00
3, h
ep-e
x/0
40501
4;
CD
F hep-e
x/0
31202
1;
D
0
hep-e
x/0
40500
4;
BaB
ar
hep-e
x/0
402
025
, B
ES
hep-p
h/0
31
0261
What is its nature? Study production and decay mechanisms!
Charmonium state?13D2,3=2--,3-- ? (Xc1,2)/(XJ/)>2
See <0.89/1.1 (Belle)1++ ? (XJ/)/(XJ/)>1
See 0.4 (Belle)1-- ? Look in ISR production (next slide) DD* molecule?
mD+mD* = 3871.5±0.5 MeV Look for X D(D)
D0D00 BR’s< ~510-5 (Belle)
not inconsistentLook for X 00J/
J/ component? Exotic state?
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DAPHNE'04 06/08/04
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12
ISR (JPC=1--)
CLEO prelim: ee B(X +-J/) < 6.8eV (or, <1/100(2S) production rate in ISR for same BJ/)
BES: ee B(X +-J/) < 10eV (22.3pb-1 at s=4.03GeV)
CLEO results on X(3872)CLEOIII, 15fb-1, s=9.46…11.30GeV, X(3872)+-J/, J/ℓ+ℓ-
2 (JPC=0±+, 2±+, …)
X(3872)
X(3
87
2)
CLEO prelim: (2J+1) B(X -+J/) <16.7eV (or, <1/10 the c production rate in )
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DAPHNE'04 06/08/04
Hanna Mahlke-Krueger, Cornell
13
Transition Options
• Hadronic:0,,, +- - no
kaons; splitting too small
• Photonic:E1: L=1, S=0M1: L=0, L=1
Transitions
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DAPHNE'04 06/08/04
Hanna Mahlke-Krueger, Cornell
14
Hadronic Transitions
No charge involved:• two charged pions
or• neutral particles
0 0 Single 0
transitions isospin suppressed
, are ‘‘rare’’
Soft process.
Q
Q
0
Q
Q
Q
Q
Q
Q
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DAPHNE'04 06/08/04
Hanna Mahlke-Krueger, Cornell
15
bJ (1S): 1st non- hadronic
transition in bb(3S)(1S)+X:
– X is photon, (1S)ℓ+ℓ-
+-0 distribn peaks at
– Fit for (3S)bJ, bJ (1S), J=1,2
• B(b1(1S))=(1.63 )%
• B(b2(1S))=(1.10 )
% 1. substantial, 2. equal Voloshin hep-ph/0304165: r2/1=1.3±0.3
E
MC
’’
b2
’ MC ’’b1’
m(+-0)
+0.35 +0.16
- 0.31 - 0.15 +0.32 +0.11
- 0.28 - 0.10
CLEO
hep
-ex/0
31
10
43, a
cc by
PR
L
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DAPHNE'04 06/08/04
Hanna Mahlke-Krueger, Cornell
16
(2S)J/B(’0J/
)=(1.430.140.13)10-3
14% relativeB(’J/) =(2.980.090.23)% 8% relative
• Predictions for B(’0J/)/B(’J/), B(’J/)/B((2S)), B(’J/)/B((3S)),
… see Prof. Mo’s talk• Neutral dipion transitions in
hep-ex/0404020…
(3S) 0/ℓ+ℓ-, 0/ ? Not seen, UL @ ‰ level
m(
)/
GeV
2
m(J/h)/GeV2
ee
m()/GeV2
1
0
2
hep-ex/0403023
BES
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DAPHNE'04 06/08/04
Hanna Mahlke-Krueger, Cornell
17
Do we understand
(2S)J/ ?Charged dipion transitions often used as
normalizing mode; single most precise measurement: (32.31.4)% (BES ’02)
Expect B((2S)00J/)/B((2S)+-J/)=0.5 from isospin. Phase space correction: a few %. Others??
• Experiment: (PDG: B((2S)00J/) = (18.91.1)%) B((2S)00J/)/B((2S)+-J/)=0.5700.0090.026 4M (2S) BESI, hep-ex/0404020 B((2S)+-J/)=0.3610.0150.037 BaBar, radiative returns, 89fb-1 ~(4S) data, hep-ex/0312063
Neutral BR too high? Charged BR too low? Expectation off?
m(+-+-)/GeV
1 2 3 4
J/
(2S)
BaBar
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DAPHNE'04 06/08/04
Hanna Mahlke-Krueger, Cornell
18
(3770) non-DD
(1,2,3S) B
J/,(2S)pp,
(1S)J/X
2body hadronic (2S) decays
Decay
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DAPHNE'04 06/08/04
Hanna Mahlke-Krueger, Cornell
19
m((3770))>2m(D) (’’DD)=5.0±0.5nb <
(’’hadrons)= 7.9±0.6nb Can the deficit be confirmed?
• BES single tag Moriond 04: (’’DD)=5.78±0.11±0.38 nb • CLEO-c prelim double tag: (’’DD)=6.51±0.44±0.39 nb • Modern (’’hadrons) would be good…
Where would a 20% deficit of tot=24MeV show up? Rosner: rad decays at most 600 keV, J/ 100keV.
Does (2S)(3770) mixing happen? Do modes expected from J/ that are rare on (2S) mix away?
Understanding (2S) will help with (3770)! (Don’t expect BIG rates.)
MarkIII P
RL 6
0(1
98
8)8
9 C
BA
L CA
LT-6
8-1
15
0
(19
84
), MarkII S
LAC
-21
9 (1
97
9)
(3770) (2S)?D-
D+
80%
Are there (3770) non-DD
decays?_
__
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20
Total decay width: tot= had + ee + + ?
Total widths: 1S total widths keV, big portions not
accounted for by exclusive decays measured thus far
Relative precision on total width: [’,’’]: 3.4%, 16.9%, 13.3%, [’,’’]: 5.7%, 7.9%,
11.4% Leptonic decay widths:
confront LQCD percent level predictions test lepton universality
compare ℓℓ relative to ggg,gg, qq
narrow resonances: tot = ℓℓ / Bℓℓ, or ee/B
(2S) scan data published last year (BES)(1,2,3S): ee under study; B preliminary results (CLEO)
(1,2,3S) B
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DAPHNE'04 06/08/04
Hanna Mahlke-Krueger, Cornell
21
Leptonic (1,2,3S) Width ee
Strategy: hadronsYeeσdEnergy
ΓΓ
6M
eeYΓhadrons
total2
2Y π
Hope to improve from 2/4/9% 2-3%.
External input
SLAC 11/25/03 Hanna Mahlke-Krueger, Cornell 41
ee(2S)
ee(1S)
• LQCD predictions
!
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DAPHNE'04 06/08/04
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22
B in % tot in keV
CLEO preliminary PDG CLEO preliminary
PDG
(1S) 2.46 0.02 0.05
2.48 0.06 53.4 1.5 52.5 1.8
(2S) 2.00 0.03 0.05
1.31 0.21 29.5 1.4 44 7
(3S) 2.34 0.07 0.05
1.81 0.17 20.7 2.1 26.3 3.5
B((1,2,3S)+-) Results
Desired precision reached (LQCD!)
B((2,3S)) larger than previous results lower tot
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DAPHNE'04 06/08/04
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23
J/XbXb, X=p,BESII, 58M J/:
B(J/pp)= (2.26 0.01 0.14)10-3
Angular distribution: dN/dcosX=1+cos2X
[1] Brodsky, Lepage, PRD24(1981)2848 [2] Claudson et al., PRD25(1982)1345 [3] Carimalo, IntJModPhysA2(1987)245 [4] hep-ex/0402034, PLB424(1998)213
Proton
1.0 1.0 Neglect mX and mq [1]
0.46 0.32 Include mX [2]
0.66 0.51 Include mX and mq [3]
0.676±0.55 0.52 ±0.35 Experiment [4]
J/,(2S)pp,
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24
• COM needed to describe P-wave quarkonium decays cpp
• Based on c[0,1,2]pp meas’t, generalized to , expect BR(cJ/cJpp) =1/2 J=1,2
c[0,1,2] see excess BESII:
c[0,1,2]pp, within 1 of previous measurement and pp cJJ/: confirm excess hep-ex/0401011 & hep-ex/0304012, BESII
c0
3415
c1
3511
c2
3556
c0
3414
c1
3513c2
3549
c[0,1,2]
c[0,1,2]pp
__
-
__ __
__
_
_
c[0,1,2]pp, from (2S) CJ
-
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DAPHNE'04 06/08/04
Hanna Mahlke-Krueger, Cornell
25
CLEO preliminary
scaled J/ momentum x; qq and continuum subtracted (use (4S) as continuum)
CDF pp J/,(2S)X rates color octet mechanism: cc in CO, become CS by radiating off a soft gluon. Problems with other data…
More information needed to distinguish production mechanisms.
(1S)J/X is gluon rich envt; CO preferred
• Example: x spectrum.CO peaks near x=1;
modifications due to multiple soft g emission
(1S) J/X
_
_
b b
CSc c,c c
c c
b b
CO
_
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26
Charmonium production in (1S) decays
(e+e- qq J/+X)=… …(1.470.100.13) pb (Belle) …(2.520.210.21) pb (BaBar) …(1.90.2(stat)) pb (CLEO prelim)
B((1S)J/+X) = (6.40.40.6)10-4 CS: 5.9 10-4, CO: 6.2 10-4
90% is ggg, gg Includes feed-down from
(1S) (2S),c0,1,2+Y J/+X+Y. Identify through (2S) +-J/, CJ J/
CLEO preliminary
_
No clear conclusion on CS vs CO possible so far.
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Hanna Mahlke-Krueger, Cornell
27
e+
e-
Q
Q
Q
Q
Q
Q
q,l-
q,l+
QQ decays
into light hadrons
)3( SD
Dbackground q,l-
q,l+
Radiative decay:
Annihilation into 3g:
Annihilation into a photon: *
Dissociation:
Q*
2body hadronic decays
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28
“The 14% rule”If mechanism is cc annihilation
decay rate |(0)|2
Compare with e+e- production:
0.9)%12.3(
eeJ/ψB
eeψ(2S)B
HJ/ψB
Hψ(2S)BQh
J/ 3.1GeV
(2S) 3.7GeV
_
Complications (and there are more): Powers of S at mJ/, m(2S) 0.845 hep-ph/09910406 Form factor ECM dependence? 3.6862/3.0972=1.4 Non-relativistic corrections Interference with continuum Prof. Mo’s talk Only for cc*, not ccggg? (Gerard/Weyers)
Compliance within a factor of two: “agreement”
12%
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Hanna Mahlke-Krueger, Cornell
29
Two-body hadronic (2S) decays
(2S) BR’s: Not many are precisely measured
(2S), 12% rule: Nail down systematic deviation of certain channels?
Experimentally, situation is
unclearTheoretically,
even more than unclear: Add’l effects in J/? (2S)? Expectation?
Good understanding of continuum background and impact of interference is crucial!
12%1/2 2
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DAPHNE'04 06/08/04
Hanna Mahlke-Krueger, Cornell
30
Branching Fraction Ratio:
(2S)/J/
, K*K measured• IV channels ~obey 12%
rule
• b1 and +-, too; f2 almost
IVIV
VP final states + some othersCLEO data, 3M (2S),
20pb-1 @ s=3.67GeVMeasure branching fractions
relative to B((2S)+-J/, J/+-)
BF’s range from 10-5 to 10-3
Background subtracted, not corrected for interference
Good statistical power of continuum sample is key!
Biggest violators: +-0, , K*+K-,
VP
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Hadronic (2S) BR’s +-0 ~6 136 +12
-13 21
4.2 24 +7 -8 2
00 3.0 9 4 1
+- 3.0 15 +6 -7 2 b1
+- ~6 205 +38 -45 30
0 3.1 23 +9 -11 2 b1
00 ~6 369 +40 -41 76
0 <1 <7 f2 (1270) 5.7 101 +21 -25 12
0 4.5 31 +11 -7 2 +- ~6 762
40
76
<1<10
f0 (980) 3.3 22 +8 -9 3
2.1 19 +10 -154 f2’ (1525) 2.0 38 +23
-32 10
K*0K0 5.2 87 +21 -259 K*+K*- 5.0 106 +23
-25 33
K*+K- 2.6 17 +8 -10 4 K*0K*0 4.9 196 +48
-54 32
Channel
stat signif in
B((2S)X) in 10-6 stat syst
CLE
O p
relim
inary
5.5pb-1(3M) (2S), [email protected] GeV BRs not corrected for interference
B(f0+-)
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DAPHNE'04 06/08/04
Hanna Mahlke-Krueger, Cornell
32
hep-ex/0402013J/+-0
BES
m
CLEO preliminary
m(+-)
m(+0
)
m(-
0)
m
(2S)+-0
production (??)
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DAPHNE'04 06/08/04
Hanna Mahlke-Krueger, Cornell
33
Transitions ,
, ,0,
C’
X(3872) (1,2,3S) B
J/,(2S)pp,
(1S)J/X2body hadronic (2S) decays
Summary
hc, hb, b() ? 12% rule?
00 /
+-
tran
s
….Interfe
rence
….
(3770) non-DD?
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BACKUP
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DAPHNE'04 06/08/04
Hanna Mahlke-Krueger, Cornell
35
J/
ee→ 2S2S→ J ?
232 events
Ecm -Mass recoiling
• 5.2±0.2 pb-1, (4.5±0.4)104 ’’decays
• efficiency: 37% < 4.75 events @ 90%CL
BR3770J(1S)) <0.26% @ 90% CL
• 28 pb-1 (3.783-3.885GeV),
1.85105 ’’decays• efficiency: 16% 17.8±4.8 events incl
6.0±0.8 bgd (0 from cont) BR3770→J)
= (0.34±0.14±0.08) % = (80 ±32±21) keV
BESII CLEO-c
T. Skwarnicki, QWG03
ee→ 2S2S→ J
M(ℓ+ℓ) GeVhep-ex/0307028
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DAPHNE'04 06/08/04
Hanna Mahlke-Krueger, Cornell
36
B((1,2,3S)+-)
• Goal: 3-4% precision on B
– Gives tot ee
• 1.0/1.2/1.2 fb-1 on-resonance + 0.2/0.4/0.2 fb-1 off-resonance
• Backgrounds: continuum, cascade decays such as (3S)b0(2S) , cosmic ray events
• Good understanding of data
MC: e+e-+- data
MC:
(1S)+- w/o FSR data
off- res.
on- res.
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DAPHNE'04 06/08/04
Hanna Mahlke-Krueger, Cornell
37
CLEO-c 1,21S0 lines
c(1S) seen @ 8.2 c(2S) in the CBAL
preferred region ruled out
CLEO-c preliminary
CBAL
CLEO-c preliminary
500 600 700 800 E (MeV)
cc’
80 85 90 95 E (MeV)
BR((2S)C(2S)):
1.5%
1.0%
0.5%
0.0%
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DAPHNE'04 06/08/04
Hanna Mahlke-Krueger, Cornell
38
(2S) Branching FractionsCLEO data, 3M (2S),
20pb-1 @ s=3.67GeVMeasure branching
fractions relative to B((2S)+-J/, J/+-)
Convert using B((2S)+-J/) =(32.31.4)% and B(J/+-)
=(5.880.10)%Background subtracted,
not corrected for interference
• A plotVP