recent results on charm decays
DESCRIPTION
Recent Results on Charm Decays. Lifetimes mesons baryons “Wrong” sign D 0 decays Mixing Doubly suppressed cabibbo decays CP violation searches Semileptonic charm decay Summary/Outlook. weak. Results from: BABAR BELLE CLEO FOCUS SELEX. Charm Particle Lifetimes. - PowerPoint PPT PresentationTRANSCRIPT
WIN02 Jan 24, 2002 Richard Kass
Recent Results on Charm Decays
• Lifetimes– mesons– baryons
• “Wrong” sign D0 decays– Mixing– Doubly suppressed cabibbo decays
• CP violation searches• Semileptonic charm decay• Summary/Outlook
Results from: BABAR BELLE CLEO FOCUS SELEX
WIN02 Jan 24, 2002 Richard Kass
Charm Particle LifetimesLifetime is a defining property of a “particle”.
necessary to convert BR’s to decay rates theoretical comparisonsWeak interaction lifetime modified by strong interaction effects non-perturbative QCD
Charmed mesons and baryons provide a rich testing ground:3 mesons (D+, D0, Ds)
4 baryons (c, c+, c
0, c)
doubly charmed baryons
spectator color suppressedinternal spectator
exchange annihilation
Interference effects are important:
0DDcc
Pattern of lifetimes “predicted” but not exact lifetime values
WIN02 Jan 24, 2002 Richard Kass
D0
K
Beampipe
Colliding Beam Fixed target
Silicondetectors
Silicondetectors
Better acceptance for short lifetimes Better L/ separationCleaner environment Large data samples
Neither actually “see” the decay as in emulsion and/or bubble chamber
Unbinned ML fit Binned ML fit1d or 2d vertex 3d vertex
Colliding Beam vs Fixed Target
WIN02 Jan 24, 2002 Richard Kass
Charmed meson lifetimes
D0K+-
signal
D0K+-
sideband
Fixed target: exponential decay
Colliding beam: exponential decay smeared by resolution
WIN02 Jan 24, 2002 Richard Kass
400
405
410
415
420
425
E691
E687
CLE
OII
E791
SELE
X
BEL
LE
BA
BA
R
D0 li
fetim
e (f
s)
460
470
480
490
500
510
520
E691
E687
CLE
OII
E791
SELE
X
BEL
LE
FOC
US
Ds
lifet
ime
(fs)
Annihilation and exchange diagramsare important for mesons.
Expect <1.07 without annihilationand exchange.Bigi & Uraltsev, Z.Phys. C.62, 623, 1994
1000
1020
1040
1060
1080
1100
E691 E687 CLEOII BELLE
D+ li
fetim
e (f
s)Lifetime results for Charmed Mesons
preliminary
PDG2001
02.020.1/:2001PDG 0 DDs
01.002.017.1/:BELLE 0 DDs
WIN02 Jan 24, 2002 Richard Kass
Charmed Baryon LifetimesBaryon lifetimes not measured as precisely as mesons: 5-30% vs 1-2%Baryon lifetimes shorter than mesons (e.g. c= 60 fs vs D0= 410 fs )Baryon cross sections are low samples smaller than mesonsLifetime calculations more complicated than mesons
New results for c+, c
+, c0
preliminary
c+
160
170
180
190
200
210
220
230
E691
NA
32
E687
NA
14
E687
CLE
OII.
V
SELE
X
FOC
US
c+
lifet
ime
(ps)
PDG2001
preliminarynot in PDG2001
WIN02 Jan 24, 2002 Richard Kass
Recent c+ lifetime Results
150
200
250
300
350
400
450
500
550
SPEC
85
SPEC
87
AC
CM
E687
CLE
OII.
V
FOC
US
c+
lifet
ime
(ps)
PDG2001
not in PDG2001
=5034718fs
c+
c+
c+
c+p
c+
25018
58132
WIN02 Jan 24, 2002 Richard Kass
Charmed Baryons LifetimesPreliminary c
0 result from FOCUS:
=109+10 fs (PDG2001: =98+23 fs)Based on a total of 13719 events (c
0, )-9 -15
Comments: Measured lifetime ratio for c
+ / c+ larger than theory:
3.08.2:V.CLEOII
c
c
1.01.2:FOCUS
c
c
Theory ranges from: 1.3 Blok and Shifman, proceedings of 3rd workshop on physics of a tau charm factory, (1993) 1.2-1.7 Guberina and Melic, Eur. Phys. J. C2, 697 (1998)
At some point in the future lifetime analyses may have to correct for:c
0c contamination of c
sample c
0c contamination of c
in sample Doubly charmed baryons
Cabibbo suppressed s uinstead of c s
NoCalculationsavailable
WIN02 Jan 24, 2002 Richard Kass
Why is D0-D0 mixing interesting?-
Only meson system where mixing has not been observedOnly meson system where mixing is generated by down quarksMixing in D sector expected to be small in Standard Model
doubly Cabibbo Suppressed (DCS)vanishes the limit of SU(3) flavor symmetry
If D mixing is large:M: large flavor SU(3) breaking ?: new physics ?
D mixing only involves the first two generations:CPV >> 10-3 New Physics
Can make measurements to look for mixing !
WIN02 Jan 24, 2002 Richard Kass
D mixing Phenomenology
0000 DqDpDDqDpD LH
Usual definitions:
)(21
LH
)(21
LH
LH mmm
)( LH
mx
2
y
Phases: is the strong phase between Cabibbo allowed and doubly Cabibbo suppressed amplitudes is the CP violating phase in mixing (very small in SM)
CP Violation: CPV in mixing due to |p/q|1 CPV in interference between decay with and without mixing sin 0 Assume no direct CPV
WIN02 Jan 24, 2002 Richard Kass
Ways to Observe D mixingMeasure lifetime difference between CP+ and/or CP- statesand with flavor specific (CP mixed) states.
CP+: D0K+K-, +-
CP-: D0Ks00, Ks
0
Mixed: D0K-+ Gives info on y:
sin2
1|)|/|(|cos2
xpqyyCPCP
CPCPCP
1
KKD
KDCPy
Requires good time (vertex) resolution
ycpy if no CPV
Measure “Wrong” sign Decays.hadronic decays: D0K+- semi-leptonic decays: D0K+l-v-
Don’t have tomeasure timedependence
WIN02 Jan 24, 2002 Richard Kass
“Wrong” sign D0 decaysThese decays can originate from:a) Double Cabibbo suppression (DCS) (hadronic decays only)
b) Mixing
Usual assumptions: CP conserved |p/q|=1 |x|, |y|, RDCS<<1
.,,,|||| 0
2
0
0etcX
DHXKDHXKRDCS
tDCSDCSWS etyxRtxyRR ])(
4))(sincos([ 2
22
=strong phase differencebetween CF and DCS decays
Wrong sign rate (RWS) has interesting time dependence due to mixing+decay:
tDCSDCSWS etyxRtyRR
])(
4)([ 2
22Convenient to rotate away : x=xcos+ysin, y=ycos-xsin
NO DCS for semi-leptonic decays:t
WS etyxR 222 ))((
WIN02 Jan 24, 2002 Richard Kass
Some Recent ycp Lifetime Results
FOCUS: PLB485, 62 (2000)
CLEO: sub. PRD
BABAR: preliminaryycp =-1.0
ycp =3.4
KK: ycp =-1.9 : ycp = 0.5
Not a full blown lifetime analysisLooking for lifetime differences
WIN02 Jan 24, 2002 Richard Kass
Recent Mixing Results via ycp
experiment ycp comments
FOCUS 3.4 Fixed target, K+K-
E791 0.8 Fixed target, K+K-
CLEO -1.2
e+e-, K+K-,+-
BELLE -0.5 e+e-, K+K-
BABAR -1.0
e+e-, K+K-
+0.7-0.8
yyKKD
KDCP
1
-4
-2
0
2
4
FOCUS E791 CLEO BELLE BABAR
y cp (%
)
preliminary
WIN02 Jan 24, 2002 Richard Kass
Mixing Limits using “wrong” sign and ycp measurements CLEO’sTime dependence of (D0K+- )/ (D0K-+)
tDCSDCSWS etyxRtyRR
])(
4)([ 2
22
Semi-leptonic (D0K+l-v)/ (D0K-l+v) limit:(D0K+l-v)/ (D0K-l+v)<0.5%@ 90%CL
ycp measurements (FOCUS, E791)
Published Data
WIN02 Jan 24, 2002 Richard Kass
Mixing Limits using “wrong” sign and ycp measurementsWhat will this plot look like in the near future?New results expected soon from CLEO, FOCUS, BABAR, BELLE
average ycp
FOCUS preliminary K
FOCUS, CLEOSL sensitivity
WIN02 Jan 24, 2002 Richard Kass
“Wrong” sign D0 Decay ratesImproved measurements of (D0K+- )/ (D0K-+):
CLEO II 0.77 0.25 0.25
ALEPH
E791 0.68
CLEO II.V 0.33
FOCUS 0.40
BABAR 0.38
BELLE 0.30
D0 K+-D*+ D0+
pre l
imin
ary
RWS=(D0K+- )/ (D0K-+) (%)
0
0.5
1
1.5
2
CLE
O II
ALE
PH
E791
CLE
O II
.V
FOC
US
BA
BA
R
BEL
LE
RW
S
preliminary10X data soon
WIN02 Jan 24, 2002 Richard Kass
More “wrong” sign D0 Decay ratesCLEO II.V result for D0 K+-+-
[0.41+0.12-0.11
(stat) 0.04(sys)] (1.070.10)(phase space)(%)
RWS=0.25 +0.36-0.34
(stat) 0.03 (sys) (%) (phase space=1)
CLEO II.V result consistent with previous E791 result:
9fb-1 of dataused in analysis
But cannot tell if this result is from DSC or mixing since:
54 14 WS eventsfrom 2D binnedML fit
)()(
0
0
KDKDRWS
)(5.0) 22 xyRyRR DCSDCSWS
Only other WS D0 result: CLEO’s %07.043.0)()( 11.0
10.000
00
KDKDRWS
WIN02 Jan 24, 2002 Richard Kass
D0K00 and K00 Preliminary result from BELLE
L S
Interference between the Cabibbo allowed decay D0K00
and the DCS decay D0K00 can lead to a rate difference betweenD0KL0 and KS0.
-
Expect a 5% (tan2c) asymmetry in:
)()()()(
000000
000000
LS
LS
KDKDKDKDA
The magnitude and sign of A provides info the strong phase difference ()between D0K+- and D0K-+ .
Experimentally very challenging !Difficult to reconstruct KL’s in an e+e- experiment
BELLE calibrates KL efficiency using D0K*-+ , with K*-KL- .
WIN02 Jan 24, 2002 Richard Kass
D0K00 and K00 L S
D0KS0D0KL0
D0K*-+ KS-+ D0K*-+ KL-+
05.005.006.0)()()()(
000000
000000
LS
LS
KDKDKDKDA
Using 23 fb-1 of data BELLE measures:
First reconstructionof D’s using KL’s!
WIN02 Jan 24, 2002 Richard Kass
CP Violation in D0 Decay
Look for particle anti-particle rate differences
)()()()(
00
00
fDfDfDfDACP
Use D* tag to distinguish D0 from D0.
)()()()(
**
**
fDfDfDfDACP
Measure:
Where f is: K+K-, +-, Ks, Ks0, 00, and KsKs
CPV expected to be small in the charm sectorSM predictions O(0.1%)CPV > 1% evidence for non-SM processes
WIN02 Jan 24, 2002 Richard Kass
CP Violation in D0 Decay
-20
-15
-10
-5
0
5
10
15
20
E691
E687
CLE
OII
E791
FOC
US
CLE
OII.
V
Acp
(KK
) (%
)
-10
-5
0
5
10
E791 FOCUS CLEOII.V
Acp
(
%)
K+K- + -
CLEO also has the following results:ACP(Ks)=-2.89.4%
ACP(Ks0)=0.11.3%ACP(00)=0.14.8%ACP(KsKs)=2319%
No evidence for CP violation in D0 decay
CLEO “wrong” sign D0K+- analysis yields: ACP(K+-)=219 1.0 %
-20No mixing in fit
WIN02 Jan 24, 2002 Richard Kass
CP Violation in D+ Decay
Look for direct CP violation, no mixing.Not much new since 2000All results are from fixed target experiments.
)()()()(
fDfDfDfDACP
For charged D’s measure the following:
-15
-10
-5
0
5
10
15
A CP (%
)
FOC
US
E791
E791
E791
E791
E691
E691
E691
K+K- K K*0 +-
No evidencefor CPV
WIN02 Jan 24, 2002 Richard Kass
CLEO Measurement of B(D+K*0l+l)This decay is sensitive to P V form factorThese form factors are related to ff’s in bulv and bsll. Can help reduce uncertainty in extraction of |Vub|CLEO Method:Use D* tag, reconstruct using jet direction for D direction 2-fold ambiguity, choose solution closest to m=MD*-MD=140.6 MeV fit K* mass in bins for m then fit resulting m with K*+data to extract signal
Re=0.74 0.04 0.06R=0.72 0.104 0.06R=0.73 0.04 0.05PDG: B(D+K-++) =(9.0 0.6)%BRe =(6.7 0.4 0.5 0.4)%BR=(6.5 0.9 0.5 0.4)% BR =(6.6 0.4 0.5 0.4)%
)()( 0*
KDBlKDBRl
preliminary
WIN02 Jan 24, 2002 Richard Kass
CLEO’s form factor ratio measurement in ce+Motivation: Alternative method for extracting |Vub| and |Vcb|
Same set of form factors in both decays: f1(q2), f2(q2)
Korner&Kramer predict: R= f2(q2)/f1(q2)=-0.25 (PL B275,495 (1992))
222222
2max2 )/1(
)/1()()( *max* ss
DD
ii mq
mqqfqf
Extract R using ML fit to 3 variables: t=(q/qmax)2
cosW= angle between e and W in cm of W cos= angle between p and in cm of Preliminary Result: R= -0.310.060.06
Improvement over previous CLEO result: R= -0.250.140.08, (PRL 75,624 (1995))
Consistent with Korner&Kramer
right signe+, e- wrong sign
e-, e+
WIN02 Jan 24, 2002 Richard Kass
c0e+
Search for c0e+ by comparing “right” (e+) sign and
“wrong” sign (e-) event yields.preliminary
(e+) (e-)
B(c0e+ )(e+e- c X)=42.214.111.9 fb
10X smallerthan ARGUS result520230130 fb
Probability of background fluctuation < 9x10-4
First observation of baryon decay with no u or d in parent particle
WIN02 Jan 24, 2002 Richard Kass
Charm Review SummaryLifetimes: mesons: lifetimes measured to 1- 2%
baryons: lifetimes measured ~2 - 30%theory may need a tune up: /|exp>2 vs /|th< 1.7 +
c c+c c
D Mixing: Exciting times aheadnew results expected from BELLE & BABAR soon
CP Violation: Keep looking !
Semileptonic Decays: Progress measuring rates and form factors
“The future of charm physics lies ahead of us !” Yogi Berra? George W.?
b-factories are charm factories tooCLEO-c