1 D 0 D 0 Quantum Correlations, Mixing, and Strong Phases David Asner, Carleton University for the CLEO-c Collaboration Discoveries in Flavour Physics at e + e - Colliders 28 February – 3 March 2006, Frascati, Italy Introduction and motivation Experimental technique Preliminary results and future plans
11
Embed
1 D 0 D 0 Quantum Correlations, Mixing, and Strong Phases David Asner, Carleton University for the CLEO-c Collaboration Discoveries in Flavour Physics.
This document is posted to help you gain knowledge. Please leave a comment to let me know what you think about it! Share it to your friends and learn new things together.
Transcript
1
D0D0 Quantum Correlations, Mixing, and
Strong Phases David Asner, Carleton University
for the CLEO-c Collaboration
Discoveries in Flavour Physics at e+e- Colliders28 February – 3 March 2006, Frascati, Italy
Introduction and motivationExperimental technique
Preliminary results and future plans
DIF06, 28 Feb-3 Mar 2006, Frascati, ItalyDavid Asner, Carleton University 2
Effect of Quantum Correlations
|D1,2> = p|D0> ± q|D0> Because of quantum correlation
between D0 and D0, not all final states allowed. This affects: total rate apparent branching fractions
Two entangled causes: Interference between CF &
DCSD D mixing: single tag rates
depend on y = (2-1)/2.
Semileptonic decays tag flavor unambiguously (if no mixing) If one D is SL, the other D decays as if isolated/incoherent.
Exploit coherence to probe DCSD and mixing—shows up in time-integrated rates.
ee * D0D0
C = 1
K K
K K
K K
K Kl
CP+ Kl
CP- Kl
Kl Kl
CP+ CP-
CP+ CP+
CP- CP-
interference
forbidden by CP
conservation
forbidden inabsence of mixing
maximalconstructiveinterference
DIF06, 28 Feb-3 Mar 2006, Frascati, ItalyDavid Asner, Carleton University 3
Introduction
In the Standard Model, D mixing strongly suppressed (CKM and GIM).
Previous searches: Double semileptonic rates give RM. Time-dependent K: x, y rotated by
Current analysis:
Uses time-independent yields. Sensitive to y at first order. No sensitivity to p/q≠1; neglect CPV
DIF06, 28 Feb-3 Mar 2006, Frascati, ItalyDavid Asner, Carleton University 4
Single and Double Tag Rates
Hadronic rates (flavored and CP eigenstates) depend on mixing/DCSD.
Semileptonic modes (r = = 0) resolve mixing and DCSD.
Rate enhancement factors, to leading order in x, y and r2:
With C=+1 D0D0 at higher energy, sensitivity to wx at first order. Not much info if w=2sinis small.
f l+ CP+ CP-
f RM/r2
f1+r2(2-
z2)
l- 1 1
CP+
1+rz 1 0
CP- 1-rz 1 2 0
X 1+rzy 1 1-y 1+y
D DSingle tag: X i
D DDouble tag: j i
DIF06, 28 Feb-3 Mar 2006, Frascati, ItalyDavid Asner, Carleton University 5
Experimental Technique
Use fitter from CLEO-c D absolute hadronic branching fraction analysis – W. Sun, Nucl.Instrum.Meth.A556:325-330,2006.
Based on MARK III double tag technique using: single tags ( ni ~ NDDBii ) and double tags ( nij ~ NDDBiBjij )
281 pb-1 = 1.0 x 106 C=-1 D0D0 pairs. Limiting statistics: CP tags—our focus is not on Bs. Kinematics analogous to (4S)BB: identify D with
(MBC) ~ 1.3 MeV, x2 with 0
(E) ~ 7—10 MeV, x2 with 0
Procedure tested with CP-correlated MC.
Modes
fK
K
CP+
KK
K0S00
CP- K0S0
lXe
Xe
ij
j
j
iji n
nB
ji
ij
ij
jiDD n
nnN
22 || DbeamBC pEM
Dbeam EEE
lCP
XCP
lCP
XCP
Xf
lfy,
,
,
,
,
,
4
fCP
XCP
fCP
XCP
Xf
ffrzy,
,
,
,
,
,
_
_
4
~ n/
DIF06, 28 Feb-3 Mar 2006, Frascati, ItalyDavid Asner, Carleton University 6
Hadronic Single Tags
Standard D reconstruction. Cut on E, fit MBC distribution to
signal and background shapes. Efficiencies from (uncorrelated)
DD Monte Carlo simulations. Peaking backgrounds for:
K from K/ particle ID swap. Modes with K0
S from non-resonant
CP+
CP-
fMode (%)
% bkg
Signal Yield (103)
K 65.7 ± 0.1
0.13 26.0 ± 0.2
K 66.7 ± 0.1
0.14 26.3 ± 0.2
KK 58.9 ± 0.2
0.00 4.70 ± 0.08
73.5 ± 0.3
0.00 2.13 ± 0.12
K0S00 14.6 ±
0.113.8 3.58 ± 0.17
K0S0 31.4 ±
0.12.2 8.06 ± 0.11
MBC for K0S0 (CP-)
MBC for (CP+)
MBC for K (f)
Note log scale DATA
(GeV)
DIF06, 28 Feb-3 Mar 2006, Frascati, ItalyDavid Asner, Carleton University 7
Hadronic Double Tags
Cut and count in MBC1 vs. MBC2 plane, define four sidebands.
Uncorrelated background: one D misreconstructed (sometimes both). Signal/sideband scale factor: integrate background function from ST fits.
Mispartition background: particles mis-assigned between D0 and D0.
Data
K K KK K0S00 K0
S0 Yields
2.5 ± 0.4
2.0 ± 0.4
622 ± 7599 ±
25
62.3 ± 2.1
70.6 ± 8.4
25.3 ± 1.3
24.0 ± 4.9
31.2 ± 1.4
38.7 ± 6.2
78.3 ± 2.3
90.4 ± 9.5
K
2.7 ± 0.4
2.0 ± 1.4
64.7 ± 2.1
53.0 ± 7.3
30.6 ± 1.4
24.3 ± 5.0
32.3 ± 1.5
37.6 ± 6.2
85.0 ± 2.4
77.0 ± 8.8
K
5.2 ± 0.4-2.2 ±
1.9
4.5 ± 0.30.1 ± 0.9
5.7 ± 0.41.6 ±1.3
16.0 ± 0.6
39.6 ± 6.3
KK
1.1 ± 0.20.2 ± 1.4
2.2 ± 0.21.6 ± 1.3
5.8 ± 0.414.0 ±
3.7
1.2 ± 0.21.0 ± 1.0
7.3 ± 0.419.0 ±
4.4K0
S00
9.7 ± 0.53.0 ± 1.7
K0S0
No-QC expectationObserved in data
MBC(KK vs. MBC(K0
S0)
DATA
(GeV)
(GeV
)
DIF06, 28 Feb-3 Mar 2006, Frascati, ItalyDavid Asner, Carleton University 8
Inclusive Semileptonic Double Tags
Tag one side with K or CP eigenstate, search for electron in remainder of event:
Fit electron spectrum for signal and background. conversion, 0 Dalitz decay: charge symmetric. Mis-ID: hadrons faking electrons. Mis-tag: estimate from tag-side MBC-E sideband.
Require right-sign electron charge for K tag. Efficiency correction in bins of pe. Tag e
e(%)
% bkg
Signal Yield
K 72.9 5.2 1206 ± 35
K 71.9 2.8 1291 ± 36
KK 69.1 23.2 145 ± 12
KK 69.0 34.8 136 ± 12
70.0 28.2 78 ± 9
70.2 29.0 55 ± 7
K0S00 69.2 43.8 146 ± 12
K0S00 69.1 65.9 140 ± 12
K0S0 69.2 8.2 231 ± 15
K0S0 75.1 19.1 221 ± 15
e vs. K e vs. K0S0
e vs. pe
pe (GeV) in DATA
DIF06, 28 Feb-3 Mar 2006, Frascati, ItalyDavid Asner, Carleton University 9