open charm physics at besiiitalks/images/8/80/phipsi11-lilei.pdf · single tag d0bar double tag d0...
TRANSCRIPT
![Page 1: Open Charm Physics at BESIIItalks/images/8/80/PHIPSI11-Lilei.pdf · single tag D0bar double tag D0 single tag D-double tag D0 MARK-III method 19 Absolute Branching fraction Measurement](https://reader035.vdocuments.net/reader035/viewer/2022071223/607be13667cd8909e000576e/html5/thumbnails/1.jpg)
1
Open Charm Physics at BESIII
Lei. Li
( for BESIII Collaboration )
Institute of High Energy Physics
From Phi to Psi 2011,
Novosibirsk, Russia, September 19-22 , 2011
![Page 2: Open Charm Physics at BESIIItalks/images/8/80/PHIPSI11-Lilei.pdf · single tag D0bar double tag D0 single tag D-double tag D0 MARK-III method 19 Absolute Branching fraction Measurement](https://reader035.vdocuments.net/reader035/viewer/2022071223/607be13667cd8909e000576e/html5/thumbnails/2.jpg)
2
Outline
• Introduction to the BESIII experiment
• Major Charm Physics at BESIII
• Physics Analysis being done
• Summary
![Page 3: Open Charm Physics at BESIIItalks/images/8/80/PHIPSI11-Lilei.pdf · single tag D0bar double tag D0 single tag D-double tag D0 MARK-III method 19 Absolute Branching fraction Measurement](https://reader035.vdocuments.net/reader035/viewer/2022071223/607be13667cd8909e000576e/html5/thumbnails/3.jpg)
3
Satellite view of BEPCII /BESIII
BESIII detector
LINAC
2004: start BEPCII construction 2008: test run of BEPCII 2009-now: BECPII/BESIII data taking Design Luminosity: 11033 cm-2s-1
Achieved Luminosity: 0.65 1033 cm-2s-1
South
![Page 4: Open Charm Physics at BESIIItalks/images/8/80/PHIPSI11-Lilei.pdf · single tag D0bar double tag D0 single tag D-double tag D0 MARK-III method 19 Absolute Branching fraction Measurement](https://reader035.vdocuments.net/reader035/viewer/2022071223/607be13667cd8909e000576e/html5/thumbnails/4.jpg)
BEPCII Storage Ring
Beam energy: 1.0-2.3 GeV Design Luminosity: 1×1033 cm-2s-1
Optimum energy: 1.89 GeV Energy spread: 5.16 ×10-4
No. of bunches: 93 Bunch length: 1.5 cm Total current: 0.91 A Circumference: 237m 4
![Page 5: Open Charm Physics at BESIIItalks/images/8/80/PHIPSI11-Lilei.pdf · single tag D0bar double tag D0 single tag D-double tag D0 MARK-III method 19 Absolute Branching fraction Measurement](https://reader035.vdocuments.net/reader035/viewer/2022071223/607be13667cd8909e000576e/html5/thumbnails/5.jpg)
5
EMC CsI(Tl) σE /E ~2.5% @ 1 GeV
Drift chamber: small sell & He-based gas σp/p = 0.5% @ 1 GeV σ(dE/dx)/dE/dx ~ 6% @ 1GeV
Time‐of‐flight(TOF) σΤ(barrel) : 90 ps σΤ(endcap): 100 ps
RPC Muon Counter Barrel : 9 layers Encaps: 8 layers SC magnet (1T)
Magnet yoke
BESIII Detector
![Page 6: Open Charm Physics at BESIIItalks/images/8/80/PHIPSI11-Lilei.pdf · single tag D0bar double tag D0 single tag D-double tag D0 MARK-III method 19 Absolute Branching fraction Measurement](https://reader035.vdocuments.net/reader035/viewer/2022071223/607be13667cd8909e000576e/html5/thumbnails/6.jpg)
Data Samples
So far BESIII has collected :
Type BES-III (106)
BES-II (106)
CLEO-c (106)
J/y 225 58 -
y(3686) 106 14 27
DDbar ~18.3(2.9 fb-1) 0.2(0.03 fb-1) 5.4(0.8fb-1)
DsDs ~0.5fb-14.01 - Scan
DsDs* - - 0.55(0.6fb-1)
BESIII will collect:
– more J/y, y’, y(3770)
Approved: 1 billion for J/y and (0.7-1.0) billion for y’ & off peak
– data at higher energies (for XYZ searches, R scan and Ds physics)
6
![Page 7: Open Charm Physics at BESIIItalks/images/8/80/PHIPSI11-Lilei.pdf · single tag D0bar double tag D0 single tag D-double tag D0 MARK-III method 19 Absolute Branching fraction Measurement](https://reader035.vdocuments.net/reader035/viewer/2022071223/607be13667cd8909e000576e/html5/thumbnails/7.jpg)
Charm plays important role in understanding the Standard Model in two respects.
Precision Measurements
Leptonic decay of D+ and Ds+
Semileptonic decay of D mesons
Absolute hadronic branching fractions
decay constant fD and fDs
|Vcs|, |Vcd| and form factors
To normalize the B and D decays
Can be used to Improve measurements in |Vub| and Dmd & Dms .
Major Charm Physics
7
![Page 8: Open Charm Physics at BESIIItalks/images/8/80/PHIPSI11-Lilei.pdf · single tag D0bar double tag D0 single tag D-double tag D0 MARK-III method 19 Absolute Branching fraction Measurement](https://reader035.vdocuments.net/reader035/viewer/2022071223/607be13667cd8909e000576e/html5/thumbnails/8.jpg)
Major Charm Physics
b
s
d
VVV
VVV
VVV
b
s
d
tbtstb
cbcscd
ubusud
)(
11
21
214
23
22
32
O
AiA
A
iA
V
---
--
--
Weak eigenstates
CKM mass eigenstates
Four quark mixing parameters (, A, , ) reside in CKM matrix
Measurement of |Vcs(d)| plays an important role in understanding the dynamics of quark mixing
To understand quark mixing and CP violation in SM, and detect new physics in flavor change sector, one must determine the CKM elements as precisely as possible.
8
![Page 9: Open Charm Physics at BESIIItalks/images/8/80/PHIPSI11-Lilei.pdf · single tag D0bar double tag D0 single tag D-double tag D0 MARK-III method 19 Absolute Branching fraction Measurement](https://reader035.vdocuments.net/reader035/viewer/2022071223/607be13667cd8909e000576e/html5/thumbnails/9.jpg)
9
The constraints in the (, ) plan of Bd UT including the most recent inputs in the global CKM fit.
Major Charm Physics
The width of the band for |Vub|, Dmd & Dms are mainly dominated by the theoretical errors in calculating B & Bs decay constant fB, fBs and B semileptonic form factors.
Charm can be used to calibrate the QCD calculations. If the QCD passed the test with the charm data, the theoretical uncertainties in calculating the B form factors and decay constants can be reduced, which in turn help to reduce the width of band for |Vub|, Dmd & Dms.
![Page 10: Open Charm Physics at BESIIItalks/images/8/80/PHIPSI11-Lilei.pdf · single tag D0bar double tag D0 single tag D-double tag D0 MARK-III method 19 Absolute Branching fraction Measurement](https://reader035.vdocuments.net/reader035/viewer/2022071223/607be13667cd8909e000576e/html5/thumbnails/10.jpg)
Probe for New Physics
Major Charm Physics
D0D0 mixing
Searching for CP violation decays of D mesons
Searching for rare decays of D mesons
Precision measurements on charm decays can be served as precisely test of the SM.
10
![Page 11: Open Charm Physics at BESIIItalks/images/8/80/PHIPSI11-Lilei.pdf · single tag D0bar double tag D0 single tag D-double tag D0 MARK-III method 19 Absolute Branching fraction Measurement](https://reader035.vdocuments.net/reader035/viewer/2022071223/607be13667cd8909e000576e/html5/thumbnails/11.jpg)
Advantage of Open Charm at Threshold
e+e- colliders at threshold: CLEO-c, BESIII
e+e- y(3770)DDbar
Benefits for charm physics at threshold
• Clean
• Initial energy and quantum number
• D and Dbar can be fully reconstructed
• Absolute measurement
11
![Page 12: Open Charm Physics at BESIIItalks/images/8/80/PHIPSI11-Lilei.pdf · single tag D0bar double tag D0 single tag D-double tag D0 MARK-III method 19 Absolute Branching fraction Measurement](https://reader035.vdocuments.net/reader035/viewer/2022071223/607be13667cd8909e000576e/html5/thumbnails/12.jpg)
Singly Tagged D0/D- events
By analyzing part of data taken @ 3.773 GeV 12
2 2| |BC beam DM E p - Beam constraint mass distribution
D0Kp D+
Kpp
D0Kppp D0
Kpp0
BESIII
Preliminary
BESIII
Preliminary
BESIII
Preliminary
BESIII
Preliminary
Resolution: 1.3 MeV for pure charged modes; 1.9 MeV for modes with one π0.
![Page 13: Open Charm Physics at BESIIItalks/images/8/80/PHIPSI11-Lilei.pdf · single tag D0bar double tag D0 single tag D-double tag D0 MARK-III method 19 Absolute Branching fraction Measurement](https://reader035.vdocuments.net/reader035/viewer/2022071223/607be13667cd8909e000576e/html5/thumbnails/13.jpg)
Singly Tagged DS events Beam constraint mass distribution
By analyzing part of data taken @ 4.01 GeV
13
BESIII
Preliminary BESIII
Preliminary
DsKKp DsKsK
s ~ 1.6 MeV s ~ 1.4 MeV
2 2| |BC beam DM E p -
![Page 14: Open Charm Physics at BESIIItalks/images/8/80/PHIPSI11-Lilei.pdf · single tag D0bar double tag D0 single tag D-double tag D0 MARK-III method 19 Absolute Branching fraction Measurement](https://reader035.vdocuments.net/reader035/viewer/2022071223/607be13667cd8909e000576e/html5/thumbnails/14.jpg)
Leptonic Decay
Motivations
The decay constant of fD is related to the decay rate by
extract out fD & fDs, which in turn be used to calibrate LQCD.
R=(fBs/fB)/(fDs/fD)~1. fDs/fD can be used to estimate fBs/fB.
Leptonic Analysis D+
mnm, e+ne and tnt
Ds+mnm, e+ne and tnt
All strong interaction effects between the two quarks within the D+ meson is simply factorized into one parameter, the decay constant fD+.
14
![Page 15: Open Charm Physics at BESIIItalks/images/8/80/PHIPSI11-Lilei.pdf · single tag D0bar double tag D0 single tag D-double tag D0 MARK-III method 19 Absolute Branching fraction Measurement](https://reader035.vdocuments.net/reader035/viewer/2022071223/607be13667cd8909e000576e/html5/thumbnails/15.jpg)
Candidate events for D+ mnm
Mmiss2 ( GeV2 )
Leptonic Decay
BESIII
Preliminary
15
2 2 2| |miss miss missM E p -
With 4 fb-1 data at BESIII
~ 2.5%D
D
f
f
D
D+mnm
D+KL
0p
![Page 16: Open Charm Physics at BESIIItalks/images/8/80/PHIPSI11-Lilei.pdf · single tag D0bar double tag D0 single tag D-double tag D0 MARK-III method 19 Absolute Branching fraction Measurement](https://reader035.vdocuments.net/reader035/viewer/2022071223/607be13667cd8909e000576e/html5/thumbnails/16.jpg)
Semileptonic Decay
Semileptonic Analysis D0
K-l+nl, p-l+nl (l=e, m)
D+p0e+ne, e+ne,
D+ w/fe+ne
Motivations extract out the form factor, which in turn be used to
calibrate LQCD calculations .
extract the |Vcs| and |Vcd|, can be used to test the sides Bd unitary triangles and provide indication for new physics.
D0
K-
l
nl
D0
p-
l
nl
16
For pseudo-scalar decays, the decay rate G relates to form factor and CKM elements by
22 3 2 2
( )2 3
( )| | | ( ) |
24
Fcs d P
Gd D PlV p f q
dq
u
p
G
![Page 17: Open Charm Physics at BESIIItalks/images/8/80/PHIPSI11-Lilei.pdf · single tag D0bar double tag D0 single tag D-double tag D0 MARK-III method 19 Absolute Branching fraction Measurement](https://reader035.vdocuments.net/reader035/viewer/2022071223/607be13667cd8909e000576e/html5/thumbnails/17.jpg)
Candidate events for D0 K(p)-e+ne
17
D0 p‒e+ne
Umiss
D0 K‒e+ne
Umiss
D0 K‒e+ne
Eve
nts
/0
.00
4 G
eV
/c2
BESIII
Preliminary
BESIII
Preliminary
Umiss = Emiss‒pmiss .
22
1
N
miss cm i i
i
E E p m
- 1
N
miss i
i
P p
-and
Semileptonic Decay
By analyzing part of data taken @ 3.773 GeV
![Page 18: Open Charm Physics at BESIIItalks/images/8/80/PHIPSI11-Lilei.pdf · single tag D0bar double tag D0 single tag D-double tag D0 MARK-III method 19 Absolute Branching fraction Measurement](https://reader035.vdocuments.net/reader035/viewer/2022071223/607be13667cd8909e000576e/html5/thumbnails/18.jpg)
18
Prospect for measurements at BESIII
|Vcs| and |Vcd| at BESIII
D
K
D
p
DVcs/Vcs~ 2.6% DVcd/Vcd~ 2.7%
PDG10: DVcs/Vcs~ 3.5% DVcd/Vcd~ 4.8%
![Page 19: Open Charm Physics at BESIIItalks/images/8/80/PHIPSI11-Lilei.pdf · single tag D0bar double tag D0 single tag D-double tag D0 MARK-III method 19 Absolute Branching fraction Measurement](https://reader035.vdocuments.net/reader035/viewer/2022071223/607be13667cd8909e000576e/html5/thumbnails/19.jpg)
single tag D0bar
double tag D0
single tag D-
double tag D0 MARK-III method
19
Absolute Branching fraction Measurement
Br[D0 K-p+] and Br[D+
K-p+p+]
jijiDD
d
ji
N
j
ji
i
jiDDiiDD
s
i
BBNN
BBNBNN
,,
1
, )(
-
-
-
NN
ji N
d
ji
d
jiN
i N
s
i
s
i
dji
si
NNNN ,
1,1
2
exp,
,,
1
2exp,
2 )())
(
,
ss
• single tag events
• double tag events
• branching fraction for hadronic decays
Normalize decay branching fractions for D and B decays
![Page 20: Open Charm Physics at BESIIItalks/images/8/80/PHIPSI11-Lilei.pdf · single tag D0bar double tag D0 single tag D-double tag D0 MARK-III method 19 Absolute Branching fraction Measurement](https://reader035.vdocuments.net/reader035/viewer/2022071223/607be13667cd8909e000576e/html5/thumbnails/20.jpg)
Other topics going on
Search for CP violation through T-violation
D0K-pp0
D+KS
0pp0
20
Dalitz plot analysis
D+K+K-pp0
D+KS
0K+pp-
![Page 21: Open Charm Physics at BESIIItalks/images/8/80/PHIPSI11-Lilei.pdf · single tag D0bar double tag D0 single tag D-double tag D0 MARK-III method 19 Absolute Branching fraction Measurement](https://reader035.vdocuments.net/reader035/viewer/2022071223/607be13667cd8909e000576e/html5/thumbnails/21.jpg)
21
Summary
BESIII is accumulating data at a record speed.
More precisely measurements will come out soon at BESIII.
– Precise measurement on decay constant fD+& fDs
– Precise measurement on form factors and CKM matrix
– Precise measurement on absolute branching fractions
– Search for CP or T violation in D-meson decays
– ……
![Page 22: Open Charm Physics at BESIIItalks/images/8/80/PHIPSI11-Lilei.pdf · single tag D0bar double tag D0 single tag D-double tag D0 MARK-III method 19 Absolute Branching fraction Measurement](https://reader035.vdocuments.net/reader035/viewer/2022071223/607be13667cd8909e000576e/html5/thumbnails/22.jpg)
22
TNANKS!!
%d0%93%d0%90%d0%a3%d0%97%20%20%d0%a0%d0%9f%d0%a6%20%d0%b3 %d0%a3%d0%bb%d0%b0%d0%bd %d0%a3%d0%b4%d1%8
%d1%81%d0%b8%d1%81%d1%82%d0%b5%d0%bc%d0%b0 %d0%bd%d0%b0%d0%bf%d0%be%d0%bb%d1%8c%d0%bd%d0%be%d0%b3%d0
%d0%a3%d1%87%d0%b5%d0%b1%d0%bd%d1%8b%d0%b9%d0%9f%d0%bb%d0%b0%d0%bd %d0%a4%d1%83%d0%bd%d0%b4%d0%9c%d0
%d0%9d%d0%b0%d0%b2%d1%87%d0%b0%d0%bb%d1%8c%d0%bd%d0%be %d0%bc%d0%b5%d1%82%d0%be%d0%b4%d0%b8%d1%87%d0
%d0%9f%d1%80%d0%be%d0%b3%d1%80%d0%b0%d0%bc%d0%bc%d0%b0 %d0%a1%d1%8a%d0%b5%d0%b7%d0%b4%d0%a2%d0%b5%d1
%d0%b5 %d0%b5%d0%ba%d1%80%d0%b0%d0%bd %d0%b4%d0%be%d1%80%d0%b0%d0%bd%d0%b8%d0%ba%d0%b8 %d0%bb%d1%8e%
%d0%9f%d0%be%d0%bb%d0%be%d0%b6%d0%b5%d0%bd%d0%b8%d0%b5 %d0%9f%d0%be%d1%81%d0%bb%d1%8b%20%d0%9f%d0%be
%d0%a3%d1%87%d0%b5%d0%b1%d0%bd%d0%b8%d0%ba%d0%b8%20%d0%98%d0%b7%d0%b4 %d0%b2%d0%b0%20%d0%9c%d0%98%d0
%d0%a8%d0%b0%d0%b1%d0%bb%d0%be%d0%bd %d0%a0%d0%9f %d0%b0%d1%81%d0%bf%d0%b8%d1%80%d0%b0%d0%bd%d1%82%d
%d0%9c%d0%b0%d0%b3 %d0%95%d0%ba%d0%b1 %d0%a2%d0%b5%d1%85%d0%bd%d0%be%d0%bb%d0%be%d0%b3%d1%96%d1%97%2
%d0%9c%d0%b0%d0%b3 %d0%95%d0%ba%d0%b1 %d0%91%d1%96%d0%be%d1%82%d0%b5%d1%85%d0%bd%d0%be%d0%bb%d0%be%d
%d0%a1%d0%b1%d0%be%d1%80%d0%bd%d0%b8%d0%ba%20%d0%9c%d0%b5%d0%b4 %20%d0%b7%d0%b0%d0%b2 %20%d0%b4%d0%b
%d0%9a%d0%a3%d0%a8%d0%9d%d0%86%d0%a0%d0%95%d0%9d%d0%9a%d0%9e%20%d0%9e %d0%90 %d0%9e%d0%91%d0%9b%d0%8
%d0%9a%d0%b0%d1%82%d0%b0%d0%bb%d0%be%d0%b3 %d0%9c%d0%be%d0%bb %d0%a1%d0%bf%d0%b5%d1%86 %d1%83%d0%ba%
1060204 %d0%bb%d0%b8%d1%81%d1%82%d0%be%d0%b2%d0%ba%d0%b0 %d0%bf%d0%be %d1%82%d0%b5%d0%bf%d0%bb%d0%be
%d0%a4%d0%93%d0%9e%d0%a1%203 %20%d0%9b%d0%b5%d1%87%d0%b5%d0%b1%d0%bd%d0%be%d0%b5%20%d0%b4%d0%b5%d0%b
%d0%bf%d1%80%d0%be%d0%b5%d0%ba%d1%82%d0%b8%d1%80%d0%be%d0%b2%d0%b0%d0%bd%d0%b8%d0%b5 %d0%b2%d0%bd%d1
%d0%a1%d0%b1%d0%be%d1%80%d0%bd%d0%b8%d0%ba %d0%a1%d1%8a%d0%b5%d0%b7%d0%b4%d0%a2%d0%b5%d1%80%d0%b0%d0