LEP programme Final report Peter Kluit
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Transcript of LEP programme Final report Peter Kluit
15 november 2004 SAC presentation 1
LEP programme Final reportPeter Kluit
Thanks to: Wes Metzger, Jan Timmermans
and my LEP collegues
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LEP construction
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L3
DELPHI
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• First study B. Richter 1976
C~43 km, E=2*100 GeV, L=1032 cm-2s-1, 8 interaction points
•Les Houches study 1979
study of Z production and decay
study of WW production
Higgs search
searches for new leptons, quarks
3 and 4 jet structures
• Start construction 1983: C=27 km
• NIKHEF joins DELPHI & L3
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Events/experiment:
4.5 M Z events LEP1
10000 WW events 600 ZZ events 250 single-W events
LEP1 (1989-1995): ~200 pb-1/exp LEP2 (1996-2000): ~700 pb-1/exp
LEP2
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Z line shape
Moriond 1990:
mZ = 91171 ± 12 ± 32 (incl. ELEP) MeV
Z = 2538 ± 26 ± 28 MeV
N = 3.04 ± 0.12
First evidence 3 generations
Now status up to end 2003:
mZ = 91187.5 ± 2.1 MeV
Z = 2495.2 ± 2.3 MeV
N = 2.9841 ± 0.0083
One of the main LEP results
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Beam energy precision 0.2 MeV from resonant depolarisation
But corrections needed due to:
TIDES LEVEL LAKE TGV
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Vertex Detectors:
Precise -lepton
b-quark studieshere the DELPHI LEP2
vertex detector
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Rb = b / had and top quark mass
Summer 1992:
b = 3739 MeV I3b = -1/2
(370 MeV; for I3b =0: 24 MeV)
Top quark must exist
Now (end 2003):
Rb determined with 0.3%
Rb is also sensitive to top quark mass,
but much less than sin2qeff !
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Top mass: predicted by LEP
Prediction mtop from EW fit
EPS93 Marseille:
mtop = 166 –19 -22 GeV
ICHEP94 Glasgow:
mtop = 178 -11 -19 GeV
and CDF saw excess due to top at
mtop = 174 -10 -23 GeV
EPS95 Brussels: both CDF and D0 observed top at predicted mass.
+17 +19
+11 +18
+10 +13
Great success Standard Model
(Nobel prizes for ‘t Hooft and Veltman)
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Two most precise sin2eff values from
SLD ALR and LEP A0,b differ by 2.9
lept
FB
SM: 0.1036
A0,b (and also A0,c ) prefer a high
value for the Higgs boson massFBFB
A puzzle left ….. : comparison sin2qefflept
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lepton: a puzzle solved
lifetime related to lifetime, mass, mass and leptonic branching ratio
Up to 1992 a 2-2.3 discrepancy between the coupling constants g and g
In 1992 a new, more precise mass by BES
Now - -e universality tested at few per-mille, thanks to high precision vertex detectors
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Bs oscillations: to be discovered
00
expcos(11
)( 00
ss B
s
B
ss
ttmABBP
ms > 14.4 ps-1 at 95% C.L.
Continuous improvements in analysis techniques
Bd oscillations discovered at LEP
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B physics and CKM matrix
Excellent agreement with sin2bfrom BaBar/Belle
Profound test of SM charged current sector
• |Vtd| from Bd0 – Bd
0 oscillations
• |Vts| from Bs0 - Bs
0 oscillations
• |Vcb| from semileptonic bcl transitions
• |Vub| from semileptonic bul transitions
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QCD: test of gluon selfcouplingFrom fit to angular distributions in 4-jet events.
Rel. strength of couplings qqg, ggg, gqq depends on gauge group through Casimir factors CF , CA , TF
TF /
CF
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QCD: running of s
Results from fits to different event shape variables.
Combined fit at all energies:
s(MZ) = 0.1201 0.0003
0.0009
0.0009
0.0047
(Note this year Nobel Prize)
(stat)
(exp.syst)
(theor.hadr.)
(theor.ev.shapes)
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only exchange
No ZWW vertex
WW cross section
Clear evidence for the
SU(2) x U(1) Gauge structure
CC03 diagrams:
Theory predictions include full O(em) corrections; theory error 0.5%
Triple
Gauge Coupling
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Single W WW
DLO
Quartic Gauge Couplings
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W mass reconstruction• Reconstructed directly from the decay products
•Constrained fits improve mass
resolution from 8 GeV to 3 GeV
before 4C fit
after 4C fit
qqqq
qqqqe
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W mass: LEP combined results (end 2003)
•Not yet final
•Working on systematics, mainly in 4q
Apart from NuTeV result ( scattering)
Very good agreement between direct and indirect measurements
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We searched…..
and searched…..
and searched…..
and searched…..
and searched…..But sometimes……
No Higgses, 4th-generation, sleptons, squarks, charginos, neutralinos....
Large part of the MSSM parameter space excluded
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•1995: 130-136 GeV
•4-jet events•Sum of di-jet masses
with smallest M
•16 events (8.3 exptd)
•Prob. accumulation in 6.3 GeV bin: 0.01%
ALEPH
Why it is good to have more than one experiment
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SM Higgs search
Higgs strahlung: dominant WW fusion: small(can go beyond ‘kinematical limit’)
Final states: (Higgs to bb or )
• bbqq (4-jet channel)
• bb (missing energy channel)
• bbee, bb (leptonic channel)
• bb, bb (tau channel)
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ALEPH Higgs candidate
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•Small excess around 116 GeV but less than 2 (mainly coming from ALEPH candidates and from four-jet events)
•Excess was 2.9 on 3/11/2000
• CLs = CLs+b / CLb
• when CLs < 0.05 the hypothesis is rejected at 95% CL
Lower limit on Higgs mass
MH > 114.4 GeV (115.3 expected)
Final LEP Higss search results
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Results of different fits:
• using only Z pole data
• using all data
• using all data but NuTeV
%3.1410/7.14/
89
5.171
2
12245
9.114.9
probndof
GeVm
GeVm
H
t
%5.415/4.25/
96
3.174
2
6038
5.44.4
probndof
GeVm
GeVm
H
t
%5.2714/7.16/
91
3.175
2
5536
4.43.4
probndof
GeVm
GeVm
H
t
Global electroweak fit
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• Good consistency between direct and indirect measurement of mt and mW
• Both prefer low Higgs boson mass
mH < 219 GeV at 95% CL
Light Higgs to be discovered at LHC
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Conclusions LEP was great!
Full gauge structure of the SM has been measured, and many measurements in good agreement with the SM prediction
Fantastic precision measurements of W and Z boson, b quark and lepton properties, including the CKM matrix
SM Higgs boson not yet found: MH > 114.4 GeV
NIKHEF was involved in many important analyses: total output: ~ 300 journal papers/experiment
PhD theses: 14 DELPHI, 35 L3 (of which 22 KUN)
Papers still to come: ~55 DELPHI and ~20 L3