standard model physics results from lep2
TRANSCRIPT
Standard Model Physics
Results from LEP2
Stephan Wynhoff
CERN
on behalf of the LEP collaborations
Aleph, Delphi, L3, Opal
5th International Symposium on Radiative CorrectionsCarmel, USA
11.-15. September 2000
• Fermion Pair Production
Cross sections and Asymmetries
S-matrix
Contact interactions
• Boson Cross Sections
ZZ Production
Single W Production
• W+W−Production
Cross Section
Branching Fractions
• W Mass Measurement
Mass extraction
Systematic Errors
Comparison of Direct and Indirect Results
• Standard Model Fits
Stephan Wynhoff Standard Model Physics Results from LEP2 2
10-4
10-3
10-2
10-1
1
10
80 100 120 140 160 180 200 220s /GeV
σ/nb
88 90 92 940
10
20
30
1990-19921993-19951996-19981999-2000 (prel.)
mH=114 GeV
e+e– → hadrons
e+e– → HZ → qq_qq
_
e+e–→ W+W−
→ qq_qq
_
e+e–→ ZZ→ qq
_qq
_
L3
• large data statistics at the Z pole:
15 million hadronic and 2 million leptonic events
• above the Z resonance:
luminosity 590 – 630 pb−1 per experiment
• more than 8000 W-pair events per experiment
Stephan Wynhoff Standard Model Physics Results from LEP2 3
See LEP2MC workshop proceedingshep-ph/0005309, hep-ph/0007180
2-Fermion Processes
• ZFITTER, KKMCbetter than 0.2% precision in σtot of hadrons, leptons
• KKMC covers LEP, LC, µ-colliders, τ - and b-factories.
4-Fermion Processes
• RacoonWW, YFSWW3σ(W+W−) to 0.4%. (double-pole approx. above thresh-old.)
• WPHACT, grc4f, WTO, ...σ(Weν) to 4-5%. (fermion loop scheme.)
• YFSZZ, ZZTOσ(ZZ) to 2%.
⇓
Excellent match in precision
Experiment ⇐⇒ Theory
Stephan Wynhoff Standard Model Physics Results from LEP2 4
e−
e+
f
f
PP
ISR
FSR
• Initial State Radiation
• Pair Production:
• Final State Radiation
√s′:= mass of outgoing lepton pair or γ∗/Z propagator
→ high energy events:√
s′ > 0.85√
s
10 2
10 3
50 100 150 2001
10
10 2
10 3
10 4
50 100 150 200
0
20
40
60
80
100
120
140
160
180
50 100 150 2000
20
40
60
80
100
120
50 100 150 200
√s′ /GeV
Eve
nts
→
√s′ /GeV
Eve
nts
√s′ /GeV
Eve
nts
→
√s′ /GeV
Eve
nts
→
OPAL 205.4 GeV preliminary
(a) hadrons (b) e+e-
(c) µ+µ- (d) τ+τ-
Stephan Wynhoff Standard Model Physics Results from LEP2 5
Cro
ss s
ectio
n (p
b)√s
´/s
> 0.85
e+e−→hadrons(γ)e+e−→µ+µ−(γ)e+e−→τ+τ−(γ)
LEPpreliminary
√s
(GeV)
σ mea
s/σ S
M
1
10
10 2
0.8
0.9
1
1.1
1.2
120 140 160 180 200 220
Stephan Wynhoff Standard Model Physics Results from LEP2 6
Differential cross sections for Muon-, Tau-pair production
Preliminary LEP Averaged dσ/dcosθ (µµ)183 GeV
cosθf
dσ/d
cosθ
(pb
)
189 GeV
cosθf
dσ/d
cosθ
(pb
)
192 GeV
cosθf
dσ/d
cosθ
(pb
)
196 GeV
cosθf
dσ/d
cosθ
(pb
)
200 GeV
cosθf
dσ/d
cosθ
(pb
)
202 GeV
cosθf
dσ/d
cosθ
(pb
)
0
2
4
-1 -0.5 0 0.5 10
1
2
3
4
-1 -0.5 0 0.5 1
0
1
2
3
4
-1 -0.5 0 0.5 10
1
2
3
4
-1 -0.5 0 0.5 1
0
1
2
3
4
-1 -0.5 0 0.5 10
1
2
3
-1 -0.5 0 0.5 1
Use for limits on
• Contact interactions
• Fermion size
• Extra dimensions, TeV strings, gravitons
Stephan Wynhoff Standard Model Physics Results from LEP2 7
For
war
d-B
ackw
ard
Asy
mm
etry √s
´/s
> 0.85
e+e−→µ+µ−(γ)e+e−→τ+τ−(γ)
LEPpreliminary
√s
(GeV)
AF
B
mea
s -AF
B
SM
0
0.2
0.4
0.6
0.8
1
-0.2
0
0.2
120 140 160 180 200 220
Stephan Wynhoff Standard Model Physics Results from LEP2 8
Fermion Pair - Heavy Flavours
s (again) the ratio of cross sections
0.14
0.16
0.18
0.2
0.22
0.24
0.26
80 100 120 140 160 180 200√s (GeV)
Rb
Rb
LEP preliminary
√s’/√s > 0.1 , 0.85
0.14
0.16
0.18
0.2
0.22
0.24
0.26
0.28
0.3
0.32
80 100 120 140 160 180 200√s (GeV)
Rc
Rc
LEP preliminary
√s’/√s > 0.1 , 0.85
-0.2
0
0.2
0.4
0.6
0.8
1
80 100 120 140 160 180 200√s (GeV)
b-A
sym
met
ry
Ab FB
LEP preliminary
√s’/√s > 0.1 , 0.85
-0.2
0
0.2
0.4
0.6
0.8
1
1.2
80 100 120 140 160 180 200√s (GeV)
c-A
sym
met
ry
Ac FB
LEP preliminary
√s’/√s > 0.1 , 0.85
Stephan Wynhoff Standard Model Physics Results from LEP2 9
• Measure Interference between γ and Z (jhad)
-4
-3
-2
-1
0
1
2
3
4
50 75 100 125 150 175 200
s [GeV]
σ int/σ
tot [
%]
no cuts'/s > 0.85
σ0a(s) =
4
3πα2
gafs
+jaf(s−m2
Z) + raf s
(s−m2Z)
2 +m2ZΓ
2Z
, for a = tot, fb,
A0fb(s) =
3
4
σ0fb(s)
σ0tot(s)
, with σ0fb =
4
3(σf − σb) .
• Photon exchange
• Z-Boson exchange
• γ/Z interference
“Standard” fits: fix gaf and jaf ZFITTER, TOPAZ0
S-Matrix fits: fix gaf only ZFITTER, SMATASY
Stephan Wynhoff Standard Model Physics Results from LEP2 10
-0.5
0
0.5
1
1.5
91.17 91.18 91.19 91.2mZ [GeV]
j had
tot
68% CL
SM
L3 Z dataL3 data ≤ 189 GeVLEP + Tristan (potential)
MZ[MeV] jtothad corr.
L3 Z data 91 185.2±10.3 0.44±0.59 -0.95L3 ≤ 189GeV 91 187.5±3.9 0.31±0.13 -0.57LEP + Tristan: ±2.3 ±0.04 -0.28
Stephan Wynhoff Standard Model Physics Results from LEP2 11
L =1
1 + δef
∑i,j=L,R
ηijg2
Λ2ij
(eiγµei)(fjγµfj),
e+
e−
l+, q−
l−, q
g2 / Λ2
g Coupling, byconvention g2/4π = 1
ηij Helicity amplitudes,choose |ηij| = 0, 1
Λ Energy scale
dσ
d cos θ=
dσSM
d cos θ+ cint(s, cos θ)
1
Λ2+ cci(s, cos θ)
1
Λ4.
ηRR ηLL ηLR ηRLAA ±1 ±1 ∓1 ∓1VV ±1 ±1 ±1 ±1RR ±1 0 0 0LL 0 ±1 0 0
LEP Preliminary 130-202 GeV
Λ- (TeV) Λ+ (TeV)
LL 10.2 12.8
RR 9.7 12.3
VV 17.2 20.4
AA 13.9 17.6
Λ- Λ+
20. 0 20.
Stephan Wynhoff Standard Model Physics Results from LEP2 12
Z
Z
e−
e+
f
f
f'
f'
Z
Z
e−
e+
f
f
f'
f'
0
0.5
1
1.5
170 180 190 200
Ecm [GeV]
σZZ
NC
02 [p
b]
LEP Summer 00 - Preliminary20/07/2000
±2.0% uncertainty
ZZTO
YFSZZ
Stephan Wynhoff Standard Model Physics Results from LEP2 13
e+ e+
γ
W
Q2→0
e− νe
WMW
2s
f– ‘
f
0
0.5
1
160 170 180 190 200 210
Ecm [GeV]
σ(e+
e– → e
νW)
[pb]
LEP Preliminary21/07/2000
±5.0% uncertainty
grc4fWPHACT IFL/α(t)
W → ff-’
Stephan Wynhoff Standard Model Physics Results from LEP2 14
• W-pair production at LEP
e– W–
f
f´νe
W+
f
f´
e+
e–
e+γ,Z
W–
f
f´
W+ f
f´
SM branchings Br(W → qq′) = 67.6%Br(W → lν) = 10.8% per lepton flavour
D E L P H I R u n : E v t :
B e a m :
DA S :
P r o c :
S c a n :
1 0 4 . 4 Ge V 2 9 - Ap r - 2 0 0 0
2 9 - Ap r - 2 0 0 0
1 1 : 4 3 : 3 4
2 9 - Ap r - 2 0 0 0
109372 8483
T a n a g r a
• Fully hadronic: 45.6% 4 jets
High Multiplicity, balanced events
Y
XZ
• Semileptonic: 3×14.6% 2 jets, 1 lepton
Hadronic energy plus high energy lepton ornarrow jet (τ )
OOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOO
OOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOO
OOOOO
OOOO
OOOOOO
OOOOOOOOOOOOO
OOOOOOOO
OOOOO
OOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOO
OOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOO
OOOOO
OOOO
OOOOOO
OOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOO
OOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOO
OOOOO
OOOO
OOOOOO
OOOOOOOOOOOOO
OOOOOOOO
OOOOO
OO
OO
OO
OO
OO
OO
OO
OO++++
• Fully leptonic: 10.6% 2 leptons
Low multiplicity, acoplanar, missing energy
Stephan Wynhoff Standard Model Physics Results from LEP2 15
0
5
10
15
20
160 170 180 190 200 210
Ecm [GeV]
σWW
[pb]
LEP Preliminary21/07/2000
Gentle 2.1 (±0.7%)
RacoonWW / YFSWW 1.14
0
5
10
15
20
160 170 180 190 200 2100
5
10
15
20
160 170 180 190 200 210
RacoonWWYFSWW 1.14
16
17
18
Excellent agreement with
• RacoonWW• YFSWW
at Ecm > 170 GeV
Stephan Wynhoff Standard Model Physics Results from LEP2 16
21/07/2000
Br(W→hadrons) [%]
ALEPH 67.22 ± 0.53
DELPHI 67.81 ± 0.61
L3 68.47 ± 0.59
OPAL 67.86 ± 0.62
LEP 67.78 ± 0.32
66 68 70
Br(W→hadrons) [%]
Summer 00 - Preliminary - [161-207] GeV
DELPHI [161-202] GeV
L3 [161-202] GeV
Stephan Wynhoff Standard Model Physics Results from LEP2 17
• Indirect determination of |Vcs|:Br(W → hadrons)
1 −Br(W → hadrons)=
∑ ∣∣∣∣∣V2ij
∣∣∣∣∣
1 +
αs
π
• Direct determination of |Vcs| from tagged charm:
OPAL :Γ(W → cX)
Γ(W → had)= 0.47 ± 0.04 ± 0.06
LEP |Vcs|Indirect 0.989 ± 0.016
Direct 0.95 ± 0.08
Stephan Wynhoff Standard Model Physics Results from LEP2 18
21/07/2000
W Leptonic Branching Ratios
ALEPH 11.19 ± 0.34DELPHI 10.33 ± 0.45L3 10.22 ± 0.36OPAL 10.52 ± 0.37
LEP W→eν 10.62 ± 0.20
ALEPH 11.05 ± 0.32DELPHI 10.68 ± 0.34L3 9.87 ± 0.38OPAL 10.56 ± 0.35
LEP W→µν 10.60 ± 0.18
ALEPH 10.53 ± 0.42DELPHI 11.28 ± 0.56L3 11.64 ± 0.51OPAL 10.69 ± 0.49
LEP W→τν 11.07 ± 0.25
LEP W→lν 10.74 ± 0.10
10 11 12
Br(W→lν) [%]
Summer 00 - Preliminary - [161-207] GeV
DELPHI [161-202] GeV
L3 [161-202] GeV
Indirect extraction from TEVATRON:
Br(W → eν) [%]
CDF 10.50 ± 0.30
D0 10.39 ± 0.35
10.43 ± 0.25
Stephan Wynhoff Standard Model Physics Results from LEP2 19
q1
q2
e,µ,τ
ν
q2q1
q4q3
• reconstruct lepton and jets
• impose kinematic constraints:
E and *p conservation → 1C for qq+ν, 4C for qqqqequal masses of recontructed W’s → +1C
• special for qqqq events: jet pairing problem
q2q1
q4q3
q2q1
q4q3
q2q1
q4q3
→ choose best pairing
• also gluon radiation is taken into account→ split into 4 and 5 jet sample (D,O)
Stephan Wynhoff Standard Model Physics Results from LEP2 20
L3
minv [GeV]
Num
ber o
f Eve
nts
/ 1 G
eV1999 Data qqeνM.C. reweighted
M.C. background (a)
preliminary
MW = 80.28 ± 0.19 GeV
0
20
40
60
60 70 80 90 1000
10
20
30
40
50
60
70
80
90
100
50 55 60 65 70 75 80 85 90 95
MW (GeV/c2)
Eve
nts
per
1 G
eV/c
2
ALEPH Preliminaryµνqq selection
√s = 191.6,195.5,199.5,201.6 GeV
Data (Luminosity = 237 pb-1)
MC (mW = 80.60 GeV/c2)
Non-WW background
DELPHI preliminary
0
10
20
30
40
50
60
70
80
90
50 55 60 65 70 75 80 85 90 95 100
W mass (GeV/c2)
even
ts /
2 G
eV/c
2
0
50
100
150
200
70 80 90m / GeV
Ev
ents
/ G
eV qqqq 4-jet
OPAL 192-202 GeV preliminary
→ compare reweighted Monte Carlo to data (A,L,O)→ convolute differential cross-section with resolution
function (D,O)→ fit Breit-Wigner curve to measured mass spectrum (O)
Stephan Wynhoff Standard Model Physics Results from LEP2 21
• all LEP2 data until 1999 included:
80 80.2 80.4 80.6 80.8 81
MW [GeV]
preliminary
80 80.2 80.4 80.6 80.8 81
ALEPH
DELPHI
L3
OPAL
LEP
80.440 ± 0.064 GeV
80.380 ± 0.071 GeV
80.375 ± 0.077 GeV
80.485 ± 0.065 GeV
80.427 ± 0.046 GeV
χ2/dof = 27.1/29
• LEP value is a combination of individual measurementsfrom the experiments for different channels and years
• contribution to total error from
statistics: 30 MeVsystematics: 36 MeV
Stephan Wynhoff Standard Model Physics Results from LEP2 22
• LEP energy error ∆Ebeam = 21 MeV
⇒ ∆MW = ∆EbeamEbeam
· MW = 17 MeV
• new LEP spectrometer → precision ∆Ebeam < 15 MeV(not yet achieved)
• Final State Interactions in qqqq events
γ,Z
W–
W+
πo πo
K+ K+
π– π–
ColourReconnection
Bose-Einstein
• cross-talk affects reconstruction of invariant masses
Stephan Wynhoff Standard Model Physics Results from LEP2 23
Identical pions close in phase space:Q2 = squared 4-momentum difference
Q [GeV]
R2
WW qqlv data - 189 GeV•
Z→light quark data - 91 GeV¬
L3 preliminary
0.8
1
1.2
1.4
1.6
1.8
2
0 0.2 0.4 0.6 0.8 1 1.2 1.4
Intra-W effects:
W± � Zdecays (Z �→ bb)
Cross talk in W+W− → qqqq ?
Q [GeV]
D, (±
,±)/
0.04
GeV
L3 data
inter-W correlation
no inter-W correlation
p < 1.5 GeVL3
0.80.9
11.11.21.31.41.5
0 0.2 0.4 0.6 0.8 1 1.2 1.4
→ BE correlations only inside each W!?
Stephan Wynhoff Standard Model Physics Results from LEP2 24
Compare particle flow between jets from
C
D
A
B
• same (A,C)
• different (B,D)
W-Boson
0
2
4
6
0 50 100 150 200 250 300 350particle flowparticle flowparticle flowparticle flowparticle flow φ
1/N
evt d
σ/dφ
ALEPHpreliminary
particle flow
data (@ 189 GeV)WWZZqqγ
0
2
4
6
0 0.5 1 1.5 2 2.5 3 3.5 4norm. particle flownorm. particle flownorm. particle flownorm. particle flownorm. particle flow φr
1/N
evt d
σ/dφ
r
norm. particle flow
data (@ 189 GeV)WWZZqqγ
W-jets W-jets
ALEPHpreliminary
A B C D
0.75
1
1.25
1.5
0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1φr
1/N
evt d
σ/dφ
r(A
+C)/
(B+D
)
ALEPH preliminary
data 189, 196, 200 GeV combined
KoralW, ki = 0.
KoralW, ki = 0.6
KoralW, ki = 2.3
KoralW, ki = 1000. L3, ALEPH:
R =dn/dφ(A+ C)
dn/dφ(B +D)
→ not yet statistically significant, but promising
Stephan Wynhoff Standard Model Physics Results from LEP2 25
• ∆MW = mqqqq −mqqlν probes possible effects of FSI
-0.5 0 0.5
∆MW [GeV]
preliminary
-0.5 0 0.5
ALEPH
DELPHI
L3
OPAL
LEP
0.032 ± 0.091 GeV
−0.011 ± 0.112 GeV
0.190 ± 0.130 GeV
−0.103 ± 0.111 GeV
0.005 ± 0.051 GeV
FSI 0.056 GeV
→ no indication for mass shift due to FSI
• FSI systematic error is estimated by comparingMC models
for BE → with and w/o cross-talkfor CR → SK I, SK II, SK II’, ARIADNE I and II,
HERWIG, GH
all experiments are affected in the same way!
• error on qqqq due to BE: 25 MeV CR: 50 MeV
statistical error component: 34 MeV (qqqq only)
Stephan Wynhoff Standard Model Physics Results from LEP2 26
typical example
Source Systematic Errors on MW in MeVqq+ν qqqq Combined
Colour Reconnection – 50 13Bose-Einstein Correlations – 25 7LEP Beam Energy 17 17 17ISR / FSR 8 10 8Hadronisation 26 23 24Detector Systematics 11 8 10Other 5 5 4Total Systematic 35 64 36Statistical 38 34 30Total 51 73 47
• due to FSI → contribution to combined MW measurement:
qqqq 27% and qq+ν 73%
Stephan Wynhoff Standard Model Physics Results from LEP2 27
• comparison with other W mass measurements:
W-Boson Mass [GeV]
mW [GeV]
χ2/DoF: 0.1 / 1
80 80.2 80.4 80.6
pp−-colliders 80.452 ± 0.062
LEP2 80.427 ± 0.046
Average 80.436 ± 0.037
NuTeV/CCFR 80.25 ± 0.11
LEP1/SLD/νN/mt 80.386 ± 0.025
Stephan Wynhoff Standard Model Physics Results from LEP2 28
0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
1.5 1.6 1.7 1.8 1.9 2 2.1 2.2 2.3 2.4 2.51.5 2.0 2.5ΓW[GeV]
ALEPH 2.17±0.20
DELPHI 2.09±0.15
L3 2.19±0.21
OPAL 2.04±0.18
LEP 2.12±0.11
LEP Preliminary : Summer 2000
• compare direct width determination by CDF
ΓW = 2.06 ± 0.13 GeV
Stephan Wynhoff Standard Model Physics Results from LEP2 29
10
10 2
10 3
80.25 80.5mW [GeV]
mH [G
eV]
W-Boson Mass [GeV]ALEPH
DELPHI
L3
OPAL
LEPpp
Average
80.440±0.064
80.380±0.071
80.375±0.077
80.485±0.065
80.427±0.04680.451±0.062
80.436±0.037
mt =174.3±5.1 GeV
∆α(5)
had =0.02755±0.00046
Stephan Wynhoff Standard Model Physics Results from LEP2 30
• compare direct MW and M t with fit to electroweak data:
80.2
80.3
80.4
80.5
80.6
130 150 170 190 210
mH [GeV]113 300 1000
mt [GeV]
mW
[G
eV]
Preliminary
68% CL
LEP1, SLD, νN Data
LEP2, pp− Data
• from electroweak fitswith LEP data: M t = 179+13
−10 GeVall data except direct MW: MW = 80.386 ± 0.025 GeV
Standard Model parameter relationsconfirmed at 1-loop level W W
b
t
Stephan Wynhoff Standard Model Physics Results from LEP2 31
•α(M2Z) is important ingredient in EW fits → M H
• running of α:
α(s) =α(0)
1 − ∆αlep(s) − ∆α(5)had(s) − ∆αtop
had(s)• ∆αlep(s) known to 3-loop level
• important is contribution from ∆α(5)had
→ less precise
∆α(5)had(s) ∝
∞∫
4M2π
R(s′) ds′
s′(s′ − s)
γ
q
q
γ
• the ratio R = σ(e+e− → hadrons)/σ(e+e− → µ+µ−)
can be measured and calculated in perturbative QCD• recent measurements by BES II are now included:
BES-II (preliminary 1999)
BES-II (1998)
MK1 normalised to pQCD
γγ2
MEA
RpQCD
√ s (GeV)
Sum of exclusive channels→
← Inclusive data {
0
0.5
1
1.5
2
2.5
3
3.5
4
1 1.25 1.5 1.75 2 2.25 2.5 2.75 3 3.25
Stephan Wynhoff Standard Model Physics Results from LEP2 32
Mass of the Higgs Boson
0
2
4
6
10 102
103
mH [GeV]
∆χ2
Excluded Preliminary
∆αhad =∆α(5)
0.02804±0.00065
0.02755±0.00046
theory uncertainty
∆α(5)had M H log(M H/ GeV) M H limit
[ GeV] (95% C.L.)
0.02804 ± 0.00065 60+52−29 1.78+0.27
−0.28 < 162 GeV
new BES included0.02755 ± 0.00046 88+60
−37 1.94+0.22−0.24 < 203 GeV
new BES and pQCD0.02738 ± 0.00020 104+59
−39 2.02+0.19−0.20 < 215 GeV
(Jegerlehner et al., Pietrzyk et al., Martin et al., includes new results on MW by Tevatronand on heavy flavours by SLD)
• the new values of ∆α(5)had yield
→ a better error on log(M H/ GeV)
→ a better agreement with Higgs searches at LEP
• the Higgs boson is light . . . but heavier than
M H > 112.3 GeV at 95% CL (limit from direct searches at LEP)
Stephan Wynhoff Standard Model Physics Results from LEP2 33
• Measurement of Fermion Pair Production in good agree-ment with Standard Model predictions
• Further improvement on MZ, jhad within S-Matrix ansatz
• No new (contact) interactions below 10-20 TeV
• Cross sections for Single W, W+W−, ZZ agree as well
• LEP measures W mass and width with increased precision
MW = 80.427 ± 0.046 GeVΓW = 2.12 ± 0.11 GeV
. . . in perfect agreement with fit to electroweak data
• outlook on LEP MW:
with 2000 data → statistical error × 0.85→ δMW = 30 − 40 MeV
• there is progress going on in α(M2Z) determination
• although we are always looking for deviations . . .
The Standard Model works
The Standard Model Higgs boson is light(and maybe already observed?)
Stephan Wynhoff Standard Model Physics Results from LEP2 34
133 - 202 GeV
0.6
0.65
0.7
0.75
0.8
0.85
0.9
-0.04 -0.02 0 0.02 0.04 0.06 0.08jb
tot
j b fb
1.2
1.3
1.4
1.5
1.6
1.7
1.8
1.9
2
-0.3 -0.2 -0.1 0 0.1 0.2 0.3jc tot
j c fb
Stephan Wynhoff Standard Model Physics Results from LEP2
133 - 202 GeV
Stephan Wynhoff Standard Model Physics Results from LEP2