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T.Hebbeker
p p
physics
Tevatron 2002
CMS 2007
UA1 1983
LHC 2008 ? 1.0
part II
Thomas HebbekerRWTH
WS 2003/2004
T.Hebbeker
p p
physics
Part I Introduction
Part II Standard Model Physics
Part III Higgs
Part IV New PhenomenaReferences
• cross section calculation• QCD and jets• W and Z• charm and bottom• top
T.HebbekerCross Section
Total inelasticcross section
Pointlike cross section
pp
2252 1010 cmfm −≈≈σ
2362
10 cms
−≈≤ασ
BACKGROUND
SIGNAL
strong
electroweak
p
p
Elastic cross section
strong, electromagnetic
Xsection relatively smallscattering angle tinyLUMINOSITY
LHCSignal / Background 1110−<
LUMINOSITY
T.HebbekerStructure FunctionsMeasurements:
F2 , F3 ... in DIS
(n,p,elm.,weak, Q2-depend.)
valence, sea, gluons...
Fits/parametrisations:• CTEQ
• MRST
T.HebbekerCross section calculation in pp
VdQsd F ),( 2σWanted:
Calculable:
Known:
VdQxxd ji
ijF ),,( 2σ
),( 2Qxf ii
kinematicalvariable
final state
sxx 21='s
),(),(),( 22
,
2
QxfQxfdxdxVdQsd
jjji
iijiF ∑∫=
σ
2Q
VdQxxd ji
ijF ),,( 2σ
Spectator jet
Q2 = („momentum transfer“)2
depends on final state
T.HebbekerCross Sections
at Hadron
Colliders
Note:
may trade:
energy luminosity
Example:
In principle top discovery at SPS !
Estimate of Xsection p p → W −X
Ansatz:
d u → W − (valence quarks)
σW (√
s) =∫ ∫
fd(x1) f u(x2) σdu(√
s′) dx1 dx2
s′ = x1 x2 s
Structure Functions:
Rough parametrisation:
fd(x) =0.2
xfu(x) = 2 fd(x)
Cross section (quark level):
σdu(√
s′) = σ0 ·
s Γ2W
(s′ − m2W )2 + m2
WΓ2W
σ0 =12π
m2W
·Γqq
ΓW
≈12π
m2W
·6
9≈
25
m2W
σdu(√
s′) ≈
25
m2W
·{
1 mW − ΓW /2 <√
s′ < mW + ΓW /20 else
Calculate:
σW (√
s) = 25 · 0.2 · 0.4·1
m2W
·∫ 1
xmin2
1
x2
[∫ xmax1
xmin1
1
x1dx1
]dx2
xmin2 ≈
m2W
s
xmin1 =
(mW − ΓW /2)2
x2 sxmax
1 =(mW + ΓW /2)2
x2 s
σW (√
s) ≈ 25 · 0.2 · 0.4 ·1
m2W
·∫ 1
xmin2
1
x2
[2
ΓW
mW
]dx2
σW (√
s) = −4 ·1
m2W
·ΓW
mW
· lnm2
W
s
Results:
1/GeV = 2 · 10−16 mmW = 80 GeVΓW = 2 GeV
σW (√
s) ≈ 4 nb · ln sm2
W
FERMILAB :σp(
√s) ≈ 25 nb
LHC(pp!) :σp(
√s) ≈ 40 nb
T.HebbekerQCD = Quantum Chromodynamics
Gauge theory: • quarks with 3 colors (r,g,b)
• 8 gluons (color + anticolor r,g,b) SU(3)spin 1
spin 1/2
T.Hebbekerself coupling, running, confinementnonabelian:
„Running“:
~ 1/distance
mesons and baryons „white“:
qqqqq
strongcoupling„constant“ Zm
T.HebbekerHadronization = Fragmentation
time
„string“
String model:
QCD:
soft
uud
d
Hadronization: non-perturbative
need models!
jet(to be defined)
hadrons
g q
q
hadrons
T.HebbekerCalculation of QCD processes
T.HebbekerHigher Order Corrections
Often: higher order corrections to differential cross section
modeled by LO prediction and „K factor“ (typ. 1 ... 2)
can be large in particular for QCD processes!
LO = Leading Order
NLO = Next to Leading Order
Difficulties for p p reactions:
• parton densities and fragmentation functions depend on order!
• factorization scale, renormalization scale, fragmentation scale
(Q2 parton density) (Q2 hard process) ....
T.Hebbekerjets
jets reveal hard processs (direction, energy)
experiment and theory must use the same language:
jets need to be defined: „jet algorithm“
parton (quark, gluon)
theory
Typical: 100 particles total
(14 TeV)
2-5 jets per event
hadrons
experiment
T.Hebbeker
Jet ev
ents
eta
3.7
0.0
-3.7
-1.2
1.2
phi
0.0
2PI
ET GeV
55
Max: 52.4
CDF
D0
T.Hebbekercone jets
potential problems: seed dependence, infrared sensitivity ...
several variations exist
Cone defined in projection, radius R = (typ = 0.7)
Isolated low energy particles are ignored
Sum of 4-momenta of objects inside cone = jet 4-momentum
ϕη , 22 )()( ϕη ∆+∆
T.HebbekerkT jets Example:
... several variations exist
b) each cluster:
2,iTi pd =
22,
2, ),min( ijjTiTij Rppd ⋅=
a) list of hadrons = clusters
each pair of clusters:
c) minimum of
combine or remove from list)
d) iterate: goto b)
till list empty
iij dd ,
T.HebbekerInclusive jet production
D0 1.8 TeV cone radius 0.7
)( 3
sO α
Conclusion: agreement with QCD over many orders of magnitude!
=NLO
T.Hebbekermultijet events
Measurealphas fromrelative fraction of events with2,3,... jets
CDF 1.8 TeV
cone radius 0.7
Test QCD
T.HebbekerSoft hadronic processes (LHC)
Elastic
(20 mb)
Inelastic
(80 mb)
(zero quantum numbers!)
diffractive (25 nb)
non-diffractive (55 nb)
T.HebbekerDouble-Diffractive Event
D0„r
apid
ityga
p“
T.HebbekerW and Z
measured at LEPreference for W mass measurement
• production cross section
• decay modes
• W mass
• W width
• (W polarization in top decays)
• ...
WWZ
W
mm
θθ 222
sin1cos −==
T.HebbekerW and Z discoveryDiscovery:
UA1, UA2
(1983)
Precision measurement
Z mass at LEP:
91.1876 +- 0.0021 GeV
νeW →
eeZ →
T.HebbekerW,Z: production and decay
W decay probability:
)(~ 22AVC ggNBr +
20%
70%
3%
3%
3%eeµµττ
bbccssdduu ++++νν
CNBr ~
33%
33%
11%
11%
11%νeνµντudcs
Z decay probability:
Clearsignature
T.HebbekerW,Z: mass
D0
1.8
TeV
Tevatron combined: GeV059.0456.80 ±GeV015.0±LHC:
LEP: GeV042.0±Run I
)cos1(22ν
ν φlTlTT EEM −=
)cos1(2 12212 φ−= ll EEM
T.HebbekerW: width
... difficult...
GeV047.0160.2 ±
D0 1.8 TeV
Monte Carlo
Tevatron combined: (indirect+direct)
T.HebbekerW,Z: production cross section
theory theory
T.Hebbekerpp-physics with charm and bottom
cross section huge !
• cross section
• new mesons/baryons/hybrids/... ?
• hadron masses
• hadron lifetimes
• branching fractions (rare decays ?)
• B0 mixing
• CP violaton
s
T.HebbekerExample: D meson masses
T.HebbekerReconstruction of decay vertices
D0
bbZ →
T.HebbekerExample:
decay length
L
)/(βγL
decay length:
Lab frame:
βγctL =
++ +→ KJB ψ/
T.HebbekerTop Discovery
Fermilab, 1995 CDF, D0
m ~ 175 GeV
GeVpp 1800
CDF
T.Hebbeker
)ln,(1sin1
2
2/1
HtWFW mmrGm
∆−⋅
=
θαπ
Top Physics• cross section
• decay modes
• top mass
• spin correlations
• ...
T.HebbekerTop Identification
cross section small (at 2 TeV)
l
b
b
ν
p p
E T
jet jet
jet
ldecay:
production:
ttpp →
bWt→Signature:
2 b jets+ leptons/jets/missing energy
νlqqW ,→
T.HebbekerTop event in D0
µ -
MTC
Jet 1
IP
SV
Jet 1
IP
SV
Jet 2
Run II(~ 100 events)
T.Hebbeker
Top event in CDFRun II
(~ 100 events)
T.HebbekerTop Pair Production
gg contributes
• 15% at 2 TeV
• 95% at 14 TeV
T.HebbekerTop Mass
CDF
Run I
νbbqqltt→
GeV1.53.174 ±
Tevatron Run I
CDF + D0:
Using massconstraints
...νlW →
LHC: +- 1 GeV
T.HebbekerTop Cross Section and Top Mass
cross section measurement = indirect mass determination!
T.Hebbeker
Spin of top related to lepton direction in
due to parity violation!
Top quark lifetime
much shorter than „hadron formation time“
Spin Correlations - introduction
smG tF
t25
32 10528 −⋅≈≈π
τ
scfmh24103~/1 −⋅>τ
If is produced in a certain spin state, e.g.
spins of the two quarks are correlated!
lbWbt ν→→
01 Stt
T.HebbekerTop Spin Correlations simulation
LHC
direction
lepton 1 direction lepton 2
ttqq →mostly
in
13 S
ttgg →mostly
in
01 S
(Tevatron)
(LHC)
can distinguish!
T.Hebbeker
p p
physics
Part I Introduction
Part II Standard Model Physics
Part III Higgs
Part IV New PhenomenaReferences
• cross section calculation• QCD and jets• W and Z• charm and bottom• top