Physics at HERA - DESYPhysics at HERA Katja Krüger ... comparison with Dirac formula ... xD xdv xD...
Transcript of Physics at HERA - DESYPhysics at HERA Katja Krüger ... comparison with Dirac formula ... xD xdv xD...
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Physics at HERA
Katja Krüger KirchhoffInstitut für Physik
H1 Collaborationemail: [email protected]
Summer Student Lectures1013 August 2009
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Katja Krüger Physics @ HERA 2
ep Scattering & Structure Functions
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Katja Krüger Physics @ HERA 3
„The“ HERA Textbook Plots
?
quarks ?
gluons ?
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Katja Krüger Physics @ HERA 4
Structure Functions F1 & F2
● the DIS cross section can be written as
● comparison with Dirac formula
➔ F2 corresponds to electric field of the parton
➔ F1 corresponds to spin of the parton
d2dx dQ2=
42
Q4
1x [1−y F2 x ,Q2
y2
22 x F1x ,Q2]
=42
Q4
1x
E 'E [F 2 x ,Q2 cos2
2
Q2
2 x2 M p2 2 x F 1 x ,Q2 sin2
2 ]
dd Q2
Dirac
=42 z2
Q4 E 'E
2
[cos2 2
Q2
2 M2 sin2 2 ]
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Katja Krüger Physics @ HERA 5
Scaling: F2 independent of Q2
SLAC 1972
independent of Q2, we always see the same partons (=quarks)
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Katja Krüger Physics @ HERA 6
(Naive) Quark Parton Model
● proton consists of 3 partons, identified with the QCD quarks
● during the interaction proton is „frozen“
● electron proton scattering is sum of incoherent electron quark scatterings
● proton structure is defined by parton distributions F2 x , Q2=x∑ eq
2 q x
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Katja Krüger Physics @ HERA 7
How does F2(x) look like?
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Katja Krüger Physics @ HERA 8
How does F2(x) look like?
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Katja Krüger Physics @ HERA 9
How does F2(x) look like?
from Povh et al., „Teilchen und Kerne“
what happens at low x?
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Katja Krüger Physics @ HERA 10
Scaling Violations
at smaller & larger x, the amount of quarks depends on Q2!
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Katja Krüger Physics @ HERA 11
Parton Evolution● number of partons changes with Q2
● Q2 can be interpreted as resolving power: Q2∝ℏ/2
small Q2:● many partons with large x● (nearly) no partons at low x
large Q2:● less partons with large x● more partons at low x
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Katja Krüger Physics @ HERA 12
Skaling Violations
large x: quarks radiate gluons, so the studied x decreases→ F2 decreases with increasing Q2
small x: gluons split into seaquarks, so more quarks become visible→ F2 increases with increasing Q2
Q2 = Q02 Q2 = Q0
2Q2 > Q02 Q2 > Q0
2
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Katja Krüger Physics @ HERA 13
DGLAP Evolution Equations
● Q2 dependence of quark densities q(x,Q2) and gluon density g(x,Q2) is predicted
● no prediction for the x dependence initial condition needed
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Katja Krüger Physics @ HERA 14
HERA Kinematic Range
beforeHERAnew
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Katja Krüger Physics @ HERA 15
Events in Different Regions
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Katja Krüger Physics @ HERA 16
F2 vs. Q2
● HERA data cover huge range: 5 orders in Q2 and 4 orders in x
● approximate scaling at large x
● clear scaling violations at small x fixed target
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Katja Krüger Physics @ HERA 17
F2 vs. Q2: example bins
● clear scaling violations at small x
● approximate scaling at large x
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Katja Krüger Physics @ HERA 18
How does F2(x) look like?
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Katja Krüger Physics @ HERA 19
F2 vs. x
strong rise towards low x, steepness rising with Q2
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Katja Krüger Physics @ HERA 20
DGLAP Evolution Equations
● Q2 dependence of quark densities q(x,Q2) and gluon density g(x,Q2) is predicted
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Katja Krüger Physics @ HERA 21
Parton Density FitsDGLAP predicts only Q2 dependence➔ assume parametrisation of the parton density functions
(PDFs) as a function of x at a starting scale Q02 (typically
around 4 7 GeV2):
➔ evolve the PDFs to all measured Q2, calculate F2, and fit
the parameters to match the data
some freedom in the procedure!– how many parameters, which Q
02 ?
– how to combine quark and antiquark densities?
x q x ,Q02=A xB 1−x C [1D xE x2F x3 ]
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Katja Krüger Physics @ HERA 22
Parton Density Fitsquark and antiquark densities:● most general:
● distinguish valence and sea quarks (ZEUS):
● distinguish uptype and downtype quarks (H1):
u ,u , d , d ,s ,s ,c ,c ,b ,b
uv , d v , sea ,d−u
U=uc , D=ds b U=uc , D=ds buv=U−U , d v=D−D
xU
vxu
Ux
xD
vxd
Dx
xg
2 = 10 GeV2 Q
ZEUSJETS fit tot. uncert.
H1 PDF 2000 tot. exp. uncert. model uncert.
410 310 210 110 1
410 310 210 110 1
0
5
10
15
0
0.5
1
1.50
0.5
1
1.5
x
xf
ZEUS
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Katja Krüger Physics @ HERA 23
Combined H1 & ZEUS Parton Density
combination of data from H1 and ZEUS gives big improvements!
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Katja Krüger Physics @ HERA 24
Longitudinal Structure Function FL
● CallanGross relation 2 x F1 = F2 only true in naive QuarkPartonModel
● the longitudinal structure function FL is defined as FL = F2 – 2 x F1
● FL is directly proportional to the gluon density● for a measurement of FL one needs data at the same x
and Q2, but different y
● only possible with different s because Q2 = xys➔ measure at different beam energies!
d 2dx dQ2 =
42
Q4
1x1−y
y2
2[ F 2 x ,Q2 −
y2/21−yy2 /2
F L x ,Q2]
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Katja Krüger Physics @ HERA 25
Longitudinal Structure Function FL
r=x Q4
22
1Y
d2dx dQ2
=F 2 x ,Q2 −y2
Y
F L x ,Q2
with Y=11−y2
● linear expression in y2/Y+
➔ use linear fits in y2/Y+ and determine FL from slope
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Katja Krüger Physics @ HERA 26
Longitudinal Structure Function FL
● ZEUS: simulatanous determination of F2 and FL
● consistent with PDF fit to F2
● most precise information on gluon still from scaling violations
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Katja Krüger Physics @ HERA 27
High Q2 & Electroweak Physics
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Katja Krüger Physics @ HERA 28
More Structure Functions
d 2NC±
dx dQ2 =22
Q4
1x
Y [F 2 x ,Q2 −y2
Y
F L x ,Q2 ∓Y−
Y
x F3 x ,Q2]
/Z 0
FL = F
2 – 2xF
1 = 0 in the QPM
F 3:−Z 0−interference
● FL relevant only at large y
● F3 relevant only at large Q2,
different sign for e+ and e–
e e
p
Y± = 1±1−y2
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Katja Krüger Physics @ HERA 29
High Q2 Neutral Current
● difference between e+p and e–p only at large
➔
Q2≈M Z2
−Z 0−interference
M Z2
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Katja Krüger Physics @ HERA 30
High Q2 Neutral Current
=x Q4
22
1Y
d 2NC±
dx dQ2
e– positive interference
e+ negative interference
x F 3∝ x∑ eq2 q−q
direct handle on valence quark distribution!
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Katja Krüger Physics @ HERA 31
High Q2 Neutral Current
● no significant deviation from Standard Model Fit at high Q2
● can be interpreted as limit on quark size: < 0.6 ∙1018 m
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Katja Krüger Physics @ HERA 32
Charged Current Interactions
e
pq
q'
e
neutrino not visiblein detector
imbalance in transverse plane
W
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Katja Krüger Physics @ HERA 33
Charged Current Cross Section
● W bosons couple differently to up and downtype quarks
● in the QPM:
➔
d2CC±
dx dQ2 =GF
2
4 x M W2
M W2 Q2
2
Y[W 2± −
y2
Y
W L± ∓
Y−
Y
x W 3±]
W 2=x UD , x W 3
=x D−U W 2
−=x UD , x W 3−=x U−D
W L±=0
CC− ∝ x [U 1−y2 D ]
CC ∝ x [U 1−y2 D ]
e+
e–
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Katja Krüger Physics @ HERA 34
Comparison NC vs. CC● at low Q2: different
dependences because of photon in NC
● at high Q2: „electroweak unification“ but:
∝1
Q4
∝1
M W2 Q22
d2CC±
dx dQ2≈
GF2
4 x⋅ M W
2
M W2 Q2
2
⋅YW 2±
d2 NC±
dx dQ2 ≈22
x⋅
1Q4 ⋅Y F2
GF≈4
2 MW2
similar because
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Katja Krüger Physics @ HERA 35
Electroweak Parameters: W Mass
● G = GF determined by normalization of the CC cross section
● Mprop = MW determined by the Q2 dependence of the CC cross section
82.87±1.82exp 0.30−0.16model GeV
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Katja Krüger Physics @ HERA 36
Summary● inclusive ep scattering reveales structure of the proton● large amount of gluons in the proton
● Standard Modell can be cross checked