precision qcd and electroweak physics at the lhec
DESCRIPTION
Precision QCD and electroweak physics at the LheC. LHeC workshop 2009, 3 Sep 2009, Divonne Les Bains. Olaf Behnke , Claire Gwenlan, Paolo Gambino, Thomas Gehrmann. 1. Need for LHeC. 27.5 GeV x 920 GeV ep HERA with integrated L~0.5 fb -1 was a high precision machine for QCD - PowerPoint PPT PresentationTRANSCRIPT
![Page 1: Precision QCD and electroweak physics at the LheC](https://reader035.vdocuments.us/reader035/viewer/2022062518/56814535550346895db1fffc/html5/thumbnails/1.jpg)
Precision QCD and electroweak physics
at the LheC
Olaf Behnke, Claire Gwenlan, Paolo Gambino, Thomas Gehrmann
LHeC workshop 2009, 3 Sep 2009, Divonne Les
Bains
1
![Page 2: Precision QCD and electroweak physics at the LheC](https://reader035.vdocuments.us/reader035/viewer/2022062518/56814535550346895db1fffc/html5/thumbnails/2.jpg)
Need for LHeC27.5 GeV x 920 GeV ep HERA
with integrated L~0.5 fb-1 was a high precision machine for QCD modest precision machine for electroweak physics
Where could we go with a 20-150 GeV x 7 TeV ep LHeC with integrated L~1-10 fb-1 ?
2
![Page 3: Precision QCD and electroweak physics at the LheC](https://reader035.vdocuments.us/reader035/viewer/2022062518/56814535550346895db1fffc/html5/thumbnails/3.jpg)
Precision QCD & electroweak physics at LHeC
Observables: Targets: Talks:
Incl. NC and CC uv, dv, Sea, gluon
Elweak: au, vu, ad, vd , Mw
Effect of LHeC pdfs on LHC Higgs
s
Jet production gluon; structure, s
Charm production gluon, intrinsic charm
Beauty production effective b density in p
sW c strange density in p
bW ->t Single top production
+ other final state topics not yet covered , e.g. prompt photons
Max Klein
Claire Gwenlan, Paolo Gambino
Soumitra Nandi
Thomas Kluge
Joerg Behr, Claudia Glasman
Goekhan Uenel
O.B.
Theory development: SHERA Programme (e.g. bW->t) Stefan Hoeche
3
Alessandro Vicini
![Page 4: Precision QCD and electroweak physics at the LheC](https://reader035.vdocuments.us/reader035/viewer/2022062518/56814535550346895db1fffc/html5/thumbnails/4.jpg)
4Max Klein - Scenarios and Measurements
Simulated Default Scenarios, April 2009
http://hep.ph.liv.ac.uk/~mklein/simdis09/lhecsim.Dmp.CC, readfirst
Not simulated
Max Klein, LHeC
![Page 5: Precision QCD and electroweak physics at the LheC](https://reader035.vdocuments.us/reader035/viewer/2022062518/56814535550346895db1fffc/html5/thumbnails/5.jpg)
5Max Klein - Scenarios and Measurements
Systematic error calculation for inclusive NC & CC pseudodata:
assumed uncertainties and effects on xsecs
At high Q2: Need <=1% hadronic energy scale uncertainty at very large Eh
1 mrad error on
1% error on Eh’
0.2% error on
Ee’
![Page 6: Precision QCD and electroweak physics at the LheC](https://reader035.vdocuments.us/reader035/viewer/2022062518/56814535550346895db1fffc/html5/thumbnails/6.jpg)
6Max Klein - Scenarios and Measurements
Kinematics – high Q2
Need excellent forward hadron calorimetry & calibration
![Page 7: Precision QCD and electroweak physics at the LheC](https://reader035.vdocuments.us/reader035/viewer/2022062518/56814535550346895db1fffc/html5/thumbnails/7.jpg)
7Max Klein - Scenarios and Measurements
Trivial, but important: largest Elep allows highest Q2 scales
Neutral Current Event Neutral Current Event RatesRates
![Page 8: Precision QCD and electroweak physics at the LheC](https://reader035.vdocuments.us/reader035/viewer/2022062518/56814535550346895db1fffc/html5/thumbnails/8.jpg)
8Max Klein - Scenarios and Measurements
Rates
LHeC: expect ~ two orders of magnitudemore events + better coverage forx>0.5
Max Klein - Scenarios and Measurements
Charged Current Event Rates
![Page 9: Precision QCD and electroweak physics at the LheC](https://reader035.vdocuments.us/reader035/viewer/2022062518/56814535550346895db1fffc/html5/thumbnails/9.jpg)
9
Study presented here is based on new
ZEUS NLO QCD fit to HERA-I and
HERA-II data
ZEUS09 fit (c.f. central values of HERA-I fit)
NLO QCD and electroweak fit
LHeC NC/CC simulated data added
to this in a combined fit for the
PDFs and electroweak parameters
Claire Gwenlan
Making use of Max pseudodata
![Page 10: Precision QCD and electroweak physics at the LheC](https://reader035.vdocuments.us/reader035/viewer/2022062518/56814535550346895db1fffc/html5/thumbnails/10.jpg)
10
Proton PDFs Q2 = 100 GeV2
scenario D
» only PDF parameters free(LHeC NC and CC ep included)
Looks very promising, model and parameterisation uncertainties to be studied
Claire Gwenlan
![Page 11: Precision QCD and electroweak physics at the LheC](https://reader035.vdocuments.us/reader035/viewer/2022062518/56814535550346895db1fffc/html5/thumbnails/11.jpg)
11
Max Klein - Scenarios and Measurements
PDF fits to expected LHeC data previous
assessment by Emmanuelle Perez
In general reasonable agreement between Claire’s & Emmanuelle’s PDF fits
Example: u/d ratio
11
![Page 12: Precision QCD and electroweak physics at the LheC](https://reader035.vdocuments.us/reader035/viewer/2022062518/56814535550346895db1fffc/html5/thumbnails/12.jpg)
12
electroweak parameters
» fit with PDF and electroweak parameters simultaneously free
neutral current axial and vector quark couplings (au, vu, ad, vd)
mass of the W boson
Claire Gwenlan
![Page 13: Precision QCD and electroweak physics at the LheC](https://reader035.vdocuments.us/reader035/viewer/2022062518/56814535550346895db1fffc/html5/thumbnails/13.jpg)
13
neutral current quark couplings
u-type quark couplings d-type quark couplings
comparison with ZEUS fit (base to which LHeC pseudo-
data added)
it’s here!
scenario D:
Pe = 0.9
Claire Gwenlan
![Page 14: Precision QCD and electroweak physics at the LheC](https://reader035.vdocuments.us/reader035/viewer/2022062518/56814535550346895db1fffc/html5/thumbnails/14.jpg)
14
Fermion couplings to Z boson
LHeC (and HERA) especially sensitive to u and d couplings: expect deviations from SM for these couplings
e.g in Leptophobic Z’ models
QuickTime™ and a decompressor
are needed to see this picture.
Soumitra
Nandi. QuickTime™ and a decompressor
are needed to see this picture.
![Page 15: Precision QCD and electroweak physics at the LheC](https://reader035.vdocuments.us/reader035/viewer/2022062518/56814535550346895db1fffc/html5/thumbnails/15.jpg)
15
Fermion couplings to Z boson
QuickTime™ and a decompressor
are needed to see this picture.
Soumitra
Nandi. QuickTime™ and a decompressor
are needed to see this picture.
General suggestion (Paolo Gambino) for LHeC electroweak studies:Try fit with sin2( w) as only free parameter; determination
as function of hard scale also interesting
![Page 16: Precision QCD and electroweak physics at the LheC](https://reader035.vdocuments.us/reader035/viewer/2022062518/56814535550346895db1fffc/html5/thumbnails/16.jpg)
16
Improved (wrt HERA) but not competitive (although still interesting as a cross-check; space-like regime)
current world average (PDG 2008): MW = 80.398 0.025 GeV (0.03% total)
also performed fit including LHeC CC, with MW free, together with the PDFs (NC quark couplings fixed to SM)
W boson mass
MW enters the fit through the propagator in the CC cross sections:
MW (= 80.4 SM)
Scenario D
MW = 80.40 0.04 (uncorr.) 0.15 (corr.) GeV (total exp. 0.2%)
Claire Gwenlan
![Page 17: Precision QCD and electroweak physics at the LheC](https://reader035.vdocuments.us/reader035/viewer/2022062518/56814535550346895db1fffc/html5/thumbnails/17.jpg)
QuickTime™ and a decompressor
are needed to see this picture.
AlessandroVicini
LHC Higgs production and improvement due to LHeC pdfs
![Page 18: Precision QCD and electroweak physics at the LheC](https://reader035.vdocuments.us/reader035/viewer/2022062518/56814535550346895db1fffc/html5/thumbnails/18.jpg)
QuickTime™ and a decompressor
are needed to see this picture.
AlessandroVicini
![Page 19: Precision QCD and electroweak physics at the LheC](https://reader035.vdocuments.us/reader035/viewer/2022062518/56814535550346895db1fffc/html5/thumbnails/19.jpg)
s from inclusive NC+CC
Sensitivity mainly from scaling
violations of F2
QuickTime™ and a decompressor
are needed to see this picture.
QuickTime™ and a decompressor
are needed to see this picture.
Thomas Kluge
Fitting to Pseudodata B+C+F+H ->
![Page 20: Precision QCD and electroweak physics at the LheC](https://reader035.vdocuments.us/reader035/viewer/2022062518/56814535550346895db1fffc/html5/thumbnails/20.jpg)
O(s) processes
q -> Jet
qbar -> Jet
![Page 21: Precision QCD and electroweak physics at the LheC](https://reader035.vdocuments.us/reader035/viewer/2022062518/56814535550346895db1fffc/html5/thumbnails/21.jpg)
QuickTime™ and a decompressor
are needed to see this picture.
Jet production
Reach scales up to 2m_t where change of 1/s slope is expected
Joerg Behr
QuickTime™ and a decompressor
are needed to see this picture.
Claudia GlasmanDIS Photoproduction
![Page 22: Precision QCD and electroweak physics at the LheC](https://reader035.vdocuments.us/reader035/viewer/2022062518/56814535550346895db1fffc/html5/thumbnails/22.jpg)
O(s) processes
![Page 23: Precision QCD and electroweak physics at the LheC](https://reader035.vdocuments.us/reader035/viewer/2022062518/56814535550346895db1fffc/html5/thumbnails/23.jpg)
Charm eg-> ecc vs g->ccQuickTime™ and a
decompressorare needed to see this picture.
QuickTime™ and a decompressor
are needed to see this picture.
QuickTime™ and a decompressor
are needed to see this picture.
Cross sections much higher for photon proton
collider
![Page 24: Precision QCD and electroweak physics at the LheC](https://reader035.vdocuments.us/reader035/viewer/2022062518/56814535550346895db1fffc/html5/thumbnails/24.jpg)
Charm p cross sections vs
detector acceptance
QuickTime™ and a decompressor
are needed to see this picture.
QuickTime™ and a decompressor
are needed to see this picture.
Detector polar angular coverage from 10-1790 highly desirable
50e 7000 p
![Page 25: Precision QCD and electroweak physics at the LheC](https://reader035.vdocuments.us/reader035/viewer/2022062518/56814535550346895db1fffc/html5/thumbnails/25.jpg)
25
Max Klein - Scenarios and Measurements
x=0.00003
x=0.00007
x=0.0003
x=0.0007
x=0.003
x=0.007
x=0.0000
x=0.03
x=0.1
x=0.3
€
1 fb−1
εc = 0.1
bgdq = 0.01
δsyst = 0.1
o−ϑ h ≥1o
• −ϑ h ≥10o
Max Klein Charm in DIS
Charm at at large x will be an interesting challenge
![Page 26: Precision QCD and electroweak physics at the LheC](https://reader035.vdocuments.us/reader035/viewer/2022062518/56814535550346895db1fffc/html5/thumbnails/26.jpg)
26
O.B.
Beauty in DIS
Largely extended phasespace
compared to HERA
x=0.2
x=0.000001
HERA
coverage
![Page 27: Precision QCD and electroweak physics at the LheC](https://reader035.vdocuments.us/reader035/viewer/2022062518/56814535550346895db1fffc/html5/thumbnails/27.jpg)
O.B.
HERA 27.5 x 920
Obtained with PYTHIA, RAPGAP and LEPTO
LHeC is a flavour factory
![Page 28: Precision QCD and electroweak physics at the LheC](https://reader035.vdocuments.us/reader035/viewer/2022062518/56814535550346895db1fffc/html5/thumbnails/28.jpg)
O.B.
HERA 27.5 x 920
Obtained with PYTHIA, RAPGAP and LEPTO
LHeC is a flavour factory
Events per 10 fb-1 Lumi
1010
108
4x106
4x105
105
103
![Page 29: Precision QCD and electroweak physics at the LheC](https://reader035.vdocuments.us/reader035/viewer/2022062518/56814535550346895db1fffc/html5/thumbnails/29.jpg)
Stefan
Hoeche
Lets make use of it for LHeC predictions, e.g. for bW-> t
QuickTime™ and a decompressor
are needed to see this picture.
QuickTime™ and a decompressor
are needed to see this picture.
SHERPA
![Page 30: Precision QCD and electroweak physics at the LheC](https://reader035.vdocuments.us/reader035/viewer/2022062518/56814535550346895db1fffc/html5/thumbnails/30.jpg)
30
Summary
The LHeC has potential to completely unfold the partonic content of the proton: u,d, c,s, t,b for the first time and in an unprecedent kinematic range. This is based on inclusive NC, CC cross sections complemented by heavy quark identification.
Puzzles as u/d at large x or a strange-antistrange asymmetry will be solved.
Precision measurements are possible of xg (up to large x) and the beauty density which are of particular relevance for the LHC. The (almost) whole p structure which the LHC assumes to know will become accurately known. Large x>0.1 programme necessiates excellent forward hadronic calorimetry and control of hadronic energy scale to <= 1 %.
First fits to LHeC pseudodata: demonstrate a high precision potential for electroweak physics, e.g. for the light quark couplings to the Z boson and for the W propagator mass,Should be continued, e.g. fits of sin(w)
The working group made substantial progess on the way towards the The working group made substantial progess on the way towards the conceptional design report; several new simulated predictions have conceptional design report; several new simulated predictions have been obtained for the agreed machine scenarios; try to complete the been obtained for the agreed machine scenarios; try to complete the studies and add some (most important) missing pieces….studies and add some (most important) missing pieces….
![Page 31: Precision QCD and electroweak physics at the LheC](https://reader035.vdocuments.us/reader035/viewer/2022062518/56814535550346895db1fffc/html5/thumbnails/31.jpg)
Backup slides
![Page 32: Precision QCD and electroweak physics at the LheC](https://reader035.vdocuments.us/reader035/viewer/2022062518/56814535550346895db1fffc/html5/thumbnails/32.jpg)
32
Proton PDFs
» only PDF parameters free(LHeC NC ep included)
Q2 = 100 GeV2
PDF uncertainties:
•
NC ep: direct constraints on
quark densities; indirect on
gluon via scaling violations
scenario D
Claire Gwenlan
13
![Page 33: Precision QCD and electroweak physics at the LheC](https://reader035.vdocuments.us/reader035/viewer/2022062518/56814535550346895db1fffc/html5/thumbnails/33.jpg)
33
Proton PDFs Q2 = 100 GeV2
scenario D
» only PDF parameters free(LHeC NC and CC ep included)
scenarios: A, B, C, D and EEe (GeV) P L (e-:e+)
A 20 0 2 (1:1)
B 50 0.4 200 (1:1)
C 50 0.4 4 (1:1)
D 100 0.9 30 (2:1)
E 150 0.9 18 (2:1)
(examples with several different Q2
values are shown in backups)
* acceptance for scenario B has been taken to be: 10 < θ < 170o
Claire Gwenlan
![Page 34: Precision QCD and electroweak physics at the LheC](https://reader035.vdocuments.us/reader035/viewer/2022062518/56814535550346895db1fffc/html5/thumbnails/34.jpg)
34
neutral current quark couplings
u-type quark couplings d-type quark couplings
comparison with other experiments
» still to come: HERA-II NC e+p data in ZEUS fit; H1+ZEUS combined HERA-II results
scenario D:
Pe = 0.9
Claire Gwenlan
![Page 35: Precision QCD and electroweak physics at the LheC](https://reader035.vdocuments.us/reader035/viewer/2022062518/56814535550346895db1fffc/html5/thumbnails/35.jpg)
35
neutral current quark couplings
25
u-type quark couplings d-type quark couplings
other scenarios: B, C, (D) and E (versus ZEUS base fit)
polarisations:
Pe = 0.4 (B,C)
Pe = 0.9 (D,E)
factors of ×10−40 improvement (depending on exact coupling and scenario)
Claire Gwenlan
![Page 36: Precision QCD and electroweak physics at the LheC](https://reader035.vdocuments.us/reader035/viewer/2022062518/56814535550346895db1fffc/html5/thumbnails/36.jpg)
36
Max Klein - Scenarios and Measurements
70 GeV x 7 TeV: F2bb in bins of x vs Q2 at the LHeC
€
1 fb−1
εb = 0.5
bgdc = 0.1
δsyst = 0.1
o−ϑ h ≥1o
• −ϑ h ≥10o
M. Klein, A. Mehta