qcd at hera - fermilab
TRANSCRIPT
![Page 1: QCD at HERA - Fermilab](https://reader034.vdocuments.site/reader034/viewer/2022051402/627c5cd737abe679694c3bc8/html5/thumbnails/1.jpg)
QCD at HERAR. Yoshida
Argonne National LaboratoryFeb. 14, 2005 Aspen
Outline• Jet measurements and αs• Parton distributions from structure
function measurements.• Parton distributions and αs from
structure functions and jets.
![Page 2: QCD at HERA - Fermilab](https://reader034.vdocuments.site/reader034/viewer/2022051402/627c5cd737abe679694c3bc8/html5/thumbnails/2.jpg)
Jet measurements at HERAjets in DIS
Jet measurementsat HERA has typicaluncertainty ~5%.
Compare to ~60% at Tevatron
![Page 3: QCD at HERA - Fermilab](https://reader034.vdocuments.site/reader034/viewer/2022051402/627c5cd737abe679694c3bc8/html5/thumbnails/3.jpg)
Jet measurements at HERA• HERA jet energies can be calibrated using the
energy balance with the scattered electron--achieve 1-2% energy uncertainty for jets.
• HERA jets are reconstructed using the theoretically robust algorithms (typically kt rather than cone)—comparison to QCD theory does not suffer from large hadronization uncertainties.
27.5 GeV electron920 GeV ProtonJet
![Page 4: QCD at HERA - Fermilab](https://reader034.vdocuments.site/reader034/viewer/2022051402/627c5cd737abe679694c3bc8/html5/thumbnails/4.jpg)
Jet production processes at HERA
DIS
Photoproduction
![Page 5: QCD at HERA - Fermilab](https://reader034.vdocuments.site/reader034/viewer/2022051402/627c5cd737abe679694c3bc8/html5/thumbnails/5.jpg)
Jet measurements and αsExample: DIS jets in Breit frame
![Page 6: QCD at HERA - Fermilab](https://reader034.vdocuments.site/reader034/viewer/2022051402/627c5cd737abe679694c3bc8/html5/thumbnails/6.jpg)
Jet measurements and αsExample: 3 to 2 jet rate ratiopdf uncertainty tends to cancel
![Page 7: QCD at HERA - Fermilab](https://reader034.vdocuments.site/reader034/viewer/2022051402/627c5cd737abe679694c3bc8/html5/thumbnails/7.jpg)
Jet measurements and αsCorrelations between pdf and αs
• Pdfs are extracted assuming some value of αs (or determines the value of αs )
• Jet cross-sections at HERA depends on pdfs
• αs from jets is extracted taking this correlation into account.
• In effect the value of αs is varied simultaneously in pdf and cross-section calculations when fitting data to optimum αs —this is done using a set of pdfs determined at various values of αs .
![Page 8: QCD at HERA - Fermilab](https://reader034.vdocuments.site/reader034/viewer/2022051402/627c5cd737abe679694c3bc8/html5/thumbnails/8.jpg)
Jet measurements and αs
NLOQCDfits to st. fcn
Measurementscombined (C. Glasman et al.)
![Page 9: QCD at HERA - Fermilab](https://reader034.vdocuments.site/reader034/viewer/2022051402/627c5cd737abe679694c3bc8/html5/thumbnails/9.jpg)
Structure functions and pdfExample: ZEUS NLO QCD fit (similar results for H1)
Fixed target results are used in fitto fix the high x pdf
![Page 10: QCD at HERA - Fermilab](https://reader034.vdocuments.site/reader034/viewer/2022051402/627c5cd737abe679694c3bc8/html5/thumbnails/10.jpg)
Structure functions and pdfUse all of HERA I data (>100 pb-1) to replace fixed target experiments in the fit
No low Q2, heavy targetcorrections. H1 data: similar for ZEUS
![Page 11: QCD at HERA - Fermilab](https://reader034.vdocuments.site/reader034/viewer/2022051402/627c5cd737abe679694c3bc8/html5/thumbnails/11.jpg)
Structure function and pdf
HERA only fit:H1 results similar for ZEUS
High x statisticsdominated
αs weakly constrained
note: αs enters multiplied by the gluon density at lowerx where HERA has high precision data.
![Page 12: QCD at HERA - Fermilab](https://reader034.vdocuments.site/reader034/viewer/2022051402/627c5cd737abe679694c3bc8/html5/thumbnails/12.jpg)
Jet measurements and pdf
Sensitivity to the gluon
Note: cross-sectionis directly proportional to gluon. For structure functionQ2 slope is proportional.
![Page 13: QCD at HERA - Fermilab](https://reader034.vdocuments.site/reader034/viewer/2022051402/627c5cd737abe679694c3bc8/html5/thumbnails/13.jpg)
Jet measurements and QCD fit• Up to now, no QCD fit made rigorous use of jet data. CTEQ,
MRST global fits use LO + k-factor for their jet descriptions.
• Although NLO jet calculations exist (DISENT, PHOJET, NLOJET etc.), their use in an iterative fitting procedure is not possible due to prohibitive computing time requirements.
• ZEUS collaboration has pioneered a fast calculation method (basically putting the cross-sections on a grid) which enables the use of jet data to be put rigorously into a NLO fit.
• This makes possible, for the first time, a rigorous use of jet data in NLOQCD fits to parton distributions of the proton.
• This enables, for example, a consistent simultaneous extraction of precision αs (mainly based on jets) and pdfstaking all correlated uncertainties into account.
![Page 14: QCD at HERA - Fermilab](https://reader034.vdocuments.site/reader034/viewer/2022051402/627c5cd737abe679694c3bc8/html5/thumbnails/14.jpg)
ZEUS-JETS QCDNLO fit results
![Page 15: QCD at HERA - Fermilab](https://reader034.vdocuments.site/reader034/viewer/2022051402/627c5cd737abe679694c3bc8/html5/thumbnails/15.jpg)
ZEUS-JETS NLOQCD fit results
Jet data constrain the medium x gluon
Gluon improvement
NC and CCconstrainquarks
![Page 16: QCD at HERA - Fermilab](https://reader034.vdocuments.site/reader034/viewer/2022051402/627c5cd737abe679694c3bc8/html5/thumbnails/16.jpg)
ZEUS-JETS simultaneous fit to pdf and αs
Gluon does not becomeunconstrained when αs freed.
![Page 17: QCD at HERA - Fermilab](https://reader034.vdocuments.site/reader034/viewer/2022051402/627c5cd737abe679694c3bc8/html5/thumbnails/17.jpg)
HERALHC workshopPredictions of LHC jet cross-sections
Improvement due to inclusion of ZEUS jet data
work by: K. Nagano, KEK
![Page 18: QCD at HERA - Fermilab](https://reader034.vdocuments.site/reader034/viewer/2022051402/627c5cd737abe679694c3bc8/html5/thumbnails/18.jpg)
ZEUS-JETS fit: possible extensions
• Use charm production data: still has some theoretical issues; also experimental systematic uncertainties are a little too large.
• Use other jet data: use e.g. 2 to 3 jet ratio, subjet multiplicity etc.
• Use “resolved” photoproduction jet data and constrain photon pdfs simultaneouly.
• …
![Page 19: QCD at HERA - Fermilab](https://reader034.vdocuments.site/reader034/viewer/2022051402/627c5cd737abe679694c3bc8/html5/thumbnails/19.jpg)
Impact of HERA II• HERA II (x5 increase
in luminosity compared to HERA I
• Planned to run to middle of 2007
• 500-1000 pb-1 data using both e+ and e-beams. (also e polarization)
• Currently taking data• Impact on these fits?
![Page 20: QCD at HERA - Fermilab](https://reader034.vdocuments.site/reader034/viewer/2022051402/627c5cd737abe679694c3bc8/html5/thumbnails/20.jpg)
HERALHC workshop
(C. Gwenlan, Oxford)
![Page 21: QCD at HERA - Fermilab](https://reader034.vdocuments.site/reader034/viewer/2022051402/627c5cd737abe679694c3bc8/html5/thumbnails/21.jpg)
(C. Gwenlan, Oxford)
![Page 22: QCD at HERA - Fermilab](https://reader034.vdocuments.site/reader034/viewer/2022051402/627c5cd737abe679694c3bc8/html5/thumbnails/22.jpg)
(C. Gwenlan, Oxford)
![Page 23: QCD at HERA - Fermilab](https://reader034.vdocuments.site/reader034/viewer/2022051402/627c5cd737abe679694c3bc8/html5/thumbnails/23.jpg)
Conclusions• HERA jet measurements are precision data (~5%
uncertainty).• αs has been measured at HERA from jets, running,
over an order of magnitude in scale, and at a precision at the level of the world average. The uncertainties are dominated by theoretical ones.
• ZEUS has developed a method to do a rigorous combined fit at NLO with structure function and jet measurements to extract pdfs and αs. The precision of the gluon determination improve markedly; a precision αs is extracted.
• The new HERA II data will lead to much improved pdfs at high x.
![Page 24: QCD at HERA - Fermilab](https://reader034.vdocuments.site/reader034/viewer/2022051402/627c5cd737abe679694c3bc8/html5/thumbnails/24.jpg)
Extras
![Page 25: QCD at HERA - Fermilab](https://reader034.vdocuments.site/reader034/viewer/2022051402/627c5cd737abe679694c3bc8/html5/thumbnails/25.jpg)
HERALHC workshop
(K. Nagano, KEK)
![Page 26: QCD at HERA - Fermilab](https://reader034.vdocuments.site/reader034/viewer/2022051402/627c5cd737abe679694c3bc8/html5/thumbnails/26.jpg)
Triumph of perturbative QCD
A part of Wilczek’s comments upon the Nobel Prize announcement
gluon
resolution
![Page 27: QCD at HERA - Fermilab](https://reader034.vdocuments.site/reader034/viewer/2022051402/627c5cd737abe679694c3bc8/html5/thumbnails/27.jpg)
(A. Cooper-Sarkar, Oxford)
HERALHC workshop
![Page 28: QCD at HERA - Fermilab](https://reader034.vdocuments.site/reader034/viewer/2022051402/627c5cd737abe679694c3bc8/html5/thumbnails/28.jpg)
HERALHC workshop
(A. Cooper-Sarkar, Oxford)
![Page 29: QCD at HERA - Fermilab](https://reader034.vdocuments.site/reader034/viewer/2022051402/627c5cd737abe679694c3bc8/html5/thumbnails/29.jpg)
HERALHC workshop
(A. Cooper-Sarkar, Oxford)
![Page 30: QCD at HERA - Fermilab](https://reader034.vdocuments.site/reader034/viewer/2022051402/627c5cd737abe679694c3bc8/html5/thumbnails/30.jpg)
HERALHC workshop
(A. Cooper-Sarkar, Oxford)Note: CDF and D0 data have large (up to 60%) systematic uncertainties not shown on the plots: in case of the CDF data systematics are “shifted” to optimal values in the course of the fit. This is not possible for the D0 data since the relevant information is not available