Difference: PhysicsResultsFSQ12031 (1 vs. 21)

Revision 212013-07-25 - IlknurHos

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META TOPICPARENT name="PhysicsResultsFSQ12031"

Measurement of Low pT Jet Cross Sections in proton-proton Collisions at √s = 8 TeV

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Figures

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Figure 1. Inclusive jet cross section (anti-kT) measured at rapidities ( ) as a function of transverse momentum, fully corrected and unfolded, compared to various hadron-level theoretical predictions: NLO calculations for various PDFs. The yellow band on the data points refers to the total experimental uncertainty. The pdf files cxsection_Y_0.pdf,cxsection_Y_1.pdf, cxsection_Y_2.pdf, cxsection_Y_3.pdf, cxsection_Y_4.pdf, cxsection_Y_5.pdf, cxsection_Y_6.pdf, and the png files cxsection_Y_0.png, cxsection_Y_1.png, cxsection_Y_2.png, cxsection_Y_3.png, cxsection_Y_4.png, cxsection_Y_5.png, cxsection_Y_6.png

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Figure 2. Inclusive jet cross sections for data over the theoretical prediction of the ABM11 PDF set for all . The experimental and theoretical systematic uncertainties are represented by the continuous and dashed lines, respectively. The pdf files ratio_ABM11_Y_0.pdf, ratio_ABM11_Y_1.pdf, ratio_ABM11_Y_2.pdf, ratio_ABM11_Y_3.pdf, ratio_ABM11_Y_4.pdf, ratio_ABM11_Y_5.pdf, ratio_ABM11_Y_6.pdf and the png files ratio_ABM11_Y_0.png, ratio_ABM11_Y_1.png, ratio_ABM11_Y_2.png, ratio_ABM11_Y_3.png, ratio_ABM11_Y_4.png, ratio_ABM11_Y_5.png, ratio_ABM11_Y_6.png
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Figure 3. Inclusive jet cross sections for data over the theoretical prediction of the CT10 PDF set for all . The experimental and theoretical systematic uncertainties are represented by the continuous and dashed lines, respectively. The pdf files ratio_CT10_Y_0.pdf, ratio_CT10_Y_1.pdf, ratio_CT10_Y_2.pdf, ratio_CT10_Y_3.pdf, ratio_CT10_Y_4.pdf, ratio_CT10_Y_5.pdf, ratio_CT10_Y_6.pdf and the png files ratio_CT10_Y_0.png, ratio_CT10_Y_1.png, ratio_CT10_Y_2.png, ratio_CT10_Y_3.png, ratio_CT10_Y_4.png, ratio_CT10_Y_5.png, ratio_CT10_Y_6.png
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Figure 4. Inclusive jet cross sections for data over the theoretical prediction of the HERAPDF1.5 PDF set for all . The experimental and theoretical systematic uncertainties are represented by the continuous and dashed lines, respectively. The pdf files ratio_HERAPDF15_Y_0.pdf, ratio_HERAPDF15_Y_1.pdf, ratio_HERAPDF15_Y_2.pdf, ratio_HERAPDF15_Y_3.pdf, ratio_HERAPDF15_Y_4.pdf, ratio_HERAPDF15_Y_5.pdf, ratio_HERAPDF15_Y_6.pdf and the png files ratio_HERAPDF15_Y_0.png, ratio_HERAPDF15_Y_1.png, ratio_HERAPDF15_Y_2.png, ratio_HERAPDF15_Y_3.png, ratio_HERAPDF15_Y_4.png, ratio_HERAPDF15_Y_5.png, ratio_HERAPDF15_Y_6.png
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Figure 5. Inclusive jet cross sections for data over the theoretical prediction of the MSTW2008 PDF set for all . The experimental and theoretical systematic uncertainties are represented by the continuous and dashed lines, respectively. The pdf files ratio_MSTW2008_Y_0.pdf, ratio_MSTW2008_Y_1.pdf, ratio_MSTW2008_Y_2.pdf, ratio_MSTW2008_Y_3.pdf, ratio_MSTW2008_Y_4.pdf, ratio_MSTW2008_Y_5.pdf, ratio_MSTW2008_Y_6.pdf and the png files ratio_MSTW2008_Y_0.png
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Figure 6. Inclusive jet cross sections for data over the theoretical prediction of the NNPDF2.1 PDF set for all . The experimental and theoretical systematic uncertainties are represented by the continuous and dashed lines, respectively. The pdf files ratio_NNPDF21_Y_0.pdf, ratio_NNPDF21_Y_1.pdf, ratio_NNPDF21_Y_2.pdf, ratio_NNPDF21_Y_3.pdf, ratio_NNPDF21_Y_4.pdf, ratio_NNPDF21_Y_5.pdf, ratio_NNPDF21_Y_6.pdf and the png files ratio_NNPDF21_Y_0.png, ratio_NNPDF21_Y_1.png, ratio_NNPDF21_Y_2.png, ratio_NNPDF21_Y_3.png, ratio_NNPDF21_Y_4.png, ratio_NNPDF21_Y_5.png, ratio_NNPDF21_Y_6.png
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Figure 7. Ratio of inclusive jet cross sections to the theoretical prediction using the central value of the ABM11 PDF set for all bins. The dashed lines show the ratio of the cross sections calculated with the other PDF sets to that calculated with ABM11. The experimental uncertainty is represented by the continuous line. The pdf files ratio_pdf_ABM11_Y_0.pdf, ratio_pdf_ABM11_Y_1.pdf, ratio_pdf_ABM11_Y_2.pdf, ratio_pdf_ABM11_Y_3.pdf, ratio_pdf_ABM11_Y_4.pdf, ratio_pdf_ABM11_Y_5.pdf, ratio_pdf_ABM11_Y_6.pdf and the png files ratio_pdf_ABM11_Y_0.png, ratio_pdf_ABM11_Y_1.png, ratio_pdf_ABM11_Y_2.png, ratio_pdf_ABM11_Y_3.png, ratio_pdf_ABM11_Y_4.png, ratio_pdf_ABM11_Y_5.png, ratio_pdf_ABM11_Y_6.png
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Figure 8. Ratio of inclusive jet cross sections to the theoretical prediction using the central value of the CT10 PDF set for all bins. The dashed lines show the ratio of the cross sections calculated with the other PDF sets to that calculated with CT10. The experimental uncertainty is represented by the continuous line. The pdf files ratio_pdf_CT10_Y_0.pdf, ratio_pdf_CT10_Y_1.pdf, ratio_pdf_CT10_Y_2.pdf, ratio_pdf_CT10_Y_3.pdf, ratio_pdf_CT10_Y_4.pdf, ratio_pdf_CT10_Y_5.pdf, ratio_pdf_CT10_Y_6.pdf and the png files ratio_pdf_CT10_Y_0.png, ratio_pdf_CT10_Y_1.png, ratio_pdf_CT10_Y_2.png, ratio_pdf_CT10_Y_3.png, ratio_pdf_CT10_Y_4.png, ratio_pdf_CT10_Y_5.png, ratio_pdf_CT10_Y_6.png
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Figure 9. Ratio of inclusive jet cross sections to the theoretical prediction using the central value of the HERAPDF1.5 PDF set for all bins. The dashed lines show the ratio of the cross sections calculated with the other PDF sets to that calculated with HERAPDF1.5. The experimental uncertainty is represented by the continuous line. The pdf files ratio_pdf_HERAPDF15_Y_0.pdf, ratio_pdf_HERAPDF15_Y_1.pdf, ratio_pdf_HERAPDF15_Y_2.pdf, ratio_pdf_HERAPDF15_Y_3.pdf, ratio_pdf_HERAPDF15_Y_4.pdf, ratio_pdf_HERAPDF15_Y_5.pdf, ratio_pdf_HERAPDF15_Y_6.pdf and the png files ratio_pdf_HERAPDF15_Y_0.png, ratio_pdf_HERAPDF15_Y_1.png, ratio_pdf_HERAPDF15_Y_2.png, ratio_pdf_HERAPDF15_Y_3.png, ratio_pdf_HERAPDF15_Y_4.png, ratio_pdf_HERAPDF15_Y_5.png, ratio_pdf_HERAPDF15_Y_6.png
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Figure 10. Ratio of inclusive jet cross sections to the theoretical prediction using the central value of the MSTW2008 PDF set for all bins. The dashed lines show the ratio of the cross sections calculated with the other PDF sets to that calculated with MSTW2008. The experimental uncertainty is represented by the continuous line. The pdf files ratio_pdf_MSTW2008_Y_0.pdf, ratio_pdf_MSTW2008_Y_1.pdf, ratio_pdf_MSTW2008_Y_2.pdf, ratio_pdf_MSTW2008_Y_3.pdf, ratio_pdf_MSTW2008_Y_4.pdf, ratio_pdf_MSTW2008_Y_5.pdf, ratio_pdf_MSTW2008_Y_6.pdf and the png files ratio_pdf_MSTW2008_Y_0.png, ratio_pdf_MSTW2008_Y_1.png, ratio_pdf_MSTW2008_Y_2.png, ratio_pdf_MSTW2008_Y_3.png, ratio_pdf_MSTW2008_Y_4.png, ratio_pdf_MSTW2008_Y_5.png, ratio_pdf_MSTW2008_Y_6.png
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Figure 11. Ratio of inclusive jet cross sections to the theoretical prediction using the central value of the NNPDF2.1 PDF set for all bins. The dashed lines show the ratio of the cross sections calculated with the other PDF sets to that calculated with NNPDF2.1. The experimental uncertainty is represented by the continuous line. The pdf files ratio_pdf_NNPDF21_Y_0.pdf, ratio_pdf_NNPDF21_Y_1.pdf, ratio_pdf_NNPDF21_Y_2.pdf, ratio_pdf_NNPDF21_Y_3.pdf, ratio_pdf_NNPDF21_Y_4.pdf, ratio_pdf_NNPDF21_Y_5.pdf, ratio_pdf_NNPDF21_Y_6.pdf and the png files ratio_pdf_NNPDF21_Y_0.png, ratio_pdf_NNPDF21_Y_1.png, ratio_pdf_NNPDF21_Y_2.png, ratio_pdf_NNPDF21_Y_3.png, ratio_pdf_NNPDF21_Y_4.png, ratio_pdf_NNPDF21_Y_5.png, ratio_pdf_NNPDF21_Y_6.png
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Figure 12. The combined differential inclusive jet cross sections in comparison to NLO predictions using the NNPDF2.1 PDF set times the NP correction factor. Open markers represent the measurement of low pT jets obtained with the integrated luminosity of 5.8 pb-1 of minimum bias data for low pile-up conditions whereas the filled markers for high pT jets obtained with integrated luminosity of 10.71 pb-1 of jet trigger data for high pile-up. The pdf file xsection.pdf and the png files xsection.png
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Figure 12. The combined differential inclusive jet cross sections in comparison to NLO predictions using the NNPDF2.1 PDF set times the NP correction factor. Open markers represent the measurement of low pT jets obtained with the integrated luminosity of 5.8 pb-1 of minimum bias data for low pile-up conditions whereas the filled markers for high pT jets obtained with integrated luminosity of 10.71 fb-1 of jet trigger data for high pile-up. The pdf file combinedxsection.pdf and the png files combinedxsection.png
 
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Figure 13. The combined results both for low and high pT jets. Ratio of data to the theoretical prediction of the ABM11 PDF set. The experimental uncertainty and the theoretical uncertainty are represented by the continuous and dashed line, respectively. The error bars correspond to the statistical uncertainty of the data. The pdf files CombinedRatio_ABM11_Y_0.pdf, CombinedRatio_ABM11_Y_1.pdf, CombinedRatio_ABM11_Y_2.pdf, CombinedRatio_ABM11_Y_3.pdf, CombinedRatio_ABM11_Y_4.pdf, CombinedRatio_ABM11_Y_5.pdf and the png files CombinedRatio_ABM11_Y_0.png, CombinedRatio_ABM11_Y_1.png, CombinedRatio_ABM11_Y_2.png, CombinedRatio_ABM11_Y_3.png, CombinedRatio_ABM11_Y_4.png, CombinedRatio_ABM11_Y_5.png
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Figure 14. The combined results both for low and high pT jets. Ratio of data to the theoretical prediction of the CT10 PDF set. The experimental uncertainty and the theoretical uncertainty are represented by the continuous and dashed line, respectively. The error bars correspond to the statistical uncertainty of the data. The pdf files CombinedRatio_CT10_Y_0.pdf, CombinedRatio_CT10_Y_1.pdf, CombinedRatio_CT10_Y_2.pdf, CombinedRatio_CT10_Y_3.pdf, CombinedRatio_CT10_Y_4.pdf, CombinedRatio_CT10_Y_5.pdf and the png files CombinedRatio_CT10_Y_0.png, CombinedRatio_CT10_Y_1.png, CombinedRatio_CT10_Y_2.png, CombinedRatio_CT10_Y_3.png, CombinedRatio_CT10_Y_4.png, CombinedRatio_CT10_Y_5.png

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Figure 15. The combined results both for low and high pT jets. Ratio of data to the theoretical prediction of the HERAPDF1.5 PDF set. The experimental uncertainty and the theoretical uncertainty are represented by the continuous and dashed line, respectively. The error bars correspond to the statistical uncertainty of the data. The pdf files CombinedRatio_HERAPDF_Y_0.pdf, CombinedRatio_HERAPDF_Y_1.pdf, CombinedRatio_HERAPDF_Y_2.pdf, CombinedRatio_HERAPDF_Y_3.pdf, CombinedRatio_HERAPDF_Y_4.pdf, CombinedRatio_HERAPDF_Y_5.pdf and the png files CombinedRatio_HERAPDF_Y_0.png, CombinedRatio_HERAPDF_Y_1.png, CombinedRatio_HERAPDF_Y_2.png, CombinedRatio_HERAPDF_Y_3.png, CombinedRatio_HERAPDF_Y_4.png, CombinedRatio_HERAPDF_Y_5.png
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Figure 16. The combined results both for low and high pT jets. Ratio of data to the theoretical prediction of the MSTW2008 PDF set. The experimental uncertainty and the theoretical uncertainty are represented by the continuous and dashed line, respectively. The error bars correspond to the statistical uncertainty of the data. The pdf files CombinedRatio_MSTW2008_Y_0.pdf, CombinedRatio_MSTW2008_Y_1.pdf, CombinedRatio_MSTW2008_Y_2.pdf, CombinedRatio_MSTW2008_Y_3.pdf, CombinedRatio_MSTW2008_Y_4.pdf, CombinedRatio_MSTW2008_Y_5.pdf and the png files CombinedRatio_MSTW2008_Y_0.png, CombinedRatio_MSTW2008_Y_1.png, CombinedRatio_MSTW2008_Y_2.png, CombinedRatio_MSTW2008_Y_3.png, CombinedRatio_MSTW2008_Y_4.png, CombinedRatio_MSTW2008_Y_5.png
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Figure 17. The combined results both for low and high pT jets. Ratio of data to the theoretical prediction of the NNPDF PDF set. The experimental uncertainty and the theoretical uncertainty are represented by the continuous and dashed line, respectively. The error bars correspond to the statistical uncertainty of the data. The pdf files CombinedRatio_NNPDF21_Y_0.pdf, CombinedRatio_NNPDF21_Y_1.pdf, CombinedRatio_NNPDF21_Y_2.pdf, CombinedRatio_NNPDF21_Y_3.pdf, CombinedRatio_NNPDF21_Y_4.pdf, CombinedRatio_NNPDF21_Y_5.pdf and the png files CombinedRatio_NNPDF21_Y_0.png, CombinedRatio_NNPDF21_Y_1.png, CombinedRatio_NNPDF21_Y_2.png, CombinedRatio_NNPDF21_Y_3.png, CombinedRatio_NNPDF21_Y_4.png, CombinedRatio_NNPDF21_Y_5.png

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Figure 18. The combined results both for low and high pT jets. Ratio of inclusive jet cross sections to the theoretical prediction using the central value of the ABM11 PDF set. The experimental uncertainty is represented by continuous line. The pdf files CombinedRatiopdf_ABM11_Y_0.pdf, CombinedRatiopdf_ABM11_Y_1.pdf, CombinedRatiopdf_ABM11_Y_2.pdf, CombinedRatiopdf_ABM11_Y_3.pdf, CombinedRatiopdf_ABM11_Y_4.pdf, CombinedRatiopdf_ABM11_Y_5.pdf and the png files CombinedRatiopdf_ABM11_Y_0.png, CombinedRatiopdf_ABM11_Y_1.png, CombinedRatiopdf_ABM11_Y_2.png, CombinedRatiopdf_ABM11_Y_3.png, CombinedRatiopdf_ABM11_Y_4.png, CombinedRatiopdf_ABM11_Y_5.png
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Figure 19. The combined results both for low and high pT jets. Ratio of inclusive jet cross sections to the theoretical prediction using the central value of the CT10 PDF set. The experimental uncertainty is represented by continuous line. The pdf files CombinedRatiopdf_CT10_Y_0.pdf, CombinedRatiopdf_CT10_Y_1.pdf, CombinedRatiopdf_CT10_Y_2.pdf, CombinedRatiopdf_CT10_Y_3.pdf, CombinedRatiopdf_CT10_Y_4.pdf, CombinedRatiopdf_CT10_Y_5.pdf and the png files CombinedRatiopdf_CT10_Y_0.png, CombinedRatiopdf_CT10_Y_1.png, CombinedRatiopdf_CT10_Y_2.png, CombinedRatiopdf_CT10_Y_3.png, CombinedRatiopdf_CT10_Y_4.png, CombinedRatiopdf_CT10_Y_5.png
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Figure 20. The combined results both for low and high pT jets. Ratio of inclusive jet cross sections to the theoretical prediction using the central value of the HERAPDF1.5 PDF set. The experimental uncertainty is represented by continuous line. The pdf files CombinedRatiopdf_HERAPDF_Y_0.pdf, CombinedRatiopdf_HERAPDF_Y_1.pdf, CombinedRatiopdf_HERAPDF_Y_2.pdf, CombinedRatiopdf_HERAPDF_Y_3.pdf, CombinedRatiopdf_HERAPDF_Y_4.pdf, CombinedRatiopdf_HERAPDF_Y_5.pdf and the png files CombinedRatiopdf_HERAPDF_Y_0.png, CombinedRatiopdf_HERAPDF_Y_1.png, CombinedRatiopdf_HERAPDF_Y_2.png, CombinedRatiopdf_HERAPDF_Y_3.png, CombinedRatiopdf_HERAPDF_Y_4.png, CombinedRatiopdf_HERAPDF_Y_5.png
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Figure 21. The combined results both for low and high pT jets. Ratio of inclusive jet cross sections to the theoretical prediction using the central value of the MSTW2008 PDF set. The experimental uncertainty is represented by continuous line. The pdf files CombinedRatiopdf_MSTW2008_Y_0.pdf, CombinedRatiopdf_MSTW2008_Y_1.pdf, CombinedRatiopdf_MSTW2008_Y_2.pdf, CombinedRatiopdf_MSTW2008_Y_3.pdf, CombinedRatiopdf_MSTW2008_Y_4.pdf, CombinedRatiopdf_MSTW2008_Y_5.pdf and the png files CombinedRatiopdf_MSTW2008_Y_0.png, CombinedRatiopdf_MSTW2008_Y_1.png, CombinedRatiopdf_MSTW2008_Y_2.png, CombinedRatiopdf_MSTW2008_Y_3.png, CombinedRatiopdf_MSTW2008_Y_4.png, CombinedRatiopdf_MSTW2008_Y_5.png
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Figure 22. The combined results both for low and high pT jets. Ratio of inclusive jet cross sections to the theoretical prediction using the central value of the NNPDF2.1 PDF set. The experimental uncertainty is represented by continuous line. The pdf files CombinedRatiopdf_NNPDF21_Y_0.pdf, CombinedRatiopdf_NNPDF21_Y_1.pdf, CombinedRatiopdf_NNPDF21_Y_2.pdf, CombinedRatiopdf_NNPDF21_Y_3.pdf, CombinedRatiopdf_NNPDF21_Y_4.pdf, CombinedRatiopdf_NNPDF21_Y_5.pdf and the png files CombinedRatiopdf_NNPDF21_Y_0.png, CombinedRatiopdf_NNPDF21_Y_1.png, CombinedRatiopdf_NNPDF21_Y_2.png, CombinedRatiopdf_NNPDF21_Y_3.png, CombinedRatiopdf_NNPDF21_Y_4.png, CombinedRatiopdf_NNPDF21_Y_5.png

Tables

Table 1: The pT differential cross section corrected to hadron level for inclusive jets at and . The first (second) uncertainty reflects the statistical (systematic) contribution.
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Table 2: The pT differential cross section corrected to hadron level for inclusive jets at and . The first (second) uncertainty reflects the statistical (systematic) contribution.
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Table 3: The pT differential cross section corrected to hadron level for inclusive jets at , and . The first (second) uncertainty reflects the statistical (systematic) contribution.
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META FILEATTACHMENT attachment="xsection.pdf" attr="" comment="Combined Cross Section" date="1374762967" name="xsection.pdf" path="xsection.pdf" size="29175" user="ilknur" version="2"
 
META FILEATTACHMENT attachment="CombinedRatio_ABM11_Y_0.pdf" attr="" comment="Combined Ratio ABM11" date="1374765236" name="CombinedRatio_ABM11_Y_0.pdf" path="CombinedRatio_ABM11_Y_0.pdf" size="23999" user="ilknur" version="1"
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META FILEATTACHMENT attachment="combinedxsection.pdf" attr="" comment="Combined Cross Section" date="1374780551" name="combinedxsection.pdf" path="combinedxsection.pdf" size="29175" user="ilknur" version="1"
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Revision 202013-07-25 - SalimCerci

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META TOPICPARENT name="PhysicsResultsFSQ12031"

Measurement of Low pT Jet Cross Sections in proton-proton Collisions at √s = 8 TeV

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Revision 192013-07-25 - IlknurHos

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META TOPICPARENT name="PhysicsResultsFSQ12031"

Measurement of Low pT Jet Cross Sections in proton-proton Collisions at √s = 8 TeV

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Revision 182013-07-25 - IlknurHos

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META TOPICPARENT name="PhysicsResultsFSQ12031"

Measurement of Low pT Jet Cross Sections in proton-proton Collisions at √s = 8 TeV

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Figure 11. Ratio of inclusive jet cross sections to the theoretical prediction using the central value of the NNPDF2.1 PDF set for all bins. The dashed lines show the ratio of the cross sections calculated with the other PDF sets to that calculated with NNPDF2.1. The experimental uncertainty is represented by the continuous line. The pdf files ratio_pdf_NNPDF21_Y_0.pdf, ratio_pdf_NNPDF21_Y_1.pdf, ratio_pdf_NNPDF21_Y_2.pdf, ratio_pdf_NNPDF21_Y_3.pdf, ratio_pdf_NNPDF21_Y_4.pdf, ratio_pdf_NNPDF21_Y_5.pdf, ratio_pdf_NNPDF21_Y_6.pdf and the png files ratio_pdf_NNPDF21_Y_0.png, ratio_pdf_NNPDF21_Y_1.png, ratio_pdf_NNPDF21_Y_2.png, ratio_pdf_NNPDF21_Y_3.png, ratio_pdf_NNPDF21_Y_4.png, ratio_pdf_NNPDF21_Y_5.png, ratio_pdf_NNPDF21_Y_6.png
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Figure 1 a
Figure 12. The combined differential inclusive jet cross sections in comparison to NLO predictions using the NNPDF2.1 PDF set times the NP correction factor. Open markers represent the measurement of low pT jets obtained with the integrated luminosity of 5.8 pb-1 of minimum bias data for low pile-up conditions whereas the filled markers for high pT jets obtained with integrated luminosity of 10.71 pb-1 of jet trigger data for high pile-up. The pdf file cxsection_Y_0.pdf and the png files cxsection_Y_0.png
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Figure 1 a
Figure 12. The combined differential inclusive jet cross sections in comparison to NLO predictions using the NNPDF2.1 PDF set times the NP correction factor. Open markers represent the measurement of low pT jets obtained with the integrated luminosity of 5.8 pb-1 of minimum bias data for low pile-up conditions whereas the filled markers for high pT jets obtained with integrated luminosity of 10.71 pb-1 of jet trigger data for high pile-up. The pdf file xsection.pdf and the png files xsection.png
 

Figure 1 a Figure 1 b Figure 1 c Figure 1 d
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Figure 16. The combined results both for low and high pT jets. Ratio of data to the theoretical prediction of the MSTW2008 PDF set. The experimental uncertainty and the theoretical uncertainty are represented by the continuous and dashed line, respectively. The error bars correspond to the statistical uncertainty of the data. The pdf files CombinedRatio_MSTW2008_Y_0.pdf, CombinedRatio_MSTW2008_Y_1.pdf, CombinedRatio_MSTW2008_Y_2.pdf, CombinedRatio_MSTW2008_Y_3.pdf, CombinedRatio_MSTW2008_Y_4.pdf, CombinedRatio_MSTW2008_Y_5.pdf and the png files CombinedRatio_MSTW2008_Y_0.png, CombinedRatio_MSTW2008_Y_1.png, CombinedRatio_MSTW2008_Y_2.png, CombinedRatio_MSTW2008_Y_3.png, CombinedRatio_MSTW2008_Y_4.png, CombinedRatio_MSTW2008_Y_5.png
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Figure 1 a Figure 1 b Figure 1 c Figure 1 d
Figure 1 e | Figure 1 f |
Figure 17. The combined results both for low and high pT jets. Ratio of data to the theoretical prediction of the NNPDF PDF set. The experimental uncertainty and the theoretical uncertainty are represented by the continuous and dashed line, respectively. The error bars correspond to the statistical uncertainty of the data. The pdf files CombinedRatio_NNPDF_Y_0.pdf, CombinedRatio_NNPDF_Y_1.pdf, CombinedRatio_NNPDF_Y_2.pdf, CombinedRatio_NNPDF_Y_3.pdf, CombinedRatio_NNPDF_Y_4.pdf, CombinedRatio_NNPDF_Y_5.pdf and the png files CombinedRatio_NNPDF_Y_0.png, CombinedRatio_NNPDF_Y_1.png, CombinedRatio_NNPDF_Y_2.png, CombinedRatio_NNPDF_Y_3.png, CombinedRatio_NNPDF_Y_4.png, CombinedRatio_NNPDF_Y_5.png
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Figure 1 a Figure 1 b Figure 1 c Figure 1 d
Figure 1 e | Figure 1 f |
Figure 17. The combined results both for low and high pT jets. Ratio of data to the theoretical prediction of the NNPDF PDF set. The experimental uncertainty and the theoretical uncertainty are represented by the continuous and dashed line, respectively. The error bars correspond to the statistical uncertainty of the data. The pdf files CombinedRatio_NNPDF21_Y_0.pdf, CombinedRatio_NNPDF21_Y_1.pdf, CombinedRatio_NNPDF21_Y_2.pdf, CombinedRatio_NNPDF21_Y_3.pdf, CombinedRatio_NNPDF21_Y_4.pdf, CombinedRatio_NNPDF21_Y_5.pdf and the png files CombinedRatio_NNPDF21_Y_0.png, CombinedRatio_NNPDF21_Y_1.png, CombinedRatio_NNPDF21_Y_2.png, CombinedRatio_NNPDF21_Y_3.png, CombinedRatio_NNPDF21_Y_4.png, CombinedRatio_NNPDF21_Y_5.png
 
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Figure 1 a Figure 1 b Figure 1 c Figure 1 d
Figure 1 e | Figure 1 f |
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Figure 21. The combined results both for low and high pT jets. Ratio of inclusive jet cross sections to the theoretical prediction using the central value of the NNPDF2.1 PDF set. The experimental uncertainty is represented by continuous line. The pdf files CombinedRatiopdf_NNPDF21_Y_0.pdf, CombinedRatiopdf_NNPDF21_Y_1.pdf, CombinedRatiopdf_NNPDF21_Y_2.pdf, CombinedRatiopdf_NNPDF21_Y_3.pdf, CombinedRatiopdf_NNPDF21_Y_4.pdf, CombinedRatiopdf_NNPDF21_Y_5.pdf and the png files CombinedRatiopdf_NNPDF21_Y_0.png, CombinedRatiopdf_NNPDF21_Y_1.png, CombinedRatiopdf_NNPDF21_Y_2.png, CombinedRatiopdf_NNPDF21_Y_3.png, CombinedRatiopdf_NNPDF21_Y_4.png, CombinedRatiopdf_NNPDF21_Y_5.png
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Figure 22. The combined results both for low and high pT jets. Ratio of inclusive jet cross sections to the theoretical prediction using the central value of the NNPDF2.1 PDF set. The experimental uncertainty is represented by continuous line. The pdf files CombinedRatiopdf_NNPDF21_Y_0.pdf, CombinedRatiopdf_NNPDF21_Y_1.pdf, CombinedRatiopdf_NNPDF21_Y_2.pdf, CombinedRatiopdf_NNPDF21_Y_3.pdf, CombinedRatiopdf_NNPDF21_Y_4.pdf, CombinedRatiopdf_NNPDF21_Y_5.pdf and the png files CombinedRatiopdf_NNPDF21_Y_0.png, CombinedRatiopdf_NNPDF21_Y_1.png, CombinedRatiopdf_NNPDF21_Y_2.png, CombinedRatiopdf_NNPDF21_Y_3.png, CombinedRatiopdf_NNPDF21_Y_4.png, CombinedRatiopdf_NNPDF21_Y_5.png
 

Tables

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Revision 172013-07-25 - IlknurHos

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META TOPICPARENT name="PhysicsResultsFSQ12031"

Measurement of Low pT Jet Cross Sections in proton-proton Collisions at √s = 8 TeV

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 Figure 1 g |
Figure 11. Ratio of inclusive jet cross sections to the theoretical prediction using the central value of the NNPDF2.1 PDF set for all bins. The dashed lines show the ratio of the cross sections calculated with the other PDF sets to that calculated with NNPDF2.1. The experimental uncertainty is represented by the continuous line. The pdf files ratio_pdf_NNPDF21_Y_0.pdf, ratio_pdf_NNPDF21_Y_1.pdf, ratio_pdf_NNPDF21_Y_2.pdf, ratio_pdf_NNPDF21_Y_3.pdf, ratio_pdf_NNPDF21_Y_4.pdf, ratio_pdf_NNPDF21_Y_5.pdf, ratio_pdf_NNPDF21_Y_6.pdf and the png files ratio_pdf_NNPDF21_Y_0.png, ratio_pdf_NNPDF21_Y_1.png, ratio_pdf_NNPDF21_Y_2.png, ratio_pdf_NNPDF21_Y_3.png, ratio_pdf_NNPDF21_Y_4.png, ratio_pdf_NNPDF21_Y_5.png, ratio_pdf_NNPDF21_Y_6.png
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Figure 1 a
Figure 12. The combined differential inclusive jet cross sections in comparison to NLO predictions using the NNPDF2.1 PDF set times the NP correction factor. Open markers represent the measurement of low pT jets obtained with the integrated luminosity of 5.8 pb-1 of minimum bias data for low pile-up conditions whereas the filled markers for high pT jets obtained with integrated luminosity of 10.71 pb-1 of jet trigger data for high pile-up. The pdf file cxsection_Y_0.pdf and the png files cxsection_Y_0.png
 
Figure 1 a Figure 1 b Figure 1 c Figure 1 d
Figure 1 e | Figure 1 f |
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Figure 12. The combined results both for low and high pT jets. Ratio of data to the theoretical prediction of the ABM11 PDF set. The experimental uncertainty and the theoretical uncertainty are represented by the continuous and dashed line, respectively. The error bars correspond to the statistical uncertainty of the data. The pdf files CombinedRatio_ABM11_Y_0.pdf, CombinedRatio_ABM11_Y_1.pdf, CombinedRatio_ABM11_Y_2.pdf, CombinedRatio_ABM11_Y_3.pdf, CombinedRatio_ABM11_Y_4.pdf, CombinedRatio_ABM11_Y_5.pdf and the png files CombinedRatio_ABM11_Y_0.png, CombinedRatio_ABM11_Y_1.png, CombinedRatio_ABM11_Y_2.png, CombinedRatio_ABM11_Y_3.png, CombinedRatio_ABM11_Y_4.png, CombinedRatio_ABM11_Y_5.png
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Figure 13. The combined results both for low and high pT jets. Ratio of data to the theoretical prediction of the ABM11 PDF set. The experimental uncertainty and the theoretical uncertainty are represented by the continuous and dashed line, respectively. The error bars correspond to the statistical uncertainty of the data. The pdf files CombinedRatio_ABM11_Y_0.pdf, CombinedRatio_ABM11_Y_1.pdf, CombinedRatio_ABM11_Y_2.pdf, CombinedRatio_ABM11_Y_3.pdf, CombinedRatio_ABM11_Y_4.pdf, CombinedRatio_ABM11_Y_5.pdf and the png files CombinedRatio_ABM11_Y_0.png, CombinedRatio_ABM11_Y_1.png, CombinedRatio_ABM11_Y_2.png, CombinedRatio_ABM11_Y_3.png, CombinedRatio_ABM11_Y_4.png, CombinedRatio_ABM11_Y_5.png
 
Figure 1 a Figure 1 b Figure 1 c Figure 1 d
Figure 1 e | Figure 1 f |
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Figure 13. The combined results both for low and high pT jets. Ratio of data to the theoretical prediction of the CT10 PDF set. The experimental uncertainty and the theoretical uncertainty are represented by the continuous and dashed line, respectively. The error bars correspond to the statistical uncertainty of the data. The pdf files CombinedRatio_CT10_Y_0.pdf, CombinedRatio_CT10_Y_1.pdf, CombinedRatio_CT10_Y_2.pdf, CombinedRatio_CT10_Y_3.pdf, CombinedRatio_CT10_Y_4.pdf, CombinedRatio_CT10_Y_5.pdf and the png files CombinedRatio_CT10_Y_0.png, CombinedRatio_CT10_Y_1.png, CombinedRatio_CT10_Y_2.png, CombinedRatio_CT10_Y_3.png, CombinedRatio_CT10_Y_4.png, CombinedRatio_CT10_Y_5.png
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Figure 14. The combined results both for low and high pT jets. Ratio of data to the theoretical prediction of the CT10 PDF set. The experimental uncertainty and the theoretical uncertainty are represented by the continuous and dashed line, respectively. The error bars correspond to the statistical uncertainty of the data. The pdf files CombinedRatio_CT10_Y_0.pdf, CombinedRatio_CT10_Y_1.pdf, CombinedRatio_CT10_Y_2.pdf, CombinedRatio_CT10_Y_3.pdf, CombinedRatio_CT10_Y_4.pdf, CombinedRatio_CT10_Y_5.pdf and the png files CombinedRatio_CT10_Y_0.png, CombinedRatio_CT10_Y_1.png, CombinedRatio_CT10_Y_2.png, CombinedRatio_CT10_Y_3.png, CombinedRatio_CT10_Y_4.png, CombinedRatio_CT10_Y_5.png
 

Figure 1 a Figure 1 b Figure 1 c Figure 1 d
Figure 1 e | Figure 1 f |
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Figure 14. The combined results both for low and high pT jets. Ratio of data to the theoretical prediction of the HERAPDF1.5 PDF set. The experimental uncertainty and the theoretical uncertainty are represented by the continuous and dashed line, respectively. The error bars correspond to the statistical uncertainty of the data. The pdf files CombinedRatio_HERAPDF_Y_0.pdf, CombinedRatio_HERAPDF_Y_1.pdf, CombinedRatio_HERAPDF_Y_2.pdf, CombinedRatio_HERAPDF_Y_3.pdf, CombinedRatio_HERAPDF_Y_4.pdf, CombinedRatio_HERAPDF_Y_5.pdf and the png files CombinedRatio_HERAPDF_Y_0.png, CombinedRatio_HERAPDF_Y_1.png, CombinedRatio_HERAPDF_Y_2.png, CombinedRatio_HERAPDF_Y_3.png, CombinedRatio_HERAPDF_Y_4.png, CombinedRatio_HERAPDF_Y_5.png
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Figure 15. The combined results both for low and high pT jets. Ratio of data to the theoretical prediction of the HERAPDF1.5 PDF set. The experimental uncertainty and the theoretical uncertainty are represented by the continuous and dashed line, respectively. The error bars correspond to the statistical uncertainty of the data. The pdf files CombinedRatio_HERAPDF_Y_0.pdf, CombinedRatio_HERAPDF_Y_1.pdf, CombinedRatio_HERAPDF_Y_2.pdf, CombinedRatio_HERAPDF_Y_3.pdf, CombinedRatio_HERAPDF_Y_4.pdf, CombinedRatio_HERAPDF_Y_5.pdf and the png files CombinedRatio_HERAPDF_Y_0.png, CombinedRatio_HERAPDF_Y_1.png, CombinedRatio_HERAPDF_Y_2.png, CombinedRatio_HERAPDF_Y_3.png, CombinedRatio_HERAPDF_Y_4.png, CombinedRatio_HERAPDF_Y_5.png
 

Figure 1 a Figure 1 b Figure 1 c Figure 1 d
Figure 1 e | Figure 1 f |
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Figure 15. The combined results both for low and high pT jets. Ratio of data to the theoretical prediction of the MSTW2008 PDF set. The experimental uncertainty and the theoretical uncertainty are represented by the continuous and dashed line, respectively. The error bars correspond to the statistical uncertainty of the data. The pdf files CombinedRatio_MSTW2008_Y_0.pdf, CombinedRatio_MSTW2008_Y_1.pdf, CombinedRatio_MSTW2008_Y_2.pdf, CombinedRatio_MSTW2008_Y_3.pdf, CombinedRatio_MSTW2008_Y_4.pdf, CombinedRatio_MSTW2008_Y_5.pdf and the png files CombinedRatio_MSTW2008_Y_0.png, CombinedRatio_MSTW2008_Y_1.png, CombinedRatio_MSTW2008_Y_2.png, CombinedRatio_MSTW2008_Y_3.png, CombinedRatio_MSTW2008_Y_4.png, CombinedRatio_MSTW2008_Y_5.png
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Figure 16. The combined results both for low and high pT jets. Ratio of data to the theoretical prediction of the MSTW2008 PDF set. The experimental uncertainty and the theoretical uncertainty are represented by the continuous and dashed line, respectively. The error bars correspond to the statistical uncertainty of the data. The pdf files CombinedRatio_MSTW2008_Y_0.pdf, CombinedRatio_MSTW2008_Y_1.pdf, CombinedRatio_MSTW2008_Y_2.pdf, CombinedRatio_MSTW2008_Y_3.pdf, CombinedRatio_MSTW2008_Y_4.pdf, CombinedRatio_MSTW2008_Y_5.pdf and the png files CombinedRatio_MSTW2008_Y_0.png, CombinedRatio_MSTW2008_Y_1.png, CombinedRatio_MSTW2008_Y_2.png, CombinedRatio_MSTW2008_Y_3.png, CombinedRatio_MSTW2008_Y_4.png, CombinedRatio_MSTW2008_Y_5.png
 

Figure 1 a Figure 1 b Figure 1 c Figure 1 d
Figure 1 e | Figure 1 f |
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Figure 16. The combined results both for low and high pT jets. Ratio of data to the theoretical prediction of the NNPDF PDF set. The experimental uncertainty and the theoretical uncertainty are represented by the continuous and dashed line, respectively. The error bars correspond to the statistical uncertainty of the data. The pdf files CombinedRatio_NNPDF_Y_0.pdf, CombinedRatio_NNPDF_Y_1.pdf, CombinedRatio_NNPDF_Y_2.pdf, CombinedRatio_NNPDF_Y_3.pdf, CombinedRatio_NNPDF_Y_4.pdf, CombinedRatio_NNPDF_Y_5.pdf and the png files CombinedRatio_NNPDF_Y_0.png, CombinedRatio_NNPDF_Y_1.png, CombinedRatio_NNPDF_Y_2.png, CombinedRatio_NNPDF_Y_3.png, CombinedRatio_NNPDF_Y_4.png, CombinedRatio_NNPDF_Y_5.png
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Figure 17. The combined results both for low and high pT jets. Ratio of data to the theoretical prediction of the NNPDF PDF set. The experimental uncertainty and the theoretical uncertainty are represented by the continuous and dashed line, respectively. The error bars correspond to the statistical uncertainty of the data. The pdf files CombinedRatio_NNPDF_Y_0.pdf, CombinedRatio_NNPDF_Y_1.pdf, CombinedRatio_NNPDF_Y_2.pdf, CombinedRatio_NNPDF_Y_3.pdf, CombinedRatio_NNPDF_Y_4.pdf, CombinedRatio_NNPDF_Y_5.pdf and the png files CombinedRatio_NNPDF_Y_0.png, CombinedRatio_NNPDF_Y_1.png, CombinedRatio_NNPDF_Y_2.png, CombinedRatio_NNPDF_Y_3.png, CombinedRatio_NNPDF_Y_4.png, CombinedRatio_NNPDF_Y_5.png
 

Figure 1 a Figure 1 b Figure 1 c Figure 1 d
Figure 1 e | Figure 1 f |
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Figure 17. The combined results both for low and high pT jets. Ratio of inclusive jet cross sections to the theoretical prediction using the central value of the ABM11 PDF set. The experimental uncertainty is represented by continuous line. The pdf files CombinedRatio_NNPDF_Y_0.pdf, CombinedRatiopdf_ABM11_Y_1.pdf, CombinedRatiopdf_ABM11_Y_2.pdf, CombinedRatiopdf_ABM11_Y_3.pdf, CombinedRatiopdf_ABM11_Y_4.pdf, CombinedRatio_NNPDFCombinedRatiopdf_ABM11_Y_5.pdf and the png files CombinedRatiopdf_ABM11_Y_0.png, CombinedRatiopdf_ABM11_Y_1.png, CombinedRatiopdf_ABM11_Y_2.png, CombinedRatiopdf_ABM11_Y_3.png, CombinedRatiopdf_ABM11_Y_4.png, CombinedRatiopdf_ABM11_Y_5.png
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Figure 18. The combined results both for low and high pT jets. Ratio of inclusive jet cross sections to the theoretical prediction using the central value of the ABM11 PDF set. The experimental uncertainty is represented by continuous line. The pdf files CombinedRatiopdf_ABM11_Y_0.pdf, CombinedRatiopdf_ABM11_Y_1.pdf, CombinedRatiopdf_ABM11_Y_2.pdf, CombinedRatiopdf_ABM11_Y_3.pdf, CombinedRatiopdf_ABM11_Y_4.pdf, CombinedRatiopdf_ABM11_Y_5.pdf and the png files CombinedRatiopdf_ABM11_Y_0.png, CombinedRatiopdf_ABM11_Y_1.png, CombinedRatiopdf_ABM11_Y_2.png, CombinedRatiopdf_ABM11_Y_3.png, CombinedRatiopdf_ABM11_Y_4.png, CombinedRatiopdf_ABM11_Y_5.png

Figure 1 a Figure 1 b Figure 1 c Figure 1 d
Figure 1 e | Figure 1 f |
Figure 19. The combined results both for low and high pT jets. Ratio of inclusive jet cross sections to the theoretical prediction using the central value of the CT10 PDF set. The experimental uncertainty is represented by continuous line. The pdf files CombinedRatiopdf_CT10_Y_0.pdf, CombinedRatiopdf_CT10_Y_1.pdf, CombinedRatiopdf_CT10_Y_2.pdf, CombinedRatiopdf_CT10_Y_3.pdf, CombinedRatiopdf_CT10_Y_4.pdf, CombinedRatiopdf_CT10_Y_5.pdf and the png files CombinedRatiopdf_CT10_Y_0.png, CombinedRatiopdf_CT10_Y_1.png, CombinedRatiopdf_CT10_Y_2.png, CombinedRatiopdf_CT10_Y_3.png, CombinedRatiopdf_CT10_Y_4.png, CombinedRatiopdf_CT10_Y_5.png

Figure 1 a Figure 1 b Figure 1 c Figure 1 d
Figure 1 e | Figure 1 f |
Figure 20. The combined results both for low and high pT jets. Ratio of inclusive jet cross sections to the theoretical prediction using the central value of the HERAPDF1.5 PDF set. The experimental uncertainty is represented by continuous line. The pdf files CombinedRatiopdf_HERAPDF_Y_0.pdf, CombinedRatiopdf_HERAPDF_Y_1.pdf, CombinedRatiopdf_HERAPDF_Y_2.pdf, CombinedRatiopdf_HERAPDF_Y_3.pdf, CombinedRatiopdf_HERAPDF_Y_4.pdf, CombinedRatiopdf_HERAPDF_Y_5.pdf and the png files CombinedRatiopdf_HERAPDF_Y_0.png, CombinedRatiopdf_HERAPDF_Y_1.png, CombinedRatiopdf_HERAPDF_Y_2.png, CombinedRatiopdf_HERAPDF_Y_3.png, CombinedRatiopdf_HERAPDF_Y_4.png, CombinedRatiopdf_HERAPDF_Y_5.png

Figure 1 a Figure 1 b Figure 1 c Figure 1 d
Figure 1 e | Figure 1 f |
Figure 21. The combined results both for low and high pT jets. Ratio of inclusive jet cross sections to the theoretical prediction using the central value of the MSTW2008 PDF set. The experimental uncertainty is represented by continuous line. The pdf files CombinedRatiopdf_MSTW2008_Y_0.pdf, CombinedRatiopdf_MSTW2008_Y_1.pdf, CombinedRatiopdf_MSTW2008_Y_2.pdf, CombinedRatiopdf_MSTW2008_Y_3.pdf, CombinedRatiopdf_MSTW2008_Y_4.pdf, CombinedRatiopdf_MSTW2008_Y_5.pdf and the png files CombinedRatiopdf_MSTW2008_Y_0.png, CombinedRatiopdf_MSTW2008_Y_1.png, CombinedRatiopdf_MSTW2008_Y_2.png, CombinedRatiopdf_MSTW2008_Y_3.png, CombinedRatiopdf_MSTW2008_Y_4.png, CombinedRatiopdf_MSTW2008_Y_5.png
 
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Figure 1 a Figure 1 b Figure 1 c Figure 1 d
Figure 1 e | Figure 1 f |
Figure 21. The combined results both for low and high pT jets. Ratio of inclusive jet cross sections to the theoretical prediction using the central value of the NNPDF2.1 PDF set. The experimental uncertainty is represented by continuous line. The pdf files CombinedRatiopdf_NNPDF21_Y_0.pdf, CombinedRatiopdf_NNPDF21_Y_1.pdf, CombinedRatiopdf_NNPDF21_Y_2.pdf, CombinedRatiopdf_NNPDF21_Y_3.pdf, CombinedRatiopdf_NNPDF21_Y_4.pdf, CombinedRatiopdf_NNPDF21_Y_5.pdf and the png files CombinedRatiopdf_NNPDF21_Y_0.png, CombinedRatiopdf_NNPDF21_Y_1.png, CombinedRatiopdf_NNPDF21_Y_2.png, CombinedRatiopdf_NNPDF21_Y_3.png, CombinedRatiopdf_NNPDF21_Y_4.png, CombinedRatiopdf_NNPDF21_Y_5.png
 

Tables

Revision 162013-07-25 - IlknurHos

Line: 1 to 1
 
META TOPICPARENT name="PhysicsResultsFSQ12031"

Measurement of Low pT Jet Cross Sections in proton-proton Collisions at √s = 8 TeV

Line: 89 to 89
 
Figure 1 a Figure 1 b Figure 1 c Figure 1 d
Figure 1 e | Figure 1 f |
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Figure 12. The combined results both for low and high pT jets. Ratio of data to the theoretical prediction of the ABM11 PDF set. The experimental uncertainty and the theoretical uncertainty are represented by the continuous and dashed line, respectively. The error bars correspond to the statistical uncertainty of the data.
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Figure 12. The combined results both for low and high pT jets. Ratio of data to the theoretical prediction of the ABM11 PDF set. The experimental uncertainty and the theoretical uncertainty are represented by the continuous and dashed line, respectively. The error bars correspond to the statistical uncertainty of the data. The pdf files CombinedRatio_ABM11_Y_0.pdf, CombinedRatio_ABM11_Y_1.pdf, CombinedRatio_ABM11_Y_2.pdf, CombinedRatio_ABM11_Y_3.pdf, CombinedRatio_ABM11_Y_4.pdf, CombinedRatio_ABM11_Y_5.pdf and the png files CombinedRatio_ABM11_Y_0.png, CombinedRatio_ABM11_Y_1.png, CombinedRatio_ABM11_Y_2.png, CombinedRatio_ABM11_Y_3.png, CombinedRatio_ABM11_Y_4.png, CombinedRatio_ABM11_Y_5.png
 
Figure 1 a Figure 1 b Figure 1 c Figure 1 d
Figure 1 e | Figure 1 f |
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Figure 13. The combined results both for low and high pT jets. Ratio of data to the theoretical prediction of the CT10 PDF set. The experimental uncertainty and the theoretical uncertainty are represented by the continuous and dashed line, respectively. The error bars correspond to the statistical uncertainty of the data.
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Figure 13. The combined results both for low and high pT jets. Ratio of data to the theoretical prediction of the CT10 PDF set. The experimental uncertainty and the theoretical uncertainty are represented by the continuous and dashed line, respectively. The error bars correspond to the statistical uncertainty of the data. The pdf files CombinedRatio_CT10_Y_0.pdf, CombinedRatio_CT10_Y_1.pdf, CombinedRatio_CT10_Y_2.pdf, CombinedRatio_CT10_Y_3.pdf, CombinedRatio_CT10_Y_4.pdf, CombinedRatio_CT10_Y_5.pdf and the png files CombinedRatio_CT10_Y_0.png, CombinedRatio_CT10_Y_1.png, CombinedRatio_CT10_Y_2.png, CombinedRatio_CT10_Y_3.png, CombinedRatio_CT10_Y_4.png, CombinedRatio_CT10_Y_5.png
 
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Figure 1 a Figure 1 b Figure 1 c Figure 1 d
Figure 1 e | Figure 1 f |
Figure 13. The combined results both for low and high pT jets. Ratio of data to the theoretical prediction of the CT10 PDF set. The experimental uncertainty and the theoretical uncertainty are represented by the continuous and dashed line, respectively. The error bars correspond to the statistical uncertainty of the data.
 
Figure 1 a Figure 1 b Figure 1 c Figure 1 d
Figure 1 e | Figure 1 f |
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Figure 14. The combined results both for low and high pT jets. Ratio of data to the theoretical prediction of the HERAPDF1.5 PDF set. The experimental uncertainty and the theoretical uncertainty are represented by the continuous and dashed line, respectively. The error bars correspond to the statistical uncertainty of the data.
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Figure 14. The combined results both for low and high pT jets. Ratio of data to the theoretical prediction of the HERAPDF1.5 PDF set. The experimental uncertainty and the theoretical uncertainty are represented by the continuous and dashed line, respectively. The error bars correspond to the statistical uncertainty of the data. The pdf files CombinedRatio_HERAPDF_Y_0.pdf, CombinedRatio_HERAPDF_Y_1.pdf, CombinedRatio_HERAPDF_Y_2.pdf, CombinedRatio_HERAPDF_Y_3.pdf, CombinedRatio_HERAPDF_Y_4.pdf, CombinedRatio_HERAPDF_Y_5.pdf and the png files CombinedRatio_HERAPDF_Y_0.png, CombinedRatio_HERAPDF_Y_1.png, CombinedRatio_HERAPDF_Y_2.png, CombinedRatio_HERAPDF_Y_3.png, CombinedRatio_HERAPDF_Y_4.png, CombinedRatio_HERAPDF_Y_5.png
 

Figure 1 a Figure 1 b Figure 1 c Figure 1 d
Figure 1 e | Figure 1 f |
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Figure 15. The combined results both for low and high pT jets. Ratio of data to the theoretical prediction of the MSTW2008 PDF set. The experimental uncertainty and the theoretical uncertainty are represented by the continuous and dashed line, respectively. The error bars correspond to the statistical uncertainty of the data.
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Figure 15. The combined results both for low and high pT jets. Ratio of data to the theoretical prediction of the MSTW2008 PDF set. The experimental uncertainty and the theoretical uncertainty are represented by the continuous and dashed line, respectively. The error bars correspond to the statistical uncertainty of the data. The pdf files CombinedRatio_MSTW2008_Y_0.pdf, CombinedRatio_MSTW2008_Y_1.pdf, CombinedRatio_MSTW2008_Y_2.pdf, CombinedRatio_MSTW2008_Y_3.pdf, CombinedRatio_MSTW2008_Y_4.pdf, CombinedRatio_MSTW2008_Y_5.pdf and the png files CombinedRatio_MSTW2008_Y_0.png, CombinedRatio_MSTW2008_Y_1.png, CombinedRatio_MSTW2008_Y_2.png, CombinedRatio_MSTW2008_Y_3.png, CombinedRatio_MSTW2008_Y_4.png, CombinedRatio_MSTW2008_Y_5.png
 

Figure 1 a Figure 1 b Figure 1 c Figure 1 d
Figure 1 e | Figure 1 f |
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Figure 16. The combined results both for low and high pT jets. Ratio of data to the theoretical prediction of the NNPDF PDF set. The experimental uncertainty and the theoretical uncertainty are represented by the continuous and dashed line, respectively. The error bars correspond to the statistical uncertainty of the data.
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Figure 16. The combined results both for low and high pT jets. Ratio of data to the theoretical prediction of the NNPDF PDF set. The experimental uncertainty and the theoretical uncertainty are represented by the continuous and dashed line, respectively. The error bars correspond to the statistical uncertainty of the data. The pdf files CombinedRatio_NNPDF_Y_0.pdf, CombinedRatio_NNPDF_Y_1.pdf, CombinedRatio_NNPDF_Y_2.pdf, CombinedRatio_NNPDF_Y_3.pdf, CombinedRatio_NNPDF_Y_4.pdf, CombinedRatio_NNPDF_Y_5.pdf and the png files CombinedRatio_NNPDF_Y_0.png, CombinedRatio_NNPDF_Y_1.png, CombinedRatio_NNPDF_Y_2.png, CombinedRatio_NNPDF_Y_3.png, CombinedRatio_NNPDF_Y_4.png, CombinedRatio_NNPDF_Y_5.png

Figure 1 a Figure 1 b Figure 1 c Figure 1 d
Figure 1 e | Figure 1 f |
Figure 17. The combined results both for low and high pT jets. Ratio of inclusive jet cross sections to the theoretical prediction using the central value of the ABM11 PDF set. The experimental uncertainty is represented by continuous line. The pdf files CombinedRatio_NNPDF_Y_0.pdf, CombinedRatiopdf_ABM11_Y_1.pdf, CombinedRatiopdf_ABM11_Y_2.pdf, CombinedRatiopdf_ABM11_Y_3.pdf, CombinedRatiopdf_ABM11_Y_4.pdf, CombinedRatio_NNPDFCombinedRatiopdf_ABM11_Y_5.pdf and the png files CombinedRatiopdf_ABM11_Y_0.png, CombinedRatiopdf_ABM11_Y_1.png, CombinedRatiopdf_ABM11_Y_2.png, CombinedRatiopdf_ABM11_Y_3.png, CombinedRatiopdf_ABM11_Y_4.png, CombinedRatiopdf_ABM11_Y_5.png
 
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Deleted:
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Revision 152013-07-23 - IlknurHos

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META TOPICPARENT name="PhysicsResultsFSQ12031"

Measurement of Low pT Jet Cross Sections in proton-proton Collisions at √s = 8 TeV

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 Figure 1 e | Figure 1 f | Figure 1 g |
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Figure 3. Inclusive jet cross sections for data over the theoretical prediction of the CT10 PDF set for all . The experimental and theoretical systematic uncertainties are represented by the continuous and dashed lines, respectively. The pdf file ratio_CT10_Y_0.pdf, ratio_CT10_Y_1.pdf, ratio_CT10_Y_2.pdf, ratio_CT10_Y_3.pdf, ratio_CT10_Y_4.pdf, ratio_CT10_Y_5.pdf, ratio_CT10_Y_6.pdf and the png file ratio_CT10_Y_0.png, ratio_CT10_Y_1.png, ratio_CT10_Y_2.png, ratio_CT10_Y_3.png, ratio_CT10_Y_4.png, ratio_CT10_Y_5.png, ratio_CT10_Y_6.png
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Figure 3. Inclusive jet cross sections for data over the theoretical prediction of the CT10 PDF set for all . The experimental and theoretical systematic uncertainties are represented by the continuous and dashed lines, respectively. The pdf files ratio_CT10_Y_0.pdf, ratio_CT10_Y_1.pdf, ratio_CT10_Y_2.pdf, ratio_CT10_Y_3.pdf, ratio_CT10_Y_4.pdf, ratio_CT10_Y_5.pdf, ratio_CT10_Y_6.pdf and the png files ratio_CT10_Y_0.png, ratio_CT10_Y_1.png, ratio_CT10_Y_2.png, ratio_CT10_Y_3.png, ratio_CT10_Y_4.png, ratio_CT10_Y_5.png, ratio_CT10_Y_6.png
 

Figure 1 a Figure 1 b Figure 1 c Figure 1 d
Figure 1 e | Figure 1 f | Figure 1 g |
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Figure 4. Inclusive jet cross sections for data over the theoretical prediction of the HERAPDF1.5 PDF set for all . The experimental and theoretical systematic uncertainties are represented by the continuous and dashed lines, respectively. The pdf file ratio_HERAPDF15_Y_0.pdf, ratio_HERAPDF15_Y_1.pdf, ratio_HERAPDF15_Y_2.pdf, ratio_HERAPDF15_Y_3.pdf, ratio_HERAPDF15_Y_4.pdf, ratio_HERAPDF15_Y_5.pdf, ratio_HERAPDF15_Y_6.pdf and the png file ratio_HERAPDF15_Y_0.png, ratio_HERAPDF15_Y_1.png, ratio_HERAPDF15_Y_2.png, ratio_HERAPDF15_Y_3.png, ratio_HERAPDF15_Y_4.png, ratio_HERAPDF15_Y_5.png, ratio_HERAPDF15_Y_6.png
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Figure 4. Inclusive jet cross sections for data over the theoretical prediction of the HERAPDF1.5 PDF set for all . The experimental and theoretical systematic uncertainties are represented by the continuous and dashed lines, respectively. The pdf files ratio_HERAPDF15_Y_0.pdf, ratio_HERAPDF15_Y_1.pdf, ratio_HERAPDF15_Y_2.pdf, ratio_HERAPDF15_Y_3.pdf, ratio_HERAPDF15_Y_4.pdf, ratio_HERAPDF15_Y_5.pdf, ratio_HERAPDF15_Y_6.pdf and the png files ratio_HERAPDF15_Y_0.png, ratio_HERAPDF15_Y_1.png, ratio_HERAPDF15_Y_2.png, ratio_HERAPDF15_Y_3.png, ratio_HERAPDF15_Y_4.png, ratio_HERAPDF15_Y_5.png, ratio_HERAPDF15_Y_6.png
 

Figure 1 a Figure 1 b Figure 1 c Figure 1 d
Figure 1 e | Figure 1 f | Figure 1 g |
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Figure 5. Inclusive jet cross sections for data over the theoretical prediction of the MSTW2008 PDF set for all . The experimental and theoretical systematic uncertainties are represented by the continuous and dashed lines, respectively. The pdf file ratio_MSTW2008_Y_0.pdf, ratio_MSTW2008_Y_1.pdf, ratio_MSTW2008_Y_2.pdf, ratio_MSTW2008_Y_3.pdf, ratio_MSTW2008_Y_4.pdf, ratio_MSTW2008_Y_5.pdf, ratio_MSTW2008_Y_6.pdf and the png file ratio_MSTW2008_Y_0.png
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Figure 5. Inclusive jet cross sections for data over the theoretical prediction of the MSTW2008 PDF set for all . The experimental and theoretical systematic uncertainties are represented by the continuous and dashed lines, respectively. The pdf files ratio_MSTW2008_Y_0.pdf, ratio_MSTW2008_Y_1.pdf, ratio_MSTW2008_Y_2.pdf, ratio_MSTW2008_Y_3.pdf, ratio_MSTW2008_Y_4.pdf, ratio_MSTW2008_Y_5.pdf, ratio_MSTW2008_Y_6.pdf and the png files ratio_MSTW2008_Y_0.png
 

Figure 1 a Figure 1 b Figure 1 c Figure 1 d
Figure 1 e | Figure 1 f | Figure 1 g |
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Figure 6. Inclusive jet cross sections for data over the theoretical prediction of the NNPDF2.1 PDF set for all . The experimental and theoretical systematic uncertainties are represented by the continuous and dashed lines, respectively. The pdf file ratio_NNPDF21_Y_0.pdf, ratio_NNPDF21_Y_1.pdf, ratio_NNPDF21_Y_2.pdf, ratio_NNPDF21_Y_3.pdf, ratio_NNPDF21_Y_4.pdf, ratio_NNPDF21_Y_5.pdf, ratio_NNPDF21_Y_6.pdf and the png file ratio_NNPDF21_Y_0.png, ratio_NNPDF21_Y_1.png, ratio_NNPDF21_Y_2.png, ratio_NNPDF21_Y_3.png, ratio_NNPDF21_Y_4.png, ratio_NNPDF21_Y_5.png, ratio_NNPDF21_Y_6.png
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Figure 6. Inclusive jet cross sections for data over the theoretical prediction of the NNPDF2.1 PDF set for all . The experimental and theoretical systematic uncertainties are represented by the continuous and dashed lines, respectively. The pdf files ratio_NNPDF21_Y_0.pdf, ratio_NNPDF21_Y_1.pdf, ratio_NNPDF21_Y_2.pdf, ratio_NNPDF21_Y_3.pdf, ratio_NNPDF21_Y_4.pdf, ratio_NNPDF21_Y_5.pdf, ratio_NNPDF21_Y_6.pdf and the png files ratio_NNPDF21_Y_0.png, ratio_NNPDF21_Y_1.png, ratio_NNPDF21_Y_2.png, ratio_NNPDF21_Y_3.png, ratio_NNPDF21_Y_4.png, ratio_NNPDF21_Y_5.png, ratio_NNPDF21_Y_6.png
 

Figure 1 a Figure 1 b Figure 1 c Figure 1 d
Figure 1 e | Figure 1 f | Figure 1 g |
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Figure 7. Ratio of inclusive jet cross sections to the theoretical prediction using the central value of the ABM11 PDF set for all bins. The dashed lines show the ratio of the cross sections calculated with the other PDF sets to that calculated with ABM11. The experimental uncertainty is represented by the continuous line. The pdf file ratio_pdf_ABM11_Y_0.pdf, ratio_pdf_ABM11_Y_1.pdf, ratio_pdf_ABM11_Y_2.pdf, ratio_pdf_ABM11_Y_3.pdf, ratio_pdf_ABM11_Y_4.pdf, ratio_pdf_ABM11_Y_5.pdf, ratio_pdf_ABM11_Y_6.pdf and the png file ratio_pdf_ABM11_Y_0.png, ratio_pdf_ABM11_Y_1.png, ratio_pdf_ABM11_Y_2.png, ratio_pdf_ABM11_Y_3.png, ratio_pdf_ABM11_Y_4.png, ratio_pdf_ABM11_Y_5.png, ratio_pdf_ABM11_Y_6.png
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Figure 7. Ratio of inclusive jet cross sections to the theoretical prediction using the central value of the ABM11 PDF set for all bins. The dashed lines show the ratio of the cross sections calculated with the other PDF sets to that calculated with ABM11. The experimental uncertainty is represented by the continuous line. The pdf files ratio_pdf_ABM11_Y_0.pdf, ratio_pdf_ABM11_Y_1.pdf, ratio_pdf_ABM11_Y_2.pdf, ratio_pdf_ABM11_Y_3.pdf, ratio_pdf_ABM11_Y_4.pdf, ratio_pdf_ABM11_Y_5.pdf, ratio_pdf_ABM11_Y_6.pdf and the png files ratio_pdf_ABM11_Y_0.png, ratio_pdf_ABM11_Y_1.png, ratio_pdf_ABM11_Y_2.png, ratio_pdf_ABM11_Y_3.png, ratio_pdf_ABM11_Y_4.png, ratio_pdf_ABM11_Y_5.png, ratio_pdf_ABM11_Y_6.png
 

Figure 1 a Figure 1 b Figure 1 c Figure 1 d
Figure 1 e | Figure 1 f | Figure 1 g |
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Figure 8. Ratio of inclusive jet cross sections to the theoretical prediction using the central value of the CT10 PDF set for all bins. The dashed lines show the ratio of the cross sections calculated with the other PDF sets to that calculated with CT10. The experimental uncertainty is represented by the continuous line. The pdf file ratio_pdf_CT10_Y_0.pdf, ratio_pdf_CT10_Y_1.pdf, ratio_pdf_CT10_Y_2.pdf, ratio_pdf_CT10_Y_3.pdf, ratio_pdf_CT10_Y_4.pdf, ratio_pdf_CT10_Y_5.pdf, ratio_pdf_CT10_Y_6.pdf and the png file ratio_pdf_CT10_Y_0.png, ratio_pdf_CT10_Y_1.png, ratio_pdf_CT10_Y_2.png, ratio_pdf_CT10_Y_3.png, ratio_pdf_CT10_Y_4.png, ratio_pdf_CT10_Y_5.png, ratio_pdf_CT10_Y_6.png
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Figure 8. Ratio of inclusive jet cross sections to the theoretical prediction using the central value of the CT10 PDF set for all bins. The dashed lines show the ratio of the cross sections calculated with the other PDF sets to that calculated with CT10. The experimental uncertainty is represented by the continuous line. The pdf files ratio_pdf_CT10_Y_0.pdf, ratio_pdf_CT10_Y_1.pdf, ratio_pdf_CT10_Y_2.pdf, ratio_pdf_CT10_Y_3.pdf, ratio_pdf_CT10_Y_4.pdf, ratio_pdf_CT10_Y_5.pdf, ratio_pdf_CT10_Y_6.pdf and the png files ratio_pdf_CT10_Y_0.png, ratio_pdf_CT10_Y_1.png, ratio_pdf_CT10_Y_2.png, ratio_pdf_CT10_Y_3.png, ratio_pdf_CT10_Y_4.png, ratio_pdf_CT10_Y_5.png, ratio_pdf_CT10_Y_6.png
 
Figure 1 a Figure 1 b Figure 1 c Figure 1 d
Figure 1 e | Figure 1 f | Figure 1 g |
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Figure 9. Ratio of inclusive jet cross sections to the theoretical prediction using the central value of the HERAPDF1.5 PDF set for all bins. The dashed lines show the ratio of the cross sections calculated with the other PDF sets to that calculated with HERAPDF1.5. The experimental uncertainty is represented by the continuous line. The pdf file ratio_pdf_HERAPDF15_Y_0.pdf, ratio_pdf_HERAPDF15_Y_1.pdf, ratio_pdf_HERAPDF15_Y_2.pdf, ratio_pdf_HERAPDF15_Y_3.pdf, ratio_pdf_HERAPDF15_Y_4.pdf, ratio_pdf_HERAPDF15_Y_5.pdf, ratio_pdf_HERAPDF15_Y_6.pdf and the png file ratio_pdf_HERAPDF15_Y_0.png, ratio_pdf_HERAPDF15_Y_1.png, ratio_pdf_HERAPDF15_Y_2.png, ratio_pdf_HERAPDF15_Y_3.png, ratio_pdf_HERAPDF15_Y_4.png, ratio_pdf_HERAPDF15_Y_5.png, ratio_pdf_HERAPDF15_Y_6.png
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Figure 9. Ratio of inclusive jet cross sections to the theoretical prediction using the central value of the HERAPDF1.5 PDF set for all bins. The dashed lines show the ratio of the cross sections calculated with the other PDF sets to that calculated with HERAPDF1.5. The experimental uncertainty is represented by the continuous line. The pdf files ratio_pdf_HERAPDF15_Y_0.pdf, ratio_pdf_HERAPDF15_Y_1.pdf, ratio_pdf_HERAPDF15_Y_2.pdf, ratio_pdf_HERAPDF15_Y_3.pdf, ratio_pdf_HERAPDF15_Y_4.pdf, ratio_pdf_HERAPDF15_Y_5.pdf, ratio_pdf_HERAPDF15_Y_6.pdf and the png files ratio_pdf_HERAPDF15_Y_0.png, ratio_pdf_HERAPDF15_Y_1.png, ratio_pdf_HERAPDF15_Y_2.png, ratio_pdf_HERAPDF15_Y_3.png, ratio_pdf_HERAPDF15_Y_4.png, ratio_pdf_HERAPDF15_Y_5.png, ratio_pdf_HERAPDF15_Y_6.png
 
Figure 1 a Figure 1 b Figure 1 c Figure 1 d
Figure 1 e | Figure 1 f | Figure 1 g |
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Figure 10. Ratio of inclusive jet cross sections to the theoretical prediction using the central value of the MSTW2008 PDF set for all bins. The dashed lines show the ratio of the cross sections calculated with the other PDF sets to that calculated with MSTW2008. The experimental uncertainty is represented by the continuous line. The pdf file ratio_pdf_MSTW2008_Y_0.pdf, ratio_pdf_MSTW2008_Y_1.pdf, ratio_pdf_MSTW2008_Y_2.pdf, ratio_pdf_MSTW2008_Y_3.pdf, ratio_pdf_MSTW2008_Y_4.pdf, ratio_pdf_MSTW2008_Y_5.pdf, ratio_pdf_MSTW2008_Y_6.pdf and the png file ratio_pdf_MSTW2008_Y_0.png, ratio_pdf_MSTW2008_Y_1.png, ratio_pdf_MSTW2008_Y_2.png, ratio_pdf_MSTW2008_Y_3.png, ratio_pdf_MSTW2008_Y_4.png, ratio_pdf_MSTW2008_Y_5.png, ratio_pdf_MSTW2008_Y_6.png
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Figure 10. Ratio of inclusive jet cross sections to the theoretical prediction using the central value of the MSTW2008 PDF set for all bins. The dashed lines show the ratio of the cross sections calculated with the other PDF sets to that calculated with MSTW2008. The experimental uncertainty is represented by the continuous line. The pdf files ratio_pdf_MSTW2008_Y_0.pdf, ratio_pdf_MSTW2008_Y_1.pdf, ratio_pdf_MSTW2008_Y_2.pdf, ratio_pdf_MSTW2008_Y_3.pdf, ratio_pdf_MSTW2008_Y_4.pdf, ratio_pdf_MSTW2008_Y_5.pdf, ratio_pdf_MSTW2008_Y_6.pdf and the png files ratio_pdf_MSTW2008_Y_0.png, ratio_pdf_MSTW2008_Y_1.png, ratio_pdf_MSTW2008_Y_2.png, ratio_pdf_MSTW2008_Y_3.png, ratio_pdf_MSTW2008_Y_4.png, ratio_pdf_MSTW2008_Y_5.png, ratio_pdf_MSTW2008_Y_6.png
 

Figure 1 a Figure 1 b Figure 1 c Figure 1 d
Figure 1 e | Figure 1 f | Figure 1 g |
Changed:
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Figure 11. Ratio of inclusive jet cross sections to the theoretical prediction using the central value of the NNPDF2.1 PDF set for all bins. The dashed lines show the ratio of the cross sections calculated with the other PDF sets to that calculated with NNPDF2.1. The experimental uncertainty is represented by the continuous line. The pdf file ratio_pdf_NNPDF21_Y_0.pdf, ratio_pdf_NNPDF21_Y_1.pdf, ratio_pdf_NNPDF21_Y_2.pdf, ratio_pdf_NNPDF21_Y_3.pdf, ratio_pdf_NNPDF21_Y_4.pdf, ratio_pdf_NNPDF21_Y_5.pdf, ratio_pdf_NNPDF21_Y_6.pdf and the png file ratio_pdf_NNPDF21_Y_0.png, ratio_pdf_NNPDF21_Y_1.png, ratio_pdf_NNPDF21_Y_2.png, ratio_pdf_NNPDF21_Y_3.png, ratio_pdf_NNPDF21_Y_4.png, ratio_pdf_NNPDF21_Y_5.png, ratio_pdf_NNPDF21_Y_6.png
>
>
Figure 11. Ratio of inclusive jet cross sections to the theoretical prediction using the central value of the NNPDF2.1 PDF set for all bins. The dashed lines show the ratio of the cross sections calculated with the other PDF sets to that calculated with NNPDF2.1. The experimental uncertainty is represented by the continuous line. The pdf files ratio_pdf_NNPDF21_Y_0.pdf, ratio_pdf_NNPDF21_Y_1.pdf, ratio_pdf_NNPDF21_Y_2.pdf, ratio_pdf_NNPDF21_Y_3.pdf, ratio_pdf_NNPDF21_Y_4.pdf, ratio_pdf_NNPDF21_Y_5.pdf, ratio_pdf_NNPDF21_Y_6.pdf and the png files ratio_pdf_NNPDF21_Y_0.png, ratio_pdf_NNPDF21_Y_1.png, ratio_pdf_NNPDF21_Y_2.png, ratio_pdf_NNPDF21_Y_3.png, ratio_pdf_NNPDF21_Y_4.png, ratio_pdf_NNPDF21_Y_5.png, ratio_pdf_NNPDF21_Y_6.png
 
Figure 1 a Figure 1 b Figure 1 c Figure 1 d
Figure 1 e |
Line: 312 to 312
 
META FILEATTACHMENT attachment="ratio_pdf_MSTW2008_Y_4.png" attr="" comment="Ratio to MSTW2008" date="1374505019" name="ratio_pdf_MSTW2008_Y_4.png" path="ratio_pdf_MSTW2008_Y_4.png" size="25720" user="salim" version="1"
META FILEATTACHMENT attachment="ratio_pdf_MSTW2008_Y_5.png" attr="" comment="Ratio to MSTW2008" date="1374505019" name="ratio_pdf_MSTW2008_Y_5.png" path="ratio_pdf_MSTW2008_Y_5.png" size="25706" user="salim" version="1"
META FILEATTACHMENT attachment="ratio_pdf_MSTW2008_Y_6.png" attr="" comment="Ratio to MSTW2008" date="1374505019" name="ratio_pdf_MSTW2008_Y_6.png" path="ratio_pdf_MSTW2008_Y_6.png" size="25845" user="salim" version="1"
Added:
>
>
META FILEATTACHMENT attachment="ratio_NNPDF21_Y_0.png" attr="" comment="" date="1374568104" name="ratio_NNPDF21_Y_0.png" path="ratio_NNPDF21_Y_0.png" size="84184" user="ilknur" version="1"
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META FILEATTACHMENT attachment="ratio_pdf_NNPDF21_Y_0.png" attr="" comment="" date="1374568387" name="ratio_pdf_NNPDF21_Y_0.png" path="ratio_pdf_NNPDF21_Y_0.png" size="98902" user="ilknur" version="1"
META FILEATTACHMENT attachment="ratio_pdf_NNPDF21_Y_1.png" attr="" comment="" date="1374568387" name="ratio_pdf_NNPDF21_Y_1.png" path="ratio_pdf_NNPDF21_Y_1.png" size="99388" user="ilknur" version="1"
META FILEATTACHMENT attachment="ratio_pdf_NNPDF21_Y_2.png" attr="" comment="" date="1374568387" name="ratio_pdf_NNPDF21_Y_2.png" path="ratio_pdf_NNPDF21_Y_2.png" size="98769" user="ilknur" version="1"
META FILEATTACHMENT attachment="ratio_pdf_NNPDF21_Y_3.png" attr="" comment="" date="1374568387" name="ratio_pdf_NNPDF21_Y_3.png" path="ratio_pdf_NNPDF21_Y_3.png" size="99195" user="ilknur" version="1"
META FILEATTACHMENT attachment="ratio_pdf_NNPDF21_Y_4.png" attr="" comment="" date="1374568387" name="ratio_pdf_NNPDF21_Y_4.png" path="ratio_pdf_NNPDF21_Y_4.png" size="99025" user="ilknur" version="1"
META FILEATTACHMENT attachment="ratio_pdf_NNPDF21_Y_5.png" attr="" comment="" date="1374568387" name="ratio_pdf_NNPDF21_Y_5.png" path="ratio_pdf_NNPDF21_Y_5.png" size="99299" user="ilknur" version="1"
META FILEATTACHMENT attachment="ratio_pdf_NNPDF21_Y_6.png" attr="" comment="" date="1374568386" name="ratio_pdf_NNPDF21_Y_6.png" path="ratio_pdf_NNPDF21_Y_6.png" size="100246" user="ilknur" version="1"

Revision 142013-07-22 - IlknurHos

Line: 1 to 1
 
META TOPICPARENT name="PhysicsResultsFSQ12031"

Measurement of Low pT Jet Cross Sections in proton-proton Collisions at √s = 8 TeV

Line: 14 to 14
 Figure 1 e| Figure 1 f| Figure 1 g|
Changed:
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Figure 1. Inclusive jet cross section (anti-kT) measured at rapidities ( ) as a function of transverse momentum, fully corrected and unfolded, compared to various hadron-level theoretical predictions: NLO calculations for various PDFs. The yellow band on the data points refers to the total experimental uncertainty.
>
>
Figure 1. Inclusive jet cross section (anti-kT) measured at rapidities ( ) as a function of transverse momentum, fully corrected and unfolded, compared to various hadron-level theoretical predictions: NLO calculations for various PDFs. The yellow band on the data points refers to the total experimental uncertainty. The pdf files cxsection_Y_0.pdf,cxsection_Y_1.pdf, cxsection_Y_2.pdf, cxsection_Y_3.pdf, cxsection_Y_4.pdf, cxsection_Y_5.pdf, cxsection_Y_6.pdf, and the png files cxsection_Y_0.png, cxsection_Y_1.png, cxsection_Y_2.png, cxsection_Y_3.png, cxsection_Y_4.png, cxsection_Y_5.png, cxsection_Y_6.png
 
Line: 23 to 23
 Figure 1 e | Figure 1 f | Figure 1 g |
Changed:
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Figure 2. Inclusive jet cross sections for data over the theoretical prediction of the ABM11 PDF set for all . The experimental and theoretical systematic uncertainties are represented by the continuous and dashed lines, respectively.
>
>
Figure 2. Inclusive jet cross sections for data over the theoretical prediction of the ABM11 PDF set for all . The experimental and theoretical systematic uncertainties are represented by the continuous and dashed lines, respectively. The pdf files ratio_ABM11_Y_0.pdf, ratio_ABM11_Y_1.pdf, ratio_ABM11_Y_2.pdf, ratio_ABM11_Y_3.pdf, ratio_ABM11_Y_4.pdf, ratio_ABM11_Y_5.pdf, ratio_ABM11_Y_6.pdf and the png files ratio_ABM11_Y_0.png, ratio_ABM11_Y_1.png, ratio_ABM11_Y_2.png, ratio_ABM11_Y_3.png, ratio_ABM11_Y_4.png, ratio_ABM11_Y_5.png, ratio_ABM11_Y_6.png
 

Figure 1 a Figure 1 b Figure 1 c Figure 1 d
Figure 1 e | Figure 1 f | Figure 1 g |
Changed:
<
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Figure 3. Inclusive jet cross sections for data over the theoretical prediction of the CT10 PDF set for all . The experimental and theoretical systematic uncertainties are represented by the continuous and dashed lines, respectively.
>
>
Figure 3. Inclusive jet cross sections for data over the theoretical prediction of the CT10 PDF set for all . The experimental and theoretical systematic uncertainties are represented by the continuous and dashed lines, respectively. The pdf file ratio_CT10_Y_0.pdf, ratio_CT10_Y_1.pdf, ratio_CT10_Y_2.pdf, ratio_CT10_Y_3.pdf, ratio_CT10_Y_4.pdf, ratio_CT10_Y_5.pdf, ratio_CT10_Y_6.pdf and the png file ratio_CT10_Y_0.png, ratio_CT10_Y_1.png, ratio_CT10_Y_2.png, ratio_CT10_Y_3.png, ratio_CT10_Y_4.png, ratio_CT10_Y_5.png, ratio_CT10_Y_6.png
 

Figure 1 a Figure 1 b Figure 1 c Figure 1 d
Figure 1 e | Figure 1 f | Figure 1 g |
Changed:
<
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Figure 4. Inclusive jet cross sections for data over the theoretical prediction of the HERAPDF1.5 PDF set for all . The experimental and theoretical systematic uncertainties are represented by the continuous and dashed lines, respectively.
>
>
Figure 4. Inclusive jet cross sections for data over the theoretical prediction of the HERAPDF1.5 PDF set for all . The experimental and theoretical systematic uncertainties are represented by the continuous and dashed lines, respectively. The pdf file ratio_HERAPDF15_Y_0.pdf, ratio_HERAPDF15_Y_1.pdf, ratio_HERAPDF15_Y_2.pdf, ratio_HERAPDF15_Y_3.pdf, ratio_HERAPDF15_Y_4.pdf, ratio_HERAPDF15_Y_5.pdf, ratio_HERAPDF15_Y_6.pdf and the png file ratio_HERAPDF15_Y_0.png, ratio_HERAPDF15_Y_1.png, ratio_HERAPDF15_Y_2.png, ratio_HERAPDF15_Y_3.png, ratio_HERAPDF15_Y_4.png, ratio_HERAPDF15_Y_5.png, ratio_HERAPDF15_Y_6.png
 

Figure 1 a Figure 1 b Figure 1 c Figure 1 d
Figure 1 e | Figure 1 f | Figure 1 g |
Changed:
<
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Figure 5. Inclusive jet cross sections for data over the theoretical prediction of the MSTW2008 PDF set for all . The experimental and theoretical systematic uncertainties are represented by the continuous and dashed lines, respectively.
>
>
Figure 5. Inclusive jet cross sections for data over the theoretical prediction of the MSTW2008 PDF set for all . The experimental and theoretical systematic uncertainties are represented by the continuous and dashed lines, respectively. The pdf file ratio_MSTW2008_Y_0.pdf, ratio_MSTW2008_Y_1.pdf, ratio_MSTW2008_Y_2.pdf, ratio_MSTW2008_Y_3.pdf, ratio_MSTW2008_Y_4.pdf, ratio_MSTW2008_Y_5.pdf, ratio_MSTW2008_Y_6.pdf and the png file ratio_MSTW2008_Y_0.png
 

Figure 1 a Figure 1 b Figure 1 c Figure 1 d
Figure 1 e | Figure 1 f | Figure 1 g |
Changed:
<
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Figure 6. Inclusive jet cross sections for data over the theoretical prediction of the NNPDF2.1 PDF set for all . The experimental and theoretical systematic uncertainties are represented by the continuous and dashed lines, respectively.
>
>
Figure 6. Inclusive jet cross sections for data over the theoretical prediction of the NNPDF2.1 PDF set for all . The experimental and theoretical systematic uncertainties are represented by the continuous and dashed lines, respectively. The pdf file ratio_NNPDF21_Y_0.pdf, ratio_NNPDF21_Y_1.pdf, ratio_NNPDF21_Y_2.pdf, ratio_NNPDF21_Y_3.pdf, ratio_NNPDF21_Y_4.pdf, ratio_NNPDF21_Y_5.pdf, ratio_NNPDF21_Y_6.pdf and the png file ratio_NNPDF21_Y_0.png, ratio_NNPDF21_Y_1.png, ratio_NNPDF21_Y_2.png, ratio_NNPDF21_Y_3.png, ratio_NNPDF21_Y_4.png, ratio_NNPDF21_Y_5.png, ratio_NNPDF21_Y_6.png
 

Figure 1 a Figure 1 b Figure 1 c Figure 1 d
Figure 1 e | Figure 1 f | Figure 1 g |
Changed:
<
<
Figure 7. Ratio of inclusive jet cross sections to the theoretical prediction using the central value of the ABM11 PDF set for all bins. The dashed lines show the ratio of the cross sections calculated with the other PDF sets to that calculated with ABM11. The experimental uncertainty is represented by the continuous line.
>
>
Figure 7. Ratio of inclusive jet cross sections to the theoretical prediction using the central value of the ABM11 PDF set for all bins. The dashed lines show the ratio of the cross sections calculated with the other PDF sets to that calculated with ABM11. The experimental uncertainty is represented by the continuous line. The pdf file ratio_pdf_ABM11_Y_0.pdf, ratio_pdf_ABM11_Y_1.pdf, ratio_pdf_ABM11_Y_2.pdf, ratio_pdf_ABM11_Y_3.pdf, ratio_pdf_ABM11_Y_4.pdf, ratio_pdf_ABM11_Y_5.pdf, ratio_pdf_ABM11_Y_6.pdf and the png file ratio_pdf_ABM11_Y_0.png, ratio_pdf_ABM11_Y_1.png, ratio_pdf_ABM11_Y_2.png, ratio_pdf_ABM11_Y_3.png, ratio_pdf_ABM11_Y_4.png, ratio_pdf_ABM11_Y_5.png, ratio_pdf_ABM11_Y_6.png
 

Figure 1 a Figure 1 b Figure 1 c Figure 1 d
Figure 1 e | Figure 1 f | Figure 1 g |
Changed:
<
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Figure 8. Ratio of inclusive jet cross sections to the theoretical prediction using the central value of the CT10 PDF set for all bins. The dashed lines show the ratio of the cross sections calculated with the other PDF sets to that calculated with CT10. The experimental uncertainty is represented by the continuous line.
>
>
Figure 8. Ratio of inclusive jet cross sections to the theoretical prediction using the central value of the CT10 PDF set for all bins. The dashed lines show the ratio of the cross sections calculated with the other PDF sets to that calculated with CT10. The experimental uncertainty is represented by the continuous line. The pdf file ratio_pdf_CT10_Y_0.pdf, ratio_pdf_CT10_Y_1.pdf, ratio_pdf_CT10_Y_2.pdf, ratio_pdf_CT10_Y_3.pdf, ratio_pdf_CT10_Y_4.pdf, ratio_pdf_CT10_Y_5.pdf, ratio_pdf_CT10_Y_6.pdf and the png file ratio_pdf_CT10_Y_0.png, ratio_pdf_CT10_Y_1.png, ratio_pdf_CT10_Y_2.png, ratio_pdf_CT10_Y_3.png, ratio_pdf_CT10_Y_4.png, ratio_pdf_CT10_Y_5.png, ratio_pdf_CT10_Y_6.png
 
Figure 1 a Figure 1 b Figure 1 c Figure 1 d
Figure 1 e | Figure 1 f | Figure 1 g |
Changed:
<
<
Figure 9. Ratio of inclusive jet cross sections to the theoretical prediction using the central value of the HERAPDF1.5 PDF set for all bins. The dashed lines show the ratio of the cross sections calculated with the other PDF sets to that calculated with HERAPDF1.5. The experimental uncertainty is represented by the continuous line.
>
>
Figure 9. Ratio of inclusive jet cross sections to the theoretical prediction using the central value of the HERAPDF1.5 PDF set for all bins. The dashed lines show the ratio of the cross sections calculated with the other PDF sets to that calculated with HERAPDF1.5. The experimental uncertainty is represented by the continuous line. The pdf file ratio_pdf_HERAPDF15_Y_0.pdf, ratio_pdf_HERAPDF15_Y_1.pdf, ratio_pdf_HERAPDF15_Y_2.pdf, ratio_pdf_HERAPDF15_Y_3.pdf, ratio_pdf_HERAPDF15_Y_4.pdf, ratio_pdf_HERAPDF15_Y_5.pdf, ratio_pdf_HERAPDF15_Y_6.pdf and the png file ratio_pdf_HERAPDF15_Y_0.png, ratio_pdf_HERAPDF15_Y_1.png, ratio_pdf_HERAPDF15_Y_2.png, ratio_pdf_HERAPDF15_Y_3.png, ratio_pdf_HERAPDF15_Y_4.png, ratio_pdf_HERAPDF15_Y_5.png, ratio_pdf_HERAPDF15_Y_6.png
 
Figure 1 a Figure 1 b Figure 1 c Figure 1 d
Figure 1 e | Figure 1 f | Figure 1 g |
Changed:
<
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Figure 10. Ratio of inclusive jet cross sections to the theoretical prediction using the central value of the MSTW2008 PDF set for all bins. The dashed lines show the ratio of the cross sections calculated with the other PDF sets to that calculated with MSTW2008. The experimental uncertainty is represented by the continuous line.
>
>
Figure 10. Ratio of inclusive jet cross sections to the theoretical prediction using the central value of the MSTW2008 PDF set for all bins. The dashed lines show the ratio of the cross sections calculated with the other PDF sets to that calculated with MSTW2008. The experimental uncertainty is represented by the continuous line. The pdf file ratio_pdf_MSTW2008_Y_0.pdf, ratio_pdf_MSTW2008_Y_1.pdf, ratio_pdf_MSTW2008_Y_2.pdf, ratio_pdf_MSTW2008_Y_3.pdf, ratio_pdf_MSTW2008_Y_4.pdf, ratio_pdf_MSTW2008_Y_5.pdf, ratio_pdf_MSTW2008_Y_6.pdf and the png file ratio_pdf_MSTW2008_Y_0.png, ratio_pdf_MSTW2008_Y_1.png, ratio_pdf_MSTW2008_Y_2.png, ratio_pdf_MSTW2008_Y_3.png, ratio_pdf_MSTW2008_Y_4.png, ratio_pdf_MSTW2008_Y_5.png, ratio_pdf_MSTW2008_Y_6.png
 

Figure 1 a Figure 1 b Figure 1 c Figure 1 d
Figure 1 e | Figure 1 f | Figure 1 g |
Changed:
<
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Figure 11. Ratio of inclusive jet cross sections to the theoretical prediction using the central value of the NNPDF2.1 PDF set for all bins. The dashed lines show the ratio of the cross sections calculated with the other PDF sets to that calculated with NNPDF2.1. The experimental uncertainty is represented by the continuous line.
>
>
Figure 11. Ratio of inclusive jet cross sections to the theoretical prediction using the central value of the NNPDF2.1 PDF set for all bins. The dashed lines show the ratio of the cross sections calculated with the other PDF sets to that calculated with NNPDF2.1. The experimental uncertainty is represented by the continuous line. The pdf file ratio_pdf_NNPDF21_Y_0.pdf, ratio_pdf_NNPDF21_Y_1.pdf, ratio_pdf_NNPDF21_Y_2.pdf, ratio_pdf_NNPDF21_Y_3.pdf, ratio_pdf_NNPDF21_Y_4.pdf, ratio_pdf_NNPDF21_Y_5.pdf, ratio_pdf_NNPDF21_Y_6.pdf and the png file ratio_pdf_NNPDF21_Y_0.png, ratio_pdf_NNPDF21_Y_1.png, ratio_pdf_NNPDF21_Y_2.png, ratio_pdf_NNPDF21_Y_3.png, ratio_pdf_NNPDF21_Y_4.png, ratio_pdf_NNPDF21_Y_5.png, ratio_pdf_NNPDF21_Y_6.png
 
Figure 1 a Figure 1 b Figure 1 c Figure 1 d
Figure 1 e |
Line: 138 to 138
 
Deleted:
<
<
  • Ratio plot for ABM11:
    ratio_ABM11_Y_0.png

  • Ratio plot for ABM11:
    ratio_ABM11_Y_1.png

  • Ratio plot for ABM11:
    ratio_ABM11_Y_2.png

  • Ratio plot for ABM11:
    ratio_ABM11_Y_3.png

  • Ratio plot for ABM11:
    ratio_ABM11_Y_5.png

  • Ratio plot for HERAPDF15:
    ratio_HERAPDF15_Y_0.png

  • Ratio plot for HERAPDF15:
    ratio_HERAPDF15_Y_1.png

  • Ratio plot for HERAPDF15:
    ratio_HERAPDF15_Y_2.png

  • Ratio plot for HERAPDF15:
    ratio_HERAPDF15_Y_4.png

  • Ratio plot for HERAPDF15:
    ratio_HERAPDF15_Y_5.png

  • Ratio plot for HERAPDF15:
    ratio_HERAPDF15_Y_6.png

  • Ratio plot for MSTW2008:
    ratio_MSTW2008_Y_0.png

  • Ratio plot for MSTW2008:
    ratio_MSTW2008_Y_1.png

  • Ratio plot for MSTW2008:
    ratio_MSTW2008_Y_2.png

  • Ratio plot for MSTW2008:
    ratio_MSTW2008_Y_3.png

  • Ratio plot for MSTW2008:
    ratio_MSTW2008_Y_4.png

  • Ratio plot for MSTW2008:
    ratio_MSTW2008_Y_5.png

  • Ratio plot for MSTW2008:
    ratio_MSTW2008_Y_6.png

  • Ratio plot for NNPDF21:
    ratio_NNPDF21_Y_2.png

  • Ratio plot for NNPDF21:
    ratio_NNPDF21_Y_3.png

  • Ratio plot for NNPDF21:
    ratio_NNPDF21_Y_4.png

  • Ratio plot for NNPDF21:
    ratio_NNPDF21_Y_5.png

  • Ratio plot for NNPDF21:
    ratio_NNPDF21_Y_6.png

  • Ratio to ABM11:
    ratio_pdf_ABM11_Y_0.png

  • Ratio to ABM11:
    ratio_pdf_ABM11_Y_1.png

  • Ratio to ABM11:
    ratio_pdf_ABM11_Y_2.png

  • Ratio to ABM11:
    ratio_pdf_ABM11_Y_3.png

  • Ratio to ABM11:
    ratio_pdf_ABM11_Y_4.png

  • Ratio to ABM11:
    ratio_pdf_ABM11_Y_5.png

  • Ratio to ABM11:
    ratio_pdf_ABM11_Y_6.png

  • Ratio to CT10:
    ratio_pdf_CT10_Y_0.png

  • Ratio to CT10:
    ratio_pdf_CT10_Y_1.png

  • Ratio to CT10:
    ratio_pdf_CT10_Y_2.png

  • Ratio to CT10:
    ratio_pdf_CT10_Y_3.png

  • Ratio to CT10:
    ratio_pdf_CT10_Y_4.png

  • Ratio to CT10:
    ratio_pdf_CT10_Y_5.png

  • Ratio to CT10:
    ratio_pdf_CT10_Y_6.png

  • Ratio to HERAPDF15:
    ratio_pdf_HERAPDF15_Y_0.png

  • Ratio to HERAPDF15:
    ratio_pdf_HERAPDF15_Y_1.png

  • Ratio to HERAPDF15:
    ratio_pdf_HERAPDF15_Y_2.png

  • Ratio to HERAPDF15:
    ratio_pdf_HERAPDF15_Y_3.png

  • Ratio to HERAPDF15:
    ratio_pdf_HERAPDF15_Y_4.png

  • Ratio to HERAPDF15:
    ratio_pdf_HERAPDF15_Y_5.png

  • Ratio to HERAPDF15:
    ratio_pdf_HERAPDF15_Y_6.png

  • Ratio to MSTW2008:
    ratio_pdf_MSTW2008_Y_0.png

  • Ratio to MSTW2008:
    ratio_pdf_MSTW2008_Y_1.png

  • Ratio to MSTW2008:
    ratio_pdf_MSTW2008_Y_2.png

  • Ratio to MSTW2008:
    ratio_pdf_MSTW2008_Y_3.png

  • Ratio to MSTW2008:
    ratio_pdf_MSTW2008_Y_4.png

  • Ratio to MSTW2008:
    ratio_pdf_MSTW2008_Y_5.png

  • Ratio to MSTW2008:
    ratio_pdf_MSTW2008_Y_6.png
 
META FILEATTACHMENT attachment="cxsection_Y_0.png" attr="" comment="xsection" date="1374503991" name="cxsection_Y_0.png" path="cxsection_Y_0.png" size="28902" user="salim" version="1"
META FILEATTACHMENT attachment="cxsection_Y_1.png" attr="" comment="xsection" date="1374503991" name="cxsection_Y_1.png" path="cxsection_Y_1.png" size="28647" user="salim" version="1"
META FILEATTACHMENT attachment="cxsection_Y_2.png" attr="" comment="xsection" date="1374503991" name="cxsection_Y_2.png" path="cxsection_Y_2.png" size="29195" user="salim" version="1"

Revision 132013-07-22 - SalimCerci

Line: 1 to 1
 
META TOPICPARENT name="PhysicsResultsFSQ12031"

Measurement of Low pT Jet Cross Sections in proton-proton Collisions at √s = 8 TeV

Line: 138 to 138
 
Changed:
<
<
META FILEATTACHMENT attachment="cxsection_Y_0.png" attr="" comment="InclusiveJetCrossSection" date="1374175802" name="cxsection_Y_0.png" path="cxsection_Y_0.png" size="28902" user="salim" version="1"
META FILEATTACHMENT attachment="cxsection_Y_1.png" attr="" comment="InclusiveJetCrossSection" date="1374175802" name="cxsection_Y_1.png" path="cxsection_Y_1.png" size="28647" user="salim" version="1"
META FILEATTACHMENT attachment="cxsection_Y_2.png" attr="" comment="InclusiveJetCrossSection" date="1374175802" name="cxsection_Y_2.png" path="cxsection_Y_2.png" size="29195" user="salim" version="1"
META FILEATTACHMENT attachment="cxsection_Y_3.png" attr="" comment="InclusiveJetCrossSection" date="1374175802" name="cxsection_Y_3.png" path="cxsection_Y_3.png" size="29247" user="salim" version="1"
META FILEATTACHMENT attachment="cxsection_Y_4.png" attr="" comment="InclusiveJetCrossSection" date="1374175801" name="cxsection_Y_4.png" path="cxsection_Y_4.png" size="29337" user="salim" version="1"
META FILEATTACHMENT attachment="cxsection_Y_5.png" attr="" comment="InclusiveJetCrossSection" date="1374175801" name="cxsection_Y_5.png" path="cxsection_Y_5.png" size="29523" user="salim" version="1"
META FILEATTACHMENT attachment="cxsection_Y_6.png" attr="" comment="InclusiveJetCrossSection" date="1374175801" name="cxsection_Y_6.png" path="cxsection_Y_6.png" size="29869" user="salim" version="1"
>
>
  • Ratio plot for ABM11:
    ratio_ABM11_Y_0.png

  • Ratio plot for ABM11:
    ratio_ABM11_Y_1.png

  • Ratio plot for ABM11:
    ratio_ABM11_Y_2.png

  • Ratio plot for ABM11:
    ratio_ABM11_Y_3.png

  • Ratio plot for ABM11:
    ratio_ABM11_Y_5.png

  • Ratio plot for HERAPDF15:
    ratio_HERAPDF15_Y_0.png

  • Ratio plot for HERAPDF15:
    ratio_HERAPDF15_Y_1.png

  • Ratio plot for HERAPDF15:
    ratio_HERAPDF15_Y_2.png

  • Ratio plot for HERAPDF15:
    ratio_HERAPDF15_Y_4.png

  • Ratio plot for HERAPDF15:
    ratio_HERAPDF15_Y_5.png

  • Ratio plot for HERAPDF15:
    ratio_HERAPDF15_Y_6.png

  • Ratio plot for MSTW2008:
    ratio_MSTW2008_Y_0.png

  • Ratio plot for MSTW2008:
    ratio_MSTW2008_Y_1.png

  • Ratio plot for MSTW2008:
    ratio_MSTW2008_Y_2.png

  • Ratio plot for MSTW2008:
    ratio_MSTW2008_Y_3.png

  • Ratio plot for MSTW2008:
    ratio_MSTW2008_Y_4.png

  • Ratio plot for MSTW2008:
    ratio_MSTW2008_Y_5.png

  • Ratio plot for MSTW2008:
    ratio_MSTW2008_Y_6.png

  • Ratio plot for NNPDF21:
    ratio_NNPDF21_Y_2.png

  • Ratio plot for NNPDF21:
    ratio_NNPDF21_Y_3.png

  • Ratio plot for NNPDF21:
    ratio_NNPDF21_Y_4.png

  • Ratio plot for NNPDF21:
    ratio_NNPDF21_Y_5.png

  • Ratio plot for NNPDF21:
    ratio_NNPDF21_Y_6.png

  • Ratio to ABM11:
    ratio_pdf_ABM11_Y_0.png

  • Ratio to ABM11:
    ratio_pdf_ABM11_Y_1.png

  • Ratio to ABM11:
    ratio_pdf_ABM11_Y_2.png

  • Ratio to ABM11:
    ratio_pdf_ABM11_Y_3.png

  • Ratio to ABM11:
    ratio_pdf_ABM11_Y_4.png

  • Ratio to ABM11:
    ratio_pdf_ABM11_Y_5.png

  • Ratio to ABM11:
    ratio_pdf_ABM11_Y_6.png

  • Ratio to CT10:
    ratio_pdf_CT10_Y_0.png

  • Ratio to CT10:
    ratio_pdf_CT10_Y_1.png

  • Ratio to CT10:
    ratio_pdf_CT10_Y_2.png

  • Ratio to CT10:
    ratio_pdf_CT10_Y_3.png

  • Ratio to CT10:
    ratio_pdf_CT10_Y_4.png

  • Ratio to CT10:
    ratio_pdf_CT10_Y_5.png

  • Ratio to CT10:
    ratio_pdf_CT10_Y_6.png

  • Ratio to HERAPDF15:
    ratio_pdf_HERAPDF15_Y_0.png

  • Ratio to HERAPDF15:
    ratio_pdf_HERAPDF15_Y_1.png

  • Ratio to HERAPDF15:
    ratio_pdf_HERAPDF15_Y_2.png

  • Ratio to HERAPDF15:
    ratio_pdf_HERAPDF15_Y_3.png

  • Ratio to HERAPDF15:
    ratio_pdf_HERAPDF15_Y_4.png

  • Ratio to HERAPDF15:
    ratio_pdf_HERAPDF15_Y_5.png

  • Ratio to HERAPDF15:
    ratio_pdf_HERAPDF15_Y_6.png

  • Ratio to MSTW2008:
    ratio_pdf_MSTW2008_Y_0.png

  • Ratio to MSTW2008:
    ratio_pdf_MSTW2008_Y_1.png

  • Ratio to MSTW2008:
    ratio_pdf_MSTW2008_Y_2.png

  • Ratio to MSTW2008:
    ratio_pdf_MSTW2008_Y_3.png

  • Ratio to MSTW2008:
    ratio_pdf_MSTW2008_Y_4.png

  • Ratio to MSTW2008:
    ratio_pdf_MSTW2008_Y_5.png

  • Ratio to MSTW2008:
    ratio_pdf_MSTW2008_Y_6.png

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Line: 255 to 408
 
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Added:
>
>
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Revision 122013-07-19 - IlknurHos

Line: 1 to 1
 
META TOPICPARENT name="PhysicsResultsFSQ12031"

Measurement of Low pT Jet Cross Sections in proton-proton Collisions at √s = 8 TeV

Line: 10 to 10
 

Figures

Changed:
<
<
Figure 1 a Figure 1 b Figure 1 c Figure 1 d
Figure 1 e| Figure 1 f| Figure 1 g|
Figure 1. Inclusive jet cross section (anti-kT) measured at rapidities ( ) as a function of transverse momentum, fully corrected and unfolded, compared to various hadron-level theoretical predictions: NLO calculations for various PDFs. The yellow band on the data points refers to the total experimental uncertainty.
>
>
Figure 1 a Figure 1 b Figure 1 c Figure 1 d
Figure 1 e| Figure 1 f| Figure 1 g|
Figure 1. Inclusive jet cross section (anti-kT) measured at rapidities ( ) as a function of transverse momentum, fully corrected and unfolded, compared to various hadron-level theoretical predictions: NLO calculations for various PDFs. The yellow band on the data points refers to the total experimental uncertainty.
 

Changed:
<
<
Figure 1 a Figure 1 b Figure 1 c Figure 1 d
Figure 1 e | Figure 1 f | Figure 1 g |
>
>
Figure 1 a Figure 1 b Figure 1 c Figure 1 d
Figure 1 e | Figure 1 f | Figure 1 g |
 
Figure 2. Inclusive jet cross sections for data over the theoretical prediction of the ABM11 PDF set for all . The experimental and theoretical systematic uncertainties are represented by the continuous and dashed lines, respectively.
Changed:
<
<
Figure 1 a Figure 1 b Figure 1 c Figure 1 d
Figure 1 e | Figure 1 f | Figure 1 g |
>
>
Figure 1 a Figure 1 b Figure 1 c Figure 1 d
Figure 1 e | Figure 1 f | Figure 1 g |
 
Figure 3. Inclusive jet cross sections for data over the theoretical prediction of the CT10 PDF set for all . The experimental and theoretical systematic uncertainties are represented by the continuous and dashed lines, respectively.
Changed:
<
<
Figure 1 a Figure 1 b Figure 1 c Figure 1 d
Figure 1 e | Figure 1 f | Figure 1 g |
>
>
Figure 1 a Figure 1 b Figure 1 c Figure 1 d
Figure 1 e | Figure 1 f | Figure 1 g |
 
Figure 4. Inclusive jet cross sections for data over the theoretical prediction of the HERAPDF1.5 PDF set for all . The experimental and theoretical systematic uncertainties are represented by the continuous and dashed lines, respectively.
Changed:
<
<
Figure 1 a Figure 1 b Figure 1 c Figure 1 d
Figure 1 e | Figure 1 f | Figure 1 g |
>
>
Figure 1 a Figure 1 b Figure 1 c Figure 1 d
Figure 1 e | Figure 1 f | Figure 1 g |
 
Figure 5. Inclusive jet cross sections for data over the theoretical prediction of the MSTW2008 PDF set for all . The experimental and theoretical systematic uncertainties are represented by the continuous and dashed lines, respectively.
Changed:
<
<
Figure 1 a Figure 1 b Figure 1 c Figure 1 d
Figure 1 e | Figure 1 f | Figure 1 g |
>
>
Figure 1 a Figure 1 b Figure 1 c Figure 1 d
Figure 1 e | Figure 1 f | Figure 1 g |
 
Figure 6. Inclusive jet cross sections for data over the theoretical prediction of the NNPDF2.1 PDF set for all . The experimental and theoretical systematic uncertainties are represented by the continuous and dashed lines, respectively.
Changed:
<
<
Figure 1 a Figure 1 b Figure 1 c Figure 1 d
Figure 1 e | Figure 1 f | Figure 1 g |
>
>
Figure 1 a Figure 1 b Figure 1 c Figure 1 d
Figure 1 e | Figure 1 f | Figure 1 g |
 
Figure 7. Ratio of inclusive jet cross sections to the theoretical prediction using the central value of the ABM11 PDF set for all bins. The dashed lines show the ratio of the cross sections calculated with the other PDF sets to that calculated with ABM11. The experimental uncertainty is represented by the continuous line.
Changed:
<
<
Figure 1 a Figure 1 b Figure 1 c Figure 1 d
Figure 1 e | Figure 1 f | Figure 1 g |
>
>
Figure 1 a Figure 1 b Figure 1 c Figure 1 d
Figure 1 e | Figure 1 f | Figure 1 g |
 
Figure 8. Ratio of inclusive jet cross sections to the theoretical prediction using the central value of the CT10 PDF set for all bins. The dashed lines show the ratio of the cross sections calculated with the other PDF sets to that calculated with CT10. The experimental uncertainty is represented by the continuous line.
Changed:
<
<
Figure 1 a Figure 1 b Figure 1 c Figure 1 d
Figure 1 e | Figure 1 f | Figure 1 g |
>
>
Figure 1 a Figure 1 b Figure 1 c Figure 1 d
Figure 1 e | Figure 1 f | Figure 1 g |
 
Figure 9. Ratio of inclusive jet cross sections to the theoretical prediction using the central value of the HERAPDF1.5 PDF set for all bins. The dashed lines show the ratio of the cross sections calculated with the other PDF sets to that calculated with HERAPDF1.5. The experimental uncertainty is represented by the continuous line.
Changed:
<
<
Figure 1 a Figure 1 b Figure 1 c Figure 1 d
Figure 1 e | Figure 1 f | Figure 1 g |
>
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Figure 1 a Figure 1 b Figure 1 c Figure 1 d
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Figure 10. Ratio of inclusive jet cross sections to the theoretical prediction using the central value of the MSTW2008 PDF set for all bins. The dashed lines show the ratio of the cross sections calculated with the other PDF sets to that calculated with MSTW2008. The experimental uncertainty is represented by the continuous line.
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Figure 11. Ratio of inclusive jet cross sections to the theoretical prediction using the central value of the NNPDF2.1 PDF set for all bins. The dashed lines show the ratio of the cross sections calculated with the other PDF sets to that calculated with NNPDF2.1. The experimental uncertainty is represented by the continuous line.
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Figure 12. The combined results both for low and high pT jets. Ratio of data to the theoretical prediction of the ABM11 PDF set. The experimental uncertainty and the theoretical uncertainty are represented by the continuous and dashed line, respectively. The error bars correspond to the statistical uncertainty of the data.
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Figure 13. The combined results both for low and high pT jets. Ratio of data to the theoretical prediction of the CT10 PDF set. The experimental uncertainty and the theoretical uncertainty are represented by the continuous and dashed line, respectively. The error bars correspond to the statistical uncertainty of the data.

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Figure 13. The combined results both for low and high pT jets. Ratio of data to the theoretical prediction of the CT10 PDF set. The experimental uncertainty and the theoretical uncertainty are represented by the continuous and dashed line, respectively. The error bars correspond to the statistical uncertainty of the data.
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Figure 14. The combined results both for low and high pT jets. Ratio of data to the theoretical prediction of the HERAPDF1.5 PDF set. The experimental uncertainty and the theoretical uncertainty are represented by the continuous and dashed line, respectively. The error bars correspond to the statistical uncertainty of the data.
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Figure 15. The combined results both for low and high pT jets. Ratio of data to the theoretical prediction of the MSTW2008 PDF set. The experimental uncertainty and the theoretical uncertainty are represented by the continuous and dashed line, respectively. The error bars correspond to the statistical uncertainty of the data.
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Figure 16. The combined results both for low and high pT jets. Ratio of data to the theoretical prediction of the NNPDF PDF set. The experimental uncertainty and the theoretical uncertainty are represented by the continuous and dashed line, respectively. The error bars correspond to the statistical uncertainty of the data.

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META TOPICPARENT name="PhysicsResultsFSQ12031"

Measurement of Low pT Jet Cross Sections in proton-proton Collisions at √s = 8 TeV

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Abstract

  We present a measurement of the inclusive jet cross section in proton-proton (pp) collisions at √s = 8 TeV based on data collected by the CMS detector with an integrated luminosity of 5.8 pb-1. The measurement was performed using the anti-kT clustering algorithm with a distance parameter R = 0.7 in the rapidity region of |y| < 4.7 for jet transverse momenta 21 < pT < 74 GeV/c. The measured jet cross-section is compared to predictions of next-to-leading order (NLO) QCD calculations.

Revision 102013-07-19 - IlknurHos

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Measurement of Low pT Jet Cross Sections in proton-proton Collisions at √s = 8 TeV

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Figure 1. Inclusive jet cross section (anti-kT) measured at rapidities ( ) as a function of transverse momentum, fully corrected and unfolded, compared to various hadron-level theoretical predictions: NLO calculations for various PDFs. The yellow band on the data points refers to the total experimental uncertainty.

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META TOPICPARENT name="PhysicsResultsFSQ12031"

Measurement of Low pT Jet Cross Sections in proton-proton Collisions at √s = 8 TeV

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  We present a measurement of the inclusive jet cross section in proton-proton (pp) collisions at √s = 8 TeV based on data collected by the CMS detector with an integrated luminosity of 5.8 pb-1. The measurement was performed using the anti-kT clustering algorithm with a distance parameter R = 0.7 in the rapidity region of |y| < 4.7 for jet transverse momenta 21 < pT < 74 GeV/c. The measured jet cross-section is compared to predictions of next-to-leading order (NLO) QCD calculations.
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Measurement of Low pT Jet Cross Sections in proton-proton Collisions at √s = 8 TeV

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Figure 1. Inclusive jet cross section (anti-kT) measured at rapidities ( ) as a function of transverse momentum, fully corrected and unfolded, compared to various hadron-level theoretical predictions: NLO calculations for various PDFs. The yellow band on the data points refers to the total experimental uncertainty.
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Measurement of Low pT Jet Cross Sections in proton-proton Collisions at √s = 8 TeV

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We present a measurement of the inclusive jet cross section in proton-proton (pp) collisions at √ s = 8 TeV based on data collected by the CMS detector with an integrated luminosity of 5.8 pb%^{-1}%. The measurement was performed using the anti-kT clustering algorithm with a distance parameter R = 0.7 in the rapidity region of |y| < 4.7 for jet transverse momenta 21 < pT < 74 GeV/c. The measured jet cross-section is compared to predictions of next-to-leading order (NLO) QCD calculations.
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Abstract

We present a measurement of the inclusive jet cross section in proton-proton (pp) collisions at √s = 8 TeV based on data collected by the CMS detector with an integrated luminosity of 5.8 pb-1. The measurement was performed using the anti-kT clustering algorithm with a distance parameter R = 0.7 in the rapidity region of |y| < 4.7 for jet transverse momenta 21 < pT < 74 GeV/c. The measured jet cross-section is compared to predictions of next-to-leading order (NLO) QCD calculations.

 
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Figure 2. Inclusive jet cross sections for data over the theoretical prediction of the ABM11 PDF set for all . The experimental and theoretical systematic uncertainties are represented by the continuous and dashed lines, respectively.
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  Measured $p_T$-dependent differential cross sections for inclusive forward jets (second column), and for central (third column) and forward (last column) jets in dijet events. The first (second) uncertainty reflects the statistical (systematic) contribution.

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------+!! Measurement of Low pT Jet Cross Sections in proton-proton Collisions at $\sqrt s = 8$ TeV ------+!! Measurement of Low pT Jet Cross Sections in proton-proton Collisions at $\sqrt s = 8$ TeV ------+!! Measurement of Low pT Jet Cross Sections in proton-proton Collisions at $\sqrt s = 8$ TeV ------+!! Abstract

We present a measurement of the inclusive jet cross section in proton-proton (pp) collisions at $\sqrt{s}~=~8$~TeV based on data collected by the CMS detector with an integrated luminosity of $5.8$~pb$^{-1}$. The measurement was performed using the anti-k<sub>T clustering algorithm with a distance parameter~$R~=~0.7$~in the rapidity region of |&y;| < 4.7 for jet transverse momenta $21 < p<sub>T < 74$~GeV/c. The measured jet cross-section is compared to predictions of next-to-leading order (NLO) QCD calculations.

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Measurement of Low pT Jet Cross Sections in proton-proton Collisions at √s = 8 TeV

Abstract

We present a measurement of the inclusive jet cross section in proton-proton (pp) collisions at √ s = 8 TeV based on data collected by the CMS detector with an integrated luminosity of 5.8 pb%^{-1}%. The measurement was performed using the anti-kT clustering algorithm with a distance parameter R = 0.7 in the rapidity region of |y| < 4.7 for jet transverse momenta 21 < pT < 74 GeV/c. The measured jet cross-section is compared to predictions of next-to-leading order (NLO) QCD calculations.

 

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Figure 1. Inclusive jet cross section (anti-k_T, R = 0.7) measured at rapidities (abs y < 4.7 ) as a function of transverse momentum, fully corrected and unfolded, compared to various hadron-level theoretical predictions: NLO calculations for various PDFs. The yellow band on the data points refers to the total experimental uncertainty.
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Figure 1. Inclusive jet cross section (anti-kT) measured at rapidities ( ) as a function of transverse momentum, fully corrected and unfolded, compared to various hadron-level theoretical predictions: NLO calculations for various PDFs. The yellow band on the data points refers to the total experimental uncertainty.

Figure 1 a Figure 1 b Figure 1 c Figure 1 d
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Figure 2. Inclusive jet cross sections for data over the theoretical prediction of the ABM11 PDF set for all . The experimental and theoretical systematic uncertainties are represented by the continuous and dashed lines, respectively.

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Figure 3. Inclusive jet cross sections for data over the theoretical prediction of the CT10 PDF set for all . The experimental and theoretical systematic uncertainties are represented by the continuous and dashed lines, respectively.

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Figure 4. Inclusive jet cross sections for data over the theoretical prediction of the HERAPDF1.5 PDF set for all . The experimental and theoretical systematic uncertainties are represented by the continuous and dashed lines, respectively.

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Figure 5. Inclusive jet cross sections for data over the theoretical prediction of the MSTW2008 PDF set for all . The experimental and theoretical systematic uncertainties are represented by the continuous and dashed lines, respectively.

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Figure 6. Inclusive jet cross sections for data over the theoretical prediction of the NNPDF2.1 PDF set for all . The experimental and theoretical systematic uncertainties are represented by the continuous and dashed lines, respectively.

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Figure 7. Ratio of inclusive jet cross sections to the theoretical prediction using the central value of the ABM11 PDF set for all bins. The dashed lines show the ratio of the cross sections calculated with the other PDF sets to that calculated with ABM11. The experimental uncertainty is represented by the continuous line.

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Figure 8. Ratio of inclusive jet cross sections to the theoretical prediction using the central value of the CT10 PDF set for all bins. The dashed lines show the ratio of the cross sections calculated with the other PDF sets to that calculated with CT10. The experimental uncertainty is represented by the continuous line.

Figure 1 a Figure 1 b Figure 1 c Figure 1 d
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Figure 9. Ratio of inclusive jet cross sections to the theoretical prediction using the central value of the HERAPDF1.5 PDF set for all bins. The dashed lines show the ratio of the cross sections calculated with the other PDF sets to that calculated with HERAPDF1.5. The experimental uncertainty is represented by the continuous line.

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Figure 10. Ratio of inclusive jet cross sections to the theoretical prediction using the central value of the MSTW2008 PDF set for all bins. The dashed lines show the ratio of the cross sections calculated with the other PDF sets to that calculated with MSTW2008. The experimental uncertainty is represented by the continuous line.

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Figure 11. Ratio of inclusive jet cross sections to the theoretical prediction using the central value of the NNPDF2.1 PDF set for all bins. The dashed lines show the ratio of the cross sections calculated with the other PDF sets to that calculated with NNPDF2.1. The experimental uncertainty is represented by the continuous line.

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Figure 12. The combined results both for low and high pT jets. Ratio of data to the theoretical prediction of the ABM11 PDF set. The experimental uncertainty and the theoretical uncertainty are represented by the continuous and dashed line, respectively. The error bars correspond to the statistical uncertainty of the data.

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Figure 13. The combined results both for low and high pT jets. Ratio of data to the theoretical prediction of the CT10 PDF set. The experimental uncertainty and the theoretical uncertainty are represented by the continuous and dashed line, respectively. The error bars correspond to the statistical uncertainty of the data.

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Figure 13. The combined results both for low and high pT jets. Ratio of data to the theoretical prediction of the CT10 PDF set. The experimental uncertainty and the theoretical uncertainty are represented by the continuous and dashed line, respectively. The error bars correspond to the statistical uncertainty of the data.

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Figure 14. The combined results both for low and high pT jets. Ratio of data to the theoretical prediction of the HERAPDF1.5 PDF set. The experimental uncertainty and the theoretical uncertainty are represented by the continuous and dashed line, respectively. The error bars correspond to the statistical uncertainty of the data.
 
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Figure 15. The combined results both for low and high pT jets. Ratio of data to the theoretical prediction of the MSTW2008 PDF set. The experimental uncertainty and the theoretical uncertainty are represented by the continuous and dashed line, respectively. The error bars correspond to the statistical uncertainty of the data.
 
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Figure 1. Comparison of data with simulations from MC event generators (PYTHIA 6 and HERWIG ++) for the transverse momentum and pseudo-rapidity for the leading (far left, centre left) and subleading (centre right, far right) jets. Only statistical uncertainties are shown for the data.
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Figure 16. The combined results both for low and high pT jets. Ratio of data to the theoretical prediction of the NNPDF PDF set. The experimental uncertainty and the theoretical uncertainty are represented by the continuous and dashed line, respectively. The error bars correspond to the statistical uncertainty of the data.
 
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<img alt="Figure 1 a" src="https://twiki.cern.ch/twiki/pub/CMSPublic/PhysicsResultsFSQ12031/cxsection_Y_0.png" height="272" />
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<p> Figure 1. Comparison of data with simulations from MC event generators (PYTHIA 6 and HERWIG ++) for the transverse momentum and pseudo-rapidity for the leading (far left, centre left) and subleading (centre right, far right) jets. Only statistical uncertainties are shown for the data. </p>
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Revision 52013-07-18 - SalimCerci

Line: 1 to 1
 
META TOPICPARENT name="PhysicsResultsFSQ12031"
Changed:
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<
---+!! Measurement of Low pT Jet Cross Sections in proton-proton Collisions at $\sqrt s = 8$ TeV
>
>
------+!! Measurement of Low pT Jet Cross Sections in proton-proton Collisions at $\sqrt s = 8$ TeV ---+!! Measurement of Low pT Jet Cross Sections in proton-proton Collisions at $\sqrt s = 8$ TeV
 ---+!! Measurement of Low pT Jet Cross Sections in proton-proton Collisions at $\sqrt s = 8$ TeV
Changed:
<
<

Abstract

>
>
---+!! Abstract
  We present a measurement of the inclusive jet cross section in proton-proton (pp) collisions at $\sqrt{s}~=~8$~TeV based on data collected by the CMS detector

Revision 42013-07-18 - IlknurHos

Line: 1 to 1
 
META TOPICPARENT name="PhysicsResultsFSQ12031"
------+!! Measurement of Low pT Jet Cross Sections in proton-proton Collisions at $\sqrt s = 8$ TeV ---+!! Measurement of Low pT Jet Cross Sections in proton-proton Collisions at $\sqrt s = 8$ TeV
Line: 66 to 66
 
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Measurement of Low pT Jet Cross Sections in proton-proton Collisions at $\sqrt s = 8$ TeV

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------+!! Measurement of Low pT Jet Cross Sections in proton-proton Collisions at $\sqrt s = 8$ TeV ------+!! Measurement of Low pT Jet Cross Sections in proton-proton Collisions at $\sqrt s = 8$ TeV
 

Abstract

We present a measurement of the inclusive jet cross section in proton-proton (pp)

Revision 22013-07-18 - IlknurHos

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META TOPICPARENT name="PhysicsResultsFSQ12031"

Measurement of Low pT Jet Cross Sections in proton-proton Collisions at $\sqrt s = 8$ TeV

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Figures

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Figure 1 a Figure 1 b Figure 1 c Figure 1 d
Figure 1 e | Figure 1 f | Figure 1 g |
Figure 1. Inclusive jet cross section (anti-k_T, R = 0.7) measured at rapidities (abs y < 4.7 ) as a function of transverse momentum, fully corrected and unfolded, compared to various hadron-level theoretical predictions: NLO calculations for various PDFs. The yellow band on the data points refers to the total experimental uncertainty.

Figure 1 a Figure 1 b Figure 1 c Figure 1 d
Figure 1. Comparison of data with simulations from MC event generators (PYTHIA 6 and HERWIG ++) for the transverse momentum and pseudo-rapidity for the leading (far left, centre left) and subleading (centre right, far right) jets. Only statistical uncertainties are shown for the data.

 
<img alt="Figure 1 a" src="https://twiki.cern.ch/twiki/pub/CMSPublic/PhysicsResultsFSQ12031/cxsection_Y_0.png" height="272" />
<img alt="Figure 1 b" src="/twiki/pub/CMSPublic/PhysicsResultsFSQ12031/cxsection_Y_1.png" height="272" /> | <img alt="Figure 1 c" src="/twiki/pub/CMSPublic/PhysicsResultsFSQ12031/cxsection_Y_2.png" height="272" /> | <img alt="Figure 1 d" src="/twiki/pub/CMSPublic/PhysicsResultsFSQ12031/cxsection_Y_3.png" height="272" /> | <img alt="Figure 1 e" src="/twiki/pub/CMSPublic/PhysicsResultsFSQ12031/cxsection_Y_4.png" height="272" /> |
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Revision 12013-07-18 - SalimCerci

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META TOPICPARENT name="PhysicsResultsFSQ12031"

Measurement of Low pT Jet Cross Sections in proton-proton Collisions at $\sqrt s = 8$ TeV

Abstract

We present a measurement of the inclusive jet cross section in proton-proton (pp)

collisions at $\sqrt{s}~=~8$~TeV based on data collected by the CMS detector

with an integrated luminosity of $5.8$~pb$^{-1}$. The measurement was

performed using the anti-k<sub>T clustering algorithm with a distance

parameter~$R~=~0.7$~in the rapidity region of |&y;| < 4.7 for jet transverse

momenta $21 < p<sub>T < 74$~GeV/c. The measured jet cross-section is compared to

predictions of next-to-leading order (NLO) QCD calculations.

Figures

<img alt="Figure 1 a" src="https://twiki.cern.ch/twiki/pub/CMSPublic/PhysicsResultsFSQ12031/cxsection_Y_0.png" height="272" />
<img alt="Figure 1 b" src="/twiki/pub/CMSPublic/PhysicsResultsFSQ12031/cxsection_Y_1.png" height="272" /> | <img alt="Figure 1 c" src="/twiki/pub/CMSPublic/PhysicsResultsFSQ12031/cxsection_Y_2.png" height="272" /> | <img alt="Figure 1 d" src="/twiki/pub/CMSPublic/PhysicsResultsFSQ12031/cxsection_Y_3.png" height="272" /> | <img alt="Figure 1 e" src="/twiki/pub/CMSPublic/PhysicsResultsFSQ12031/cxsection_Y_4.png" height="272" /> | <img alt="Figure 1 f" src="/twiki/pub/CMSPublic/PhysicsResultsFSQ12031/cxsection_Y_5.png" height="272" /> | <img alt="Figure 1 g" src="/twiki/pub/CMSPublic/PhysicsResultsFSQ12031/cxsection_Y_6.png" height="272" /> | <img alt="Figure 1 h" src="/twiki/pub/CMSPublic/PhysicsResultsFSQ12031/cxsection_Y_7.png" height="272" /> |

<p> Figure 1. Comparison of data with simulations from MC event generators (PYTHIA 6 and HERWIG ++) for the transverse momentum and pseudo-rapidity for the leading (far left, centre left) and subleading (centre right, far right) jets. Only statistical uncertainties are shown for the data. </p>

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