Determination of the absolute jet energy scale in the DØ calorimeters

Abbott, B.; Abolins, M.; Acharya, B. S.; Адам, И.; Adams, T.; Adams, M. R.; Ahn, Shihyun; Aihara, H.; Alves, G. A.; Amos, N.; Anderson, E. W.; Astur, R.; Baarmand, M. M.; Babukhadia, L.; Baden, A.; Balamurali, V.; Balderston, J.; Baldin, B.; Banerjee, S.; Bantly, J.; Barberis, E.; Bartlett, J. F.; Belyaev, A.; Beri, S. B.; Bertram, I.; Bezzubov, V. A.; Bhat, P. C.; Bhatnagar, V.; Bhattacharjee, M.; Biswas, N. N.; Blazey, G.; Blessing, S.; Bloom, P. C.; Boehnlein, A.; Bojko, N. I.; Borcherding, F.; Boswell, C.; Brandt, A.; Brock, R.; Bross, A.; Buchholz, D.; Буртовой, В. С.; Butler, J. M.; Carvalho, W.; Casey, D.; Casilum, Z.; Castilla‐Valdez, H.; Chakraborty, D.; Chang, S. M.; Chekulaev, S. V.; Chen, L.-P; Chen, W; Choi, S.; Chopra, S.; Choudhary, B. C.; Christenson, J. H.; Chung, M.; Claes, D. R.; Clark, A. R.; Cobau, W. G.; Cochran, J.; Coney, L.; Cooper, W. E.; Cretsinger, C.; Cullen-Vidal, D.; Cummings, M. A.C.; Ćutts, D.; Dahl, O. I.; Davis, K.; De, K.; Signore, K. Del; Demarteau, M.; Denisov, D.; Denisov, S. P.; Diehl, H. T.; Diesburg, M.; Loreto, G. Di; Draper, P.; Ducros, Y.; Dudko, L.; Dugad, S.; Edmunds, D.; Ellison, J.; Elvira, V. D.; Engelmann, R.; Eno, S. C.; Eppley, G.; Ermolov, P.; Eroshin, O. V.; Евдокимов, В. Н.; Fahland, T.; Fatyga, M.; Fehér, S.; Fein, D.; Ferbel, T.; Finocchiaro, G.; Fisk, H. E.; Fisyak, Y.; Flattum, E.; Forden, G. E.; Fortner, M.; Frame, K. C.; Fuess, S.; Gallas, E. J.; Galyaev, A. N.; Gartung, P.; Gavrilov, V.; Geld, T. L.; Genik, R. J.; Genser, K.; Gerber, C. E.; Gershtein, Y.; Gibbard, B.; Glenn, S.; Gobbi, B.; Goldschmidt, A.; Gómez, B.; Gómez, G.; Goncharov, P. I.; González‐Solís, J. L.; Gordon, H. A.; Goss, L. T.; Gounder, K.; Goussiou, A. G.; Graf, N.; Grannis, P. D.; Green, D.R; Greenlee, H.; Grinstein, S.; Grudberg, P.; Grünendahl, S.; Guglielmo, G.; Guida, J. A.; Guida, J. M.; Gupta, A.; Gurzhiev, S. N.; Gutiérrez, G.; Gutiérrez, P.; Hadley, N. J.; Haggerty, H.; Hagopian, S.; Hagopian, V.; Hahn, K. S.; Hall, R. E.; Hanlet, P.; Hansen, S.; Hauptman, J. M.; Hedin, D.; Heinson, A. P.; Heintz, U.; Hernández-Montoya, R.; Heuring, T.; Hirosky, R.; Hobbs, J.; Hoeneisen, B.; Hoftun, J. S.; Hsieh, F.; Hu, Ting; Hu, Tong; Huehn, T.; Ito, A. S.; James, E.; Jaques, J.; Jerger, S. A.; Jesik, R.; Jiang, Jun; Joffe–Minor, T.; Johns, K. A.; Johnson, M.; Jonckheere, A.; Jones, M.; Jöstlein, H.; Jun, S. Y.; Jung, C. K.; Kahn, S.; Kalbfleisch, G.; Kang, J. S.; Karmanov, D.; Karmgard, Daniel John; Kehoe, R.; Kelly, M.; Kim, C.L; Kim, S.K; Klima, B.; Klopfenstein, C.; Kohli, J. M.; Koltick, D.; Kostritskiy, A. V.; Kotcher, J.; Kotwal, A.; Kourlas, J.; Kozelov, A. V.; Kozlovsky, E. A.; Krane, J.; Krishnaswamy, M. R.; Krzywdziński, S.; Kuleshov, S.; Kunori, S.; Landry, F.; Landsberg, G.; Lauer, B.; Leflat, A.; Li, H; Li, J; Li-Demarteau, Q. Z.; Lima, J. G.R.; Lincoln, D.; Linn, S.; Linnemann, J.; Lipton, R.; Liu, Y.C; Lobkowicz, F.; Loken, S.; Lökòs, S.; Lueking, L.; Lyon, A. L.; Maciel, A. K.A.; Madaras, R. J.; Madden, R.; Magaña-Mendoza, L.; Manankov, V.; Mani, S.; Mao, H. S.; Markeloff, R.; Marshall, T.; Martin, M.; Mauritz, K. M.; May, B.; Mayorov, A. A.; McCarthy, R. L.; McDonald, John; McKibben, T.; McKinley, J.; McMahon, T. J.; Melanson, H. L.; Merkin, M.; Merritt, K. W.; Miettinen, H.; Mincer, A. I.; Mishra, C. S.; Mokhov, N.; Mondal, N. K.; Montgomery, H. E.; Mooney, P.; Motta, H. da; Murphy, C.; Nang, F.; Narain, M.; Narasimham, V. S.; Narayanan, A.; Neal, H. A.; Negret, J. P.; Némethy, P.; Norman, D.; Oesch, L.; Oguri, V.; Oliveira, E. G. de; Oltman, E.; Oshima, N.; Owen, D.; Padley, P.; Para, A.; Park, Y.M; Partridge, R.; Parua, N.; Paterno, M.; Pawlik, B.; Perkins, J.; Peters, Michael; Piegaia, R.; Piekarz, H.; Pischalnikov, Y.; Pope, B. G.; Prosper, H.; Protopopescu, S.; Qian, J.; Quintas, P. Z.; Raja, R.; Rajagopalan, S.; Ramírez, O.; Rasmussen, L.; Reucroft, S.; Rijssenbeek, M.; Rockwell, T.; Roco, M.; Rubinov, P.; Ruchti, R.; Rutherfoord, J. P.; Sánchez-Hernández, A.; Santoro, A.; Sawyer, L.; Schamberger, R. D.; Schellman, H.; Sculli, J.; Shabalina, E.; Shaffer, C.; Shankar, H. C.; Shivpuri, R. K.; Shupe, M. A.; Singh, H.; Singh, J. B.; Sirotenko, V.; Smart, W.; Smith, E.; Smith, R. P.; Snihur, R.; Snow, G. R.; Snow, J.; Snyder, S.; Solomon, J.; Sosebee, M.; Sotnikova, N.; Souza, M.; Spadafora, A. L.; Steinbrück, G.; Stephens, R. W.; Stevenson, M. L.; Stewart, David J.; Stichelbaut, F.; Stoker, D. P.; Stolin, V.; Stoyanova, D. A.; Strauss, M.; Streets, K.; Strovink, M.; Sznajder, A.; Tamburello, P.; Tarazi, J.; Tartaglia, M.; Thomas, T. L.; Thompson, J.; Trippe, T. G.; Tuts, P. M.; Varelas, N.; Varnes, E. W.; Vititoe, D.; Volkov, A.; Vorobiev, A. P.; Wahl, H. D.; Wang, G; Warchol, J.; Watts, G.; Wayne, M.; Weerts, H.; White, A.; White, J. T.; Wightman, J. A.; Willis, S.; Wimpenny, S.; Wirjawan, J. V.D.; Womersley, J.; Won, E.; Wood, D.; Xu, H.; Yamada, R.; Yamin, P.; Yang, J.; Yasuda, T.; Yepes, P.; Yoshikawa, C.; Youssef, S.; Yu, J.; Yu, Y.; Zhou, Z.; Zhu, Z. H.; Ziemińska, D.; Ziemiński, A.; Zverev, E. G.; Zylberstejn, A.

doi:10.1016/s0168-9002(98)01368-0

Cited by 73 publications

(45 citation statements)

References 6 publications

Supporting

Mentioning

Contrasting

Unclassified

Order By: Relevance

“…D0's jet calibration [84] applies three scale factors and one offset to the jet energy to convert to the particle jet energy scale. The calibrations are expressed as follows:…”

Section: E Jet Propertiesmentioning

confidence: 99%

“…The absolute energy scale for jets in data is calibrated using γ+jet data with photon p T > 7 GeV and |η γ | < 1.0, and jet p T > 15 GeV and |η jet | < 0.4, using the " E T projection fraction" method [84]. Simulated samples of γ+jets and Z+jets events are compared to data and used to correct the energy scale for jets in MC events.…”

Section: Light-jet Response (2)mentioning

confidence: 99%

See 1 more Smart Citation

Combination of the top-quark mass measurements from the Tevatron collider

Aaltonen¹,

Abazov²,

Abbott³

et al. 2012

Phys. Rev. D

128

View full text Add to dashboard Cite

The top quark is the heaviest known elementary particle, with a mass about 40 times larger than the mass of its isospin partner, the bottom quark. It decays almost 100% of the time to a W boson and a bottom quark. Using top-antitop pairs at the Tevatron proton-antiproton collider, the CDF and D0 Collaborations have measured the top quark's mass in different final states for integrated luminosities of up to 5.8 fb −1 . This paper reports on a combination of these measurements that results in a more precise value of the mass than any individual decay channel can provide. It describes the treatment of the systematic uncertainties and their correlations. The mass value determined is 173.18 ± 0.56 (stat) ± 0.75 (syst) GeV or 173.18 ± 0.94 GeV, which has a precision of ±0.54%, making this the most precise determination of the top-quark mass.

show abstract

“…D0's jet calibration [84] applies three scale factors and one offset to the jet energy to convert to the particle jet energy scale. The calibrations are expressed as follows:…”

Section: E Jet Propertiesmentioning

confidence: 99%

Section: Light-jet Response (2)mentioning

confidence: 99%

Combination of the top-quark mass measurements from the Tevatron collider

Aaltonen¹,

Abazov²,

Abbott³

et al. 2012

Phys. Rev. D

128

View full text Add to dashboard Cite

show abstract

“…A complete discussion of the jet energy calibration can be found in Ref. [11]. An independent test of the jet energy scale, based on the balance in transverse energy in photon-jet and jet-jet data, confirms the validity of the D0 jet-calibration procedure up to jhj 3 [6].…”

mentioning

confidence: 89%

“…[11]. Uncertainties in the showering correction arise dominantly from the lack of full agreement of the lateral shower profiles observed in the data and in the Monte Carlo.…”

mentioning

confidence: 99%

Inclusive Jet Production inpp¯Collisions

Abbott¹,

Abdesselam²,

Abolins³

et al. 2001

Phys. Rev. Lett.

View full text Add to dashboard Cite

“…Jet energies determined from the initial cell energies do not correspond to the energies of final state particles striking the calorimeter. As a result, a detailed calibration is applied [19,20] in the data and Monte Carlo separately. In general, the energy of all final state particles inside the jet cone, E ptcl j , can be related to the energy measured inside the jet cone, E j , by E ptcl j ¼ ðE j À OÞ=ðRSÞ.…”

Section: Particle Identificationmentioning

confidence: 99%

Measurement of the top quark mass in final states with two leptons

Abazov¹,

Abbott²,

Abolins³

et al. 2009

Phys. Rev. D

View full text Add to dashboard Cite

Petersburg Nuclear Physics Institute, St. Petersburg, Russia V. M. ABAZOV et al.PHYSICAL REVIEW D 80, 092006 (2009) We present measurements of the top quark mass (m t ) in t " t candidate events with two final state leptons using 1 fb À1 of data collected by the D0 experiment. Our data sample is selected by requiring two fully identified leptons or by relaxing one lepton requirement to an isolated track if at least one jet is tagged as a b jet. The top quark mass is extracted after reconstructing the event kinematics under the t " t hypothesis using two methods. In the first method, we integrate over expected neutrino rapidity distributions, and in the second we calculate a weight for the possible top quark masses based on the observed particle momenta and the known parton distribution functions. We analyze 83 candidate events in the data and obtain m t ¼ 176:2 AE 4:8ðstatÞ AE 2:1ðsysÞ GeV and m t ¼ 173:2 AE 4:9ðstatÞ AE 2:0ðsysÞ GeV for the two methods, respectively. Accounting for correlations between the two methods, we combine the measurements to obtain m t ¼ 174:7 AE 4:4ðstatÞ AE 2:0ðsysÞ GeV.

show abstract

Determination of the absolute jet energy scale in the DØ calorimeters

Cited by 73 publications

References 6 publications

Combination of the top-quark mass measurements from the Tevatron collider

Combination of the top-quark mass measurements from the Tevatron collider

Inclusive Jet Production inpp¯Collisions

Measurement of the top quark mass in final states with two leptons

Contact Info

Product

Resources

About