skip to main content
OSTI.GOV title logo U.S. Department of Energy
Office of Scientific and Technical Information

Title: Study of the $$t\bar{t}$$ in the dilepton channel at $$\sqrt{s} = 1.96$$ TeV with the Collider Detector at Fermilab

Abstract

This study presents new measurement of the top quark mass in the t$$\bar{t}$$ to the dilepton decay channel. It is based on the observed linear dependence of the top mass to the transverse momentum PT of the leptons that are two of the fi products of the top-antitop pair decay. It uses data collected by the CDF detector from December 2004 to March 2007 that correspond to an integrated luminosity of 1.8 fb -1 .Two independent and mutually compatible methods have been implemented for this reason, both depending on the leptons’ PT. The final method, called the ”Straight Line”, exploits just the linear relation between the leptons’ PT and the top mass. With the second one, called the ”Likelihood”, the full PT spectrum is modeled by an analytical function and the top mass is estimated using the likelihood minimization procedure. A top quark mass of mtop=156±20(stat)±4.6(syst) GeV/c 2 is obtained with the Likelihood method and of 149±21(stat)±5.0(syst) GeV/c 2 is obtained with the Straight Line one.This study is complementary to other CDF mass studies in the dilepton channel. It differs by the fact that is not dependent on the jets and does not use the b quark secondary vertex b-tagging technique. It is therefore not dependent on the jet energy scale uncertainty that is at this moment the biggest systematic contribution to all other methods. This method is a simple and straightforward method that aims to a small systematic uncertainty. The statistical uncertainty is still not competitive with respect to the other methods, due to the relatively small sensitivity of the leptons' PT to the top mass. On the other hand, this study is a very good preview of the method with the upcoming LHC data, where the statistical error is expected to be greatly suppressed. The dominating error will then be the systematic one and this method promises to be competitive or even better, regarding this point, with respect to the other methods.

Authors:
 [1]
  1. Univ. of Athens (Greece)
Publication Date:
Research Org.:
Fermi National Accelerator Lab. (FNAL), Batavia, IL (United States)
Sponsoring Org.:
USDOE Office of Science (SC), High Energy Physics (HEP) (SC-25)
OSTI Identifier:
1345597
Report Number(s):
FERMILAB-THESIS-2007-100
1515145
DOE Contract Number:
AC02-07CH11359
Resource Type:
Thesis/Dissertation
Country of Publication:
United States
Language:
English
Subject:
72 PHYSICS OF ELEMENTARY PARTICLES AND FIELDS

Citation Formats

Giakoumopoulou, Victoria. Study of the $t\bar{t}$ in the dilepton channel at $\sqrt{s} = 1.96$ TeV with the Collider Detector at Fermilab. United States: N. p., 2007. Web. doi:10.2172/1345597.
Giakoumopoulou, Victoria. Study of the $t\bar{t}$ in the dilepton channel at $\sqrt{s} = 1.96$ TeV with the Collider Detector at Fermilab. United States. doi:10.2172/1345597.
Giakoumopoulou, Victoria. Mon . "Study of the $t\bar{t}$ in the dilepton channel at $\sqrt{s} = 1.96$ TeV with the Collider Detector at Fermilab". United States. doi:10.2172/1345597. https://www.osti.gov/servlets/purl/1345597.
@article{osti_1345597,
title = {Study of the $t\bar{t}$ in the dilepton channel at $\sqrt{s} = 1.96$ TeV with the Collider Detector at Fermilab},
author = {Giakoumopoulou, Victoria},
abstractNote = {This study presents new measurement of the top quark mass in the t$\bar{t}$ to the dilepton decay channel. It is based on the observed linear dependence of the top mass to the transverse momentum PT of the leptons that are two of the fi products of the top-antitop pair decay. It uses data collected by the CDF detector from December 2004 to March 2007 that correspond to an integrated luminosity of 1.8 fb-1 .Two independent and mutually compatible methods have been implemented for this reason, both depending on the leptons’ PT. The final method, called the ”Straight Line”, exploits just the linear relation between the leptons’ PT and the top mass. With the second one, called the ”Likelihood”, the full PT spectrum is modeled by an analytical function and the top mass is estimated using the likelihood minimization procedure. A top quark mass of mtop=156±20(stat)±4.6(syst) GeV/c2 is obtained with the Likelihood method and of 149±21(stat)±5.0(syst) GeV/c2 is obtained with the Straight Line one.This study is complementary to other CDF mass studies in the dilepton channel. It differs by the fact that is not dependent on the jets and does not use the b quark secondary vertex b-tagging technique. It is therefore not dependent on the jet energy scale uncertainty that is at this moment the biggest systematic contribution to all other methods. This method is a simple and straightforward method that aims to a small systematic uncertainty. The statistical uncertainty is still not competitive with respect to the other methods, due to the relatively small sensitivity of the leptons' PT to the top mass. On the other hand, this study is a very good preview of the method with the upcoming LHC data, where the statistical error is expected to be greatly suppressed. The dominating error will then be the systematic one and this method promises to be competitive or even better, regarding this point, with respect to the other methods.},
doi = {10.2172/1345597},
journal = {},
number = ,
volume = ,
place = {United States},
year = {Mon Jan 01 00:00:00 EST 2007},
month = {Mon Jan 01 00:00:00 EST 2007}
}

Thesis/Dissertation:
Other availability
Please see Document Availability for additional information on obtaining the full-text document. Library patrons may search WorldCat to identify libraries that hold this thesis or dissertation.

Save / Share:
  • Although the standard model of particle physics has been very successfull in describing nature it needs to be extended by the Higgs mechanism to explain the particle masses observed in experiments. This mechanism introduces a new elementary particle called the Higgs boson. Current research at particle accelerators focuses on the search for the Higgs boson as a major goal. This analysis uses the data recorded with the D0-detector of the Tevatron at the Fermi National Accelerator Laboratory (FNAL). The Tevatron collides protons and antiprotons at a center of mass energy of √s=1.96 TeV. The primary goal of the analysis wasmore » the search for a light Higgs boson in the WH channel. For this the process pp→ WH → ev bb was used. Furthermore a measurement of the Wbb production cross section has been performed. For the measurements a total intagrated luminosity of L=255pb -1 was available. For the selection of the desired processes events with electrons, missing transverse momentum and at least two jets have been used. At least two of the jets were required to be identified as b-jets. To obtain an efficient event selection many event properties had to be calculated and methods to cut on them needed to be optimized. Based on the selected events the Wbb production cross section has been calculated. After includinng the branching ratio BR(W→ev)=0.108 the result is σ(Wbb)=21.8 pb (+15.5; -20.0 pb(sys+stat)) for events where the b-quarks satisfy p_T>8 GeV und |η|<3. Since the significance of the signal is only about 1.2σ the data has also been used to calculate an upper limit on the production cross section. For a confidence level of 95% a value of σ 95(Wbb)=60.9 pb has been obtained. The same basic event selection has been used to obtain an upper limit for the WH production cross section. For the statistical analysis of these events the method of Cousins and Feldman was used. This method was extended to include background uncertainties as proposed by Conrad et al. Finally for a standard model Higgs boson of 115 GeV mass an upper limit for the production cross section of σ 95 (WH)=12.2 pb has been obatined at a confidence level of 95%. Although this limit is about two orders of magnitude above the prediction of the standard model this type of analysis will improve sufficiently as more data becomes available in the next few years.« less
  • We present a measurement of the W boson charge asymmetry in pmore » $$\bar{p}$$ collisions using W →ev decays using 750 pb -1 of data collected with the D detector at the Fermilab Tevatron. The electron coverage is extended to |η| < 3.2 and is thus sensitive to W s generated with low and high x partons. We also measured the charge asymmetry for events with electron E T > 25 GeV, 25 < E T < 35 GeV and E T > 35 GeV. By dividing events into di erent electron E T regions, we can probe di erent W boson rapidity regions, and can provide more constraints on the parton distribution functions (PDFs). Theoretical predictions made using CTEQ6.6 and MRST2004NLO PDFs are compared with the measurement. Our measurement is the most precise W charge asymmetry measurement to date, and this single measurement is superior in precision to the combined world average of all previous W charge asymmetry measurements done at the Tevatron. The measured asymmetry errors are less than the CTEQ6.6 PDF uncertainty for most rapidity bins. The inclusion of our results will further constrain future PDF ts and improve the predictions.« less
  • The analysis presented in this thesis focuses on kinematic distributions in the tmore » $$\bar{t}$$ system and studies in detail selected differential cross sections of top quarks as well as the reconstructed t$$\bar{t}$$ pair, namely the top quark transverse momentum and the t$$\bar{t}$$ system mass. The structure of the thesis is organized as follows: first the Standard Model of the particle physics is briefly introduced in Chapter 1, with relevant aspects of electroweak and strong interactions discussed. The physics of the top quark and its properties are then outlined in Chapter 2, together with the motivation for measuring the transverse top quark momentum and other kinematic-related variables of the t$$\bar{t}$$ system. The concepts of present-day high energy physics collider experiments and the explicit example of Fermilab Tevatron collider and the D0 detector in Chapters 3 and 4 are followed by the description of basic detector-level objects, i.e. tracks, leptons and jets, in Chapter 5; their identification and calibration following in next chapter with the emphasis on the jet energy scale in Chapter 6 and jet identification at the D0. The analysis itself is outlined in Chapter 7 and is structured so that first the data and simulation samples and the basic preselection are described in Chapter 8 and 9, followed by the kinematic reconstruction part in Chapter 10. Chapter 11 on background normalization and Chapter 12 with raw reconstructed spectra results (at the detector-smeared level) are followed by the purity-based background subtraction method and examples of signal-level corrected spectra in Chapter 13. Next, the procedure of correcting measured spectra for detector effects (unfolding) is described in Chapters 14-15, including migration matrix studies, acceptance correction determination as well as the regularized unfolding procedure itself. Final differential cross sections are presented in Chapter 16 with the main results in Figures 16.19-16.20. Summary and discussion close the main analysis part in Chapter 17, supplemented by appendices on the wealthy of analysis control plots of the t$$\bar{t}$$ → ℓ + jets channel, selected D0 event displays and finally the list of publications and references. Preliminary results of this analysis have been documented in D0 internal notes [UnfoldTop], [p17Top], [p14Top]; as well as presented at conferences [APS08], [APS05]. The author has also been a co-author of more than 135 D0 collaboration publications since 2005. The author has taken part in the jet energy scale calibration efforts performing final closure tests and deriving a correction to jet energy offset due to the suppression of the calorimeter signal. The author has also co-performed the Φ-intercalibration of the hadronic calorimeter and co-supervised the electromagnetic Φ-intercalibration; recently has also been involved in maintaining the jet identification efficiencies measurement as a JetID convener. During the years in Fermilab, many events have taken place in the course of the analysis in persuasion, including more than 170 shifts served for the D0 detector with or without the beam, 168 talks presented with mixed results and reactions; and tens of thousands of code lines in C (and sometimes perhaps even really C++) written while terabytes of data were processed, analyzed, and sometimes also lost. It has been a long but profoundly enriching chapter of my life.« less