Search for Single Top Quark Production with the CDF Run II Detector Using a Multivariate Likelihood Method

Search for Single Top Quark Production with the CDF Run II Detector Using a Multivariate Likelihood Method
Author:
Publisher:
Total Pages: 207
Release: 2008
Genre:
ISBN:

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The top quark is most often produced in t$\bar{t}$ pairs via the strong interaction, however, electroweak production of a single top quark is also possible. Electroweak or 'single-top' quark production is more difficult to observe than t$\bar{t}$ production. A measurement of single-top quark production can provide an interesting test of the Standard Model as well as a measurement of the CKM matrix element Vtb. This thesis describes a measurement of single-top quark production in pp collisions at √s=1.96 TeV usign the CDF II detector at the Fermilab Tevatron. This search is performed using a Multivariate Likelihood technique with 2.2 fb-1 of data.

Search for Single Top Quark Production with the CDF Run II Detector Using a Multivariate Likelihood Method

Search for Single Top Quark Production with the CDF Run II Detector Using a Multivariate Likelihood Method
Author: Sarah Rebecca Budd
Publisher: ProQuest
Total Pages: 194
Release: 2008
Genre:
ISBN: 9780549909347

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The top quark is most often produced in tt pairs via the strong interaction, however, electroweak production of a single top quark is also possible. Electroweak or 'single-top' quark production is more difficult to observe than tt production. A measurement of single-top quark production can provide an interesting test of the Standard Model as well as a measurement of the CKM matrix element Vtb.

Multivariate Searches for Single Top Quark Production with the D0 Detector

Multivariate Searches for Single Top Quark Production with the D0 Detector
Author:
Publisher:
Total Pages: 28
Release: 2006
Genre:
ISBN:

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We present a search for electroweak production of single top quarks in (p{bar p} --> t{bar b} + X) and t-channel (p{bar p} --> tq{bar b} + X) modes. We have analyzed 230 pb−1 of data collected with the D0 detector at the Fermilab Tevatron collider at a center-of-mass energy of (square root)s = 1.96 TeV. Two separate analysis methods are used: neural networks and a cut-based analysis. No evidence for a single top quark signal is found. We set 95% confidence level upper limits on the production cross sections using Bayesian statistics, based on event counts and binned likelihoods formed from the neural network output. The limits from the neural network (cut-based) analysis are 6.4 pb (10.6 pb) in the s-channel and 5.0 pb (11.3 pb) in the t-channel.

Fundamental Interactions - Proceedings Of The 23rd Lake Louise Winter Institute 2008

Fundamental Interactions - Proceedings Of The 23rd Lake Louise Winter Institute 2008
Author: Alan Astbury
Publisher: World Scientific
Total Pages: 429
Release: 2009-09-03
Genre: Science
ISBN: 981446709X

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This book contains pedagogical lectures on both theoretical and experimental particle physics, cosmology, and atomic trap physics. Numerous additional contributions provide up-to-date information on new experimental results from accelerators, underground laboratories, and nuclear astrophysics. This combination of pedagogical talks and topical short discussions presents a comprehensive amount of information and latest developments to researchers.

Search for Electroweak Single Top Quark Production with Cdf in Proton - Anti-proton Collisions at S**(1/2)

Search for Electroweak Single Top Quark Production with Cdf in Proton - Anti-proton Collisions at S**(1/2)
Author: Thorsten Walter
Publisher:
Total Pages: 157
Release: 2005
Genre:
ISBN:

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In this thesis two searches for electroweak single top quark production with the CDF experiment have been presented, a cutbased search and an iterated discriminant analysis. Both searches find no significant evidence for electroweak single top production using a data set corresponding to an integrated luminosity of 162 pb{sup -1} collected with CDF. Therefore limits on s- and t-channel single top production are determined using a likelihood technique. For the cutbased search a likelihood function based on lepton charge times pseudorapidity of the non-bottom jet was used if exactly one bottom jet was identified in the event. In case of two identified bottom jets a likelihood function based on the total number of observed events was used. The systematic uncertainties have been treated in a Bayesian approach, all sources of systematic uncertainties have been integrated out. An improved signal modeling using the MadEvent Monte Carlo program matched to NLO calculations has been used. The obtained limits for the s- and t-channel single top production cross sections are 13.6 pb and 10.1 pb, respectively. To date, these are most stringent limits published for the s- and the t-channel single top quark production modes.

Fundamental Interactions

Fundamental Interactions
Author: Alan Astbury
Publisher: World Scientific
Total Pages: 429
Release: 2009
Genre: Science
ISBN: 9814280933

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This book contains pedagogical lectures on both theoretical and experimental particle physics, cosmology, and atomic trap physics. Numerous additional contributions provide up-to-date information on new experimental results from accelerators, underground laboratories, and nuclear astrophysics. This combination of pedagogical talks and topical short discussions presents a comprehensive amount of information and latest developments to researchers.

Search for the Top Quark at D0 Using Multivariate Methods

Search for the Top Quark at D0 Using Multivariate Methods
Author:
Publisher:
Total Pages: 12
Release: 1995
Genre:
ISBN:

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We report on the search for the top quark in p{bar p} collisions at the Fermilab Tevatron (√s = 1.8 TeV) in the di-lepton and lepton+jets channels using multivariate methods. An H-matrix analysis of the e[mu] data corresponding to an integrated luminosity of 13.5±1.6 pb−1 yields one event whose likelihood to be a top quark event, assuming m{sub top} = 180 GeV/c2, is ten times more than that of WW and eighteen times more than that of Z → [tau][tau]. A neural network analysis of the e+jets channel using a data sample corresponding to an integrated luminosity of 47.9±5.7 pb−1 shows an excess of events in the signal region and yields a cross-section for t{bar t} production of 6.7±2.3 (stat.) pb, assuming a top mass of 200 GeV/c2. An analysis of the e+jets data using the probability density estimation method yields a cross-section that is consistent with the above result.

Search for Electroweak Single-Top Quark Production with the CDF II Experiment

Search for Electroweak Single-Top Quark Production with the CDF II Experiment
Author:
Publisher:
Total Pages: 84
Release: 2006
Genre:
ISBN:

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The CDF II experiment and the Tevatron proton-antiproton collider are parts of the Fermi National Laboratories (Fermilab). The Fermilab is located in the vicinity of Chicago, USA. Today, the Tevatron is the only collider which is able to produce the heaviest known elementary particle, the top quark. The top quark was discovered at the Tevatron by the CDF and the D0 collaborations in 1995 [1]. So far, all the top quarks found are produced via the strong interaction as top-antitop pairs. The Standard Model of elementary particle physics also predicts single-top quark production via the electroweak interaction. This production mode has not yet been observed. The CDF and the D0 collaborations have set upper limits on the cross section for that process in Run I [2, 3] and improved those results in Run II [4, 5]. Single-top quark production is one of the major interests in Run II of the Tevatron as it offers several ways to test the Standard Model and to search for potential physics beyond the Standard Model. The measurement of the cross section of singly produced top quarks via the electroweak interaction offers the possibility to determine the Cabbibo-Kobayashi-Maskawa (CKM) matrix element V{sub tb} directly. The CKM matrix defines the transformation from the eigenstates of the electroweak interactions to the mass eigenstates of the quarks. V{sub tb} gives the strength of the coupling at the Wtb vertex. The single-top quark is produced at this vertex and therefore the cross section of the single-top quark production is directly proportional to.

Observation of Electroweak Single Top-Quark Production with the CDF II Experiment

Observation of Electroweak Single Top-Quark Production with the CDF II Experiment
Author:
Publisher:
Total Pages: 180
Release: 2009
Genre:
ISBN:

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The standard model of elementary particle physics (SM) predicts, besides the top-quark pair production via the strong interaction, also the electroweak production of single top-quarks [19]. Up to now, the Fermilab Tevatron proton-antiproton-collider is the only place to produce and study top quarks emerging from hadron-hadron-collisions. Top quarks were directly observed in 1995 during the Tevatron Run I at a center-of-mass energy of √s = 1.8 TeV simultaneously by the CDF and D0 Collaborations via the strong production of top-quark pairs. Run II of the Tevatron data taking period started 2001 at √s = 1.96 TeV after a five year upgrade of the Tevatron accelerator complex and of both experiments. One main component of its physics program is the determination of the properties of the top quark including its electroweak production. Even though Run II is still ongoing, the study of the top quark is already a successful endeavor, confirmed by dozens of publications from both Tevatron experiments. A comprehensive review of top-quark physics can be found in reference. The reasons for searching for single top-quark production are compelling. As the electroweak top-quark production proceeds via a Wtb vertex, it provides the unique opportunity of the direct measurement of the CKM matrix element.