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Search for the Standard Model Higgs boson produced in association with a W Boson in the isolated-track charged-lepton channel using the Collider Detector at Fermilab.

机译:使用费米实验室的对撞机探测器在隔离轨道带电轻子通道中搜索与W玻色子关联产生的标准模型希格斯玻色子。

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摘要

The Higgs boson is the only elementary particle predicted by the Standard Model (SM) that has not yet been observed experimentally. If it exists, it explains the spontaneous electroweak symmetry breaking and the origin of mass for gauge bosons and fermions. We test the validity of the SM by performing a search for the associated production of a Higgs boson and a W boson in the channel where the Higgs boson decays to a bottom-antibottom quark pair and the W boson decays to a charged lepton and a neutrino (the WH channel). We study a dataset of proton-antiproton collisions at a centre-of-mass energy of 1.96 TeV provided by the Tevatron accelerator, corresponding to an integrated luminosity of 5.7 inverse femtobarns , and recorded using the Collider Detector at Fermilab (CDF). We select events consistent with the signature of exactly one charged lepton (electron or muon), missing transverse energy due to the undetected neutrino (MET) and two collimated streams of particles (jets), at least one of which is required to be identified as originating from a bottom quark. We improve the discrimination of Higgs signal from backgrounds through the use of an artificial neural network. Using a Bayesian statistical inference approach, we set for each hypothetical Higgs boson mass in the range 100 - 150 GeV/c2 with 5 GeV/c 2 increments a 95% credibility level (CL) upper limit on the ratio between the Higgs production cross section times branching fraction and the SM prediction.;The ISOTRK candidate is a high-transverse-momentum good-quality track isolated from other activity in the tracking system and not required to match a calorimeter cluster, as for a tight electron candidate, or an energy deposit in the muon detector, as for a tight muon candidate. The ISOTRK category recovers real charged leptons that otherwise would be lost in the non-instrumented regions of the detector. This allows the reconstruction of more W boson candidates, which in turn increases the number of reconstructed WH signal candidate events, and therefore improves the sensitivity of the WH search.;Since there is no ISOTRK-dedicated trigger at CDF, for the ISOTRK charged lepton category we employ three MET-plus-jets-based triggers using a novel method, which allows the combination of any number of triggers in order to maximize the event yield while avoiding trigger correlations. On an event-by-event basis, only the trigger with the largest efficiency is used. By avoiding a logical "OR" between triggers, the loss in the yield of events accepted by the trigger combination is compensated by a smaller and easier-to-compute corresponding systematic uncertainty.;The addition of the ISOTRK charged lepton category to the TIGHT category produces an increase of 33% in the WH signal yield and a decrease of 15.5 % to 19.0 % in the median expected 95 % CL cross-section upper limits across the entire studied Higgs mass interval. The observed (median expected) 95 % CL SM Higgs upper limits on cross section times branching ratio vary between 2.39 x SM (2.73 x SM) for a Higgs mass of 100 GeV/ c2 to 31.1 x SM (31.2 x SM) for a Higgs mass of 150 GeV/c2, while the value for a 115 GeV/ c2 Higgs boson is that of 5.08 x SM (3.79 x SM).;Our main original contributions are the addition of a novel charged lepton reconstruction algorithm with looser requirements (ISOTRK) with respect the electron or muon tight criteria (TIGHT), as well as the introduction of a novel trigger-combination method that allows to maximize the event yield while avoiding trigger correlations and that is used for the ISOTRK category.;The novel trigger combination method is already in use by several CDF analyses. It is applicable to any analysis that uses triggers based on MET and jets, such as supersymmetry searches at the ATLAS and CMS experiments at the Large Hadron Collider. In its most general form, the method can be used by any analysis that combines any number of different triggers.
机译:希格斯玻色子是由标准模型(SM)预测的唯一尚未通过实验观察到的基本粒子。如果存在,则说明自发性电弱对称性破裂以及规范玻色子和费米子的质量起源。我们通过搜索通道中希格斯玻色子和W玻色子的相关产生来测试SM的有效性,在该通道中,希格斯玻色子衰变成底部反底夸克对,W玻色子衰变成带电的轻子和中微子(WH频道)。我们研究了由Tevatron加速器提供的质量中心能量为1.96 TeV的质子-反质子碰撞的数据集,对应于5.7个反飞巴姆的综合光度,并使用费米实验室(CDF)的对撞探测器进行了记录。我们选择与正好一个带电的轻子(电子或介子)的特征相符的事件,由于未检测到的中微子(MET)和两个准直的粒子流(射流)而缺少横向能量,其中至少一个需要被识别为源于底夸克。通过使用人工神经网络,我们改善了对背景希格斯信号的识别能力。使用贝叶斯统计推断方法,我们为每个假设的希格斯玻色子质量设置在100-150 GeV / c2范围内,其中5 GeV / c 2递增了希格斯生产截面之间比率的95%可信度(CL)上限ISOTRK候选对象是与跟踪系统中的其他活动隔离开的高横动量优质轨道,不需要与量热仪簇匹配,例如紧密电子候选对象或能量沉积在μ子检测器中,例如候选的μ子。 ISOTRK类别可恢复实际带电的轻子,否则,它们会在检测器的非仪器区域丢失。这允许重建更多的W玻色子候选物,从而增加了重建的WH信号候选事件的数量,因此提高了WH搜索的灵敏度。;由于CDF没有ISOTRK专用的触发器,因此对于ISOTRK带电的轻子类别中,我们使用一种新颖的方法,使用了三个基于MET + jets的触发器,该触发器允许组合任意数量的触发器,以便在避免触发器相关的同时最大化事件的产生。在逐事件的基础上,仅使用效率最高的触发器。通过避免触发器之间的逻辑“或”,触发器组合所接受的事件的收益损失将由更小且更易于计算的相应系统不确定性来补偿。;将ISOTRK带电轻子类别添加到TIGHT类别中在整个研究的希格斯质量区间内,WH信号的收率提高了33%,预期的中值95%CL截面上限的中值下降了15.5%至19.0%。对于100 GeV / c2的希格斯质量,观察到的(预期的中值)95%CL SM希格斯截面时间的上限在2.39 x SM(2.73 x SM)到31.1 x SM(31.2 x SM)之间变化质量为150 GeV / c2,而115 GeV / c2希格斯玻色子的值为5.08 x SM(3.79 x SM).;我们的主要原始贡献是增加了具有更宽松要求的新型带电轻子重构算法(ISOTRK )关于电子或介子密封性标准(TIGHT),以及引入了一种新颖的触发组合方法,该方法可在避免触发相关的同时最大化事件的产生,并用于ISOTRK类别。 CDF分析已经使用了这种方法。它适用于使用基于MET和喷射的触发器的任何分析,例如ATLAS的超对称搜索和大型强子对撞机的CMS实验。以其最一般的形式,该方法可用于结合了任意数量不同触发器的任何分析。

著录项

  • 作者

    Buzatu, Adrian.;

  • 作者单位

    McGill University (Canada).;

  • 授予单位 McGill University (Canada).;
  • 学科 Physics Elementary Particles and High Energy.
  • 学位 Ph.D.
  • 年度 2011
  • 页码 209 p.
  • 总页数 209
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

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