Global ETD Search

11	Search for neutral MSSM Higgs bosons in the fully hadronic di-tau decay channel with the ATLAS detector Wahrmund, Sebastian 18 July 2017 (has links) (PDF) The search for additional heavy neutral Higgs bosons predicted in Minimal Supersymmetric Extensions of the Standard Model is presented, using the direct decay channel into two tau leptons which themselves decay hadronically. The study is based on proton-proton collisions recorded in 2011 at a center-of-mass energy of 7 TeV with the ATLAS detector at the Large Hadron Collider at CERN. With a sample size corresponding to an integrated luminosity of 4.5 fb−1, no significant excess above the expected Standard Model background prediction is observed and CLs exclusion limits at a 95% confidence level are evaluated for values of the CP-odd Higgs boson mass mA between 140 GeV to 800 GeV within the context of the mhmax and mhmod± benchmark scenarios. The results are combined with searches for neutral Higgs bosons performed using proton-proton collisions at a center-of-mass energy of 8 TeV recorded with the ATLAS detector in 2012, with a corresponding integrated luminosity of 19.5 fb−1. The combination allowed an improvement of the exclusion limit at the order of 1 to 3 units in tan β. Within the context of this study, the structure of additional interactions during a single proton-proton collision (the “underlying event”) in di-jet final states is analyzed using collision data at a center-of-mass energy of 7 TeV recorded with the ATLAS detector in 2010, with a corresponding integrated luminosity of 37 pb−1. The contribution of the underlying event is measured up to an energy scale of 800 GeV and compared to the predictions of various models. For several models, significant deviations compared to the measurements are found and the results are provided for the optimization of simulation algorithms. Teilchenphysik CERN ATLAS LHC Higgs Tau MSSM Supersymmetrie Suche particle physics CERN ATLAS LHC Higgs Tau MSSM Supersymmetry Search ddc:530 rvk:UO 6420 Elementarteilchenphysik CERN LHC Supersymmetrie
12	Measurement of Electroweak Gauge Boson Scattering in the Channel pp → W ± W ± jj with the ATLAS Detector at the Large Hadron Collider / Messung der Streuung von elektroschwachen Eichbosonen im Kanal pp → W ± W ± jj mit dem ATLAS Detektor am Large Hadron Collider Gumpert, Christian 17 April 2015 (has links) (PDF) Particle physics deals with the elementary constituents of our universe and their interactions. The electroweak symmetry breaking mechanism in the Standard Model of Particle Physics is of paramount importance and it plays a central role in the physics programmes of current high-energy physics experiments at the Large Hadron Collider. The study of scattering processes of massive electroweak gauge bosons provides an approach complementary to the precise measurement of the properties of the recently discovered Higgs boson. Owing to the unprecedented energies achieved in proton-proton collisions at the Large Hadron Collider and the large amount of data collected, experimental studies of these processes become feasible for the first time. Especially the scattering of two W± bosons of identical electric charge is considered a promising process for an initial study due to its distinct experimental signature. In the course of this work, 20.3 fb−1 of proton-proton collision data recorded by the ATLAS detector at a centre-of-mass energy of √s = 8 TeV are analysed. An analysis of the production of two W± bosons of identical electric charge in association with two jets, pp → W ± W ± jj, is conducted in the leptonic decay channel of the W± bosons. Thereby, emphasis is put on the development of methods for the estimation of experimental backgrounds as well as on the optimisation of the event selection. As a result of this work, first experimental evidence for the existence of the aforementioned process is established with an observed significance of 4.9. Based on the number of observed events in the selected phase space the extracted fiducial cross section is σ(fid) = (2.3 ± 0.5(stat.) +0.4/−0.3 (sys.)) fb which is in agreement with the prediction of the Standard Model of σ(fid,SM) = (1.6 ± 0.2) fb. Of particular theoretical interest are electroweak contributions to the pp → W ± W ± jj process due to their sensitivity to the nature of the electroweak symmetry breaking mechanism. Criteria for a dedicated event selection are investigated and implemented in the analysis with the goal of enhancing the sensitivity to these contributions. First experimental evidence for the presence of electroweak contributions to the pp → W ± W ± jj process can be claimed with an observed significance of 4.1. The cross section extracted in the selected phase space region is found to be σ(fid) = (1.7 +0.5/−0.4 (stat.) ± 0.3(sys.)) fb which is 1.3 standard deviations above the theoretical prediction of the Standard Model of σ(fid,SM) = (1.0 ± 0.1) fb. A variety of extensions to the Standard Model predict modifications to the electroweak gauge sector. In the context of the electroweak chiral Lagrangian, which serves as an effective approximation of these theories in the energy regime E = 1 − 3 TeV, anomalous contributions to the quartic WWWW gauge coupling can be described by the parameters α4 and α5 . The selection of events is optimised again to enhance the sensitivity to these two parameters. On the basis of the number of events observed in this phase space region, the following one-dimensional confidence intervals at the 95% confidence level are derived: −0.09 ≤ α4 ≤ 0.10 and −0.15 ≤ α5 ≤ 0.15. At present, these limits represent the most stringent constraints on contributions from new physics processes to the quartic WWWW gauge coupling. Teilchenphysik Eichboson anomale Kopplungen Standardmodell W Boson LHC Particle Physics Standard Model electroweak gauge boson scattering W boson anomalous couplings LHC ddc:530 rvk:UO 6420 Elementarteilchenphysik Vektorboson Streuung Unitarität LHC Wirkungsquerschnitt
13	Relational Structure Theory / Relationale Strukturtheorie Behrisch, Mike 01 August 2013 (has links) (PDF) This thesis extends a localisation theory for finite algebras to certain classes of infinite structures. Based on ideas and constructions originally stemming from Tame Congruence Theory, algebras are studied via local restrictions of their relational counterpart (Relational Structure Theory). In this respect, first those subsets are identified that are suitable for such a localisation process, i. e. that are compatible with the relational clone structure of the counterpart of an algebra. It is then studied which properties of the global algebra can be transferred to its localisations, called neighbourhoods. Thereafter, it is discussed how this process can be reversed, leading to the concept of covers. These are collections of neighbourhoods that allow information retrieval about the global structure from knowledge about the local restrictions. Subsequently, covers are characterised in terms of a decomposition equation, and connections to categorical equivalences of algebras are explored. In the second half of the thesis, a refinement concept for covers is introduced in order to find optimal, non-refinable covers, eventually leading to practical algorithms for their determination. Finally, the text establishes further theoretical foundations, e. g. several irreducibility notions, in order to ensure existence of non-refinable covers via an intrinsic characterisation, and to prove under some conditions that they are uniquely determined in a canonical sense. At last, the applicability of the developed techniques is demonstrated using two clear expository examples. / Diese Dissertation erweitert eine Lokalisierungstheorie für endliche Algebren auf gewisse Klassen unendlicher Strukturen. Basierend auf Ideen und Konstruktionen, die ursprünglich der Tame Congruence Theory entstammen, werden Algebren über lokale Einschränkungen ihres relationalen Gegenstücks untersucht (Relationale Strukturtheorie). In diesem Zusammenhang werden zunächst diejenigen Teilmengen identifiziert, welche für einen solchen Lokalisierungsprozeß geeignet sind, d. h., die mit der Relationenklonstruktur auf dem Gegenstück einer Algebra kompatibel sind. Es wird dann untersucht, welche Eigenschaften der globalen Algebra auf ihre Lokalisierungen, genannt Umgebungen, übertragen werden können. Nachfolgend wird diskutiert, wie dieser Vorgang umgekehrt werden kann, was zum Begriff der Überdeckungen führt. Dies sind Systeme von Umgebungen, welche die Rückgewinnung von Informationen über die globale Struktur aus Kenntnis ihrer lokalen Einschränkungen erlauben. Sodann werden Überdeckungen durch eine Zerlegungsgleichung charakterisiert und Bezüge zu kategoriellen Äquivalenzen von Algebren hergestellt. In der zweiten Hälfte der Arbeit wird ein Verfeinerungsbegriff für Überdeckungen eingeführt, um optimale, nichtverfeinerbare Überdeckungen zu finden, was letztlich zu praktischen Algorithmen zu ihrer Bestimmung führt. Schließlich erarbeitet der Text weitere theoretische Grundlagen, beispielsweise mehrere Irreduzibilitätsbegriffe, um die Existenz nichtverfeinerbarer Überdeckungen vermöge einer intrinsischen Charakterisierung sicherzustellen und, unter gewissen Bedingungen, zu beweisen, daß sie in kanonischer Weise eindeutig bestimmt sind. Schlußendlich wird die Anwendbarkeit der entwickelten Methoden an zwei übersichtlichen Beispielen demonstriert. allgemeine Algebra relationale Strukturen Lokalisierungstheorie Relationale Strukturtheorie (RST) Tame Congruence Theory Umgebungen nichtverfeinerbare Überdeckungen general algebra relational structures localisation theory Relational Structure Theory (RST) Tame Congruence Theory (TCT) neighbourhoods non-refinable covers ddc:530 rvk:UO 1560 rvk:UO 6420 Allgemeine Algebra Algebraische Struktur
14	Search for Charged Higgs Bosons with the ATLAS Detector at the LHC Czodrowski, Patrick 23 August 2013 (has links) (PDF) Die Entdeckung eines geladenen Higgs-Bosons, H+, wäre ein unbestreitbarer Nachweis von Physik jenseits des Standardmodells. In der vorliegenden Arbeit wird die Suche nach dem H+ mit Hilfe von Proton-Proton-Kollisionen, welche im Jahr 2011 mit dem ATLAS Experiment am Large Hadron Collider, LHC, des CERN aufgenommen wurden, beschrieben. Im Rahmen dieser Arbeit wurde eine überarbeitete Analyse der Suche nach geladenen Higgs-Bosonen, die eine Verhältnismethode anwendet und damit die Sensitivität des traditionell direkten Suchansatzes stark verbessert, durchgeführt. Leichte geladene Higgs-Bosonen, welche eine Masse geringer als die des Top-Quarks aufweisen, können aus einem Top-Quark-Zerfall hervorgehen. Im Gegensatz zu den schweren geladenen Higgs-Bosonen sind die leichten aufgrund des hohen Produktionswirkungsquerschnitts von Top-Quark-Paaren am LHC potenziell mit den ersten Daten des Experiments beobachtbar. In den meisten Theorien und Szenarien sowie dem größten Bereich ihres Phasenraumes zerfallen leichte geladene Higgs-Bosonen meist im H± → τ±ν Kanal. Demzufolge spielen sowohl die τ-Identifikation als auch die τ-Fehlidentifikation eine besondere Rolle für die Suche nach geladenen Higgs-Bosonen. Eigens für die Ermittlung der Fehlidentifikationswahrscheinlichkeiten von Elektronen als hadronisch zerfallende τ-Leptonen wurde eine “tag-and-probe”-Methode, basierend auf Z → ee Ereignissen, entwickelt. Diese Messungen sind mit den allerersten Daten durchgeführt worden. Dabei haben diese einerseits für alle Analysen, welche die Elektronenveto-Algorithmen der τ-Identifikation nutzen, essenzielle Skalenfaktoren hervorgebracht. Andererseits wurde, beruhend auf diesen Ergebnissen, eine datenbasierte Abschätzungsmethode entwickelt und für die Untergründe der geladenen Higgs-Boson-Suche, die von der Fehlidentifikation von Elektronen als hadronisch zerfallende τ-Leptonen stammen, erfolgreich implementiert. Im Rahmen dieser Arbeit wurden Triggerstudien, mit dem Ziel höchstmögliche Signaleffizienzen zu gewährleisten, durchgeführt. Neuartige Triggerobjekte, basierend auf einer Kombination aus τ-Trigger und fehlender transversaler Energie-Trigger, wurden entworfen, überprüft und in das Triggermenü für die Datennahme im Jahr 2012 aufgenommen. Eine direkte Suche nach dem geladenen Higgs-Boson wurde in drei Kanälen mit einem τ-Lepton im Endzustand unter Berücksichtigung des gesamten Datensatzes des Jahres 2011 durchgeführt. Da kein signifikanter Überschuss, der von den Vorhersagen des Standardmodells abweicht, in den Daten beobachtet wurde, sind obere Ausschlussgrenzen auf B(t → bH+) gesetzt worden. Letztlich ist die Analyse des Kanals mit einem hadronisch zerfallenden τ-Lepton und einem Myon oder Elektron im Endzustand des tt ̄-Zerfalls, unter Anwendung der sogenannten Verhältnismethode, wiederholt worden. Diese Methode misst Verhältnisse von Ereignisausbeuten, anstatt die Verteilungen diskriminierender Variablen zu evaluieren. Folglich kürzen sich die meisten dominant beitragenden systematischen Unsicherheiten intrinsisch heraus. Die Daten stimmen mit den Vorhersagen des Standardmodells überein. Durch Zuhilfenahme der Verhältnismethode wurden die oberen Ausschlussgrenzen, im Vergleich zur direkten Suche, signifikant verbessert. Die Resultate der Verhältnismethode sind mit denen der direkten Suche, welche ein hadronisch zerfallendes τ-Lepton und zwei Jets im Endzustand des tt ̄-Zerfalls nutzt, kombiniert worden. Auf diese Art und Weise konnten obere Ausschlussgrenzen auf B(t → bH+) in einem Bereich von 0,8 %–3,4 % für geladene Higgs-Bosonen in einem Massenbereich für m_H+ zwischen 90 GeV und 160 GeV gesetzt werden. Sollte das Minimal Supersymmetrische Standardmodell (MSSM) in der Natur realisiert sein, so haben die hier ermittelten oberen Ausschlussgrenzen auf B(t → bH+) direkte Konsequenzen für die Identität des Higgs-Boson-ähnlichen Teilchens, welches im Jahr 2012 am LHC entdeckt wurde. ATLAS LHC geladenes Higgs Higgs Physik MSSM Tau hadronisch Trigger 2HMD Supersymmetrie Teilchen und Resonanz Produktion experimentelle Resultate ATLAS LHC charged Higgs Higgs Physics MSSM Tau hadronic Trigger 2HMD Supersymmetry Particle and Resonance Production experimental Results ddc:530 rvk:UO 6420 rvk:UO 1560
15	Search for heavy resonances decaying into the fully hadronic di-tau final state with the ATLAS detector Morgenstern, Marcus Matthias 11 April 2014 (has links) (PDF) The discovery of a heavy neutral particle would be a direct hint for new physics beyond the Standard Model. In this thesis searches for new heavy neutral particles decaying into two tau leptons, which further decay into hadrons, are presented. They cover neutral Higgs bosons in the context of the minimal supersymmetric extension of the Standard Model (MSSM) as well as Z′ bosons, predicted by various theories with an extended gauge sector. Both analyses are based on the full 2012 proton-proton collision dataset taken by the ATLAS experiment at the Large Hadron Collider (LHC). The extended Higgs sector in the MSSM suggests additional heavy neutral Higgs bosons which decay into tau leptons in about 10% of the time. Given that the dominant final state, φ → b¯b, suffers from tremendous QCD initiated backgrounds, the decay into two tau leptons is the most promising final state to discover such new resonances. The fully hadronic final state is the dominant one with a branching fraction of about 42%. It governs the sensitivity, in particular at high transverse momentum when the QCD multijet background becomes small. Other theoretical extensions of the Standard Model, which are mainly driven by the concept of gauge unification, predict additional heavy particles arising from an extended underlying gauge group. Some of them further predict an enhanced coupling to fermions of the third generation. This motivates the search for Z′ bosons in the fully hadronic di-tau final state. One major challenge in physics analyses involving tau leptons is to have an outstanding performance of trigger and identification algorithms suitable to select real tau leptons with high efficiency, while rejecting fake taus originating from quark or gluon initiated jets. In this work a new tau trigger concept based on multivariate classifiers has been developed and became the default tau trigger algorithm in 2012 data-taking. An updated tau identification technique based on the log-likelihood approach has been provided for 2011 data-taking. Furthermore, a new framework has been developed to perform the tuning of the tau identification algorithm and exploited for the optimisation for 2012 data-taking, accordingly. The search for new heavy neutral Higgs bosons in the context of the MSSM has been performed exploiting the full 2012 dataset corresponding to an integrated luminosity of 19.5 fb−1 taken at a centre-of-mass energy of √s = 8 TeV. Updated event selection criteria and novel data-driven background estimation techniques have been developed and are suitable to increase the sensitivity of the analysis significantly. No deviations from the Standard Model prediction are observed, and thus 95% C.L. exclusion limits on the production cross section times branching ratio, σ(pp → φ) × BR(φ → ττ), are derived exploiting the CLs method. The exclusion ranges from 13.0 pb at 150GeV to 7.0 fb at 1 TeV for Higgs boson production in association with b-quarks and from 23.6 pb at 150GeV to 7.5 fb at 1 TeV for Higgs bosons produced via gluon-gluon fusion. The obtained exclusion limit on σ(pp → φ) × BR(φ → ττ) can be related to an exclusion of the MSSM parameter space in the MA-tan β-plane. Various benchmark scenario are considered. The ”standard candle” is the mhmax scenario, for which tan β values between 13.3 and 55 can be excluded at 95% C.L. in the considered mass range. Updated benchmark scenarios designed to incorporate the recently discovered SM-like Higgs boson were suggested and analysed as well. In the mhmod+ (mhmod−) scenario tan β values between 13.5 (13.3 ) and 55 (52 ) can be excluded. Finally, a search for heavy neutral resonances in the context of Z′ bosons was performed. As in the search for new Higgs bosons, no deviation from the Standard Model prediction is observed, and hence exclusion limits on the production cross section times branching ratio, σ(pp → Z′) × BR(Z′ → ττ), and on the Z′ boson mass are derived exploiting the Bayesian approach. Z′ bosons with MZ′ < 1.9 TeV can be excluded at 95% credibility, and thus mark the strongest exclusion limit obtained in the di-tau final state by any collider experiment so far. ATLAS LHC neutrale Higgs Bosonen Higgs Physik MSSM Tau hadronisch Trigger 2HMD Supersymmetrie Teilchen und Resonanz Production experimentelle Ergebnisse Z' zprime schwere Resonanz ATLAS LHC neutral Higgs Higgs Physics MSSM Tau hadronic Trigger 2HMD Supersymmetry Particle and Resonance Production experimental Results Z' zprime heavy resonance Exotics ddc:530 rvk:UO 6420
16	Probing Electroweak Gauge Boson Scattering with the ATLAS Detector at the Large Hadron Collider Anger, Philipp 07 October 2014 (has links) (PDF) Electroweak gauge bosons as central components of the Standard Model of particle physics are well understood theoretically and have been studied with high precision at past and present collider experiments. The electroweak theory predicts the existence of a scattering process of these particles consisting of contributions from triple and quartic bosonic couplings as well as Higgs boson mediated interactions. These contributions are not separable in a gauge invariant way and are only unitarized in the case of a Higgs boson as it is described by the Standard Model. The process is tied to the electroweak symmetry breaking which introduces the longitudinal modes for the massive electroweak gauge bosons. A study of this interaction is also a direct verification of the local gauge symmetry as one of the fundamental axioms of the Standard Model. With the start of the Large Hadron Collider and after collecting proton-proton collision data with an integrated luminosity of 20.3/fb at a center-of-mass energy of 8 TeV with the ATLAS detector, first-ever evidence for this process could be achieved in the context of this work. A study of leptonically decaying WWjj, same-electric-charge diboson production in association with two jets resulted in an observation of the electroweak WWjj production with same electric charge of the W bosons, inseparably comprising WW->WW electroweak gauge boson scattering contributions, with a significance of 3.6 standard deviations. The measured production cross section is in agreement with the Standard Model prediction. In the course of a study for leptonically decaying WZ productions, methods for background estimation, the extraction of systematic uncertainties and cross section measurements were developed. They were extended and applied to the WZjj final state whereof the purely electroweakly mediated contribution is intrinsically tied to the scattering of all Standard Model electroweak gauge bosons: Wγ->WZ and WZ->WZ. Three charged leptons and a neutrino from the decay of the final state bosons allow inferences about the scattering process. A distinct signature is provided by the two accompanying tagging jets as remnants of the incoming quarks radiating the initial electroweak gauge bosons. The cross section of the electroweak WZjj production was measured to σ(fiducial, observed) = (0.63 +0.32 -0.28 (stat.) +0.41 -0.24 (syst.)) fb and was found to be consistent with the Standard Model prediction at next-to-leading order in perturbative quantum chromodynamics, σ(fiducial, theory) = (0.31 +0.03 -0.05) fb. Unfolded differential cross sections of kinematic variables sensitive to models of new physics were derived. Anomalous quartic electroweak gauge couplings are introduced as dimensionless coupling parameters of additional operators within an effective field theory approach. Constraints on the parameters of operators with dimension eight were set employing a unitarization prescription based on form factors. CERN LHC ATLAS 2014 Standardmodell Teilchenphysik Elementarteilchenphysik VBS Eichboson-Streuung Vektorboson-Streuung Vektor-Boson-Streuung aQGC aqgc anomale Eichkopplung anomale Vierer-Eichboson-Kopplung Effektive Lagrangedichte Vierer-Vertex Vierer-Eichboson-Vertex Higgs WZ-Endzustand Sherpa VBFNLO Whizard K-Matrix Form-Faktor Formfaktor Unitarisierung Boson CERN LHC ATLAS 2014 Standard Model Particle Physics VBS Vector Boson Scattering Vector-Boson-Scattering Vector-Boson Scattering Gauge Boson Scattering Electroweak Gauge Boson Scattering aQGC aqgc Anomalous Quartic Gauge Boson Coupling Anomalous Gauge Boson Coupling Effective Lagrangian Quartic Vertex Quartic Gauge Boson Vertex Higgs WZ Final State Sherpa VBFNLO Whizard K-Matrix Form-Factor Unitarization Unitarisation Boson ddc:530 rvk:UO 6420 CERN LHC 2014 Elementarteilchenphysik Boson

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