Search for new phenomena in final states with large jet multiplicities and missing transverse momentum using sqrt s = 7 TeV pp collisions with the ATLAS detector

The Journal of High Energy Physics 2011:11

Authors:

AJ Barr, more than 10, The ATLAS Collaboration

Search for pair-produced higgsinos decaying via Higgs or 𝒁 bosons to final states containing a pair of photons and a pair of 𝒃-jets with the ATLAS detector

Physics Letters B Elsevier

Authors:

Alan Barr, Daniela Bortoletto, Federico Celli, Min Chen, Eimear Conroy, Amanda Cooper-Sarkar, Maxence Draguet, Gregor Eberwein, James Frost, Elizabeth Gallas, Claire Gwenlan, Christopher Hays, Brian Huffman, Simon Koch, Zhenlong Li, Koichi Nagai, Luka Nedic, Richard Nickerson, Eleonora Rossi, Alessandro Ruggiero, Elisabeth Schopf, Ian Shipsey, Iza Veliscek, Georg Viehhauser, Yajing Wei, Anthony Weidberg, Siyu Yan

Abstract:

A search is presented for the pair production of higgsinos 𝜒˜ in gauge-mediated supersymmetry models, where the lightest neutralinos 𝜒˜ 0 1 decay into a light gravitino 𝐺˜ either via a Higgs ℎ or 𝑍 boson. The search is performed with the ATLAS detector at the Large Hadron Collider using 139 fb−1 of proton–proton collisions at a centre-of-mass energy of √ 𝑠 = 13 TeV. It targets final states in which a Higgs boson decays into a photon pair, while the other Higgs or 𝑍 boson decays into a 𝑏𝑏¯ pair, with missing transverse momentum associated with the two gravitinos. Search regions dependent on the amount of missing transverse momentum are defined by the requirements that the diphoton mass should be consistent with the mass of the Higgs boson, and the 𝑏𝑏¯ mass with the mass of the Higgs or 𝑍 boson. The main backgrounds are estimated with data-driven methods using the sidebands of the diphoton mass distribution. No excesses beyond Standard Model expectations are observed and higgsinos with masses up to 320 GeV are excluded, assuming a branching fraction of 100% for 𝜒˜ 0 1 → ℎ𝐺˜. This analysis excludes higgsinos with masses of 130 GeV for branching fractions to ℎ𝐺˜ as low as 36%, thus providing complementarity to previous ATLAS searches in final states with multiple leptons or multiple 𝑏-jets, targeting different decays of the electroweak bosons.

Sensor Compendium

Office of Scientific and Technical Information (OSTI)

Authors:

M Artuso, et al.

Simulation of LiCAS Error Propagation

ECONF C0705302:MET05,2007

Authors:

G Grzelak, A Reichold, J Dale, M Dawson, J Green, Y Han, M Jones, G Moss, B Ottewell, R Wastie, D Kämptner, J Prenting, M Schlösser

Abstract:

Linear Collider Alignment and Survey (LiCAS) R&D group is proposing a novel automated metrology instrument dedicated to align and monitor the mechanical stability of a future linear high energy e+e- collider. LiCAS uses Laser Straightness Monitors (LSM) and Frequency Scanning Interferometry (FSI) for straightness and absolute distance measurements, respectively. This paper presents detailed simulations of a LiCAS system operating inside a Rapid Tunnel Reference Surveyor (RTRS train). With the proposed design it is feasible to achieve the required vertical accuracy of the order of 200 micons over 600 m tunnel sections meeting the specification for the TESLA collider.

Technical design of the phase I Mu3e experiment

Authors:

K Arndt, H Augustin, P Baesso, N Berger, F Berg, C Betancourt, D Bortoletto, A Bravar, K Briggl, D vom Bruch, A Buonaura, F Cadoux, C Chavez Barajas, H Chen, K Clark, P Cooke, S Corrodi, A Damyanova, Y Demets, S Dittmeier, P Eckert, F Ehrler, D Fahrni, L Gerritzen, J Goldstein, D Gottschalk, C Grab, R Gredig, A Groves, J Hammerich, U Hartenstein, U Hartmann, H Hayward, A Herkert, G Hesketh, S Hetzel, M Hildebrandt, Z Hodge, A Hofer, Qh Huang, S Hughes, L Huth, Dm Immig, T Jones, M Jones, H-C Kästli, M Köppel, P-R Kettle, M Kiehn, S Kilani

Abstract:

The Mu3e experiment aims to find or exclude the lepton flavour violating decay $\mu \rightarrow eee$ at branching fractions above $10^{-16}$. A first phase of the experiment using an existing beamline at the Paul Scherrer Institute (PSI) is designed to reach a single event sensitivity of $2\cdot 10^{-15}$. We present an overview of all aspects of the technical design and expected performance of the phase~I Mu3e detector. The high rate of up to $10^{8}$ muon decays per second and the low momenta of the decay electrons and positrons pose a unique set of challenges, which we tackle using an ultra thin tracking detector based on high-voltage monolithic active pixel sensors combined with scintillating fibres and tiles for precise timing measurements.