Search for pair-produced third-generation squarks decaying via charm quarks or in compressed supersymmetric scenarios in pp collisions at √s =8 TeV with the ATLAS detector
2014
- Georges Aad
- Brad Abbott
- Jalal Abdallah
- S. Abdel Khalek
- Ovsat Abdinov
- Rosemarie Aben
- Babak Abi
- M. Abolins
- O. S. AbouZeid
- Halina Abramowicz
- Henso Abreu
- Ricardo Abreu
- Yiming Abulaiti
- Bobby Samir Acharya
- Leszek Adamczyk
- D. L. Adams
- J. Adelman
- Stefanie Adomeit
- T. Adye
- Tatjana Agatonovic-Jovin
- J.A. Aguilar Saavedra
- Marco Agustoni
- S. P. Ahlen
- Faig Ahmadov
- Giulio Aielli
- Henrik Akerstedt
- T. P. A. Åkesson
- Ginga Akimoto
- A. V. Akimov
- G. L. Alberghi
- J. Albert
- Solveig Albrand
- M. J. Alconada Verzini
- Martin Aleksa
- I. N. Aleksandrov
- Calin Alexa
- G. Alexander
- Gauthier Alexandre
- Theodoros Alexopoulos
- Muhammad Alhroob
- Gianluca Alimonti
- Lion Alio
- John Alison
- B. M M Allbrooke
- Lee John Allison
- P. P. Allport
- J. Almond
- Alberto Aloisio
- Alejandro Alonso
- Francisco Alonso
- C. Alpigiani
- Andrew David Altheimer
- B. Alvarez-Gonzalez
- M. G. Alviggi
- Katsuya Amako
- Y. Amaral Coutinho
- Christoph Amelung
- Dante Amidei
- S. P. Amor Dos Santos
- António Amorim
- S. Amoroso
- Nir Amram
- Glenn Amundsen
- Christos Anastopoulos
- Lucian Stefan Ancu
- Nansi Andari
- Timothy Andeen
- Christoph Falk Anders
- Gabriel Anders
- K J Anderson
- Attilio Andreazza
- V. Andrei
- X. S. Anduaga
- Stylianos Angelidakis
- Ivan Angelozzi
- Philipp Anger
- Aaron Angerami
- Francis Anghinolfi
- A. V. Anisenkov
- N. Anjos
- A. Annovi
- Ariadni Antonaki
- Massimo Antonelli
- Alexey Antonov
- J. Antos
- F. Anulli
- Masato Aoki
- L. Aperio Bella
- Rudi Apolle
- Giorgi Arabidze
- Ignacio Aracena
- Yasuo Arai
- J. P. Araque
- A. T. H. Arce
- Jean-Francois Arguin
- Spyridon Argyropoulos
- Mehmet Arik
- Aaron James Armbruster
- Olivier Arnaez
- Vanessa Arnal
- Hannah Arnold
- Miguel Arratia
- Ozan Arslan
- A Artamonov
- Giacomo Artoni
- Shoji Asai
- Nedaa Asbah
- Adi Ashkenazi
- B. Åsman
- Lily Asquith
- Ketevi Assamagan
- Robert Astalos
- Markus Atkinson
- Naim Bora Atlay
- Benjamin Auerbach
- K. Augsten
- Mathieu Aurousseau
- Giuseppe Avolio
- Georges Azuelos
- Yuya Azuma
- M. A. Baak
- Alessandra Baas
- C. Bacci
- H. Bachacou
- Konstantinos Bachas
- Moritz Backes
- Malte Backhaus
- J. Backus Mayes
- Elisabeta Badescu
- P. Bagiacchi
- P. Bagnaia
- Y. Bai
- Travis Bain
- J. T. Baines
- Oliver Keith Baker
- Petr Balek
- F. Balli
- Elzbieta Banas
- Sw. Banerjee
- Arwa A E Bannoura
- Vikas Bansal
- H. S. Bansil
- Liron Barak
- S.P. Baranov
- Elisabetta Luigia Barberio
- Dario Barberis
- Marlon Barbero
- T. Barillari
- Marcello Barisonzi
- T. Barklow
- Nick Barlow
- B. M. Barnett
- R. M. Barnett
- Zuzana Barnovska
- Antonio Baroncelli
- Gaetano Barone
- Alan Barr
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- Rainer Bartoldus
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- V. Bartsch
- Ahmed Bassalat
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- Michele Battistin
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- S. Becker
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- S Constantinescu
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- M. A. Diaz
- E. B. Diehl
- J P Dietrich
- T. A. Dietzsch
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- P Dita
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Results of a search for supersymmetry via direct production of third-generation squarks are reported, using 20.3 fb(-1) of proton-proton collision data at root s = 8 TeV recorded by the ATLAS experiment at the LHC in 2012. Two different analysis strategies based on monojetlike and c-tagged event selections are carried out to optimize the sensitivity for direct top squark-pair production in the decay channel to a charm quark and the lightest neutralino ((t) over tilde (1) -> c + (chi) over tilde (0)(1)) across the top squark-neutralino mass parameter space. No excess above the Standard Model background expectation is observed. The results are interpreted in the context of direct pair production of top squarks and presented in terms of exclusion limits in the (m((t) over tilde1), m((chi) over tilde 10)) parameter space. A top squark of mass up to about 240 GeV is excluded at 95% confidence level for arbitrary neutralino masses, within the kinematic boundaries. Top squark masses up to 270 GeV are excluded for a neutralino mass of 200 GeV. In a scenario where the top squark and the lightest neutralino are nearly degenerate in mass, top squark masses up to 260 GeV are excluded. The results from the monojetlike analysis are also interpreted in terms of compressed scenarios for top squark-pair production in the decay channel (t) over tilde (1) -> b + ff' + (chi) over tilde (0)(1) and sbottom pair production with (b) over tilde -> b + (chi) over tilde (0)(1), leading to a similar exclusion for nearly mass-degenerate third-generation squarks and the lightest neutralino. The results in this paper significantly extend previous results at colliders.
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