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Related papers: Chargino and Neutralino Masses at ILC

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One of the benchmark processes for the optimisation of the detector concepts proposed for the International Linear Collider is Chargino and Neutralino pair production in an mSugra scenario where Chargino-1 and Neutralino-2 are mass…

High Energy Physics - Experiment · Physics 2009-09-09 Taikan Suehara , Jenny List

We consider a specific class of events of the SUSY particle production at the LHC without missing p_T. Namely, we discuss the chargino pair production with a further decay into the W-boson and the neutralino when the masses of the chargino…

High Energy Physics - Phenomenology · Physics 2016-04-01 A. S. Belyaev , D. I. Kazakov , A. Sperling

Bounds on cross section measurements of chargino pair production at LEP yield a bound on the chargino mass. If the GUT relation is assumed, the lightest neutralino must be heavier than $\approx 45 -50\GeV$. If no GUT relation is assumed, no…

High Energy Physics - Phenomenology · Physics 2007-08-09 Ulrich Langenfeld

In supersymmetric extensions of the Standard Model, higgsino-like charginos and neutralinos are preferred to have masses of the order of the electroweak scale by naturalness arguments. Such light $\widetilde{\chi}^0_1$,…

High Energy Physics - Phenomenology · Physics 2014-01-10 Mikael Berggren , Felix Brümmer , Jenny List , Gudrid Moortgat-Pick , Tania Robens , Krzysztof Rolbiecki , Hale Sert

We present a study performed for the CLIC CDR on the measurement of chargino and neutralino production at sqrt(s) = 3 TeV. Fully hadronic final states with four jets and missing transverse energy were considered. Results obtained using full…

High Energy Physics - Experiment · Physics 2012-04-03 Philipp Roloff , Timothy L. Barklow , Astrid Münnich

Very precise measurements of masses and cross sections, with errors of <1%, are expected to be achievable with a future linear collider. Such an accuracy gives sensitivity at the level of quantum corrections, which therefore must be…

High Energy Physics - Phenomenology · Physics 2012-08-09 Aoife Bharucha , Jan Kalinowski , Gudrid Moortgat-Pick , Krzysztof Rolbiecki , Georg Weiglein

For points in SUSY parameter space where the sneutrino is lighter than the lightest chargino and next-to-lightest neutralino, its direct mass determination from sneutrino pair production process at e+e- collider is impossible since it…

High Energy Physics - Phenomenology · Physics 2011-07-19 J. Kalinowski , W. Kilian , J. Reuter , T. Robens , K. Rolbiecki

A search is conducted for the electroweak pair production of a chargino and a neutralino $pp \rightarrow \tilde\chi^\pm_1 \tilde\chi^0_2$, where the chargino decays into the lightest neutralino and a $W$ boson, $\tilde\chi^\pm_1 \rightarrow…

High Energy Physics - Experiment · Physics 2019-09-10 ATLAS Collaboration

A statistical combination of several searches for the electroweak production of charginos and neutralinos is presented. All searches use proton-proton collision data at $\sqrt{s}=$ 13 TeV, recorded with the CMS detector at the LHC in 2016…

High Energy Physics - Experiment · Physics 2018-04-17 CMS Collaboration

A search for charginos and neutralinos at the Large Hadron Collider is reported using fully hadronic final states and missing transverse momentum. Pair-produced charginos or neutralinos are explored, each decaying into a high-$p_{\text{T}}$…

High Energy Physics - Experiment · Physics 2022-01-10 ATLAS Collaboration

This note reports the results of a study of the accuracy in the determination of chargino and neutralino masses in two high-mass supersymmetric scenarios through kinematic endpoints and threshold scans at a multi-TeV e+e- collider. The…

High Energy Physics - Experiment · Physics 2011-04-05 Natali Alster , Marco Battaglia

A search for charginos and neutralinos, predicted by supersymmetric theories, is performed using a data sample of 182.1 pb-1 taken at a centre-of-mass energy of 189 GeV with the OPAL detector at LEP. No evidence for chargino or neutralino…

High Energy Physics - Experiment · Physics 2016-08-31 The OPAL Collaboration , G. Abbiendi

We present the results of a search for associated production of the chargino and neutralino supersymmetric particles using up to 1.1 fb-1 of integrated luminosity collected by the CDF II experiment at the Tevatron ppbar collider at a…

High Energy Physics - Experiment · Physics 2010-08-23 CDF Collaboration , T. Aaltonen , Giulia Manca

A search for electroweak production of supersymmetric particles is performed in two-lepton and three-lepton final states using recursive jigsaw reconstruction. The search uses data collected in 2015 and 2016 by the ATLAS experiment in…

High Energy Physics - Experiment · Physics 2019-03-21 ATLAS Collaboration

The fully hadronic final states of two signal processes from an mSUGRA inspired scenario (SUSY-P5) are studied within a full simulation of the LDC' detector model. These are chargino pair and neutralino pair production, i.e. e+e- -> C1C1 ->…

High Energy Physics - Experiment · Physics 2009-02-02 Daniela Käfer , Jenny List , Taikan Suehara

The requirement of electroweak naturalness in simple supersymmetric models implies the existence of a cluster of four light higgsinos with mass $\sim 100-300$\,GeV, the lighter the better. While such light compressed spectra may be…

High Energy Physics - Experiment · Physics 2020-05-27 Howard Baer , Mikael Berggren , Keisuke Fujii , Jenny List , Suvi-Leena Lehtinen , Tomohiko Tanabe , Jacqueline Yan

A direct search for electroweak production of charginos and neutralinos is presented. Events with three or four leptons, with up to two hadronically decaying $\tau$ leptons, or two same-sign light leptons are analyzed. The data sample…

High Energy Physics - Experiment · Physics 2022-05-04 CMS Collaboration

The tree-level-massless gaugino scenario predicts that the lighter chargino mass is less than m_W and that gluino and lightest neutralino masses are $\lsi 1$ GeV. In this case the dominant decay mode of charginos and non-LSP neutralinos is…

High Energy Physics - Phenomenology · Physics 2007-05-23 Glennys R. Farrar

Precision measurement of the stop mass at the ILC is done in a method based on cross-sections measurements at two different center-of-mass energies. This allows to minimize both the statistical and systematic errors. In the framework of the…

High Energy Physics - Phenomenology · Physics 2011-03-18 C. Milstene , A. Freitas , M. Schmitt , A. Sopczak

Searches for electroweak production of chargino pairs, $\tilde{\chi}^{+}_{1}\tilde{\chi}^{-}_{1}$, and of chargino and next-to-lightest neutralino, $\tilde{\chi}^{\pm}_{1}\tilde{\chi}^{0}_{2}$, are presented. The models explored assume that…

High Energy Physics - Experiment · Physics 2024-03-21 ATLAS Collaboration
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