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Most supersymmetric models predict new particles within the reach of the next generation of colliders. For an understanding of the model structure and the mechanism(s) of electroweak symmetry breaking, it is important to know the masses of…

High Energy Physics - Phenomenology · Physics 2007-12-28 A. Sopczak , A. Freitas , C. Milstene , M. Schmitt

A compelling framework to explain dark matter and electroweak baryogenesis is supersymmetry with light scalar top quarks (stops) and a small mass difference between the stop and the lightest neutralino. In this work, the stop detection…

High Energy Physics - Phenomenology · Physics 2010-01-27 C. Milstene , M. Carena , A. Finch , A. Freitas , H. Nowak , A. Sopczak

Many supersymmetric models predict new particles within the reach of the next generation of colliders. For an understanding of the model structure and the mechanism(s) of symmetry breaking, it is important to know the masses of the new…

High Energy Physics - Phenomenology · Physics 2009-04-30 Ayres Freitas , Caroline Milstene , Michael Schmitt , Andre Sopczak

The Minimal Supersymmetric Standard Model opens the possibility of electroweak baryogenesis provided that the light scalar top quark (stop) is lighter than the top quark. In addition, the lightest neutralino is an ideal candidate to explain…

High Energy Physics - Phenomenology · Physics 2008-11-26 M. Carena , A. Finch , A. Freitas , C. Milstene , H. Nowak , A. Sopczak

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

We consider the discovery potential of light stops in the MSSM at the LHC. Here, we assume that the lightest neutralino is the LSP and that the lighter stop is the NLSP. Direct stop pair production is difficult to probe in scenarios with a…

High Energy Physics - Phenomenology · Physics 2013-04-30 M. Drees , M. Hanussek , J. S. Kim

The International Linear Collider (ILC) is a proposed electron-positron collider with a center-of-mass energy of 500~GeV, and a peak luminosity of $2 \cdot 10^{34}~\mathrm{cm}^{-2}\mathrm{s}^{-1}$. The ILC will complement the Large Hadron…

Accelerator Physics · Physics 2010-10-29 Iftach Sadeh

If the cosmic dark matter consists of weakly-interacting massive particles, these particles should be produced in reactions at the next generation of high-energy accelerators. Measurements at these accelerators can then be used to determine…

High Energy Physics - Phenomenology · Physics 2008-11-26 Edward A. Baltz , Marco Battaglia , Michael E. Peskin , Tommer Wizansky

Very precise measurements of masses and cross sections are expected to be achievable with a future linear collider. With such an accuracy one must incorporate loop corrections in order to make meaningful predictions for the underlying new…

High Energy Physics - Phenomenology · Physics 2013-09-26 Aoife Bharucha

The LEP experiments give a lower bound on the neutralino mass of about 46 GeV which, however, relies on a supersymmetric grand unification relation. Dropping this assumption, the experimental lower bound on the neutralino mass vanishes…

High Energy Physics - Phenomenology · Physics 2011-05-10 John A. Conley , Herbert K. Dreiner , Peter Wienemann

We show that the interplay between the LHC and the e^+ e^- International Linear Collider (ILC) with sqrt{s}=500 GeV might be crucial for the discrimination between the minimal and next-to-minimal supersymmetric standard model. We present an…

High Energy Physics - Phenomenology · Physics 2009-11-11 G. Moortgat-Pick , S. Hesselbach , F. Franke , H. Fraas

If supersymmetry exists at the electroweak scale, then it should be discovered at the LHC. Determining masses, of supersymmetric particles however, is more difficult. In this paper, methods are discussed to determine combinations of masses…

High Energy Physics - Phenomenology · Physics 2008-11-26 I. Hinchliffe , F. E. Paige , M. D. Shapiro , J. Soderqvist , W. Yao

The precision determination of scalar top quark properties will play an important role at a future International Linear Collider (ILC). Recent and ongoing studies are discussed for different experimental topologies in the detector. First…

High Energy Physics - Phenomenology · Physics 2007-05-23 A. Sopczak , M. Carena , A. Finch , A. Freitas , C. Milstene , H. Nowak

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

The measurement of sparticle masses in the Minimal Supersymmetric Standard Model at the LHC is analysed, in the scenario where the lightest neutralino decays into three quarks. Such decays, occurring through the baryon-number violating…

High Energy Physics - Phenomenology · Physics 2011-07-19 B. C. Allanach , A. J. Barr , L. Drage , C. G. Lester , D. Morgan , M. A. Parker , P. Richardson B. R. Webber

We investigate the need and prospects for measuring dark matter properties at particle collider experiments. We discuss the connections between the inferred properties of particle dark matter and the physics that is expected to be uncovered…

High Energy Physics - Phenomenology · Physics 2009-11-11 Andreas Birkedal

The purpose of this study is to determine the experimental uncertainties in measuring mass and cross section parameters of SUSY particles at a 500 GeV Linear Collider. In this study SUSY is a point in the focus point region of mSUGRA…

High Energy Physics - Experiment · Physics 2009-10-09 R. Gray , J. Alexander , K. M. Ecklund , L. Fields , D. Hertz , C. D. Jones , J. Pivarski , A. Birkedal , K. Matchev

Measurement of the integrated luminosity at the International Linear Collider (ILC) will be accomplished by counting the rate of small angle Bhabha scattering events. The physics requirements for ILC set the constraint on the relative…

Instrumentation and Detectors · Physics 2013-01-14 M. Pandurovic , I. Bozovic-Jelisavcic

We consider light top squarks (stops) in the minimal supersymmetric Standard Model at the Large Hadron Collider. Here, we assume that the lightest neutralino is the lightest supersymmetric particle (LSP) and the lighter stop is the…

High Energy Physics - Phenomenology · Physics 2013-05-30 Manuel Drees , M. Hanussek , Jong Soo Kim

We address the question of how to determine the stop mixing angle and its CP-violating phase at the LHC. As an observable we discuss ratios of branching ratios for different decay modes of the light stop ~t_1 to charginos and neutralinos.…

High Energy Physics - Phenomenology · Physics 2015-03-13 Krzysztof Rolbiecki , Jamie Tattersall , Gudrid Moortgat-Pick
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