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Related papers: Re-interpreting the Oxbridge stransverse mass vari…

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We consider a class of on-shell constrained mass variables that are 3+1 dimensional generalizations of the Cambridge $M_{T2}$ variable and that automatically incorporate various assumptions about the underlying event topology. The presence…

High Energy Physics - Phenomenology · Physics 2015-03-26 Won Sang Cho , James S. Gainer , Doojin Kim , Konstantin T. Matchev , Filip Moortgat , Luc Pape , Myeonghun Park

We propose to use the MT2 concept to measure the masses of all particles in SUSY-like events with two unobservable, identical particles. To this end we generalize the usual notion of MT2 and define a new MT2(n,p,c) variable, which can be…

High Energy Physics - Phenomenology · Physics 2009-04-06 Michael Burns , Kyoungchul Kong , Konstantin T. Matchev , Myeonghun Park

Although numerical methods are required to evaluate the stransverse mass, MT2, for general input momenta, non-numerical methods have been proposed for some special clases of input momenta. One special case, considered in this note, is the…

High Energy Physics - Phenomenology · Physics 2013-09-11 Colin H. Lally , Christopher G. Lester

We advocate the use of on-shell constrained $M_2$ variables in order to mitigate the combinatorial problem in SUSY-like events with two invisible particles at the LHC. We show that in comparison to other approaches in the literature, the…

High Energy Physics - Phenomenology · Physics 2017-10-18 Dipsikha Debnath , Doojin Kim , Jeong Han Kim , Kyoungchul Kong , Konstantin T. Matchev

The stransverse mass variable $M_{T2}$ was originally proposed for the study of hadron collider events in which $N=2$ parent particles are produced and then decay semi-invisibly. Here we consider the generalization to the case of $N\ge 3$…

High Energy Physics - Phenomenology · Physics 2024-11-21 Zhongtian Dong , Kyoungchul Kong , Konstantin T. Matchev , Katia Matcheva

We propose a new model-independent technique for mass measurements in missing energy events at hadron colliders. We illustrate our method with the most challenging case of a short, single-step decay chain. We consider inclusive same-sign…

High Energy Physics - Phenomenology · Physics 2015-03-13 Partha Konar , Kyoungchul Kong , Konstantin T. Matchev , Myeonghun Park

We present the kinematic variable, m_T2, which is in some ways similar to the more familiar `transverse-mass', but which can be used in events where two or more particles have escaped detection. We define this variable and describe the…

High Energy Physics - Phenomenology · Physics 2008-11-26 Alan Barr , Christopher Lester , Phil Stephens

The MT2 or "s-transverse mass" statistic was developed to associate a parent mass scale to a missing transverse energy signature, given that escaping particles are generally expected in pairs, while collider experiments are sensitive to…

High Energy Physics - Phenomenology · Physics 2014-09-02 Joel W. Walker

This document describes some special cases in which the stransverse mass, MT2, may be calculated by non-iterative algorithms. The most notable special case is that in which the visible particles and the hypothesised invisible particles are…

High Energy Physics - Phenomenology · Physics 2011-10-04 Christopher G. Lester

We propose a new method to resolve combinatorial ambiguities in hadron collider events involving two invisible particles in the final state. This method is based on the kinematic variable MT2 and on the MT2-assisted-on-shell reconstruction…

High Energy Physics - Phenomenology · Physics 2015-05-30 Kiwoon Choi , Diego Guadagnoli , Chan Beom Park

We consider SUSY-like events with two decay chains, each terminating in an invisible particle, whose true energy and momentum are not measured in the detector. Nevertheless, a useful educated guess about the invisible momenta can still be…

High Energy Physics - Phenomenology · Physics 2017-09-13 Doojin Kim , Konstantin T. Matchev , Filip Moortgat , Luc Pape

We revisit mass determination techniques for the minimum symmetric event topology, namely $X$ pair production followed by $X \to \ell N$, where $X$ and $N$ are unknown particles with the masses to be measured, and $N$ is an invisible…

High Energy Physics - Phenomenology · Physics 2014-07-09 Lucian A. Harland-Lang , Chun-Hay Kom , Kazuki Sakurai , Marco Tonini

The algebraic singularity method is a framework for analyzing collider events with missing energy. It provides a way to draw out a set of singularity variables that can catch singular features originating from the projection of full phase…

High Energy Physics - Phenomenology · Physics 2021-11-10 Chan Beom Park

We propose a scheme to assign a 4-momentum to each WIMP in new physics event producing a pair of mother particles each of which decays to an invisible weakly interacting massive particle (WIMP) plus some visible particle(s). The transverse…

High Energy Physics - Phenomenology · Physics 2009-11-13 Won Sang Cho , Kiwoon Choi , Yeong Gyun Kim , Chan Beom Park

We introduce a new collider variable, MCT2, named as constransverse mass. It is a mixture of `stransverse mass(MT2)' and `contransverse mass(MCT)' variables, where the usual endpoint structure of MT2 distribution can be amplified in the…

High Energy Physics - Phenomenology · Physics 2015-03-13 Won Sang Cho , Jihn E. Kim , Ji-Hun Kim

We present a general solution to the long standing problem of determining the masses of pair-produced, semi-invisibly decaying particles at hadron colliders. We define two new transverse kinematic variables, $M_{CT_\perp}$ and…

High Energy Physics - Phenomenology · Physics 2011-08-22 Konstantin T. Matchev , Myeonghun Park

We propose a class of kinematic variables, which is a smooth generalization of min-max type mass variables such as the Cambridge-$M_{T2}$ and $M_2$, for measuring a mass spectrum of intermediate resonances in a semi-invisibly decaying pair…

High Energy Physics - Phenomenology · Physics 2016-08-24 Sung Hak Lim

We present a comment on the kinematic variable $m_{CT2}$ recently proposed in "Amplification of endpoint structure for new particle mass measurement at the LHC". The variable is designed to be applied to models such as R-parity conserving…

High Energy Physics - Experiment · Physics 2011-06-13 A. J. Barr , C. Gwenlan , C. G. Lester , C. J. S. Young

We further develop the constrained mass variable techniques to determine the mass scale of invisible particles pair-produced at hadron colliders. We introduce the constrained mass variable M_3C which provides an event-by-event lower bound…

High Energy Physics - Phenomenology · Physics 2009-04-22 Alan J. Barr , Alex Pinder , Mario Serna

We clarify the relation between the variable MT2 and the method of kinematic constraints, both of which can be used for mass determination in events with two missing (dark matter) particles at hadron colliders. We identify a set of minimal…

High Energy Physics - Phenomenology · Physics 2009-01-16 Hsin-Chia Cheng , Zhenyu Han
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