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Related papers: Minimal Kinematic Constraints and MT2

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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 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 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 report a new possibility of using the $\mct2$ (Constransverse mass) variable for mass measurement in single step decay chains involving missing particles with moderate transverse momentum. We show that its experimental feasibility is…

High Energy Physics - Phenomenology · Physics 2011-09-12 Won Sang Cho , William Klemm , Mihoko M. Nojiri

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 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

The mass-constraining variable $M_2$, a $(1+3)$-dimensional natural successor of extremely popular $M_{T2}$, possesses an array of rich features having the ability to use on-shell mass constraints in semi-invisible production at a hadron…

High Energy Physics - Phenomenology · Physics 2016-02-02 Partha Konar , Abhaya Kumar Swain

Recently, much progress has been made on techniques to measure the masses of new particles with partially-invisible decays at a hadron collider. We examine for the first time the realistic application of MT2-based measurement methods to a…

High Energy Physics - Phenomenology · Physics 2013-05-30 David Curtin

We re-examine the kinematic variable m_T2 and its relatives in the light of recent work by Cheng and Han. Their proof that m_T2 admits an equivalent, but implicit, definition as the `boundary of the region of parent and daughter masses that…

High Energy Physics - Phenomenology · Physics 2010-09-24 Alan J. Barr , Ben Gripaios , Christopher G. Lester

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 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

We discuss kinematic methods for determining the masses of the particles in events at a hadron collider in which a pair of identical particles is produced with each decaying via a series of on-shell intermediate beyond-the-SM (BSM)…

High Energy Physics - Phenomenology · Physics 2010-05-21 Hsin-Chia Cheng , John F. Gunion , Zhenyu Han , Bob McElrath

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

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

A search for supersymmetry or other new physics resulting in similar final states is presented using a data sample of 4.73 inverse femtobarns of pp collisions collected at sqrt(s)=7 TeV with the CMS detector at the LHC. Fully hadronic final…

High Energy Physics - Experiment · Physics 2013-05-01 CMS Collaboration

Reconstructed mass variables, such as $M_2$, $M_{2C}$, $M_T^\star$, and $M_{T2}^W$, play an essential role in searches for new physics at hadron colliders. The calculation of these variables generally involves constrained minimization in a…

High Energy Physics - Phenomenology · Physics 2016-01-13 Won Sang Cho , James S. Gainer , Doojin Kim , Sung Hak Lim , Konstantin T. Matchev , Filip Moortgat , Luc Pape , Myeonghun Park

We describe a kinematic method which is capable of determining the overall mass scale in SUSY-like events at a hadron collider with two missing (dark matter) particles. We focus on the kinematic topology in which a pair of identical…

High Energy Physics - Phenomenology · Physics 2011-01-13 Hsin-Chia Cheng , John F. Gunion , Zhenyu Han , Guido Marandella , Bob McElrath

We consider the mass measurement at hadron colliders for a decay chain of two steps, which ends with a missing particle. Such a topology appears as a subprocess of signal events of many new physics models which contain a dark matter…

High Energy Physics - Phenomenology · Physics 2015-05-30 Hsin-Chia Cheng , Jiayin Gu

A search for new physics is performed using events that contain one or more jets, no isolated leptons, and a large transverse momentum imbalance, as measured through the MT2 variable, which is an extension of the transverse mass in events…

High Energy Physics - Experiment · Physics 2016-10-10 CMS Collaboration
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