Using Subsystem MT2 for Complete Mass Determinations in Decay Chains with Missing Energy at Hadron Colliders
arXiv:0810.5576 · doi:10.1088/1126-6708/2009/03/143
Abstract
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 applied to various subsystem topologies, as well as the full event topology. We derive analytic formulas for its endpoint MT2{max}(n,p,c) as a function of the unknown test mass Mc of the final particle in the subchain and the transverse momentum pT due to radiation from the initial state. We show that the endpoint functions MT2{max}(n,p,c)(Mc,pT) may exhibit three different types of kinks and discuss the origin of each type. We prove that the subsystem MT2(n,p,c) variables by themselves already yield a sufficient number of measurements for a complete determination of the mass spectrum (including the overall mass scale). As an illustration, we consider the simple case of a decay chain with up to three heavy particles, X2 -> X1 -> X0, which is rather problematic for all other mass measurement methods. We propose three different MT2-based methods, each of which allows a complete determination of the masses of particles X0, X1 and X2. The first method only uses MT2(n,p,c) endpoint measurements at a single fixed value of the test mass Mc. In the second method the unknown mass spectrum is fitted to one or more endpoint functions MT2{max}(n,p,c)(Mc,pT) exhibiting a kink. The third method is hybrid, combining MT2 endpoints with measurements of kinematic edges in invariant mass distributions. As a practical application of our methods, we show that the dilepton W+W- and tt-bar samples at the Tevatron can be used for an independent determination of the masses of the top quark, the W boson and the neutrino, without any prior assumptions.
47 pages, 9 figures. revised version, published in JHEP. Major addition: a new appendix with the complete set of formulas for the MT2 endpoints as functions of the upstream transverse momentum pT and test mass Mc
References in corpus (19)
- Gluino Stransverse Mass
- Measuring superparticle masses at hadron collider using the transverse mass kink
- Minimal Kinematic Constraints and MT2
- Accurate Mass Determinations in Decay Chains with Missing Energy
- Transverse Observables and Mass Determination at Hadron Colliders
- Hunting for the Top Partner in the Littlest Higgs Model with T-parity at the LHC
- A Supersymmetric U(1)' Model with Multiple Dark Matters
- Mass Determination of New States at Hadron Colliders
- Inclusive transverse mass analysis for squark and gluino mass determination
- Handling jets + missing E_T channel using inclusive mT2
- The Precision Determination of Invisible-Particle Masses at the LHC
- A General Method for Model-Independent Measurements of Particle Spins, Couplings and Mixing Angles in Cascade Decays with Missing Energy at Hadron Colliders
- Missing energy look-alikes with 100 pb-1 at the LHC
- A short comparison between m_T2 and m_CT
- Study of the top reconstruction in top-partner events at the LHC
- Proposal for a New Reconstruction Technique for SUSY Processes at the LHC
- Lightest U-parity Particle (LUP) dark matter
- Measuring the top quark mass with m_T2 at the LHC
- Hidden Thresholds: A Technique for Reconstructing New Physics Masses at Hadron Colliders
Cited by in corpus (9)
- Using kinematic boundary lines for particle mass measurements and disambiguation in SUSY-like events with missing energy
- Precise reconstruction of sparticle masses without ambiguities
- Measuring the Dark Force at the LHC
- Squark Flavor Violation at the LHC
- Mass determination in sequential particle decay chains
- Precision Determination of Invisible-Particle Masses at the CERN LHC: II
- Effects of QCD radiation on inclusive variables for determining the scale of new physics at hadron colliders
- Sparticle masses in deflected mirage mediation
- Fake Dark Matter at Colliders