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A straightforward new technique is introduced which enables measurement at hadron colliders of an analytical combination of the masses of pair-produced semi-invisibly decaying particles and their invisible decay products. The new technique…

High Energy Physics - Phenomenology · Physics 2009-07-21 Daniel R. Tovey

We derive finite boost transformations based on the Lorentz sector of the bicross-product-basis $\kappa$-Poincare' Hopf albegra. We emphasize the role of these boost transformations in a recently-proposed new relativistic theory. We find…

High Energy Physics - Theory · Physics 2009-11-07 N. R. Bruno , G. Amelino-Camelia , J. Kowalski-Glikman

A modification to the contransverse mass (MCT) technique for measuring the masses of pair-produced semi-invisibly decaying heavy particles is proposed in which MCT is corrected for non-zero boosts of the centre-of-momentum (CoM) frame of…

High Energy Physics - Phenomenology · Physics 2010-03-19 Giacomo Polesello , Daniel R. Tovey

We investigate the effects of the repeated application of Lorentz-boosts to the four momentum of a photon in the transverse direction and observe that this can take us to a reference frame in which the direction of the photon's momentum is…

General Physics · Physics 2024-05-27 Tugdual LeBohec

We introduce a variable useful for measuring masses of particles pair produced at hadron colliders, where each particle decays to one particle that is directly observable and another particle whose existence can only be inferred from…

High Energy Physics - Phenomenology · Physics 2010-04-06 C. G. Lester , D. J. Summers

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

Collisions of composite particles impose an arbitrary boost in the longitudinal direction on a given event. This implies that the centre-of-mass frame at hadron colliders is undetermined for processes with missing energy in the final state.…

High Energy Physics - Phenomenology · Physics 2016-03-23 Laurence Anthony Spiller

We extend a recent approach to Deformed Special Relativity based on deformed dispersion laws, entailing modified Lorentz transformations and, at the same time, noncommutative geometry and intrinsically discrete spacetime. In so doing we…

High Energy Physics - Theory · Physics 2017-06-20 G. Salesi , M. Greselin , L. Deleidi , R. A. Peruzza

I consider the two-body decay of a particle at a hadron collider into a visible and an invisible particle, generalizing $W \to e \nu$, where the masses of the decaying particle and the invisible decay particle are, {\em a priori}, unknown.…

High Energy Physics - Phenomenology · Physics 2008-11-26 Ben Gripaios

Formulae are derived for the positions of end-points in the invariant mass and transverse mass distributions obtained from the products of heavy states decaying to pairs of semi-invisibly decaying lighter states. Formulae are derived both…

High Energy Physics - Phenomenology · Physics 2010-12-06 Daniel R. Tovey

This paper describes a particularly didactic and transparent derivation of basic properties of the Lorentz group. The generators for rotations and boosts along an arbitrary direction, as well as their commutation relations, are written as…

General Physics · Physics 2011-12-12 Bernard R. Durney

We present a novel method for studying the shape of the Z boson transverse momentum distribution, Q_T, at hadron colliders in ppbar/pp -> Z/gamma* -> l^+l^-. The Q_T is decomposed into two orthogonal components; one transverse and the other…

High Energy Physics - Experiment · Physics 2009-04-17 M. Vesterinen , T. R. Wyatt

Charged Higgs boson may be produced at hadron colliders via the decay of top quarks. At the LHC, The large production cross section of top quarks pairs will make it one of the earliest channels allowing to search for physics beyond the…

High Energy Physics - Phenomenology · Physics 2010-04-14 Eilam Gross , Ofer Vitells

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 the transverse-momentum distribution of colourless high-mass systems (lepton pairs, vector bosons, Higgs particles...) produced in hadronic collisions. We briefly review a formalism for the all-order resummation of the…

High Energy Physics - Phenomenology · Physics 2009-08-11 M. Grazzini

We explore a novel method of mass reconstruction in events with missing transverse momentum at hadron colliders. In events with sizeable boost factors in the final steps of dual multi-stage decay chains, the missing energy particles may…

High Energy Physics - Phenomenology · Physics 2013-05-29 Jay Hubisz , Jing Shao

The concept of the Lorentz-invariant mass of a group of particles is shown to be applicable to biphoton states formed in the process of spontaneous parametric down conversion. The conditions are found when the Lorentz-invariant mass is…

Quantum Physics · Physics 2019-06-26 S. V. Vintskevich , D. A. Grigoriev , M. V. Fedorov

The transverse momentum distributions of various hadrons produced in most central Pb+Pb collisions at LHC energy Root(s_NN) = 2.76 TeV have been studied using our earlier proposed unified statistical thermal freeze-out model. The calculated…

High Energy Physics - Phenomenology · Physics 2014-11-18 Saeed Uddin , Inam-ul Bashir , Riyaz Ahmed Bhat , M. Farooq Mir

This paper seeks to demonstrate that many of the existing mass-measurement variables proposed for hadron colliders (mT, mEff, mT2, missing pT, hT, rootsHatMin, etc.) are far more closely related to each other than is widely appreciated, and…

High Energy Physics - Phenomenology · Physics 2013-05-29 A. J. Barr , T. J. Khoo , P. Konar , K. Kong , C. G. Lester , K. T. Matchev , M. Park

The transverse momentum spectra of weak vector bosons are measured in the CMS experiment at the LHC. The measurement uses a sample of proton-proton collisions at sqrt(s) = 8 TeV, collected during a special low-luminosity running that…

High Energy Physics - Experiment · Physics 2017-02-27 CMS Collaboration
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