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Related papers: Color Sextet Scalars at the CERN Large Hadron Coll…

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Heavy colored scalar particles, which exist in many models of new physics, can be pair produced at the Large Hadron Collider (LHC) via gluon-gluon fusion and possibly form quarkonium-like bound states. If the scalars are also charged under…

High Energy Physics - Phenomenology · Physics 2010-11-09 Ahmad Idilbi , Chul Kim , Thomas Mehen

The search for Dark Matter (DM) at colliders is primarily pursued via the detection of missing energy in particular final states. These searches are based on the production and decay processes where final states include DM particles and at…

High Energy Physics - Phenomenology · Physics 2023-08-15 Pedro Gabriel , Margarete Mühlleitner , Daniel Neacsu , Rui Santos

We investigate threshold resummation effects in the production of a color sextet (antitriplet) scalar at next-to-next-to-leading logarithmic (NNLL) order at the LHC in the frame of soft-collinear effective theory. We show the total cross…

High Energy Physics - Phenomenology · Physics 2014-03-04 Yong Chuan Zhan , Ze Long Liu , Shi Ang Li , Chong Sheng Li , Hai Tao Li

The scalar color octet contribution to the resonance $t\bar{t}$-pair production at the LHC is calculated and analysed with account of the one loop effective two gluon vertex. It is shown that this contribution from the scalar color octet…

High Energy Physics - Phenomenology · Physics 2016-12-02 I. V. Frolov , M. V. Martynov , A. D. Smirnov

A search is presented for heavy-quark pair production (QQbar) under the decay hypothesis QQbar to WqWq with q = u,d,c,s,b. The search is performed with 1.04 fb^-1 of integrated luminosity from pp collisions at sqrt(s) = 7 TeV collected by…

High Energy Physics - Experiment · Physics 2013-06-25 ATLAS Collaboration

We study the properties and production mechanisms of color-octet scalars at the LHC. We focus on the single production of both charged and neutral members of an (8,2)_1/2 doublet through bottom quark initial states. These channels provide a…

High Energy Physics - Phenomenology · Physics 2009-01-08 Pavel Fileviez Pérez , Ryan Gavin , Thomas McElmurry , Frank Petriello

We introduce an effort to catalog the gauge-invariant interactions of Standard Model (SM) particles and new fields in a variety of representations of the SM color gauge group $\text{SU}(3)_{\text{c}}$. In this first installment, we direct…

High Energy Physics - Phenomenology · Physics 2022-09-09 Linda M. Carpenter , Taylor Murphy , Tim M. P. Tait

We present a method for simulating the production and decay of particles in the sextet representation of $SU(3)_C$ including the simulation of QCD radiation. First results from the Monte Carlo simulation of sextet diquark production at the…

High Energy Physics - Phenomenology · Physics 2015-05-30 Peter Richardson , David Winn

We study properties of a hypothetical scalar particle, $\Theta$, which is a color octet and an electroweak singlet. At hadron colliders, $\Theta$ is pair produced through its QCD coupling to gluons, so that its mass determines the cross…

High Energy Physics - Phenomenology · Physics 2026-04-16 Bogdan A. Dobrescu , Max H. Fieg

Higgs pair production is studied in the extension of the Standard Model by color octet scalar and vector particles in TeV mass range for the LHC. The relevant parameters are their masses and portal couplings to the Higgs boson.The rate is…

High Energy Physics - Phenomenology · Physics 2015-05-01 Tsedenbaljir Enkhbat

Many new-physics models, especially those with a color-triplet top-quark partner, contain a heavy color-octet state. The "naturalness" argument for a light Higgs boson requires that the color-octet state be not much heavier than a TeV, and…

High Energy Physics - Phenomenology · Physics 2015-06-24 Chien-Yi Chen , Ayres Freitas , Tao Han , Keith S. M. Lee

New physics at the weak scale that can couple to quarks typically gives rise to unacceptably large flavor changing neutral currents. An attractive way to avoid this problem is to impose the principal of minimal flavor violation (MFV).…

High Energy Physics - Phenomenology · Physics 2008-11-26 Moira I. Gresham , Mark B. Wise

We study contributions of a scalar diquark particle in a color representation of anti-triplet and sextet to the top quark pair production at the Tevatron and the Large hadron collider (LHC). The model can give Forward-Backward (FB)…

High Energy Physics - Phenomenology · Physics 2015-06-05 Kaoru Hagiwara , Junya Nakamura

A search for pseudoscalar or scalar bosons decaying to a top quark pair ($\mathrm{t\bar{t}}$) in final states with one or two charged leptons is presented. The analyzed proton-proton collision data was recorded at $\sqrt{s}$ = 13 TeV by the…

High Energy Physics - Experiment · Physics 2025-12-09 CMS Collaboration

A search for pair-produced massive coloured scalar particles decaying to a four-jet final state is performed by the ATLAS experiment at the LHC in proton-proton collisions at sqrt(s) = 7 TeV. The analysed data sample corresponds to an…

High Energy Physics - Experiment · Physics 2013-06-24 ATLAS Collaboration

Structure and production of doubly charmed tetraquarks T_cc (cc ubar dbar) are studied from the viewpoint of color configurations. Based on the diquark correlation, the tetraquark T_cc with I(JP)=0(1+) is considered to be stable against…

High Energy Physics - Phenomenology · Physics 2013-03-28 Tetsuo Hyodo , Yan-Rui Liu , Makoto Oka , Kazutaka Sudoh , Shigehiro Yasui

Adding two color sextet quarks to QCD gives many special features. The high-energy S-Matrix, constructed via reggeon diagrams and chiral anomalies, contains the Critical Pomeron and electroweak symmetry breaking is produced, by sextet…

High Energy Physics - Phenomenology · Physics 2016-09-06 Alan. R. White

We discuss the phenomenology of colour scalar octets. Namely, we consider the discovery potential of scalar octets at LEP, FNAL and LHC. Scalar octets decay mainly into two gluons and new hadrons composed from scalar colour octets are…

High Energy Physics - Phenomenology · Physics 2007-05-23 N. V. Krasnikov

If electroweak symmetry breaking is a consequence of color sextet quark chiral symmetry breaking, dramatic, large cross-section, effects are to be expected at the LHC - with the pomeron playing a prominent role. The symmetry breaking is…

High Energy Physics - Phenomenology · Physics 2007-05-23 Alan R. White

We study electron-positron annihilations into six jets at the parton level in perturbative Quantum Chromo-Dynamics (QCD), via the elementary processes $e^+e^-\ar q\bar q gggg$, $e^+e^-\ar q\bar q q'\bar q' gg$ and $e^+e^-\ar q\bar q q'\bar…

High Energy Physics - Phenomenology · Physics 2009-10-31 Stefano Moretti