<i>Collider Physics</i>

Barger, V.; Phillips, R. J.; Siegrist, J.

doi:10.1063/1.2810885

Cited by 139 publications

(187 citation statements)

References 8 publications

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“…µ √ s). After renormalization all the dependence of observables on the energy scale appears through the running coupling in a well prescribed form (for more details see, for instance, [6][7][8][9][10]). …”

Section: Elements Of Qcd 11 Renormalization and The Running Couplingmentioning

confidence: 99%

Dynamical parton distributions of the nucleon

Jimenez-Delgado¹

2009

Nuclear Physics B - Proceedings Supplements

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Section: Elements Of Qcd 11 Renormalization and The Running Couplingmentioning

confidence: 99%

Dynamical parton distributions of the nucleon

Jimenez-Delgado¹

2009

Nuclear Physics B - Proceedings Supplements

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“…55, and are given via [172,225]: ) is defined in appendix A. The quark level asymmetries of interest can be converted to the hadron (i.e., pp) level by folding in the structure functions in the standard manner [61]. The results for the 2HDM case are shown in Fig.…”

Section: Hdm and The Cp-violating Asymmetriesmentioning

confidence: 95%

“…However, 9 of these 18 parameters are eliminated by the unitarity constraints V † ik V kj = δ ij , therefore we are left with only 9 free parameters. Moreover, there is a freedom to absorb 5 phases into 5 out of the 6 left handed fields [61]:…”

Section: General Remarksmentioning

confidence: 99%

CP violation in top physics

et al. 2001

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CP violation in top physics is reviewed. The Standard Model has negligible effects, consequently CP violation searches involving the top quark may constitute the best way to look for physics beyond the Standard Model. Non-standard sources of CP violation due to an extended Higgs sector with and without natural flavor conservation and supersymmetric theories are discussed. Experimental feasibility of detecting CP violation effects in top quark production and decays in high energy e + e − , γγ, µ + µ − , pp and pp colliders are surveyed. Searches for the electric, electro-weak and the chromo-electric dipole moments of the top quark in e + e − → tt and in pp → ttX are descibed. In addition, other mechanisms that appear promising for experiments, e.g., tree-level CP violation in e + e − → tth, ttZ, ttν eνe and in the top decay t → bτ ν τ and CP violation driven by s-channel Higgs exchanges in pp, γγ, µ + µ − → tt etc., are also discussed. * A 2-up version of this postscript file may be obtained at the url

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“…The 3-body phase-space integral can be written in terms of dimensionless variables (see for example [34]) dP S 3 (q → p l + + p l − + pÑ For the total number of events N + + N − we must include the entire amplitude…”

Section: Discussionmentioning

confidence: 99%

A T-odd observable sensitive to CP violating phases in squark decay

Langacker

Paz

Wang

et al. 2007

J. High Energy Phys.

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We present a new observable sensitive to a certain combination of CP violating phases in supersymmetric extensions of the Standard Model, viz. a triple product of momenta in the cascade decay of a heavy squark via an on-shell neutralino and off-shell slepton. We investigate the regions of parameter space in which the signal is strong enough to be detectable at the LHC with ∼ 10 2 −10 3 / sin 2 (2∆ϕ) identified events, where ∆ϕ is a certain combination of phases in the MSSM presented in the text.

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Collider Physics

Cited by 139 publications

References 8 publications

Dynamical parton distributions of the nucleon

Dynamical parton distributions of the nucleon

CP violation in top physics

A T-odd observable sensitive to CP violating phases in squark decay

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