Version 8 (modified by CP3Origins, 10 years ago) (diff) 

Technicolor
Authors
 Matti Järvinen ( mjarvine @ physics.uoc.gr )
 Tuomas Hapola ( hapola @ cp3.sdu.dk )
 Eugenio Del Nobile ( delnobile @ cp3.sdu.dk )
 Claudio Pica ( pica @ cp3.sdu.dk )
An earlier implementation of this model on LanHEP was written by M. Frandsen, R. Foadi, M. Järvinen.
Description of the model
We have implemented the simplest of the recently identified walking technicolor models, which can pass the electroweak precision tests.
 Minimal Walking Technicolor (MWT) is an extension of the Standard Model featuring a new strong sector based on a new gauge group SU(2) technicolor with a doublet of Dirac fermions in the adjoint representation.
 Next to Minimal Walking Technicolor (NMWT) is a similar extension, but based on the gauge group SU(3) technicolor with a doublet of Dirac fermions in the twoindex symmetric representation.
Our implementation makes use of the effective lowenergy model containing scalars, pseudoscalars, vector mesons and other fields predicted by the models. The implemented model is the simplest one, which contains only the composite states, which are expected to be the most important for collider phenomenology. These are the composite Higgs, and the vector and axial spinone resonances. For these states the effective theories of MWT and NMWT coincide.
References
The most relevant references for this model implementation are:
 Phys. Rev. D 71, 051901 (2005) http://arxiv.org/abs/hepph/0405209  F. Sannino and K. Tuominen, Orientifold Theory Dynamics and Symmetry Breaking. Note that the original name was Techniorientifold.
 Phys. Rev. D 76, 055005 ( 2007) http://arxiv.org/abs/0706.1696  R. Foadi, M.T. Frandsen, T. A. Ryttov, F. Sannino, Minimal Walking Technicolor: Set Up for Collider Physics. This article derives the effective theory for MWT.
 Phys. Rev. D 79, 035006 (2009) http://arxiv.org/abs/0809.0793 – A. Belyaev, R. Foadi, M.T. Frandsen, M. Jarvinen, A. Pukhov, F. Sannino, Technicolor Walks at the LHC. This article presents the Lagrangian used in this implementation, and analyses LHC phenomenology by using the earlier LanHEP implementation.
See also:
 Phys. Lett. B597:8993,2004 http://arxiv.org/abs/hepph/0406200  Deog Ki Hong, Stephen D.H. Hsu, F. Sannino, Composite Higgs from higher representations.
 Phys. Rev. D72:055001, 2005 http://arxiv.org/abs/hepph/0505059  D.D. Dietrich, F. Sannino, K. Tuominen Light composite Higgs from higher representations versus electroweak precision measurements: Predictions for CERN LHC.
 Phys. Rev. D 75, 085018 (2007) http://arxiv.org/abs/hepph/0611341  D. D. Dietrich and F. Sannino, Conformal window of SU(N) gauge theories with fermions in higher dimensional representations. Note that the original name was Walking in the SU(N).
 For the construction at the Lagrangian level of the terms involving the spacetime epsilon tensor – representing the correct generalization of the WessZuminoWitten topological term – involving massive spin one fields see Acta Phys. Polon. B40:35333743, 2009.
 http://arxiv.org/abs/0911.0931 – F. Sannino, Conformal Dynamics for TeV Physics and Cosmology.
Model files and extensions
 AAAAAAAAA.fr is the main FeynRules file.
 BBBBBBBBB.nb is a Mathematica® notebook that can be used to load the MWT FeynRules model.
 CCCCCCCCC.fr is an extension introducing the effective coupling Hgg (Higgs + two nonabelian gauge bosons) arising at loop level.
Interfaces and related files
 CalcHEP: ch.tgz (12.06.09), sps1a.ch.tgz (08.07.09).
 MadGraph: mg.tgz (12.06.09), sps1a.mg.tgz (05.07.09).
 the calculator needed in MadGraph in order to generate the param_card.dat for a different set of model parameters.
Instructions and details
The model file is loaded as usual. The attached Mathematica® notebook can be used for this task.
The calculator is needed by the MadGraph implementation in order to change the parameters of the model. The directory is provided by a README file with the instructions on the usage. ...Say something about Tuomas HGG
The model file implements a (linear) effective theory for the spinzero and spinone sectors in technicolor, with the minimal SU(2)_{L} x SU(2)_{R} > SU(2)_{V} chiral symmetry breaking pattern. The strong technicolor interactions is linked to the electroweak sector as stipulated by the electroweak gauge transformations of the techniquarks. The modifications to the effective theory due to the electroweak interactions are mostly small. The composite scalar sector contains the composite Higgs boson and a triplet of massless technipions, which are eaten by the heavy gauge boson Z and W. The Higgs is expected to be relatively light (mass less than 500 GeV). We also have vector and axial spinone triplets, which mix with each other and with the electroweak gauge bosons.
In addition to the standard model fermions, we thus have the following new particles:
 Composite Higgs scalar H
 Neutral heavy vector R_{1}^{0}
 Charged heavy vector R_{1}^{+}, R_{1}^{}
 Neutral heavy vector R_{2}^{0}
 Charged heavy vector R_{2}^{+}, R_{2}^{}
The numbering convention for the heavy spinone states is such that R_{1} is always the lighter one. When the mass scale is below 1 TeV R_{1} (R_{2}) has larger component of the axial (vector) spinone composite state than of the vector (axial) state. When masses are increased to about 2 TeV, the situation is reversed.
Using the effective theory introduces several new coupling constants. These can be constrained by linking to the underlying gauge theory via the Weinberg sum rules and the definition of the electroweak S parameter. After taking into account the Weinberg sum rules, the free parameters can be expressed in terms of:
 MA: The spinone mass scale. More precisely, the mass of the axial spinone state in the limit where the electroweak interactions are turned off. Allowed range is from about 500 GeV to about 3 TeV, depending on the values of other parameters.
 gt: The effective strength of technicolor interactions. Parametrizes the corrections of the electroweak interactions to the technicolor sector, which are typically O(g/gt), with g being the weak coupling constant. In particular, the mixing of the composite spinone states with the electroweak gauge bosons, and therefore also the coupling of the composite spinone states to the standard model fermions, is O(g/gt). Allowed values range from about 1 to about 10.
 S: The (contribution of the lowest spinone states to the) S parameter. Recommended values come from naive estimates of the S parameter (calculation of techniquark loops), which gives S=0.15 for MWT and S=0.3 for NMWT.
 MH: The mass of the composite Higgs boson.
 rs: Parametrizes the couplings of the Higgs to the composite spinone states. Expected to be O(1).
The implementation supports unitary gauge. The standard model section has only Cabibbo mixing, and the electron and the muon, as well as the up, down and strange quarks, are taken to be massless.
Validation
The implementation of the following MWTC processes through the FeynRules interface was crosschecked with the already existing implementation in LanHEP (see references):
 pp > jj at 1400 GeV
 pp > mu+mu at 1400 GeV
Furthermore, the matrix element generated for qq~>mu+mu was checked by hand for a few phase space points.
Toumas also crosschecked some associate production processes (i.e. Wstrahlung from technirho)
Attachments (7)

MWT_ch.zip
(14.3 KB) 
added by CP3Origins 10 years ago.
CalcHEP model files

MWT_101030.nb
(92.6 KB) 
added by CP3Origins 10 years ago.
Mathematica notebook for the MWT FeynRules file

MWT_101030.fr
(30.9 KB) 
added by CP3Origins 10 years ago.
MWT FeynRules file

HiggsEffective.fr
(612 bytes) 
added by CP3Origins 10 years ago.
Higgsgluongluon effective vertex FeynRules file

MWT_Calculator.zip
(11.2 KB) 
added by CP3Origins 10 years ago.
Calculator for MadGraph

MWT_HEC_Calculator.zip
(11.9 KB) 
added by CP3Origins 10 years ago.
MadGraph calculator extended for the Higgsgluongluon effective coupling

MWT_mg.zip
(36.7 KB) 
added by CP3Origins 10 years ago.
MadGraph model folder
Download all attachments as: .zip