Title: Model independent FCNC top physics at the LHC
1Model independent FCNC top physics at the LHC
- Pedro Ferreira
- ISEL e CFTC, Universidade de Lisboa
Jornadas do LIP 2008, 12/1/08
2THE WORK
- P. M. Ferreira, O. Oliveira and R. Santos,
PHYSICAL REVIEW D 73, 034011 (2006) - P. M. Ferreira and R. Santos, PHYSICAL REVIEW D
73, 054025 (2006) - P. M. Ferreira and R. Santos, PHYSICAL REVIEW D
74, 014006 (2006) - P. M. Ferreira, R. B. Guedes and R. Santos,
PHYSICAL REVIEW D 75, 055015 (2007) - Contribution to the Yellow Report for the CERN
Workshop Flavour in the Era of the LHC (2007)
(in the arXiv on Monday!) - Two more being produced as we speak
3 ProjectsPOCI/FP/81950/2007
PTDC/FIS/70156/2006POCI/FP/63926/2005POCI/FP/63
420/2005POCTI/FIS/59741/2004PDCTI/FP/FNU/50155/2
003
THE TEAM
People Juan Aguilar-Saavedra, Augusto Barroso,
João Bastos, João Carvalho, Matilde Castanheira,
Nuno Castro, Pedro Ferreira, Miguel Fiolhais,
Agostinho Gomes, Renato Guedes, Amélia Maio,
Paulo Martins, Rita Monteiro, Miguel Oliveira,
Orlando Oliveira, Sancho Oliveira, António
Onofre, Rui Santos, Sergey Slabospitsky, Filipe
Veloso, Helmut Wolters, Miguel Won.
4top FCNCcombination
THE CONNECTIONS
Granada
Southampton
tbW measurements(BSM physics)
NExT
tbW measurements
CFTC
LIP
RAL
Generators, tbW physics
RHUL LONDON
Valencia
5EFFECTIVE OPERATOR FORMALISM
- New physics generated in extensions of the
standard model would manifest itself at lower
energy scales in the form of effective operators
of dimension superior to 4. - Complete list of dimension 5 and 6 effective
operators Buchmüller e Wyler, Nucl. Phys. B268
(1986) 621. - Dimension 5 operators violate baryon/lepton
number.
Dimension 6 operators a great many of them.
We are interested in processes of single top
production via flavour changing neutral currents
(FCNCs) at the LHC.
6EFFECTIVE OPERATOR FORMALISM
All terms are invariant under the SM gauge group
? is the energy scale of new physics. This
formalism allows us to make predictions in a
model-independent manner.
- To select among the many dimension 6 terms, we
employed some physical selection criteria - The operators must contribute to FCNCs
involving the top quark and the strong
interaction, with impact on single top
production. - They must not have sizeable contributions to
physics below the TeV scale, so as to not ruin
the successful predictions of the SM.
7Strong FCNC contributions decays t ? q g, with
q u, c.
8Weak FCNC contributions decays t ? q Z and t ?
q ?
9RESULTS
We found a direct proportionality between the
cross sections of several FCNC processes and the
FCNC Branching ratios. For instance, for single
top production of a top quark at the LHC (in
picobarn)
10RESULTS
In the SM, BR(t?cg) 10-12 In other models, it
can reach BR(t?cg) 10-4
11The branching ratios of t ? q Z and t ? q ? are
related
12RESULTS FOR t ? PRODUCTION
Analysing the combined effects of FCNC in the
strong and weak sector yields information on the
sum of the branching ratios.
13DIFFERENTIAL CROSS SECTIONS ALLOW TO DISTINGUISH
STRONG AND WEAK FCNC CONTRIBUTIONS
14THE FUTURE
- Continue (and survive) the fruitful
collaboration between theoreticians and
experimentalists. - Top gluon FCNC interactions have been introduced
in an event generator (latest version of TopReX).
We wish to implement ALL FCNC interactions in
generators and study their effects in LHC
physics. - Publish loads of very nice papers
15NEXT THEORETICIANS EXPERIMENTALISTS PAPER