Mikael Chala, DISCRETE 2014, London
Mikael Chala (DESY) & Francisco del Águila (UGR)
Based on JHEP 1403 (2014) 027, Phys.Lett. B725 (2013) 310
Lepton number violation in non-standard Higgs sectors Mikael Chala - - PowerPoint PPT Presentation
Lepton number violation in non-standard Higgs sectors Mikael Chala (DESY) & Francisco del guila (UGR) Based on JHEP 1403 (2014) 027, Phys.Lett. B725 (2013) 310 Mikael Chala, DISCRETE 2014, London The discovery of the Higgs boson shows a
Mikael Chala, DISCRETE 2014, London
Based on JHEP 1403 (2014) 027, Phys.Lett. B725 (2013) 310
Alex Pomarol, CPAN 2014
Mikael Chala, DISCRETE 2014, London
Planck scale
TeV scale EW scale
Many orders of magnitude
Mikael Chala, DISCRETE 2014, London
Planck scale
TeV scale EW scale
Mikael Chala, DISCRETE 2014, London
Planck scale
TeV scale EW scale
Mikael Chala, DISCRETE 2014, London
Planck scale
TeV scale EW scale
Mikael Chala, DISCRETE 2014, London
Planck scale
TeV scale EW scale
Mikael Chala, DISCRETE 2014, London
About Lepton Number Violation
Accidental from gauge symmetry Majorana neutrinos...
Where to look for LN violation? decay Testable at the LHC?
Mikael Chala, DISCRETE 2014, London
Planck scale
TeV scale EW scale
Natural assumption Mikael Chala, DISCRETE 2014, London
Planck scale
TeV scale EW scale
Natural assumption Mikael Chala, DISCRETE 2014, London
Planck scale
TeV scale EW scale
Natural assumption
See for instance del Águila et al, 1204.5986; del Águila et al, 1111.6960
Mikael Chala, DISCRETE 2014, London
Can LNV scalar interactions be observed at the LHC? A generic approach to LNV scalars
Mikael Chala, DISCRETE 2014, London
LNV extensions of the SM can accommodate neutrino Majorana masses Only three scalar fields at the renormalizable level
Mikael Chala, DISCRETE 2014, London
Experiment scale
Different doubly-charged scalar at a lower scale can mix with
LNV extensions of the SM can accommodate neutrino Majorana masses Only three scalar fields at the renormalizable level
Mikael Chala, DISCRETE 2014, London
After integrating out scale, higher multiplets ( ) couple to same-sign leptons via Yukawa-like interactions
Mikael Chala, DISCRETE 2014, London
After integrating out scale, higher multiplets ( ) couple to same-sign leptons via Yukawa-like interactions
and suppressed by powers of Mikael Chala, DISCRETE 2014, London
What is the phenomenology of these scalars? VS What current analyses assume (see-saw II)?
ATLAS
E u r . P h y s . J
C72-2244
CMS
E u r . P h y s . J
C72-2189
Mikael Chala, DISCRETE 2014, London
Using current CMS three- and four-lepton analyses, set bounds on LNV processes mediated by doubly-charged scalars Mikael Chala, DISCRETE 2014, London
Mikael Chala, DISCRETE 2014, London
Mikael Chala, DISCRETE 2014, London
Mikael Chala, DISCRETE 2014, London
Mikael Chala, DISCRETE 2014, London
Using current CMS three- and four-lepton analyses, set bounds on LNV processes mediated by doubly-charged scalars Mikael Chala, DISCRETE 2014, London
Using current CMS three- and four-lepton analyses, set bounds on LNV processes mediated by doubly-charged scalars Mikael Chala, DISCRETE 2014, London
(see also King, Merle and Panizzi, arXiv:1406.4137)
E f f i c i e n c i e s i n %
Can we discriminate among the different multiplets? LNV can be very difficult to be established at the LHC But doubly-charged scalars can be still present Discrimination is possible if two-body decays dominate
Measure the neutral cross section using four-lepton events
arXiv:1305.3904
Mikael Chala, DISCRETE 2014, London
Mikael Chala, DISCRETE 2014, London
Mikael Chala, DISCRETE 2014, London
Mikael Chala, DISCRETE 2014, London
Mikael Chala, DISCRETE 2014, London
How well can we discriminate among the different multiplets?
14 TeV, L = 100, 300, 3000/fb
leptons
and taus
and Ws
taus and Ws
Águila, MC, Santamaría, Wudka, '13
Mikael Chala, DISCRETE 2014, London
Can be a background of
Mikael Chala, DISCRETE 2014, London
Charged signals VS neutral current backgrounds
mainly signal
Mikael Chala, DISCRETE 2014, London
Mikael Chala, DISCRETE 2014, London
The SM describes nature to a very good accuracy, although there are still open questions: neutrino masses LNV scalar interactions can be very difficult to be proved at the LHC For the first time, bounds on LNV scalar interactions, and many other channels
Even if no LNV, doubly-charged scalars can be distinguished in a large run of LHC
Mikael Chala, DISCRETE 2014, London
What do we know on neutrino masses? Quantum numbers
Singlet!
Neutrinos can be Majorana
Other fermions are charged, so they can not be self-conjugated
Mikael Chala, DISCRETE 2014, London
Mikael Chala, DISCRETE 2014, London
Using current CMS three- and four-lepton analyses, bound non-LNV processes mediated by doubly-charged scalars Mikael Chala, DISCRETE 2014, London
Mikael Chala, DISCRETE 2014, London