scholarly journals TeV Scale Seesaw Model, Scalar Dark Matter and Electroweak Vacuum Stability

2019 ◽  
Author(s):  
Srubabati Goswami ◽  
Ila Garg ◽  
Vishnudath. K.N. ◽  
Najimuddin Khan
2020 ◽  
Vol 101 (5) ◽  
Author(s):  
Arindam Das ◽  
Srubabati Goswami ◽  
Vishnudath K. N. ◽  
Takaaki Nomura

2020 ◽  
Vol 102 (7) ◽  
Author(s):  
Debasish Borah ◽  
Rishav Roshan ◽  
Arunansu Sil
Keyword(s):  

2018 ◽  
Vol 97 (7) ◽  
Author(s):  
Purusottam Ghosh ◽  
Abhijit Kumar Saha ◽  
Arunansu Sil

2021 ◽  
Vol 81 (9) ◽  
Author(s):  
Mark D. Goodsell ◽  
Rhea Moutafis

AbstractWe describe the automation of the calculation of perturbative unitarity constraints including scalars that have colour charges, and its release in . We apply this, along with vacuum stability constraints, to a simple dark matter model with colourful mediators and interesting decays, and show how it leads to a bound on a thermal relic dark matter mass well below the classic Griest-Kamionkowski limit.


2016 ◽  
Vol 93 (11) ◽  
Author(s):  
Takaaki Nomura ◽  
Hiroshi Okada ◽  
Yuta Orikasa
Keyword(s):  

2014 ◽  
Vol 89 (1) ◽  
Author(s):  
Emidio Gabrielli ◽  
Matti Heikinheimo ◽  
Kristjan Kannike ◽  
Antonio Racioppi ◽  
Martti Raidal ◽  
...  

2007 ◽  
Vol 16 (05) ◽  
pp. 1541-1556
Author(s):  
HIROSHI OKADA

It is now clear that the masses of the neutrino sector are much lighter than those of the other three sectors. Canonial seesaw model would be the most famous for the above explanation. But one must introduce heavy particles that will not be able to observed with present scientific technologies. On the other hand, there are many attempts to explain the neutrino masses radiatively by means of inert Higgses, which do not have the vacuum expectation values. Then one can discuss cold dark matter candidates, because of no needing so heavy particles. The most famous work would be the Zee model17. Recently a new type model (hep-ph/0601225)4 along this line of thought was proposed by E. Ma. We adopted this idea, and then we introduced a new flavor symmetry to constrain the Yukawa sector. So our model might be more predictive, and can be investigated at LHC. I will present how we can obserb the particular signal at LHC, and what we can predict about the neutrino sector.


Sign in / Sign up

Export Citation Format

Share Document