scholarly journals Brief on Dark Matter in the Type Ib Seesaw Model: a GeV-scale Dirac neutrino portal

2022 ◽  
Author(s):  
Bowen Fu
2016 ◽  
Vol 93 (11) ◽  
Author(s):  
Takaaki Nomura ◽  
Hiroshi Okada ◽  
Yuta Orikasa
Keyword(s):  

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.


2014 ◽  
Vol 90 (4) ◽  
Author(s):  
Dean J. Robinson ◽  
Yuhsin Tsai
Keyword(s):  

2010 ◽  
Vol 82 (1) ◽  
Author(s):  
Daijiro Suematsu ◽  
Takashi Toma ◽  
Tetsuro Yoshida
Keyword(s):  

2018 ◽  
Vol 97 (7) ◽  
Author(s):  
Brian Batell ◽  
Tao Han ◽  
David McKeen ◽  
Barmak Shams Es Haghi
Keyword(s):  

2008 ◽  
Vol 2008 (05) ◽  
pp. 004 ◽  
Author(s):  
H Sung Cheon ◽  
Sin Kyu Kang ◽  
C S Kim
Keyword(s):  

1992 ◽  
Vol 07 (09) ◽  
pp. 2021-2031 ◽  
Author(s):  
ANJAN S. JOSHIPURA

A model for the 17 keV Dirac neutrino is considered in the framework of the SU(2) × U(1) theory. No right-handed neutrinos are introduced. The Dirac mass for the neutrino arises from the Le+Lτ–Lμ invariant couplings of the left-handed neutrinos to an SU(2) triplet. An SU(2) singlet field is introduced to suppress the Majoron coupling to the Z. This makes the model consistent with the LEP results on the invisible Z width. The singlet vacuum expectation value ω is constrained to be ≤O(80 MeV) from cosmological considerations. For, ω≈80 MeV, the 17 keV neutrino is shown to provide the bulk of the dark matter.


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