• Aucun résultat trouvé

On a Singular Solution in Higgs Field (5) -The degenerates into the candidates for dark matter and dark energy from ur-Higgs bosons

N/A
N/A
Protected

Academic year: 2021

Partager "On a Singular Solution in Higgs Field (5) -The degenerates into the candidates for dark matter and dark energy from ur-Higgs bosons"

Copied!
2
0
0

Texte intégral

(1)

HAL Id: hal-01407441

https://hal.archives-ouvertes.fr/hal-01407441

Submitted on 2 Dec 2016

HAL is a multi-disciplinary open access archive for the deposit and dissemination of sci- entific research documents, whether they are pub- lished or not. The documents may come from teaching and research institutions in France or abroad, or from public or private research centers.

L’archive ouverte pluridisciplinaire HAL, est destinée au dépôt et à la diffusion de documents scientifiques de niveau recherche, publiés ou non, émanant des établissements d’enseignement et de recherche français ou étrangers, des laboratoires publics ou privés.

On a Singular Solution in Higgs Field (5) -The degenerates into the candidates for dark matter and

dark energy from ur-Higgs bosons

Kazuyoshi Kitazawa

To cite this version:

Kazuyoshi Kitazawa. On a Singular Solution in Higgs Field (5) -The degenerates into the candidates for dark matter and dark energy from ur-Higgs bosons. EPS HEP 2013 , Jul 2013, Stockholm, Sweden.

Astroparticle Physics. �hal-01407441�

(2)

“On a Singular Solution in Higgs Field (5) -The degenerates into the candidates for dark matter and dark energy from ur-Higgs bosons” Kazuyoshi KITAZAWA (RISP Japan)





 

     

     



   

   

       

   



     

    

 

 

 

  

 

    



 

  













  







 

 

 







 















 

 

         

   

 

    

  







 

 







 









   

       

 

  



  

  

    





     

 

 

 

 

      



  

  

 

  



   

    

  

 



 



 

  









   

 

    



   

 

    





  



 

      

 

 



 

  





 









    

  

 

   

 

 

  

 

            

 

   

 

 



 



 









    

  

 

  

 



   

    

  

    



 



 







 











 



 

  











 





 

 



 





 



 





 

 

  





  







 

 





 





 



   

 

 

 

       

   

  

 

      

    

 



 

  

 

 

  





 

   

 

  

 

 

 

    

 

   

 



 



 





  



       

   

  



    

  

  



 

 

 

 

   

  

  

 



 

䞉䞉䞉

Références

Documents relatifs

We find that the Abell Cluster A586 exhibits evidence of the interaction between dark matter and dark energy and argue that this interaction suggests evidence of violation of the

A formula for mass of Standard Model Higgs boson is derived by considering certain asymptotic behavior for singular solution of equation of motion (EOM) of Higgs field

Like most Higgs portal singlet models, the parameter space in this model is tightly constrained, mainly by direct detection experiments.. Yet, due to the nonlinear nature of the

In this model there is an EW singlet pNGB which has been studied as a composite scalar Dark Matter (DM) candidate in an effective theory approach [ 46 , 47 ], how- ever decays

Let us consider a spherical concentration of dark substance with a density in 1/r 2 (that we defined in previous sections) moving in the space. We could expect that its velocity

One can describe the virtual pairs forming and annihilating in quantum vac- uum – considered as a fundamental, scalar, quantum field – as vortex-antivortex pairs of vacuum’s quanta,

Several astronomical observations, last decades, seems in contradiction with the classical laws of gravitation. For example, the curve of rotation of galaxies can’t be explain

In the case in which Universe is a sphere (or any finite convex volume with a finite surface) constituted of dark substance, we avoid the previous problem