Science-advisor
REGISTER info/FAQ
Login
username
password
     
forgot password?
register here
 
Research articles
  search articles
  reviews guidelines
  reviews
  articles index
My Pages
my alerts
  my messages
  my reviews
  my favorites
 
 
Stat
Members: 3645
Articles: 2'503'724
Articles rated: 2609

24 April 2024
 
  » arxiv » 1509.4096

 Article overview


Checking T and CPT violation with sterile neutrino
Yogita Pant ; Sujata Diwakar ; Jyotsna Singh ; R.B. Singh ;
Date 14 Sep 2015
AbstractPost LSND results, sterile neutrinos have drawn attention and motivated the high energy physics, astronomy and cosmology to probe physics beyond the standard model considering minimal 3+1 (3 active and 1 sterile) to 3+N neutrino schemes. The analytical equations for neutrino conversion probabilities are devloped in this work for 3+1 neutrino scheme. Here we have tried to explore the possible signals of T and CPT violations with four flavor neutrino scheme at neutrino factory. To investigate the T violation we have taken into consideration the golden and discovery channels. In our analysis the optimal values of Jarlskog factor for discovery channel coming from the constrained values of sterile parameters from long baseline and short baseline experiments are 0.169 and 0.163 respectively. Whereas the values of Jarlskog factor for golden channel are 0.0131 and 0.0143 coming from long and short baseline constraints respectively. This obesrevation promotes discovery channel to be the potential channel for probing T violation in 3+1 neutrino scheme. The CPT violation is checked for the disappearance channel. We have pointed out the obeservables which can distangle the sterile contribution from the rest of the contributing factors in any observation. These observables promote setup with baselines beyond 4000 km and energy range 9-12 GeV to check CPT violation. We find that to observe CPT violation at 90\% C.L., the product of sterile angles $ heta_{24} $ and $ heta_{34} $ can be constrained as $ heta_{24}. heta_{34}gtrsim 0.006$ $rad^{2}$ with liquid argon detector and with magnetized iron detector the constraint imposed is $ heta_{24}. heta_{34}gtrsim 0.007$ $rad^{2}$.
Source arXiv, 1509.4096
Services Forum | Review | PDF | Favorites   
 
Visitor rating: did you like this article? no 1   2   3   4   5   yes

No review found.
 Did you like this article?

This article or document is ...
important:
of broad interest:
readable:
new:
correct:
Global appreciation:

  Note: answers to reviews or questions about the article must be posted in the forum section.
Authors are not allowed to review their own article. They can use the forum section.

browser Mozilla/5.0 AppleWebKit/537.36 (KHTML, like Gecko; compatible; ClaudeBot/1.0; +claudebot@anthropic.com)






ScienXe.org
» my Online CV
» Free


News, job offers and information for researchers and scientists:
home  |  contact  |  terms of use  |  sitemap
Copyright © 2005-2024 - Scimetrica