Right-Handed Neutrinos: Interactions & Weight Explained

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SUMMARY

Right-handed neutrinos, if they exist, are hypothesized to be heavier than left-handed neutrinos and are considered standard model singlets. The introduction of right-handed neutrinos allows for the formulation of a Majorana mass term, which is essential for explaining the light masses of neutrinos through the seesaw mechanism. Right-handed neutrinos do not interact with Z-bosons directly; however, they exhibit a small mixing with light neutrinos due to the Yukawa term, leading to suppressed interactions. Detecting these interactions remains a challenge, as producing right-handed neutrinos is currently beyond experimental capabilities.

PREREQUISITES
  • Understanding of Majorana mass terms in particle physics
  • Familiarity with the seesaw mechanism for neutrino mass generation
  • Knowledge of Z-boson interactions and Yukawa coupling
  • Basic concepts of particle production in high-energy physics experiments
NEXT STEPS
  • Research the implications of the seesaw mechanism on neutrino mass scales
  • Study the role of Yukawa terms in particle interactions
  • Explore current experimental techniques for detecting heavy neutrinos
  • Investigate the concept of leptogenesis and its relation to baryon asymmetry
USEFUL FOR

Particle physicists, researchers in neutrino physics, and anyone interested in the theoretical implications of right-handed neutrinos and their interactions.

bsaucer
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I've read that if right-handed neutrinos exist, they should be heavier than left-handed neutrinos (why?). I figured if an observer moves faster than a left-handed neutrino, he'd see it as right-handed. Also, would right-handed neutrinos interact with Z-bosons? How would such interactions be detected?
 
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bsaucer said:
I've read that if right-handed neutrinos exist, they should be heavier than left-handed neutrinos (why?).
Right handed neutrinos are standard model singlets. As soon as you add them to your model, there is nothing stopping you from writing down a Majorana mass term for them. A priori, you have no handle on what this mass should be - it is a new scale in your theory. To put it very large is popular for several reasons, among them explaining the light masses of neutrinos through the seesaw mechanism, but by no means is this a necessary requirement.

bsaucer said:
I figured if an observer moves faster than a left-handed neutrino, he'd see it as right-handed.
This is quite a bit of over-simplification. Suffice to say, if you do this for a Majorana neutrino, you will obtain a right handed anti-neutrino.

bsaucer said:
Also, would right-handed neutrinos interact with Z-bosons? How would such interactions be detected?
No. However, since there would be an ever so small mixing with the light neutrinos due to the Yukawa term, the actual physical state with definite mass will have a Z interaction suppressed by the mixing squared. The interaction with the W, or with the Z and a light neutrino, would be linearly suppressed by the mixing and cause decays of the heavy states. This is the main mechanism behind leptogenesis, which is a proposed solution to the baryon asymmetry.

In order to test the interactions of the right handed neutrinos directly, you would have to produce them. This is far beyond current experimental limits for most viable models.
 

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