Majorana particles and U(1) charges

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Discussion Overview

The discussion revolves around the nature of Majorana particles, particularly in relation to neutrinos and their charge properties under various symmetries, including U(1) electromagnetic symmetry. Participants explore the implications of Majorana mass terms and the conditions under which a particle can be its own antiparticle.

Discussion Character

  • Debate/contested
  • Technical explanation
  • Conceptual clarification

Main Points Raised

  • Some participants propose that Majorana particles cannot have any charge if they are to be their own antiparticles, as this would contradict the requirement for antiparticles to have opposite charges.
  • Others argue that a Majorana particle can carry charges under symmetries that are broken in the physical world, suggesting that the conservation of charge is violated only for certain additive charges.
  • A participant asserts that a Majorana mass term violates conservation of any additive charge that reverses under electromagnetic charge conjugation, but allows for charges that remain the same under charge conjugation and reverse under parity.
  • Another participant questions the implications of coupling Majorana fields to axial currents and the physical significance of such interactions, particularly regarding parity behavior.

Areas of Agreement / Disagreement

Participants express differing views on the charge properties of Majorana particles and the implications of Majorana mass terms. There is no consensus on whether Majorana particles can carry charges or the conditions under which this is permissible.

Contextual Notes

The discussion includes unresolved assumptions about the nature of charge conservation and the definitions of charge conjugation and parity in the context of Majorana particles.

krishna mohan
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Hi...

Recently read that neutrinos can be Majorana particles only because they are singlets under the unbroken U(1) electromagnetic..

I can understand that...Majorana means that the particle is its own antiparticle..this can't happen if it is charged, as the antiparticle should have the opposite charge as the particle...

Does this mean that a Majorana particle cannot have any charge? Or is it fine for it to have charges under symmetries which are broken in our world?


Krishna
 
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krishna mohan said:
Hi...

Recently read that neutrinos can be Majorana particles only because they are singlets under the unbroken U(1) electromagnetic..

I can understand that...Majorana means that the particle is its own antiparticle..this can't happen if it is charged, as the antiparticle should have the opposite charge as the particle...

Does this mean that a Majorana particle cannot have any charge? Or is it fine for it to have charges under symmetries which are broken in our world?


Krishna

A Majorana mass term explicitly violates the conservation of any additive charge. Therefore, the only charges that can be carried by a Majorana particle are those belonging to symmetry groups that are broken by the same physics that generates the Majorana mass.
 
A Majorana mass term explicitly violates the conservation of any additive charge. Therefore, the only charges that can be carried by a Majorana particle are those belonging to symmetry groups that are broken by the same physics that generates the Majorana mass.

This is wrong, A Majorana mass term stops conservation of any charge that reverses under electromagnetic charge conjugation, but is just fine if stays the same under C, but reverses under P, I've been looking at such an axial force for 5+ years, and still believe it is possible.
 
BDOA said:
This is wrong, A Majorana mass term stops conservation of any charge that reverses under electromagnetic charge conjugation, but is just fine if stays the same under C, but reverses under P, I've been looking at such an axial force for 5+ years, and still believe it is possible.

Several things. First, this thread is almost a year and a half old. Did you really just drag it up out of the ether to tell me I'm wrong?

Second, the charge conjugation that shows up in the definition of a Majorana field is pretty much defined to include all charges (conserved or not), not just EM.

Third, while I already knew that Majorana fields can couple to axial currents, I'm not really clear on the physical implications of what you're suggesting. Are you saying that you have an axial interaction that has the opposite sign behavior under parity than would be expected just from the action of the parity operator on an axial current?
 

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