Difference Between Weyl & Majorana Spinnors

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Discussion Overview

The discussion revolves around the differences between Weyl spinors and Majorana spinors, focusing on their definitions, properties, and mathematical representations. It includes theoretical aspects and mathematical reasoning related to spin-1/2 particles in quantum field theory.

Discussion Character

  • Technical explanation
  • Mathematical reasoning
  • Debate/contested

Main Points Raised

  • Some participants describe a Weyl spinor as a 4-component complex-valued spinor representing a spin-1/2 particle with an anti-particle, while a Majorana spinor is characterized as a real-valued spinor that is its own anti-particle.
  • Others clarify that Weyl fields consist of two-component spinors, and that Dirac and Majorana fields are constructed from these Weyl fields.
  • One participant notes that Weyl spinors can be purely right or left-handed, contrasting with Majorana spinors which are their own antiparticles.
  • A mathematical representation is provided for Weyl spinors, indicating that they describe right-moving and left-moving waves through uncoupled equations, while Majorana fields involve coupled equations introduced by a mass term in the Dirac Equation.
  • Another participant offers additional mathematical expressions for right and left-moving particles, emphasizing their respective representations in terms of derivatives.
  • A participant acknowledges a correction regarding an imaginary number in a previously stated equation related to Majorana fields.

Areas of Agreement / Disagreement

Participants express various perspectives on the definitions and properties of Weyl and Majorana spinors, indicating that multiple competing views remain without a consensus on certain aspects.

Contextual Notes

Some statements rely on specific definitions and assumptions about spinors and their mathematical representations, which may not be universally agreed upon. The discussion includes unresolved mathematical details and varying interpretations of the relationships between different types of spinors.

zaybu
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Can anyone explain to me what is the difference between a Weyl spinnor and a Majorana spinnor?

Thanks
 
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welcome to pf!

hi zaybu! welcome to pf! :smile:

a Weyl spinor (one "n" :wink:) is an ordinary 4-component complex-valued spinor representing a spin-1/2 particle like an electron which has an anti-particle

a Majorana spinor is a real-valued spinor representing a spin-1/2 particle which is its own anti-particle

for details, see page 95 ff. (page 102 of the .pdf) of David Tong's "Quantum Field Theory" at http://www.damtp.cam.ac.uk/user/tong/qft/qft.pdf" :wink:
 
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aren't Weyl fields two comp spinors? with the Dirac and Majorana fields are four comp being built up from two Weyl fields
 
A Weyl spinor is one that is purely right or left handed.
A Majorana spinor is one that is its own antiparticle.
 
LAHLH said:
aren't Weyl fields two comp spinors? with the Dirac and Majorana fields are four comp being built up from two Weyl fields

Yes, a 4-component spinor is make up of two 2-component spinors.
 
zaybu said:
Can anyone explain to me what is the difference between a Weyl spinnor and a Majorana spinnor?

Thanks

Weyl Spinors are when you have right moving and left moving waves, but are not coupled equations. For instance:

[tex]i\dot{\psi_R}=-i \partial_x \psi_R+M \psi_L[/tex]

described right moving waves. Left movers are described as thus:

[tex]i \dot{\psi_L}=+i \partial_x \psi_L+M \psi_R[/tex]

a Majorana field is a coupled equation, which happens when you introduce a mass term into the Dirac Equation:

[tex]i\dot{\psi}=-i \alpha \partial_x \psi + M\beta[/tex]
 
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Or if you like, Right moving particles are expressed as:

[tex]\frac{\partial \psi_R}{\partial t}=-\frac{\partial \psi_R}{\partial x}[/tex]

which represent right moving particles for (ω/k = +1).

Left moving particles are represented by:

[tex]\frac{\partial \psi_L}{\partial t}=+\frac{\partial \psi_L}{\partial x}[/tex]
 
I missed out an imaginary number in the coupled equation. I fixed this early this morning, I am surprised to see it still unfixed.

[tex]i\dot{\psi}=-i \alpha \partial_x \psi + M\beta[/tex]
 

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