Spin group for the Weyl equation

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In summary, the "Spin group for the Weyl equation" discusses the mathematical framework surrounding the Weyl equation, which describes massless fermions in quantum mechanics. It focuses on the role of the spin group, particularly the representations of the group that correspond to the behavior of these particles. The spin group encapsulates the symmetry properties of the Weyl equation, allowing for a deeper understanding of the underlying physical phenomena, including chirality and the transformation of fermionic states. This exploration highlights the connection between group theory and quantum field theory, offering insights into the fundamental aspects of particle physics.
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TL;DR Summary
What is the spin group classification for Weyl particles?
I never considered this until now. Dirac particles have a spin representation of ##(1/2,0) \oplus (0,1/2)##. This represents both parts of the 4-spinor. But what is the representation of Weyl particles? Is it still ##(1/2,0) \oplus (0,1/2)## or is it just (1/2,0), since we have a definite helicity?

Thanks!

-Dan

Addendum: I'm going to add to this. The question about helicity may be a bit of a red herring: the photon is ##(1,0) \oplus (0,1)##, which covers both A and B subAlgebras. But Proca particles are (1/2, 1/2). I'm not sure what to do about the m = 0 case for Dirac particles.
 
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topsquark said:
TL;DR Summary: What is the spin group classification for Weyl particles?

I never considered this until now. Dirac particles have a spin representation of ##(1/2,0) \oplus (0,1/2)##. This represents both parts of the 4-spinor. But what is the representation of Weyl particles? Is it still ##(1/2,0) \oplus (0,1/2)## or is it just (1/2,0), since we have a definite helicity?

Thanks!

-Dan

Addendum: I'm going to add to this. The question about helicity may be a bit of a red herring: the photon is ##(1,0) \oplus (0,1)##, which covers both A and B subAlgebras. But Proca particles are (1/2, 1/2). I'm not sure what to do about the m = 0 case for Dirac particles.
After pondering some more I think the only conclusion that I can draw is that the Weyl representation of the Poincare Algebra must be ##(1/2,0) \oplus (0.1/2)##, just like the Dirac representation.

Mathematically, the groups A and B are independent, so if the spin representations aren't the same we need to add equivalent (but switched) groups to make it symmetric. The reason the Proca and Maxwell representations are different is due to the fact that the Maxwell representation admits no spin 0 (well, helicity 0) particles, so we need to change it. The spins of the Weyl particles are not actually restricted, they are just fixed to particles/antiparticles. But the m = 0 condition doesn't actually change the wave equation, so it shouldn't change the Lagrangian, so it shouldn't change the representation, either.

I'm not completely satisfied with this answer. My logic chain only works in one direction: I don't know how to derive this result from first principles, but it may simply be that the extra condition on Weyl particles does not affect the representation we are using, which does make some sense to me.

-Dan
 

FAQ: Spin group for the Weyl equation

What is the Spin Group in the context of the Weyl equation?

The Spin group, denoted as Spin(n), is a mathematical concept that arises in the study of spinors and the Clifford algebra associated with a given space. In the context of the Weyl equation, which describes massless spin-1/2 particles like neutrinos, the Spin group provides the necessary framework to understand the symmetries and transformations of the spinors that are solutions to the equation.

How does the Spin group relate to the Lorentz group in the Weyl equation?

The Spin group is the double cover of the special orthogonal group SO(n), which means it is closely related to the Lorentz group, particularly in 3+1 dimensions. For the Weyl equation, which deals with massless particles, the relevant Spin group is Spin(3,1), which covers the Lorentz group SO(3,1). This relationship allows for a more detailed understanding of how spinors transform under Lorentz transformations.

Why is the Spin group important for understanding the Weyl equation?

The Spin group is crucial for understanding the Weyl equation because it provides the mathematical structure needed to describe the spin-1/2 particles. Spinors, which are the solutions to the Weyl equation, transform under the Spin group rather than the Lorentz group directly. This distinction is important for accurately describing the behavior of these particles under rotations and boosts.

What role do spinors play in the Weyl equation?

Spinors are the fundamental objects in the Weyl equation, representing the quantum states of massless spin-1/2 particles. They are elements of a complex vector space that transforms under the Spin group. The Weyl equation itself is a first-order differential equation that governs the dynamics of these spinors, making them central to the equation's formulation and solutions.

Can the Spin group be generalized to higher dimensions for the Weyl equation?

Yes, the concept of the Spin group can be generalized to higher dimensions, and this generalization is important for theories that extend beyond the standard 3+1 dimensional spacetime. In higher dimensions, the relevant Spin group would be Spin(p,q) for a spacetime with p spatial dimensions and q temporal dimensions. This generalization allows for the study of spinors and the Weyl equation in various dimensional frameworks, which is particularly useful in theoretical physics and string theory.

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