The Dirac equation in Weyl representation

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Homework Help Overview

The discussion revolves around computing the antiparticle spinor solutions of the free Dirac equation in the Weyl representation. Participants are examining the Dirac matrices and their implications for the energy-momentum relation.

Discussion Character

  • Exploratory, Assumption checking, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the correct form of the Dirac matrices in the Weyl representation and question the sign conventions used for the Minkowski metric. There are attempts to clarify the placement of terms in the Dirac equation and how they relate to the matrix elements.

Discussion Status

The discussion has seen participants identifying errors in their initial setups, particularly regarding the sign in the gamma matrices and the treatment of the mass term. Some guidance has been provided on how to correctly interpret the momentum terms and their signs.

Contextual Notes

There is mention of varying sign conventions for the Minkowski metric, which may affect the interpretation of the components involved. Participants are also navigating their comfort with LaTeX formatting in their explanations.

Milsomonk
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Homework Statement


Compute the antiparticle spinor solutions of the free Dirac equation whilst working in the Weyl representation.

Homework Equations


Dirac equation
$$(\gamma^\mu P_\mu +m)v_{(p)}=0$$
Dirac matrices in the Weyl representation
$$

\gamma^\mu=
\begin{bmatrix}
0 & \sigma^i \\
-\sigma^i & 0
\end{bmatrix}, \
\gamma^0=
\begin{bmatrix}
0 & I \\
-I & 0
\end{bmatrix}
$$

The Attempt at a Solution


I have worked through the algebra numerous times but I can't seem to get the correct energy momentum relation out, my workings are attached, apologies I'm not too strong with Latex yet. Any ideas on where I may be going wrong would be greatly appreciated :)
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Milsomonk said:
$$

\gamma^\mu=
\begin{bmatrix}
0 & \sigma^i \\
-\sigma^i & 0
\end{bmatrix}, \
\gamma^0=
\begin{bmatrix}
0 & I \\
-I & 0
\end{bmatrix}
$$
Are you sure you have the correct form for ##\gamma^0## in the Weyl representation?

Also, you haven't specified the sign convention that you are using for the Minkowski metric: (1, -1, -1, -1) or (-1, 1, 1, 1). The choice will determine which components of a 4-vector change sign when raising or lowering an index.
 
Ah somehow I managed to shove a minus sign in the gamma zero matrix that shouldn't be there. Also, sorry, I'm using mostly minus :). I have tried again with the correct matrices but I'm having a similar issue...
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How did you get E+m in the locations indicated below?
upload_2017-11-20_11-17-9.png


Another thing to consider. For most people, the vector ##\vec p## would denote the 3-vector with contravariant components ##(p^1, p^2, p^3)##. So, for example, ##\gamma^1 p_1 = \gamma^1 (-p^1) = -\gamma^1 p^1##.
 

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Hi,
Its just the mass term from the Dirac equation which I have to add to each matrix element, unless I've done something daft. Ah so my momentum terms should have an overall change of sign?
 
Milsomonk said:
Hi,
Its just the mass term from the Dirac equation which I have to add to each matrix element, unless I've done something daft.
You don't want to add m to all the matrix elements. You should think of m in the Dirac equation as multiplied by the unit matrix.

Ah so my momentum terms should have an overall change of sign?
Yes.
 
Thanks very much for your help :) Looks like I have the correct solution now.
 
OK. Good work.
 

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