Is the following a matrix? (yes/no)

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Homework Help Overview

The discussion revolves around the classification of certain mathematical expressions involving Dirac matrices and differential operators, specifically in the context of whether they can be considered a matrix or a vector. The original poster presents identities and equations that involve these elements and seeks clarification on their nature.

Discussion Character

  • Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Participants explore the nature of the terms involved, questioning whether the expressions represent matrices or vectors. There is an examination of the roles of differential operators and one-forms in the context of vector contractions.

Discussion Status

Some participants have provided insights into the nature of one-forms and vector contractions, suggesting that the terms discussed yield scalars. Others have pointed out the role of Dirac matrices in the contractions, indicating a potential connection to matrix representations. The discussion is ongoing with various interpretations being explored.

Contextual Notes

The original poster expresses uncertainty regarding the notation and the implications of the mathematical expressions, indicating a need for further clarification on the definitions and properties of the involved elements.

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Homework Statement



Is the following a matrix?

Given: these identities (ordinarily in "Feynman slash notation": not sure how to do slashes in LaTeX):

[tex]\begin{array}{c}<br /> ({\gamma _\mu }{a^\mu }){\gamma _\nu }{b^\nu } + {\gamma _\nu }{b^\nu }({\gamma _\mu }{a^\mu }) \equiv 2{a_\mu }{b^\mu } \\ <br /> ({\gamma _\mu }{a^\mu })({\gamma _\mu }{a^\mu }) \equiv {a_\mu }{a^\mu } \\ <br /> \end{array}[/tex]

Homework Equations



[tex]({\gamma ^\mu }{\partial _\mu })({\gamma ^\nu }{A_\nu }) + ({\gamma ^\nu }{A_\nu })({\gamma ^\mu }{\partial _\mu }) =[/tex] ... a matrix or a vector?

The Attempt at a Solution



Maybe it is a matrix. My final answer needs a matrix answer (specifically: I need the field-strength tensor, [tex]F^{\mu, \nu}[/tex], to pop up eventually.

Maybe it isn't a matrix. The operator [tex]\partial _\mu[/tex] is a differential operator, and A is the four-vector-potential. that suggests I should wind up with a differentiated version of the field-strenght tensor, which would be awfully-boring in a certain gauge I forget the name of (it'd be zero/divergenceless, a la Griffiths Intro Elementary Particles, p. 239-240).

?
 
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\partial_{mu} is a one-form. Contracting a one-form with a vector yields a scalar. In fact, all your terms are one-form vector contractions.
 
Phrak said:
\partial_{mu} is a one-form. Contracting a one-form with a vector yields a scalar. In fact, all your terms are one-form vector contractions.

Oh dear...back to the drawing board...
 
Phrak said:
\partial_{mu} is a one-form. Contracting a one-form with a vector yields a scalar. In fact, all your terms are one-form vector contractions.
But [itex]\gamma^\mu[/itex] are the Dirac matrices, so the contraction [itex]\gamma^\mu A_\mu[/itex] is actually a linear combination of matrices.

http://en.wikipedia.org/wiki/Gamma_matrices
 
In which case the contraction yields the same type as the Dirac matrix.
 

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