Trying to Make a (p[slash])^2 operator - is this right?

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The discussion focuses on the calculation of the Feynman slash notation operator p[slash]p[slash] and its implications in matrix multiplication. It highlights that Maple struggles with this notation and emphasizes the need to consider the symmetry of the operator in terms of d^mu and d^nu. A key point is that p[slash]^2 can be expressed in a symmetric form, allowing for simplifications in the calculations. The conversation also clarifies that symmetry refers to the equality of the product when the order of the derivatives is swapped. The participants conclude that understanding these properties is crucial for correctly manipulating the operator.
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Homework Statement



Find out what p[slash]p[slash] is (Feynman slash-notation), because Maple doesn't like it when you feed it p[slash]p[slash], and let it uber-"FOIL" out the (four non-commuting terms) x (four non-commuting terms), where the "x" denotes plain Jane matrix-multiplication.

Homework Equations


\begin{array}{c}<br /> [{\partial _\mu },{\gamma _\nu }] \equiv 0 \\ <br /> {\gamma _0}^2 = - {\gamma _i}^2 \equiv {\bf{I}} \\ <br /> \end{array}

The Attempt at a Solution



\begin{array}{c}<br /> {p_{{\rm{slash}}}}{p_{{\rm{slash}}}} = - ({\gamma _\mu }{\partial ^\mu })({\gamma _\nu }{\partial ^\nu }) \\ <br /> = - \left( {{\gamma _0}{\partial ^0} - \vec \gamma \bullet \vec \partial } \right)\left( {{\gamma _0}{\partial ^0} - \vec \gamma \bullet \vec \partial } \right) \\ <br /> = - \left( {{\gamma _0}^2{{({\partial ^0})}^2} + (\vec \gamma \bullet \vec \gamma ){\nabla ^2} - 2({\gamma _0}{\partial ^0})(\vec \gamma \bullet \vec \partial )} \right) \\ <br /> {p_{{\rm{slash}}}}{p_{{\rm{slash}}}} = - \left( {({\bf{I}}){{({\partial ^0})}^2} + ( - 3{\bf{I}}){\nabla ^2} - 2({\gamma _0}{\partial ^0})(\vec \gamma \bullet \vec \partial )} \right) \\ <br /> \end{array}
 
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sorry! LaTeX is bad.
 
bjnartowt said:
sorry! LaTeX is bad.

Um...writing text below the thread-start actually fixed the problem :-P
 
No, it is not right. To get the right answer, begin by noting that pslash^2 is symmetric in d^mu and d^nu.

There is one more relevant equation that the gammas satisfy that you need to solve this, as well.
 
chrispb said:
pslash^2 is symmetric in d^mu and d^nu.

Hi chrispb, thank you for stopping to help us answer this question.

May I ask: does "symmetric" mean pslash^2 is equal to its own transpose?
 
No, I just mean {\gamma _\mu }{\partial ^\mu }{\gamma _\nu }{\partial ^\nu }={\gamma _\mu }{\gamma _\nu }{\partial ^\mu }{\partial ^\nu }={\gamma _\mu }{\gamma _\nu }{\partial ^\nu }{\partial ^\mu }.

What this means is you can write {\partial ^\mu }{\partial ^\nu }=\frac{1}{2}({\partial ^\mu }{\partial ^\nu }+{\partial ^\nu }{\partial ^\mu }) free of charge.
 

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