## Archive for the ‘**Science Education**’ Category

## Los Alamos Science

Continuing the expository theme of my last post, I want to bring to your attention a collection of beautiful, crisp and entertaining articles by Richard Slansky in a 1984 publication of Los Alamos Science. They are available at

http://www.fas.org/sgp/othergov/doe/lanl/pubs/number11.htm

and are (in my opinion) must readings for students of theoretical physics, particularly those specializing in high energy theory, string theory, etc. In case you didn’t know, Slansky is also the author of a definitive review on group theory, which is a standard resource for particle physicists. It is worth having a printout of the review at your desk (and also an online copy in your tablet, smartphone, etc.) if you are interested in doing anything serious with group theory.

I should also take this opportunity to bring a list of Physics articles that have appeared over the years in Los Alamos Science. The comprehensive list of these articles with hyperlinks to online versions is at

http://la-science.lanl.gov/cat_physics.shtml

## The Yang Mills Field Strength: a motivation for differential forms

Although their importance and applications are widely recognized in theoretical physics, differential forms are not part of the standard curriculum in physics courses, except for the rare mention in a general relativity course, e.g. if you have used the book by Sean Carroll. In this blog post, we describe the construction of the field strength tensor for Yang Mills Theory, using differential forms. The derivation (which is based on the one given by Tony Zee in his QFT book) is elegant, and mathematically less tedious than the more conventional derivation based on the matrix gauge field. It also illustrates the power of the differential forms approach.

To begin with, let me define a normalized matrix gauge field which is times the usual matrix gauge field. So in the equations that appear below, the covariant derivative has no lurking factors of . This greatly simplifies the algebra for us, as we don’t have to keep track of conjugations and sign changes associated with . The covariant derivative is thus in terms of this new gauge field. The matrix 1-form is

So, . But since , only the antisymmetric part of the product survives and hence we can write

We want to construct an appropriate 2-form from this 1-form A. Now, if d denotes the *exterior derivative, *then dA is a 2-form, as is A^2. These are the only two forms we can construct from A. So, must be a linear combination of these two forms. This is a very simple, and neat argument!

Now, the transformation law for the gauge potential is

where is a 0 form (so ). Applying d to the transformation law, we get

where the negative sign in the third term comes from moving the 1-form d past the 1-form A. Squaring the transformation law yields

Now, $UU^\dagger = 1$, so applying d again to both sides we get . So, we can write the square transformation law as

whereas if we recall the expression for the transformation of , it was just

Clearly if we merely add and , the last 3 terms on the RHS of each cancel out, and we get

which is the expected transformation law for a field strength of the form :

The differential form approach uses compact notation that suppresses the Lorentz index as well as the group index , and gives us a fleeting glimpse into the connection between gauge theory and fibre bundles.

For a gentle yet semi-rigorous introduction to differential forms, the reader is referred to the book on General Relativity by Sean Carroll.