168 karma · joined August 9, 2009
-1/2 Tr F_{\mu\nu} F^{\mu\nu}
for a suitably defined F. Or further abbreviated to something like L_g.
It just depends on how much detail you need to expose.
Interesting about colour - perhaps a "less is more" thing. The end of Andrei Rublev is breathtaking, for instance.
I saw Mirror three times at the cinema, and there are not many flicks I can say that about.
These ran into all sorts of problems, largely to do with the proximity of the pseudolites to the receivers such as synchronisation and signal strength issues. Locatanets (http://locata.com/) are the in thing nowadays.
Of course that should not preclude the possibility of replication as described here.
I find the idea of threats to job security misguided. In the particle physics world some significant code (not everything, granted) has been made available for some time; e.g. Monte-Carlo simulators like Geant or lattice gauge theory codes like those from MILC, SciDAC or FermiQCD. Even highly optimised code has been available. Users are requested to cite the authors. No careers have been harmed, as far as I can tell.
Also, the code itself is not much use for replicating results without making the data available too. This can be more problematic politically and technically, but even here there are good precedents in the particle physics world.