R^a_buv A_a = [&;_u, &;_v]A_b (2)
which defines the Riemann tensor. The calculation is in the one-page
file
http://jayryablon.files.wordpress.com/2009/10/can-you-find-the-error-in-this-calculation.pdf
The contracted result I end up with is:
R_au A^a = [&;_a, &;u] A^a (2)
where R_au is the Ricci tensor, but the mixed symmetry and antisymmetry
strikes me funny. I would like to know if this is a correct
calculation, and if I am missing anything.
Thanks,
Jay
____________________________
Jay R. Yablon
Email: jya...@nycap.rr.com
co-moderator: sci.physics.foundations
Weblog: http://jayryablon.wordpress.com/
Web Site: http://home.roadrunner.com/~jry/FermionMass.htm
I think the basic problem is that when you switch indices in R_mu_alpha
you correctly do not change sign, but then you seem to think this
enables you to do the same for the commutator. The bit you think follows
by considering R in isolation does not in fact follow.
Regards
--
Charles Francis
moderator sci.physics.foundations.
charles (dot) e (dot) h (dot) francis (at) googlemail.com (remove spaces and
braces)
R_au A^a = [&;_a, &;u] A^a (2)
a correct result, and if not, at what exact step is there a mistake?
Jay.
That looked right to me, depending possibly on sign conventions.