Skip to main content
8 events
when toggle format what by license comment
Aug 30, 2022 at 17:16 history edited Martin Sleziak CC BY-SA 4.0
fixed the dead link
Jul 22, 2010 at 2:14 comment added Theo Johnson-Freyd @George Lowther: That's correct. Feynman's idea works for any analytic function of a noncommuting (but time-indexed) variable, provided that terms at the same time don't contribute. A large part of the value is that the user can manipulate time-ordered mathematics as in regular mathematics. For example, let $x(t)$ be a $\operatorname{Lie}(G)$-valued function. Then $\exp(\int_a^b x(t)dt)\exp(\int_b^c x(t)dt) \neq \exp(\int_a^c x(t)dt)$ in general, whereas the corresponding time-ordered equation is true.
Jul 21, 2010 at 12:46 comment added Steve Huntsman I've seen both TO and PO used as well.
Jul 21, 2010 at 2:56 comment added George Lowther Yes, but you have even numbers of anticommuting terms in the products at each point. So grouped together they will commute. (I think)
Jul 21, 2010 at 2:48 comment added José Figueroa-O'Farrill "terms associated to space-like separated points commute"... or anticommute! Remember there's a spin-statistics theorem, at least in 4-dimensional relativistic quantum field theory.
Jul 21, 2010 at 2:43 comment added George Lowther As far as I can make out, physicists have a habit of simply slapping a capital T in front of an expression and declaring it to be "time-ordered". Not just exponentials, but whatever takes their fancy really. I guess, this assumes that everything can be expanded out into a sum of products of terms associated with a time index which are then ordered. Or, into fields associated with space-time points where it is assumed that terms associated to space-like separated points commute.
Jul 21, 2010 at 2:15 comment added Theo Johnson-Freyd Now I see that George Lowther has given the same answer above.
Jul 21, 2010 at 2:14 history answered Theo Johnson-Freyd CC BY-SA 2.5