Conversation started Jul 31, 2020 at 17:50.
user434058
Jul 31, 2020 17:50
Hi! Could anybody explain me the comments by zwim in this comment thread?
@FakeMod: The problem is that the indefinite integral is not a function, so it makes no sense to differentiate it with respect to the parameter. The constant of integration could very well be a function of the parameter as well. I think it's hopeless. You have to fix limits of integration (one of which will be your independent variable, if you like), and then you have a well-defined antiderivative.
user434058
@TedShifrin Hmmm... I understand your second sentence, however, I don't see why the final expression of the indefinite integral won't be a function of the parameter we introduced in the integrand?
It's not a well-defined function. The indefinite integral is not a function. It's a symbol for "any antiderivative."
user434058
@TedShifrin Oh, yeah. So except the arbitrary integration constant, the rest is a well characterised function in the parameter that we introduced, and the integration variable, right?
But the integration constant is not actually a constant, as I already said. That's the fallacy. It may vary and be an arbitrary function of your parameter $b$.
user434058
Jul 31, 2020 18:00
@TedShifrin "You have to fix limits of integration (one of which will be your independent variable, if you like), and then you have a well-defined antiderivative." But how do I get any closer to using Feynman's technique after doing that?
user434058
@TedShifrin Oh! I see.
I don't know why Feynman's name gets attached to this, incidentally. That's totally bizarre.
If it were a Feynman path integral, OK.
user434058
@TedShifrin Prolly, 'cause he thought of it first (I may be terribly wrong)
That's totally not true.
It was around in mathematics and in physics long before him.
user434058
@TedShifrin Then the only reason I can think of is that he popularized it.
Jul 31, 2020 18:04
Nah. I've never heard of this before.
user434058
@TedShifrin Anyways, I still don't know why you said ths \/
user434058
5 mins ago, by FakeMod
@TedShifrin "You have to fix limits of integration (one of which will be your independent variable, if you like), and then you have a well-defined antiderivative." But how do I get any closer to using Feynman's technique after doing that?
If you consider $F(x,b) = \int_a^x g(t,b)\,dt$, then $\partial F/\partial b = \int_a^x \partial g/\partial b\,dt$ is valid.
user434058
@TedShifrin That's alright, but does it get me any closer to evaluating the integral this way?
I think the story is Feynman liked to say to people that no matter how complicated an integral a mathematician can give to him he can always do it very fast, and differentiation under the integral sign with respect to a different parameter thing was a trick upon his sleeve
Jul 31, 2020 18:09
I have no idea if it gets you closer to evaluating the integral. The differentiation under the integral trick works sometimes and doesn't work others.
user434058
@TedShifrin So any chances, whatsoever, of it working with indefinite integrals transformed to indefinite integrals?
I explained why it's nonsensical.
 
Conversation ended Jul 31, 2020 at 18:10.