@DanielSank Can you represent the lowpass filter as a system of SDEs? Like you would for e.g. RLC as a system of ODEs effectively. Then the integration would work out as usual (should be a trivial generalization of the ODE).
I want to have a product sign analogously to $A \amalg B$. I tried $A \Pi B$, but as $\Pi$ isn't a binary operator, this does not look that good.
Can you help me?
@DanielSank Calling someone "sick" is mean in my perception. If you actually mean that as an assessment of mental health, please don't diagnose people over the internet.
@AccidentalFourierTransform One can, for the actual Wiener path integral measure in 1d, actually show that the differentiable functions are of measure zero :O
@AccidentalFourierTransform Several talks in our physical mathematics seminar dealt with it recently, I have a decent high-level understanding but nothing detailed
@0celo7 I think I was wrong about my previous statement. Singular cochain complex does admit a commutative differential graded algebra structure, since cup product can be defined on cochains.
@0celo7 I don't know yet but I suspect what's happening is this. Look at the kernel of $\omega$ on $TM$: that a codimension 1 distribution. Because $\omega$ is closed, that's integrable. So you have a codimension 1 foliation.
since $\omega$ is nowhere zero, you get a nowhere zero transverse vector field on the foliation.
Flowing along that tells you nearby leaves are diffeomorphic. Aka, you have a codim 1 foliation with diffeomorphic leaves
Now that's not sufficient, because you can get things like the irrational foliation on the torus. So I think a generic perturbation of this foliation should be a fiber bundle over the circle
@0celo7 Diffractive scattering. Any kind of diffractive scattering is sensitive to wave-length. Do it with massive particles and you are measuring the de Broglie wavelength of the particle.
And that is why people need to do an advanced lab course just as badly as they need demanding whiteboard electives.