Laplace transform as rotation. In what space?

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SUMMARY

The Laplace transform serves as a generalization of the Fourier transform, extending its application to complex frequencies. It can be interpreted as a rotation of the basis in the space of complex-valued functions, transitioning from a delta-function basis to a new basis represented by e^{(\alpha + i\beta) t}. The integral form of the Laplace transform, F(s) = ∫_{ℂ} e^{-su} f(u) du, emphasizes the importance of analytical continuation of f(t) into the complex plane. The discussion highlights the relationship between Laplace and Fourier transforms, particularly through the concept of Wick rotation.

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mclaudt
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Sorry for thumb terminology, I just would like to grasp the main idea, as a physicist, without unnecessary complications, associated with system of axioms and definitions.

Fourier transform can be seen as rotation of basis in space of all complex-valued functions from basis of delta-functions to a new basis of waves e^{i\omega t}.

Laplace transform can be seen as generalization of Fourier transform to complex frequencies. Is it correct to see the Laplace transform as a rotation of basis in space of complex-valued functions of complex argument, from delta-functions basis to a new basis of e^{(\alpha + i\beta) t}and, if it is so, what is the basis in that space, and why does summation go only along line (-\infty, +\infty) in direct transform and (\gamma - i\infty, \gamma + i\infty) in reverse transform?
 
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There is also an operation known as Wick rotation, it is a candidate to interpret the interconnection between Fourier and Laplace, it could be interesting if they both constitute some beautiful scheme.
 
It seems that the key point is the analytical continuation. The raw form of Laplace transform is F(s) = \int_{ℂ}e^{-su}f(u)du, where f(u) is analytical continuation of f(t) to complex plane. And in that case the Laplace transform will be the rotation of basis in {f(u)} space of complex functions of complex argument, just as Fourier transform is the rotation of basis in {f(t)} space of complex functions of real argument, and integral is in both cases just a generalization of matrix multiplication to infinite dimension.

It's just guess, I'm not sure if it is correct to define F(s) that way.
 
I am studying the mathematical formalism behind non-commutative geometry approach to quantum gravity. I was reading about Hopf algebras and their Drinfeld twist with a specific example of the Moyal-Weyl twist defined as F=exp(-iλ/2θ^(μν)∂_μ⊗∂_ν) where λ is a constant parametar and θ antisymmetric constant tensor. {∂_μ} is the basis of the tangent vector space over the underlying spacetime Now, from my understanding the enveloping algebra which appears in the definition of the Hopf algebra...

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