Understanding H=L^2 in Quantum Mathematics

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H is defined as L^2(R^n), representing a Hilbert space of square-integrable functions over the nth product of the real line. L^2 refers to functions whose square integral converges, with L^2([0,1]) specifically indicating convergence over the interval from 0 to 1. The discussion clarifies that L^2(R^n) encompasses functions whose square integral converges over the entire real line, from -∞ to ∞. An example provided illustrates this with a triple integral for n=3, confirming the concept of integration across R^n. Understanding these definitions is crucial for grasping quantum mathematics in a rigorous context.
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Let H=L^2(R^n)

Here H is a Hilbert space, R^n is of course the nth product of the real line. what is L-squared? context is a quantum text for mathematicians.

Later the author uses H=L^2([0,1]) in another example.
 
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That makes perfect sense. Thank you!
 
L^2([0,1]) means functions whose square integral from 0 to 1 converges, but what is L^2(R^n)? Functions whose square integral from -\infty to \infty converges? Or any sub interval of R^n?
 
It is the integral over all of Rn. For example, if n=3, then \int_{-\infty}^\infty \int_{-\infty}^\infty \int_{-\infty}^\infty f(x,y,z) dx dy dz, which is also written in more compact form as \int_{\textbf{R}^3} f(\textbf{x}) d\textbf{x}
 
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