Discussion Overview
The discussion revolves around the possibility of expanding a function that is not in the L² space into an orthonormal basis of functions. Participants explore the conditions under which such an expansion might be valid, particularly focusing on the convergence of the series and the nature of the coefficients involved.
Discussion Character
- Debate/contested
- Mathematical reasoning
Main Points Raised
- One participant suggests that if the coefficients \( c_{n} = \int_{0}^{\infty} dx f(x) \phi_{n}(x) \) are finite, then it may be valid to express the function \( f(x) \) as a series expansion \( f(x) = \sum_{n=0}^{\infty} \phi_{n}(x) \), despite the divergence of \( \sum_{n=0}^{\infty} |c_{n}|^{2} \).
- Another participant questions the validity of the proposed expansion, stating that the function cannot be equal to the sum for any reason and challenges the assumption that an L² function is equal to its Fourier series.
- A later reply clarifies that the orthonormal functions are part of L² space, while the function \( f(x) \) is not, and proposes that the series could represent an "asymptotic" approximation of the function using a finite number of coefficients.
- Further challenges arise regarding the definition of the basis and the nature of the equivalence relation, with participants seeking clarification on what the basis is a part of and the meaning of the notation used.
Areas of Agreement / Disagreement
Participants express disagreement on the validity of the proposed expansion and the conditions under which it might hold. There is no consensus on whether the series can represent the function or the implications of the coefficients being finite.
Contextual Notes
Participants highlight missing definitions regarding the basis and the nature of the equivalence relation used in the proposed expansion. The discussion also reflects uncertainty about the convergence of the series for specific values of \( x \) and the conditions under which the equality or asymptotic representation might be valid.