Discussion Overview
The discussion revolves around the eigenfunctions of the momentum operator in quantum mechanics, specifically addressing their membership in Hilbert space and the conditions for square integrability. Participants reference the text "Introduction to QM" by D. Griffiths and explore the implications of these mathematical properties.
Discussion Character
- Technical explanation
- Debate/contested
Main Points Raised
- One participant questions the assertion that eigenfunctions of the momentum operator do not belong to Hilbert space, arguing that the integral gives a finite value.
- Another participant clarifies that in quantum mechanics, functions must be square integrable, noting that the integral of \( e^{ipx} \) over all space does not exist, thus disqualifying it from being a member of the space of square integrable functions.
- A participant presents a solution for the eigenfunction of the momentum operator as \( A \exp(ihx/p) \), claiming it satisfies the condition for the \( L^2(a,b) \) space, suggesting that the integral of its modulus squared is finite.
- A later reply corrects the notation to \( A \exp(i px/\hbar) \) and states that such functions are square-integrable only if the domain is compact, while they are not square-integrable over the entire real line.
Areas of Agreement / Disagreement
Participants express differing views on the square integrability of the eigenfunctions of the momentum operator, with some asserting that they do not belong to Hilbert space while others argue for their inclusion under certain conditions. The discussion remains unresolved regarding the conditions under which these functions may or may not belong to the Hilbert space.
Contextual Notes
There is an ongoing debate about the definitions and conditions for square integrability, particularly concerning the domain of integration (compact vs. non-compact). The discussion highlights the dependence on the interpretation of mathematical properties in quantum mechanics.