Discussion Overview
The discussion revolves around the differences between Hermitian and self-adjoint operators, particularly in the context of functional analysis and quantum mechanics. Participants explore definitions, conventions, and implications of these terms, addressing both bounded and unbounded operators.
Discussion Character
- Debate/contested
- Technical explanation
- Conceptual clarification
Main Points Raised
- Some participants note that while many people use "Hermitian" and "self-adjoint" interchangeably, there is a distinction, especially for unbounded operators.
- One participant states that a Hermitian operator is defined as a bounded self-adjoint operator, implying that all Hermitian operators are self-adjoint, but not all self-adjoint operators are Hermitian.
- Another participant questions whether the distinction mentioned is an example of the difference or if it represents another difference altogether, referencing a source that highlights differing definitions between physicists and mathematicians.
- Definitions are provided: an operator is Hermitian if it is bounded and satisfies a specific inner product condition for all elements in the Hilbert space; it is symmetric if the condition holds for all elements in its domain; and it is self-adjoint if it is symmetric and its domain equals the domain of its adjoint.
- Concerns are raised about the implications of these definitions in the context of physical observables and the canonical commutation relations, particularly regarding unbounded operators.
Areas of Agreement / Disagreement
Participants express differing views on the definitions and implications of Hermitian versus self-adjoint operators, indicating that multiple competing perspectives remain without a clear consensus.
Contextual Notes
Some definitions and distinctions depend on the context of bounded versus unbounded operators, and the discussion acknowledges that terminology may vary between physics and mathematics.