Can a self adjoint operator have a continous spectrum ?

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SUMMARY

A self-adjoint operator can indeed have a continuous spectrum, allowing for eigenvalues to take arbitrary real values. The orthonormality condition for eigenfunctions in this context is expressed as = \delta (n-m), where 'δ' represents the Dirac delta function. This concept is rooted in functional analysis rather than differential equations, and it is essential to understand the relationship between compact subsets of C and commutative C* algebras. The use of Dirac deltas in physics serves as a practical extension of the completeness condition, although it may lack rigorous mathematical development.

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Can a self adjoint operator have a continuous spectrum ??

If we have a self adjoint operator

[tex]Ly_{n} = \lambda _{n}[/tex]

can n take arbitrary real values (n >0 ) in the sense that the spectrum will be continuous ?

and in that case, what is the orthonormality condition for eigenfunctions

[tex]<y_{n} |y_{m}>= \delta (n-m)[/tex]

where 'd' is dirac delta, as a generalization of discrete case of Kronecker delta. could someone put an example ? (since all the cases from QM i know the spectrum is discrete) thankx
 
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Just look up spectral analysis, please, Jose. C* algebras, stuff like that. (I seem to remember making this request a lot in the past - have you followed that advice?)

The orthonormality condition is precisely what it ought to be - two things are orthogonal if their (inner) product is 0. I don't know what makes you think that Dirac deltas have anything to do with taking an inner product (which by definition is just a complex number, not a distribution).

This is basic functional analysis, and not differential equations anyway - one of the first things you learn is that there is, I seem to think, a bijection between (arbitrary) compact subsets of C and commutative C* algebras. Perhaps I have missed some hypotheses, but that is a well known result.
 
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If this is a physics question (rather than a math question) then yes, physicists indeed use the Dirac delta to represent the inner product between states in a space spanned by continuous eigenkets (but then, physicists do a lot of things that make mathematicians cringe). A reason for this choice is that it provides a working extension to the completeness condition. I've never seen a rigorous development for this though.

If you want to use produce some new math, I strongly advise against starting from physics.
 
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