Open main menu
Home
Random
Recent changes
Special pages
Community portal
Preferences
About Wikipedia
Disclaimers
Incubator escapee wiki
Search
User menu
Talk
Dark mode
Contributions
Create account
Log in
Editing
Unbounded operator
(section)
Warning:
You are not logged in. Your IP address will be publicly visible if you make any edits. If you
log in
or
create an account
, your edits will be attributed to your username, along with other benefits.
Anti-spam check. Do
not
fill this in!
==Importance of self-adjoint operators== The class of '''self-adjoint operators''' is especially important in mathematical physics. Every self-adjoint operator is densely defined, closed and symmetric. The converse holds for bounded operators but fails in general. Self-adjointness is substantially more restricting than these three properties. The famous [[Self-adjoint operator#Spectral theorem|spectral theorem]] holds for self-adjoint operators. In combination with [[Stone's theorem on one-parameter unitary groups]] it shows that self-adjoint operators are precisely the infinitesimal generators of strongly continuous one-parameter unitary groups, see {{slink|Self-adjoint operator#Self-adjoint extensions in quantum mechanics}}. Such unitary groups are especially important for describing [[time evolution]] in classical and quantum mechanics.
Edit summary
(Briefly describe your changes)
By publishing changes, you agree to the
Terms of Use
, and you irrevocably agree to release your contribution under the
CC BY-SA 4.0 License
and the
GFDL
. You agree that a hyperlink or URL is sufficient attribution under the Creative Commons license.
Cancel
Editing help
(opens in new window)