Talk:Quantum operation: Difference between revisions
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imported>Paul Wormer (→Comment on pure v. impure states: new section) |
imported>Paul Wormer (→Typo?: new section) |
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After projective measurement the state has become pure, i.e., <math>\scriptstyle \rho'=\frac{P_i \rho P_i}{{\rm tr}(P_i \rho P_i)}</math>, describe a density that is a delta-function with as peak the pure state ψ<sub>i</sub>. --[[User:Paul Wormer|Paul Wormer]] 20:36, 11 April 2009 (UTC) | After projective measurement the state has become pure, i.e., <math>\scriptstyle \rho'=\frac{P_i \rho P_i}{{\rm tr}(P_i \rho P_i)}</math>, describe a density that is a delta-function with as peak the pure state ψ<sub>i</sub>. --[[User:Paul Wormer|Paul Wormer]] 20:36, 11 April 2009 (UTC) | ||
== Typo? == | |||
Second paragraph: | |||
:for all <math>\scriptstyle \rho \,\in\, \mathcal{D}(\mathcal{K})</math>, | |||
Should this not be: | |||
:for all <math>\scriptstyle \rho \,\in\, \mathcal{D}(\mathcal{H})</math>? | |||
Or do I miss something completely? | |||
--[[User:Paul Wormer|Paul Wormer]] 20:40, 11 April 2009 (UTC) |
Revision as of 14:40, 11 April 2009
Comment on pure v. impure states
In usual textbooks of QM one distinguishes pure and impure states (at the moment I do not have access to any text on QM, I'm writing from memory, so I cannot quote sources). I would write:
- An impure state of a quantum system is represented on a Hilbert space by a non-negative definite trace class operator on with trace equal to one. Such operators are called density operators.
After projective measurement the state has become pure, i.e., , describe a density that is a delta-function with as peak the pure state ψi. --Paul Wormer 20:36, 11 April 2009 (UTC)
Typo?
Second paragraph:
- for all ,
Should this not be:
- for all ?
Or do I miss something completely? --Paul Wormer 20:40, 11 April 2009 (UTC)
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