Talk:Quantum operation: Difference between revisions

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imported>Paul Wormer
imported>Paul Wormer
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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 &psi;<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 &psi;<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)

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 Definition A mathematical formalism used to describe a broad class of transformations that a quantum mechanical system can undergo. [d] [e]
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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)