A Purification of a Density Matrix

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The discussion centers on finding the purification of a specific density matrix, expressed as a combination of states. The user expresses uncertainty about the process of purification, particularly in equating coefficients of a generic state Psi with its bra. There is a mention of a substantial body of literature on the topic, but the user struggles with understanding due to a lack of formal education on the subject. Suggestions are made to consult resources like introductory texts and online lectures to clarify the concept of purification. The conversation emphasizes the importance of determining whether the density matrix is already a pure state, as this affects the purification process.
Pete5876
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I'm trying to find the purification of this density matrix
$$\rho=\cos^2\theta \ket{0}\bra{0} + \frac{\sin^2\theta}{2} \left(\ket{1}\bra{1} + \ket{2}\bra{2} \right)
$$

So I think the state (the purification) we're looking for is such Psi that
$$
\ket{\Psi}\bra{\Psi}=\rho
$$

But I'm not confident this is right because this would involve considering a generic state Psi, multiplying it with its bra and equating the coefficients which is too complicated to be right.

How do you "purify" a mixed state expressed as a density matrix?
 
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There is a substantial body of literature on this. Have you consulted that literature and if so what conclusions have you drawn?
 
I did and as you pointed out there is a substantial body of literature. I'm a slow reader and an even slower learner. We don't go by any textbook at uni and I have no idea what purification might possibly entail.

After all, we're not tensor-crossing with any other space so tracing one space out of another can't even be applied. What could they possibly mean by "purification"?
 
First of all you should check whether ##\hat{\rho}## is a pure state to begin with. It's a pure state if and only if ##\hat{\rho}^2=\hat{\rho}##!
 
For the quantum state ##|l,m\rangle= |2,0\rangle## the z-component of angular momentum is zero and ##|L^2|=6 \hbar^2##. According to uncertainty it is impossible to determine the values of ##L_x, L_y, L_z## simultaneously. However, we know that ##L_x## and ## L_y##, like ##L_z##, get the values ##(-2,-1,0,1,2) \hbar##. In other words, for the state ##|2,0\rangle## we have ##\vec{L}=(L_x, L_y,0)## with ##L_x## and ## L_y## one of the values ##(-2,-1,0,1,2) \hbar##. But none of these...

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