How Does a Mixed Quantum State Relate to Bloch Sphere Representation?

bowlbase
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Homework Statement


What is reduced density matrix ##\rho_A## and the Bloch vector representation for a state that is 50% ##|0 \rangle## and 50% ##\frac{1}{\sqrt{2}}(|0 \rangle + |1 \rangle)##

Homework Equations


The Attempt at a Solution


[/B]
I haven't seen many (any?) examples of this so I'm trying to feel my way through it. So first matrix should be
##\begin{bmatrix}
1 & 0 \\
0 & 0
\end{bmatrix}##
and the second:
##\frac{1}{2}\begin{bmatrix}
1 & 1 \\
1 & 1
\end{bmatrix}##
Both have a 50% chance so ##\frac{1}{4}\begin{bmatrix}
1 & 1 \\
1 & 1
\end{bmatrix}+\frac{1}{2}\begin{bmatrix}
1 & 0 \\
0 & 0
\end{bmatrix}##
Giving:
##\rho_A=\begin{bmatrix}
\frac{3}{4} & \frac{1}{4} \\
\frac{1}{4} & \frac{1}{4}
\end{bmatrix}##

I think this is correct.

I'm not sure about the Bloch sphere portion. Can anyone give me some direction?
 
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I would look up the Bloch vector representation of spin-1/2 systems. In short, any
bowlbase said:

Homework Statement


What is reduced density matrix ##\rho_A## and the Bloch vector representation for a state that is 50% ##|0 \rangle## and 50% ##\frac{1}{\sqrt{2}}(|0 \rangle + |1 \rangle)##

Homework Equations


The Attempt at a Solution


[/B]
I haven't seen many (any?) examples of this so I'm trying to feel my way through it. So first matrix should be
##\begin{bmatrix}
1 & 0 \\
0 & 0
\end{bmatrix}##
and the second:
##\frac{1}{2}\begin{bmatrix}
1 & 1 \\
1 & 1
\end{bmatrix}##
Both have a 50% chance so ##\frac{1}{4}\begin{bmatrix}
1 & 1 \\
1 & 1
\end{bmatrix}+\frac{1}{2}\begin{bmatrix}
1 & 0 \\
0 & 0
\end{bmatrix}##
Giving:
##\rho_A=\begin{bmatrix}
\frac{3}{4} & \frac{1}{4} \\
\frac{1}{4} & \frac{1}{4}
\end{bmatrix}##

I think this is correct.

I'm not sure about the Bloch sphere portion. Can anyone give me some direction?

Any 2\otimes 2 matrix can be expressed as a sum over the 4 basis matrices I,\sigma_{x},\sigma_{y} and \sigma_{z}. For convenience, we'll define \sigma_{0}=I as the 2\otimes 2 identity matrix.

These matrices form an orthogonal basis with the inner product between two matrices defined as the trace of the product of the two matrices:
Tr[\sigma_{i}\sigma_{j}]=2\delta_{ij}

As an example, we can have a 2\otimes 2 matrix A expressed as
A=a_{0} \sigma_{0} +a_{1}\sigma_{x}+a_{2}\sigma_{y}+a_{3}\sigma_{z}

We can use the orthogonality of the basis matrices to find a_{0} through a_{3}.

For example:
a_{2}= \frac{Tr[A\sigma_{2}]}{Tr[\sigma_{2}\sigma_{2}]}

Now for a density matrix, A=\rho, and (a_{1},a_{2},a_{3}) form a vector \vec{a} on the Bloch sphere. Once you know the components of \vec{a}, you will have the Bloch vector of the spin-1/2 system.
 
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