Can Bloch sphere be used to represent mixed states in quantum computation?

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Homework Help Overview

The discussion revolves around the representation of mixed states in quantum computation using the Bloch sphere, specifically focusing on the properties of density matrices and their implications in quantum mechanics.

Discussion Character

  • Exploratory, Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Participants explore the properties of density matrices, questioning their definitions and implications. Some express uncertainty about the direction of their reasoning, while others suggest verifying the properties of the density matrix, such as positivity and trace conditions. Questions about the importance of the Bloch sphere in quantum computation and requests for additional resources are also raised.

Discussion Status

The discussion is active, with participants sharing insights and resources. Some have provided guidance on verifying the properties of density matrices, while others are still grappling with the concepts and seeking clarification. There is no explicit consensus, but a productive exchange of ideas is evident.

Contextual Notes

Participants express concerns about the comprehensiveness of existing resources, particularly Nielsen's book, and seek additional references to better understand the Bloch sphere's role in quantum computation.

Haorong Wu
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Homework Statement
From Nielsen's QC exercise 2.72:
Show that an arbitrary density matrix for a mixed state qubit may be written as
##\rho = \frac {I+ \vec r \cdot \vec \sigma} 2##,
where ##\vec r## is a real three-dimensional vector such that ##\| \vec r \| \leq 1##. This vector is known as the Bloch vector for the state ##\rho##
Relevant Equations
##\vec \sigma## are Pauli matrices
##\rho \equiv \sum_i p_i \left | \psi _i \right > \left < \psi_i \right |##
Well, I have no clues for this problem.

Since I can get nothing from the definition of ##\rho##, I tried from the right part.

Also, I know that ##\left ( \vec r \cdot \vec \sigma \right ) ^2={r_1}^2 {\sigma _1}^2+{r_2}^2 {\sigma _2}^2+{r_3}^2 {\sigma _3}^2##.

Plus, ##\rho## is positive; then I only need to show that ##\rho ^2=I^2+2 \vec r \cdot \vec \sigma +{r_1}^2 {\sigma _1}^2+{r_2}^2 {\sigma _2}^2+{r_3}^2 {\sigma _3}^2##.

Well, I'm stuck again.

Maybe I went the wrong direction?

Also, Are there any places I can find the solutions for Nielsen's book? I feel nervous that I can not check my solutions to see whether I'm right or not.

Oh, another question. I'm wondering, is Bloch sphere important in quantum computation? Maybe some references I should read? Nielsen's book doesn't introduce it comprehensively.

Thank you for reading!
 
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I would start by showing that ##\rho## possesses all the properties of a density matrix, namely that the diagonal elements are all real, positive, and ##\leq 1## and
$$
\rho = \rho^\dagger
$$
$$
\mathrm{tr}(\rho) = 1
$$
$$
\mathrm{tr}(\rho^2) \leq 1
$$

I would then show that any 2x2 density matrix can be written by specifying ##\mathbf{r}## only.
 
Haorong Wu said:
Thanks, DrClaude.

Bloch sphere really makes me nervous.

(*_*)
It shouldn't :smile:. It is simply another way of looking at qubits.
 
DrClaude said:
I would start by showing that ##\rho## possesses all the properties of a density matrix, namely that the diagonal elements are all real, positive, and ##\leq 1## and
$$
\rho = \rho^\dagger
$$
$$
\mathrm{tr}(\rho) = 1
$$
$$
\mathrm{tr}(\rho^2) \leq 1
$$

I would then show that any 2x2 density matrix can be written by specifying ##\mathbf{r}## only.
Great! I solved the problem with your hint. Thanks, DrClaude. I can sleep well tonight.
 

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