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

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SUMMARY

The discussion centers on the use of the Bloch sphere to represent mixed states in quantum computation, specifically addressing the properties of the density matrix ##\rho##. Participants confirm that the Bloch sphere is indeed significant in quantum computation and provide resources for further understanding. Key properties of density matrices, such as positivity, trace, and Hermitian nature, are emphasized as essential for representing mixed states effectively.

PREREQUISITES
  • Understanding of quantum mechanics concepts, particularly density matrices.
  • Familiarity with the Bloch sphere representation of qubits.
  • Knowledge of the mathematical properties of matrices, including trace and Hermitian operators.
  • Basic grasp of quantum computation principles as outlined in Nielsen's textbook.
NEXT STEPS
  • Study the mathematical properties of density matrices in quantum mechanics.
  • Explore the significance of the Bloch sphere in quantum computation through academic papers and resources.
  • Review the solutions and exercises in Nielsen's "Quantum Computation and Quantum Information" for practical applications.
  • Investigate online resources such as physics.stackexchange.com for community insights on the Bloch sphere.
USEFUL FOR

Quantum computing students, researchers in quantum mechanics, and anyone interested in the mathematical representation of qubits and mixed states.

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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