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doc/src/week7/Latexfiles/pauli.tex

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\documentclass{article}
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\usepackage{amsmath}
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\usepackage{physics}
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\begin{document}
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\section*{Rewriting a String of Pauli Matrices for Measurement}
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In quantum mechanics, Pauli matrices are often used to represent spin operators. A string of Pauli matrices can appear in various contexts, such as in the Hamiltonian or in the context of quantum error correction. To perform a measurement, it is often useful to rewrite the string of Pauli matrices in a specific order or to simplify the expression.
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\subsection*{Pauli Matrices}
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The Pauli matrices are defined as:
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\[
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\sigma_x = \begin{pmatrix} 0 & 1 \\ 1 & 0 \end{pmatrix}, \quad
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\sigma_y = \begin{pmatrix} 0 & -i \\ i & 0 \end{pmatrix}, \quad
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\sigma_z = \begin{pmatrix} 1 & 0 \\ 0 & -1 \end{pmatrix}.
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\]
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\subsection*{Rewriting a String of Pauli Matrices}
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Consider a string of Pauli matrices of the form:
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\[
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P = \sigma_{i_1} \otimes \sigma_{i_2} \otimes \cdots \otimes \sigma_{i_n},
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\]
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where each $\sigma_{i_k}$ is one of the Pauli matrices $\sigma_x$, $\sigma_y$, $\sigma_z$, or the identity matrix $I$.
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To rewrite this string for measurement purposes, follow these steps:
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\begin{enumerate}
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\item \textbf{Commute and reorder}: Use the commutation relations of the Pauli matrices to reorder the string. The commutation relations are:
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\[
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[\sigma_i, \sigma_j] = 2i \epsilon_{ijk} \sigma_k,
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\]
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where $\epsilon_{ijk}$ is the Levi-Civita symbol. This allows you to move certain Pauli matrices to the left or right in the string.
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\item \textbf{Simplify using identities}: Use the fact that $\sigma_i^2 = I$ and $\sigma_i \sigma_j = -\sigma_j \sigma_i$ for $i \neq j$ to simplify the expression. For example:
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\[
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\sigma_x \sigma_y = -\sigma_y \sigma_x = i \sigma_z.
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\]
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\item \textbf{Group terms}: Group terms that are easier to measure together. For example, if you have a term like $\sigma_x \otimes \sigma_x$, you can measure both qubits in the $X$-basis simultaneously.
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\item \textbf{Diagonalize if necessary}: If the final expression is not diagonal, you may need to apply a unitary transformation to diagonalize it before measurement. For example, to measure $\sigma_x$, you can apply the Hadamard gate $H$ to transform it into $\sigma_z$:
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\[
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H \sigma_x H = \sigma_z.
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\]
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\end{enumerate}
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\subsection*{Example}
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Consider the following string of Pauli matrices:
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\[
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P = \sigma_x \otimes \sigma_y \otimes \sigma_z.
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\]
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To rewrite this for measurement:
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\begin{enumerate}
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\item Use the commutation relations to reorder the terms if needed.
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\item Simplify using identities:
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\[
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\sigma_x \sigma_y = i \sigma_z.
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\]
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\item Group terms:
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\[
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P = (i \sigma_z) \otimes \sigma_z = i (\sigma_z \otimes \sigma_z).
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\]
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\item The term $\sigma_z \otimes \sigma_z$ is already diagonal and can be measured directly in the $Z$-basis.
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\end{enumerate}
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Thus, the rewritten string is:
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\[
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P = i (\sigma_z \otimes \sigma_z).
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\]
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\end{document}

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