MHB Matrices Often Used in Quantum Computing

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The discussion focuses on the matrices commonly used in quantum computing, highlighting their properties such as whether they are unitary and self-adjoint. Key matrices discussed include the Hadamard, Pauli X, Y, Z, Phase, and pi/8 gates, along with their eigenvalues and normalized eigenvectors. The conversation also touches on the implementation of a quantum computer simulator that currently includes Shor's and Grover's algorithms, with plans for further development. Participants express interest in moving the discussion to a more relevant forum for quantum mechanics or computer science. Overall, the thread serves as a resource for those studying quantum computing and its mathematical foundations.
Ackbach
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I am beginning a study I have long wanted to engage in: quantum computing. This is a field lying at the intersection of mathematics, physics, computer science, and electrical engineering - all topics I studied, to varying levels. From time to time, I plan on posting notes and summaries that might prove useful to others studying the same thing. Without further ado:

$$\begin{array}{|c|c|c|c|c|c|} \hline
\textbf{Name} &\textbf{Matrix} &A^{\dagger}A=I? &A=A^{\dagger}? &\textbf{E-values} &\textbf{Norm. E-vectors} \\
\hline
\text{Hadamard} &H=\dfrac{1}{\sqrt{2}}\begin{bmatrix}1 &1\\1 &-1\end{bmatrix} &\text{Yes} &\text{Yes}
&1,\; -1 &\dfrac{1}{\sqrt{4-2\sqrt{2}}}\begin{bmatrix}1 \\ \sqrt{2}-1\end{bmatrix}, \;
\dfrac{1}{\sqrt{4+2\sqrt{2}}}\begin{bmatrix}1 \\ -\sqrt{2}-1\end{bmatrix} \\ \hline
\text{Pauli }X &X=\begin{bmatrix}0 &1\\1 &0\end{bmatrix} &\text{Yes} &\text{Yes} &1, \; -1
&\dfrac{1}{\sqrt{2}}\begin{bmatrix}1\\1\end{bmatrix}, \; \dfrac{1}{\sqrt{2}}
\begin{bmatrix}1\\-1\end{bmatrix} \\ \hline
\text{Pauli }Y &Y=\begin{bmatrix}0&-i\\i&0\end{bmatrix} &\text{Yes} &\text{Yes}
&1, \; -1 &\dfrac{1}{\sqrt{2}}\begin{bmatrix}1\\i\end{bmatrix}, \; \dfrac{1}{\sqrt{2}}
\begin{bmatrix}1\\-i\end{bmatrix} \\ \hline
\text{Pauli }Z &Z=\begin{bmatrix}1&0\\0&-1\end{bmatrix} &\text{Yes} &\text{Yes}
&1, \; -1 &\begin{bmatrix}1\\0\end{bmatrix}, \; \begin{bmatrix}0\\1\end{bmatrix} \\ \hline
\text{Phase} &S=\begin{bmatrix}1&0\\0&i\end{bmatrix} &\text{Yes} &\text{No} &1,\;i
&\begin{bmatrix}1\\0\end{bmatrix}, \; \begin{bmatrix}0\\1\end{bmatrix} \\ \hline
\pi/8 &T=\begin{bmatrix}1&0\\0&e^{i\pi/4}\end{bmatrix} &\text{Yes} &\text{No} &1, \; e^{i\pi/4}
&\begin{bmatrix}1\\0\end{bmatrix}, \; \begin{bmatrix}0\\1\end{bmatrix} \\ \hline
\end{array}$$
 
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Greg Bernhardt said:
Thanks @Ackbach! Think we can move to QM or Comp Sci forum?
Let's put these two in QM. I don't think they're useful enough for stickying.
 
A few days ago, I started to implement a quantum computer simulator. It's very basic but the things I tried seem to work ok.
For now only Shor (the quantum part) and Grover algorithms are there but I intend to add more.
Source code here: https://github.com/aromanro/QCSim
Phase and pi/8 gates mentioned above can be used with the more general PhaseShiftGate.
 
Insights auto threads is broken atm, so I'm manually creating these for new Insight articles. Towards the end of the first lecture for the Qiskit Global Summer School 2025, Foundations of Quantum Mechanics, Olivia Lanes (Global Lead, Content and Education IBM) stated... Source: https://www.physicsforums.com/insights/quantum-entanglement-is-a-kinematic-fact-not-a-dynamical-effect/ by @RUTA

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