x-gate
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| x-gate [June 09, 2026 at 22:53] – Ivan Janevski | x-gate [June 15, 2026 at 15:23] (current) – Ivan Janevski | ||
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| - | # X-gate | + | # $X$ gate (NOT gate) |
| - | **X-gate** (or **Pauli-X gate**, or **Quantum | + | **X gate** (or **Pauli-X gate**, or **quantum |
| - | $$ X = \begin{pmatrix}0 & 1\\ 1 & 0\end{pmatrix}$$ | + | $$X = \begin{pmatrix}0 & 1\\ 1 & 0\end{pmatrix}$$ |
| - | On the Bloch sphere, it rotates | + | The gate flips the computational basis states and leaves |
| - | If you apply the gate twice, you will flip the state twice, meaning you go back to where you started. This means. This property is called the " | + | $$X\lvert 0\rangle = \lvert 1\rangle \qquad X\lvert 1\rangle = \lvert 0\rangle$$ |
| - | $$X^2 = I$$ | + | $$X\lvert +\rangle |
| + | On the [[bloch-sphere|Bloch sphere]], $X$ corresponds to a rotation of $\pi$ radians about the $x$-axis. Applying the gate twice returns the qubit to its original state — this is the involution property, $X^2 = I$, shared by all Pauli gates. The $X$ gate appears in virtually every quantum algorithm as the quantum equivalent of setting or flipping a bit. | ||
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| + | ## List of code implementations | ||
| + | |||
| + | - [[x-gate-qiskit|X gate (Qiskit)]] | ||
| + | - [[x-gate-custatevec|X gate (cuStateVec)]] | ||
| + | - [[x-gate-cudaq|X gate (CUDA-Q)]] | ||
x-gate.1781045616.txt.gz · Last modified: by Ivan Janevski
