y-gate
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| y-gate [May 25, 2026 at 10:23] – Ivan Janevski | y-gate [May 25, 2026 at 13:55] (current) – external edit 127.0.0.1 | ||
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| - | # Y-gate | + | # Y gate |
| - | **Y-gate** (or **Pauli-Y | + | **Y gate** (or **Pauli-Y gate**) is a single-qubit quantum gate represented by the second Pauli matrix. It combines the actions of the X gate (bit flip) and the Z gate (phase flip), and also introduces a factor of $i$. |
| $$Y = \begin{pmatrix}0 & -i \\ i & 0\end{pmatrix}$$ | $$Y = \begin{pmatrix}0 & -i \\ i & 0\end{pmatrix}$$ | ||
| + | The gate maps the computational basis states as $Y\lvert 0\rangle = i\lvert 1\rangle$ and $Y\lvert 1\rangle = -i\lvert 0\rangle$. On the [[bloch-sphere]], | ||
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| + | ## Relation to X and Z gates | ||
| + | The Y gate can be decomposed as $Y = iXZ$. The eigenstates of the Y gate are the [[i-state|plus-i state]] $\lvert i\rangle$ (eigenvalue $+1$) and the [[minus-i-state|minus-i state]] $\lvert -i\rangle$ (eigenvalue $-1$). Together with the X and Z Pauli gates, the Y gate generates the Pauli group and forms the basis of quantum error correction, where X, Y, and Z errors must be detected and corrected. | ||
y-gate.1779704602.txt.gz · Last modified: by Ivan Janevski
