quantum-gate-single-qubit
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| quantum-gate-single-qubit [August 26, 2026 at 16:41] – Ivan Janevski | quantum-gate-single-qubit [August 26, 2026 at 18:16] (current) – Ivan Janevski | ||
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| ## List of gates | ## List of gates | ||
| - | - **Pauli gates** | + | |
| - | - [[quantum-gate-i|Identity (I)]] | + | - [[quantum-gate-i|Identity (I)]] |
| - | - [[quantum-gate-x|Pauli X (NOT)]] | + | - [[quantum-gate-x|Pauli X (NOT)]] |
| - | - [[quantum-gate-y|Pauli Y]] | + | - [[quantum-gate-y|Pauli Y]] |
| - | - [[quantum-gate-z|Pauli Z]] | + | - [[quantum-gate-z|Pauli Z]] |
| - | - **Hadamard** | + | |
| - [[quantum-gate-h|Hadamard (H)]] | - [[quantum-gate-h|Hadamard (H)]] | ||
| - | - **Phase gates** | + | |
| - | - [[quantum-gate-s|S | + | - [[quantum-gate-s|S (phase) |
| - | - [[quantum-gate-s-dagger|S† (inverse phase)]] | + | - [[quantum-gate-s-dagger|S† (inverse phase gate)]] |
| - | - [[quantum-gate-t|T gate]] | + | - [[quantum-gate-t|T gate]] |
| - | - [[quantum-gate-t-dagger|T† (inverse T)]] | + | - [[quantum-gate-t-dagger|T† |
| - | - **Parametric rotations** | + | - [[quantum-gate-rotation]] |
| - | - [[quantum-gate-rx|RX (rotation around X)]] | + | - [[quantum-gate-rx|Rx (rotation around X)]] |
| - | - [[quantum-gate-ry|RY (rotation around Y)]] | + | - [[quantum-gate-ry|Ry (rotation around Y)]] |
| - | - [[quantum-gate-rz|RZ (rotation around Z)]] | + | - [[quantum-gate-rz|Rz (rotation around Z)]] |
| - | - **Universal** | + | - [[quantum-gate-u|U (universal single-qubit)]] |
| - | | + | |
| ## Bloch sphere action | ## Bloch sphere action | ||
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| Composing rotations around different axes yields a rotation around a third axis. The $2 \times 2$ unitary matrices $\mathrm{SU}(2)$ are isomorphic to the unit quaternions $\mathrm{Sp}(1)$, | Composing rotations around different axes yields a rotation around a third axis. The $2 \times 2$ unitary matrices $\mathrm{SU}(2)$ are isomorphic to the unit quaternions $\mathrm{Sp}(1)$, | ||
| + | |||
| + | ## Dagger | ||
| + | |||
| + | The dagger operator (†) computes the conjugate transpose of a gate's matrix. For unitary gates, $U^\dagger = U^{-1}$, meaning the dagger is the inverse: applying $U^\dagger$ undoes $U$ ($U^\dagger U = I$). On the Bloch sphere, dagger reverses the direction of rotation: a rotation by angle $\theta$ becomes a rotation by angle $-\theta$. This explains why $U^\dagger U = I$—two opposite rotations cancel. | ||
| + | |||
| + | ## Square root | ||
| + | |||
| + | Taking the square root of a gate produces a gate that, applied twice, yields the original. Examples: $T^2 = S$ (T is the square root of S), $S^2 = Z$ (S is the square root of Z). On the Bloch sphere, square root halves the rotation angle: a gate rotating by $\theta$ yields a square root rotating by $\theta/2$. This explains why square roots compose: $\sqrt{U}$ applied twice returns to $U$. | ||
| ## Matrix representations | ## Matrix representations | ||
quantum-gate-single-qubit.1787762468.md.gz · Last modified: by Ivan Janevski
