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quantum-gate-single-qubit [August 26, 2026 at 16:41] – Ivan Janevskiquantum-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-pauli]] 
-  - [[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-phase]] 
-  - [[quantum-gate-s|S gate (phase)]] +    - [[quantum-gate-s|S (phase) gate]] 
-  - [[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† gate (inverse T gate)]] 
-- **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)]]
-  - [[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 $\mathrm{Sp}(1)$, which naturally represent 3D rotations via quaternion multiplication. This explains the double-cover relationship between $\mathrm{SU}(2)$ and $\mathrm{SO}(3)$: two distinct quantum gates (differing by a global phase factor of $-1$) represent the same Bloch sphere rotation. 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 $\mathrm{Sp}(1)$, which naturally represent 3D rotations via quaternion multiplication. This explains the double-cover relationship between $\mathrm{SU}(2)$ and $\mathrm{SO}(3)$: two distinct quantum gates (differing by a global phase factor of $-1$) represent the same Bloch sphere rotation.
 +
 +## 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