quantum-gate-yy
Table of Contents
YY Gate (Parametric)
YY gate is a parametric two-qubit gate implementing correlated Y rotations on both qubits.
Matrix:
$$\text{YY}(\theta) = e^{-i\theta Y_1 Y_2 / 2} = \begin{pmatrix} \cos(\theta/2) & 0 & 0 & i\sin(\theta/2) \\ 0 & \cos(\theta/2) & -i\sin(\theta/2) & 0 \\ 0 & -i\sin(\theta/2) & \cos(\theta/2) & 0 \\ i\sin(\theta/2) & 0 & 0 & \cos(\theta/2) \end{pmatrix}$$
Action: entangling two-qubit rotation around YY axis.
Special Cases
- $\text{YY}(0) = I$
- $\text{YY}(\pi/2)$ creates entanglement
- $\text{YY}(\pi)$ full rotation
Properties
- Parametric: tune interaction strength
- Symmetric: both qubits interact equally
- Entangling gate
- Hamiltonian form: $\text{YY}(\theta) = e^{-i\theta Y \otimes Y / 2}$
Physical Origin
Arises from:
- Superconducting qubits: some coupling geometries
- Trapped ions: laser interactions
- Spin systems: YY coupling (less common than XX or ZZ in nature, but engineerable)
Relation to XX and ZZ
- Gate family: Pauli axis determines interaction character
- XX: $e^{-i\theta X \otimes X / 2}$ (correlate X rotations)
- YY: $e^{-i\theta Y \otimes Y / 2}$ (correlate Y rotations)
- ZZ: $e^{-i\theta Z \otimes Z / 2}$ (correlate Z rotations)
Uses
- Ansatze: YY gates in variational circuits for certain problems
- Quantum simulation: simulate YY-coupled systems
- Native gates: some platforms implement YY directly
Decomposition
- Typical composition: X rotations, CNOT gates, and single-qubit gates if not native
- Availability: less common native gate than XX or ZZ, but available on some platforms
quantum-gate-yy.md · Last modified: by 127.0.0.1
