quantum gate directory
Mølmer-Sørensen
Symbol
$MS$
Qubits: $n$ Parameters: $n(n-1)/2$
Description:
A native entangling interaction in ion-trap systems based on collective spin-motion coupling.
Alternate notations:
- $\mathrm{MS}$
- $\mathrm{MS}(\chi_{ij})$
- $\mathrm{GMS}$
SDK Support
| SDK | Name |
|---|---|
| Qiskit |
qiskit.circuit.library.MSGate
|
| PennyLane | — ⓘ |
| Cirq |
cirq.MSGate
ⓘ
|
| Q# | — |
| PyQuil | — |
| Braket |
braket.circuits.gates.MS
ⓘ
|
| BQSKit |
bqskit.ir.gates.XXGate
ⓘ
|
| Qibo |
qibo.gates.MS
ⓘ
|
| pytket |
pytket.circuit.OpType.AAMS
ⓘ
|
| Stim |
SQRT_XX
ⓘ
|
| OpenQASM | — |
Reference
The Mølmer-Sørensen (MS) gate acts on $n$ qubits and, for $n = 2$, reduces to an $XX$ rotation. In full generality the MS gate (sometimes referred to as global MS or GMS) takes $n(n-1)/2$ parameters $\chi_{ij}$.
$$ \mathrm{MS}(\chi_{ij}) = \exp\left(-i \sum_{i=1}^n\sum_{j=i+1}^n X_i\otimes X_j \, \chi_{ij} / 2\right) $$
Where $X_i$ denotes a Pauli X on qubit $i$.
Properties
- For two qubits, $\mathrm{MS}(\chi) = R_{xx}(\chi)$.
- Entangling for nontrivial angles; $\chi = \pi/2$ yields a maximally entangling gate.
- Symmetric under qubit exchange in the two-qubit case.
Usage
- Native two-qubit entangling gate in trapped-ion hardware.
- Building blocks for GHZ states, parity checks, and variational layers.
References
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