Multi-Control-X¶

The multi-control-X gate applies X gate to one target qubit bit if and only if the logical AND of all control qubits is satisfied. The multi-control-X function incorporates numerous implementations for the multi-control-X gate, each with different depth and number of auxiliary qubits. These implementations generically outperform the Gray-code, V-chain and recursive implementations of Ref. [1], as well as the relative-phase-Toffoli implementation of Ref. [2]. Given a sufficient number of auxiliary qubits some implementations allow for logarithmic depth and linear CX-count. The synthesis process selects the appropriate implementation depending on the defined constraints.

Syntax¶

Function: Mcx

Parameters:

num_ctrl_qubits: Optional[int]
ctrl_state: Optional[str]
arguments: Optional[List[RegisterUserInput]]

One has to pass either "num_ctrl_qubits" or "arguments". When the function is called with "arguments", the last qubit of the last argument is taken to be the target (the qubit on which the X gate is applied). All other qubits are the control qubits. The following two calls are equivalent.

{
  "function": "Mcx",
  "function_params": {
    "num_ctrl_qubits": 3,
    "ctrl_state": "011"
  }
}

{
  "function": "Mcx",
  "function_params": {
    "arguments": [{ "size": 4, "name": "reg" }],
    "ctrl_state": "011"
  }
}

Example¶

The following example shows how to "mark" a single state in a superposition. First we load a uniform superposition over 3 qubits using StatePreparation. In order to mark a single state, e.g '011', within this superposition, we apply the multi-control-X gate on a target qubit where the 3-qubit register serves as the control register. We specify the state '011' in the ctrl_state field of the multi-control-X gate. Thus, an X gate is applied to the target qubit only for the control state '011'. As a result, the target qubit is in state '1' if and only if the control register is in state '011'.

Textual ModelSDK

{
    "constraints": {
      "max_width": 20,
      "max_depth": 50
    },
    "logic_flow": [
        {
          "function": "StatePreparation",
          "function_params": {
            "num_qubits": 3,
            "probabilities": [0.125, 0.125, 0.125, 0.125, 0.125, 0.125, 0.125, 0.125],
            "error_metric": { "KL": {"upper_bound": 0.3}}
          },
          "outputs": "sp_out"
        },
        {
            "function": "Mcx",
            "function_params": {"num_ctrl_qubits": 3, "ctrl_state": "011"},
         "inputs": {
            "CTRL_IN": "sp_out"
          }
        }
    ]
    }

from classiq import ModelDesigner, QReg
from classiq.builtin_functions import Mcx, StatePreparation

QUBIT_COUNT = 20
MAX_DEPTH = 50

model_designer = ModelDesigner()
x = QReg(size=3)

probabilities = (0.125, 0.125, 0.125, 0.125, 0.125, 0.125, 0.125, 0.125)
sp_params = StatePreparation(probabilities=probabilities, num_qubits=x.size)
model_designer.StatePreparation(sp_params, out_wires=x)

mcx_params = Mcx(num_ctrl_qubits=x.size, ctrl_state="011")
model_designer.Mcx(mcx_params, in_wires={"CTRL_IN": x})

circuit = model_designer.synthesize()
circuit.show()

Different constraints for the circuit depth and number of qubits results in different implementations selected for the Mcx function, as can be seen in the image below.

Mcx example

References¶

[1] A. Barenco et al, Elementary gates for quantum computation, Phys. Rev. A 52 (1995). https://journals.aps.org/pra/abstract/10.1103/PhysRevA.52.3457

[2] D. Maslov, On the advantages of using relative phase Toffolis with an application to multiple control Toffoli optimization, Phys. Rev. A 93 (2016). https://journals.aps.org/pra/abstract/10.1103/PhysRevA.93.022311