qml.labs.resource_estimation.ResourceTwoQubitComparator¶
- class ResourceTwoQubitComparator(wires=None)[source]¶
Bases:
ResourceOperatorResource class for comparing the integer values encoded in two quantum registers of two qubits each.
This operation modifies the input registers. The original values can be restored by applying the operation’s adjoint.
- Parameters:
wires (Sequence[int], optional) – the wires the operation acts on
- Resources:
The resources are obtained from appendix B, Figure 3 in arXiv:1711.10460. Specifically, the resources are given as \(2\)
CSWAPgates, \(3\)CNOTgates, and \(1\)Xgate. This decomposition requires one clean auxiliary qubit. The circuit which applies the comparison operation on registers \((x0,x1)\) and \((y0, y1)\) is defined as:x1 : ─╭X─╭●────╭●───────┤ y1 : ─╰●─│─────├SWAP────┤ x0 : ─╭X─├SWAP─│─────╭X─┤ y0 : ─╰●─│─────╰SWAP─╰●─┤ |1> : ────╰SWAP──────────┤
Example
The resources for this operation are computed using:
>>> two_qubit_compare = plre.ResourceTwoQubitComparator() >>> print(plre.estimate(two_qubit_compare)) --- Resources: --- Total qubits: 5 Total gates : 10 Qubit breakdown: clean qubits: 1, dirty qubits: 0, algorithmic qubits: 4 Gate breakdown: {'Toffoli': 2, 'CNOT': 7, 'X': 1}
Attributes
Returns a dictionary containing the minimal information needed to compute the resources.
- num_wires = 4¶
- resource_keys = {}¶
- resource_params¶
Returns a dictionary containing the minimal information needed to compute the resources.
- Returns:
An empty dictionary
- Return type:
dict
Methods
adjoint_resource_decomp(*args, **kwargs)Returns a list representing the resources for the adjoint of the operator.
Returns a list representing the resources for a controlled version of the operator.
dequeue(op_to_remove[, context])Remove the given resource operator(s) from the Operator queue.
pow_resource_decomp(pow_z, *args, **kwargs)Returns a list representing the resources for an operator raised to a power.
queue([context])Append the operator to the Operator queue.
resource_decomp(**kwargs)Returns a list representing the resources of the operator.
Returns a compressed representation containing only the parameters of the Operator that are needed to compute the resources.
Returns a compressed representation directly from the operator
tempand_based_decomp(**kwargs)Returns a list representing the resources of the operator.
tracking_name(*args, **kwargs)Returns a name used to track the operator during resource estimation.
Returns the tracking name built with the operator's parameters.
- classmethod adjoint_resource_decomp(*args, **kwargs)¶
Returns a list representing the resources for the adjoint of the operator.
- classmethod controlled_resource_decomp(ctrl_num_ctrl_wires, ctrl_num_ctrl_values, *args, **kwargs)¶
Returns a list representing the resources for a controlled version of the operator.
- Parameters:
ctrl_num_ctrl_wires (int) – the number of qubits the operation is controlled on
ctrl_num_ctrl_values (int) – the number of control qubits, that are controlled when in the \(|0\rangle\) state
- static dequeue(op_to_remove, context=<class 'pennylane.queuing.QueuingManager'>)¶
Remove the given resource operator(s) from the Operator queue.
- classmethod pow_resource_decomp(pow_z, *args, **kwargs)¶
Returns a list representing the resources for an operator raised to a power.
- Parameters:
pow_z (int) – exponent that the operator is being raised to
- queue(context=<class 'pennylane.queuing.QueuingManager'>)¶
Append the operator to the Operator queue.
- classmethod resource_decomp(**kwargs)[source]¶
Returns a list representing the resources of the operator. Each object in the list represents a gate and the number of times it occurs in the circuit.
- Resources:
The resources are obtained from appendix B, Figure 3 in arXiv:1711.10460. Specifically, the resources are given as \(2\)
CSWAPgates, \(3\)CNOTgates, and \(1\)Xgate. This decomposition requires one clean auxiliary qubit. The circuit which applies the comparison operation on registers \((x0,x1)\) and \((y0, y1)\) is defined as:x1 : ─╭X─╭●────╭●───────┤ y1 : ─╰●─│─────├SWAP────┤ x0 : ─╭X─├SWAP─│─────╭X─┤ y0 : ─╰●─│─────╰SWAP─╰●─┤ |1> : ────╰SWAP──────────┤
- Returns:
A list of
GateCountobjects, where each object represents a specific quantum gate and the number of times it appears in the decomposition.- Return type:
list[GateCount]
- classmethod resource_rep()[source]¶
Returns a compressed representation containing only the parameters of the Operator that are needed to compute the resources.
- Returns:
the operator in a compressed representation
- Return type:
- resource_rep_from_op()¶
Returns a compressed representation directly from the operator
- classmethod tempand_based_decomp(**kwargs)[source]¶
Returns a list representing the resources of the operator. Each object in the list represents a gate and the number of times it occurs in the circuit.
- Resources:
The resources are obtained from appendix B, Figure 3 in arXiv:1711.10460. Specifically, the resources are given as \(2\)
CSWAPgates, \(3\)CNOTgates, and \(1\)Xgate. This decomposition is modified to use TempAND gates for building blocks of CSWAP gates.x1 : ─╭X─╭●────╭●───────┤ y1 : ─╰●─│─────├SWAP────┤ x0 : ─╭X─├SWAP─│─────╭X─┤ y0 : ─╰●─│─────╰SWAP─╰●─┤ |1> : ────╰SWAP──────────┤
- classmethod tracking_name(*args, **kwargs)¶
Returns a name used to track the operator during resource estimation.
- tracking_name_from_op()¶
Returns the tracking name built with the operator’s parameters.