Source code for pennylane.measurements.vn_entropy

# Copyright 2018-2021 Xanadu Quantum Technologies Inc.

# Licensed under the Apache License, Version 2.0 (the "License");
# you may not use this file except in compliance with the License.
# You may obtain a copy of the License at

#     http://www.apache.org/licenses/LICENSE-2.0

# Unless required by applicable law or agreed to in writing, software
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# WITHOUT WARRANTIES OR CONDITIONS OF ANY KIND, either express or implied.
# See the License for the specific language governing permissions and
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# pylint: disable=protected-access
"""
This module contains the qml.vn_entropy measurement.
"""
from collections.abc import Sequence
from typing import Optional

import pennylane as qml
from pennylane.wires import Wires

from .measurements import StateMeasurement, VnEntropy


[docs]def vn_entropy(wires, log_base=None) -> "VnEntropyMP": r"""Von Neumann entropy of the system prior to measurement. .. math:: S( \rho ) = -\text{Tr}( \rho \log ( \rho )) Args: wires (Sequence[int] or int): The wires of the subsystem log_base (float): Base for the logarithm. Returns: VnEntropyMP: Measurement process instance **Example:** .. code-block:: python3 dev = qml.device("default.qubit", wires=2) @qml.qnode(dev) def circuit_entropy(x): qml.IsingXX(x, wires=[0, 1]) return qml.vn_entropy(wires=[0]) Executing this QNode: >>> circuit_entropy(np.pi/2) 0.6931472 It is also possible to get the gradient of the previous QNode: >>> param = np.array(np.pi/4, requires_grad=True) >>> qml.grad(circuit_entropy)(param) tensor(0.62322524, requires_grad=True) .. note:: Calculating the derivative of :func:`~pennylane.vn_entropy` is currently supported when using the classical backpropagation differentiation method (``diff_method="backprop"``) with a compatible device and finite differences (``diff_method="finite-diff"``). .. note:: ``qml.vn_entropy`` can also be used to compute the entropy of entanglement between two subsystems by computing the Von Neumann entropy of either of the subsystems. .. seealso:: :func:`pennylane.math.vn_entropy`, :func:`pennylane.math.vn_entanglement_entropy` """ wires = Wires(wires) return VnEntropyMP(wires=wires, log_base=log_base)
[docs]class VnEntropyMP(StateMeasurement): """Measurement process that computes the Von Neumann entropy of the system prior to measurement. Please refer to :func:`~pennylane.vn_entropy` for detailed documentation. Args: wires (.Wires): The wires the measurement process applies to. This can only be specified if an observable was not provided. id (str): custom label given to a measurement instance, can be useful for some applications where the instance has to be identified log_base (float): Base for the logarithm. """ def _flatten(self): metadata = (("wires", self.raw_wires), ("log_base", self.log_base)) return (None, None), metadata # pylint: disable=too-many-arguments, unused-argument def __init__( self, wires: Optional[Wires] = None, id: Optional[str] = None, log_base: Optional[float] = None, ): self.log_base = log_base super().__init__(wires=wires, id=id) @property def hash(self): """int: returns an integer hash uniquely representing the measurement process""" fingerprint = (self.__class__.__name__, tuple(self.wires.tolist()), self.log_base) return hash(fingerprint) @property def return_type(self): return VnEntropy @property def numeric_type(self): return float
[docs] def shape(self, shots: Optional[int] = None, num_device_wires: int = 0) -> tuple: return ()
[docs] def process_state(self, state: Sequence[complex], wire_order: Wires): state = qml.math.dm_from_state_vector(state) return qml.math.vn_entropy( state, indices=self.wires, c_dtype=state.dtype, base=self.log_base )
[docs] def process_density_matrix(self, density_matrix: Sequence[complex], wire_order: Wires): return qml.math.vn_entropy( density_matrix, indices=self.wires, c_dtype=density_matrix.dtype, base=self.log_base )