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* Preliminary implementation of the Result class * First `plot_histogram()` implementation * Changing nomenclature in Results class * Update typing * Renaming `Result.sample()` to `Result.get_samples()` * Adding `Result.get_state()` * Refactoring test_simresults.py * Finish UTs
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# Copyright 2023 Pulser Development Team | ||
# | ||
# 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 | ||
# distributed under the License is distributed on an "AS IS" BASIS, | ||
# WITHOUT WARRANTIES OR CONDITIONS OF ANY KIND, either express or implied. | ||
# See the License for the specific language governing permissions and | ||
# limitations under the License. | ||
"""Classes to store measurement results.""" | ||
from __future__ import annotations | ||
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from abc import ABC, abstractmethod | ||
from collections import Counter | ||
from dataclasses import dataclass | ||
from typing import Any | ||
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import matplotlib.pyplot as plt | ||
import numpy as np | ||
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from pulser.register import QubitId | ||
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@dataclass | ||
class Result(ABC): | ||
"""Base class for storing the result of a sequence run.""" | ||
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atom_order: tuple[QubitId, ...] | ||
meas_basis: str | ||
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@property | ||
def sampling_dist(self) -> dict[str, float]: | ||
"""Sampling distribution of the measured bitstring. | ||
Args: | ||
atom_order: The order of the atoms in the bitstrings that | ||
represent the measured states. | ||
meas_basis: The measurement basis. | ||
""" | ||
n = self._size | ||
return { | ||
np.binary_repr(ind, width=n): prob | ||
for ind, prob in enumerate(self._weights()) | ||
if prob != 0 | ||
} | ||
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@property | ||
@abstractmethod | ||
def sampling_errors(self) -> dict[str, float]: | ||
"""The sampling error associated to each bitstring's sampling rate. | ||
Uses the standard error of the mean as a quantifier for sampling error. | ||
""" | ||
pass | ||
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@property | ||
def _size(self) -> int: | ||
return len(self.atom_order) | ||
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@abstractmethod | ||
def _weights(self) -> np.ndarray: | ||
"""The sampling rate for every state in an ordered array.""" | ||
pass | ||
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def get_samples(self, n_samples: int) -> Counter[str]: | ||
"""Takes multiple samples from the sampling distribution. | ||
Args: | ||
n_samples: Number of samples to return. | ||
Returns: | ||
Samples of bitstrings corresponding to measured quantum states. | ||
""" | ||
dist = np.random.multinomial(n_samples, self._weights()) | ||
return Counter( | ||
{ | ||
np.binary_repr(i, self._size): dist[i] | ||
for i in np.nonzero(dist)[0] | ||
} | ||
) | ||
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def get_state(self) -> Any: | ||
"""Gets the quantum state associated with the result. | ||
Can only be defined for emulation results that don't resort to | ||
sampling a quantum state (which is the case for certain types of | ||
noise). | ||
""" | ||
raise NotImplementedError( | ||
f"`{self.__class__.__name__}.get_state()` is not implemented." | ||
) | ||
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def plot_histogram( | ||
self, | ||
min_rate: float = 0.001, | ||
max_n_bitstrings: int | None = None, | ||
show: bool = True, | ||
) -> None: | ||
"""Plots the result in an histogram. | ||
Args: | ||
min_rate: The minimum sampling rate a bitstring must have to be | ||
displayed. | ||
max_n_bitstrings: An optional limit on the number of bitrstrings | ||
displayed. | ||
show: Whether or not to call `plt.show()` before returning. | ||
""" | ||
# TODO: Add error bars | ||
probs = np.array( | ||
Counter(self.sampling_dist).most_common(max_n_bitstrings), | ||
dtype=object, | ||
) | ||
probs = probs[probs[:, 1] >= min_rate] | ||
plt.bar(probs[:, 0], probs[:, 1]) | ||
plt.xticks(rotation="vertical") | ||
plt.ylabel("Probabilites") | ||
if show: | ||
plt.show() | ||
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@dataclass | ||
class SampledResult(Result): | ||
"""Represents the result of a run from a series of samples. | ||
Args: | ||
atom_order: The order of the atoms in the bitstrings that | ||
represent the measured states. | ||
meas_basis: The measurement basis. | ||
bitstring_counts: The number of times each bitstring was | ||
measured. | ||
""" | ||
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bitstring_counts: dict[str, int] | ||
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def __post_init__(self) -> None: | ||
self.n_samples = sum(self.bitstring_counts.values()) | ||
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@property | ||
def sampling_errors(self) -> dict[str, float]: | ||
"""The sampling error associated to each bitstring's sampling rate. | ||
Uses the standard error of the mean as a quantifier for sampling error. | ||
""" | ||
return { | ||
bitstr: np.sqrt(p * (1 - p) / self.n_samples) | ||
for bitstr, p in self.sampling_dist.items() | ||
} | ||
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def _weights(self) -> np.ndarray: | ||
weights = np.zeros(2**self._size) | ||
for bitstr, counts in self.bitstring_counts.items(): | ||
weights[int(bitstr, base=2)] = counts / self.n_samples | ||
return weights / sum(weights) |
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# Copyright 2023 Pulser Development Team | ||
# | ||
# 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 | ||
# distributed under the License is distributed on an "AS IS" BASIS, | ||
# WITHOUT WARRANTIES OR CONDITIONS OF ANY KIND, either express or implied. | ||
# See the License for the specific language governing permissions and | ||
# limitations under the License. | ||
"""Defines a special Result subclass for simulation runs returning states.""" | ||
from __future__ import annotations | ||
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from dataclasses import dataclass | ||
from typing import Union, cast | ||
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import numpy as np | ||
import qutip | ||
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from pulser.result import Result | ||
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@dataclass | ||
class QutipResult(Result): | ||
"""Represents the result of a run as a Qutip QObj. | ||
Args: | ||
atom_order: The order of the atoms in the bitstrings that | ||
represent the measured states. | ||
meas_basis: The measurement basis. | ||
state: The Qobj representing the state. Can be a statevector | ||
or a density matrix. | ||
matching_meas_basis: Whether the measurement basis is the | ||
same as the state's basis. | ||
""" | ||
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state: qutip.Qobj | ||
matching_meas_basis: bool | ||
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@property | ||
def sampling_errors(self) -> dict[str, float]: | ||
"""The sampling error associated to each bitstring's sampling rate. | ||
Uses the standard error of the mean as a quantifier for sampling error. | ||
""" | ||
return {bitstr: 0.0 for bitstr in self.sampling_dist} | ||
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@property | ||
def _dim(self) -> int: | ||
full_state_size = np.prod(self.state.shape) | ||
if not self.state.isket: | ||
full_state_size = np.sqrt(full_state_size) | ||
return cast( | ||
int, np.rint(full_state_size ** (1 / self._size)).astype(int) | ||
) | ||
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@property | ||
def _basis_name(self) -> str: | ||
if self._dim > 2: | ||
return "all" | ||
if self.meas_basis == "XY": | ||
return "XY" | ||
if not self.matching_meas_basis: | ||
return ( | ||
"digital" | ||
if self.meas_basis == "ground-rydberg" | ||
else "ground-rydberg" | ||
) | ||
return self.meas_basis | ||
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def _weights(self) -> np.ndarray: | ||
n = self._size | ||
if not self.state.isket: | ||
probs = np.abs(self.state.diag()) | ||
else: | ||
probs = (np.abs(self.state.full()) ** 2).flatten() | ||
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if self._dim == 2: | ||
if self.matching_meas_basis: | ||
# State vector ordered with r first for 'ground_rydberg' | ||
# e.g. n=2: [rr, rg, gr, gg] -> [11, 10, 01, 00] | ||
# Invert the order -> [00, 01, 10, 11] correspondence | ||
# The same applies in XY mode, which is ordered with u first | ||
weights = ( | ||
probs if self.meas_basis == "digital" else probs[::-1] | ||
) | ||
else: | ||
# Only 000...000 is measured | ||
weights = np.zeros(probs.size) | ||
weights[0] = 1.0 | ||
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elif self._dim == 3: | ||
if self.meas_basis == "ground-rydberg": | ||
one_state = 0 # 1 = |r> | ||
ex_one = slice(1, 3) | ||
elif self.meas_basis == "digital": | ||
one_state = 2 # 1 = |h> | ||
ex_one = slice(0, 2) | ||
else: | ||
raise RuntimeError( | ||
f"Unknown measurement basis '{self.meas_basis}' " | ||
"for a three-level system.'" | ||
) | ||
probs = probs.reshape([3] * n) | ||
weights = np.zeros(2**n) | ||
for dec_val in range(2**n): | ||
ind: list[Union[int, slice]] = [] | ||
for v in np.binary_repr(dec_val, width=n): | ||
if v == "0": | ||
ind.append(ex_one) | ||
else: | ||
ind.append(one_state) | ||
# Eg: 'digital' basis : |1> = index2, |0> = index0, 1 = 0:2 | ||
# p_11010 = sum(probs[2, 2, 0:2, 2, 0:2]) | ||
# We sum all probabilites that correspond to measuring | ||
# 11010, namely hhghg, hhrhg, hhghr, hhrhr | ||
weights[dec_val] = np.sum(probs[tuple(ind)]) | ||
else: | ||
raise NotImplementedError( | ||
"Cannot sample system with single-atom state vectors of " | ||
"dimension > 3." | ||
) | ||
# Takes care of numerical artefacts in case sum(weights) != 1 | ||
return cast(np.ndarray, weights / sum(weights)) | ||
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def get_state( | ||
self, | ||
reduce_to_basis: str | None = None, | ||
ignore_global_phase: bool = True, | ||
tol: float = 1e-6, | ||
normalize: bool = True, | ||
) -> qutip.Qobj: | ||
"""Gets the state with some optional post-processing. | ||
Args: | ||
reduce_to_basis: Reduces the full state vector | ||
to the given basis ("ground-rydberg" or "digital"), if the | ||
population of the states to be ignored is negligible. Doesn't | ||
apply to XY mode. | ||
ignore_global_phase: If True and if the final state is a vector, | ||
changes the final state's global phase such that the largest | ||
term (in absolute value) is real. | ||
tol: Maximum allowed population of each eliminated state. | ||
normalize: Whether to normalize the reduced state. | ||
Returns: | ||
The resulting state. | ||
Raises: | ||
TypeError: If trying to reduce to a basis that would eliminate | ||
states with significant occupation probabilites. | ||
""" | ||
state = self.state.copy() | ||
is_density_matrix = state.isoper | ||
if ignore_global_phase and not is_density_matrix: | ||
full = state.full() | ||
global_ph = float(np.angle(full[np.argmax(np.abs(full))])) | ||
state *= np.exp(-1j * global_ph) | ||
if self._dim != 3: | ||
if reduce_to_basis not in [None, self._basis_name]: | ||
raise TypeError( | ||
f"Can't reduce a system in {self._basis_name}" | ||
+ f" to the {reduce_to_basis} basis." | ||
) | ||
elif reduce_to_basis is not None: | ||
if is_density_matrix: # pragma: no cover | ||
# Not tested as noise in digital or all basis not implemented | ||
raise NotImplementedError( | ||
"Reduce to basis not implemented for density matrix" | ||
" states." | ||
) | ||
if reduce_to_basis == "ground-rydberg": | ||
ex_state = "2" | ||
elif reduce_to_basis == "digital": | ||
ex_state = "0" | ||
else: | ||
raise ValueError( | ||
"'reduce_to_basis' must be 'ground-rydberg' " | ||
+ f"or 'digital', not '{reduce_to_basis}'." | ||
) | ||
ex_inds = [ | ||
i | ||
for i in range(3**self._size) | ||
if ex_state in np.base_repr(i, base=3).zfill(self._size) | ||
] | ||
ex_probs = np.abs(state.extract_states(ex_inds).full()) ** 2 | ||
if not np.all(np.isclose(ex_probs, 0, atol=tol)): | ||
raise TypeError( | ||
"Can't reduce to chosen basis because the population of a " | ||
"state to eliminate is above the allowed tolerance." | ||
) | ||
state = state.eliminate_states(ex_inds, normalize=normalize) | ||
return state.tidyup() |
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