Source code for qiskit_experiments.library.characterization.analysis.drag_analysis

# This code is part of Qiskit.
#
# (C) Copyright IBM 2021.
#
# This code is licensed under the Apache License, Version 2.0. You may
# obtain a copy of this license in the LICENSE.txt file in the root directory
# of this source tree or at http://www.apache.org/licenses/LICENSE-2.0.
#
# Any modifications or derivative works of this code must retain this
# copyright notice, and modified files need to carry a notice indicating
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"""DRAG pulse calibration experiment."""

import warnings
from typing import List, Union

import lmfit
import numpy as np

import qiskit_experiments.curve_analysis as curve
from qiskit_experiments.framework import ExperimentData
from qiskit_experiments.exceptions import AnalysisError


[docs] class DragCalAnalysis(curve.CurveAnalysis): r"""Drag calibration analysis based on a fit to a cosine function. # section: fit_model Analyse a Drag calibration experiment by fitting multiple series each to a cosine function. All functions share the phase parameter (i.e. beta), amplitude, and baseline. The frequencies of the oscillations are related through the number of repetitions of the Drag gates. Several initial guesses are tried if the user does not provide one. The fit function is .. math:: y_i = {\rm amp} \cos\left(2 \pi\cdot {\rm reps}_i \cdot {\rm freq}\cdot x - 2 \pi\cdot {\rm reps}_i \cdot {\rm freq}\cdot \beta\right) + {\rm base} Here, the fit parameter :math:`freq` is the frequency of the oscillation of a single pair of Drag plus and minus rotations and :math:`{\rm reps}_i` is the number of times that the Drag plus and minus rotations are repeated in curve :math:`i`. Note that the aim of the Drag calibration is to find the :math:`\beta` that minimizes the phase shifts. This implies that the optimal :math:`\beta` occurs when all :math:`y` curves are minimum, i.e. they produce the ground state. This occurs when .. math:: {\rm reps}_i * {\rm freq} * (x - \beta) = N is satisfied with :math:`N` an integer. Note, however, that this condition produces a minimum only when the amplitude is negative. To ensure this is the case, we bound the amplitude to be less than 0. # section: fit_parameters defpar \rm amp: desc: Amplitude of all series. init_guess: The maximum y value scaled by -1, -0.5, and -0.25. bounds: [-2, 0] scaled to the maximum signal value. defpar \rm base: desc: Base line of all series. init_guess: Half the maximum y-value of the data. bounds: [-1, 1] scaled to the maximum y-value. defpar {\rm freq}: desc: Frequency of oscillation as a function of :math:`\beta` for a single pair of DRAG plus and minus pulses. init_guess: For the curve with the most Drag pulse repetitions, the peak frequency of the power spectral density is found and then divided by the number of repetitions. bounds: [0, inf]. defpar \beta: desc: Common beta offset. This is the parameter of interest. init_guess: Linearly spaced between the maximum and minimum scanned beta. bounds: [-min scan range, max scan range]. """ @classmethod def _default_options(cls): """Return the default analysis options.""" default_options = super()._default_options() default_options.plotter.set_figure_options( xlabel="Beta", ylabel="Signal (arb. units)", ) default_options.result_parameters = ["beta"] default_options.normalization = True return default_options
[docs] def set_options(self, **fields): if "reps" in fields: warnings.warn( "Analysis option 'reps' has been dropped and analysis is bootstrapped by " "circuit metadata. Setting this option no longer impacts analysis result.", DeprecationWarning, ) del fields["reps"] super().set_options(**fields)
def _generate_fit_guesses( self, user_opt: curve.FitOptions, curve_data: curve.ScatterTable, ) -> Union[curve.FitOptions, List[curve.FitOptions]]: """Create algorithmic initial fit guess from analysis options and curve data. Args: user_opt: Fit options filled with user provided guess and bounds. curve_data: Formatted data collection to fit. Returns: List of fit options that are passed to the fitter function. """ # Use the highest-frequency curve to estimate the oscillation frequency. max_rep_model_name = self.model_names()[-1] max_rep = self.options.data_subfit_map[max_rep_model_name]["nrep"] curve_data = curve_data.filter(series=max_rep_model_name) x_data = curve_data.x min_beta, max_beta = min(x_data), max(x_data) freqs_guess = curve.guess.frequency(curve_data.x, curve_data.y) / max_rep user_opt.p0.set_if_empty(freq=freqs_guess) avg_x = (max(x_data) + min(x_data)) / 2 span_x = max(x_data) - min(x_data) beta_bound = max(5 / user_opt.p0["freq"], span_x) ptp_y = np.ptp(curve_data.y) user_opt.bounds.set_if_empty( amp=(-2 * ptp_y, 0), freq=(0, np.inf), beta=(avg_x - beta_bound, avg_x + beta_bound), base=(min(curve_data.y) - ptp_y, max(curve_data.y) + ptp_y), ) base_guess = (max(curve_data.y) - min(curve_data.y)) / 2 user_opt.p0.set_if_empty(base=(user_opt.p0["amp"] or base_guess)) # Drag curves can sometimes be very flat, i.e. averages of y-data # and min-max do not always make good initial guesses. We therefore add # 0.5 to the initial guesses. Note that we also set amp=-0.5 because the cosine function # becomes +1 at zero phase, i.e. optimal beta, in which y data should become zero # in discriminated measurement level. options = [] for amp_factor in (-1, -0.5, -0.25): for beta_guess in np.linspace(min_beta, max_beta, 20): new_opt = user_opt.copy() new_opt.p0.set_if_empty(amp=ptp_y * amp_factor, beta=beta_guess) options.append(new_opt) return options def _run_curve_fit( self, curve_data: curve.ScatterTable, ) -> curve.CurveFitResult: r"""Perform curve fitting on given data collection and fit models. .. note:: This class post-processes the fit result from a Drag analysis. The Drag analysis should return the beta value that is closest to zero. Since the oscillating term is of the form .. math:: \cos(2 \pi\cdot {\rm reps}_i \cdot {\rm freq}\cdot [x - \beta]) There is a periodicity in beta. This post processing finds the beta that is closest to zero by performing the minimization using the modulo function. .. math:: n_\text{min} = \min_{n}|\beta_\text{fit} + n / {\rm freq}| and assigning the new beta value to .. math:: \beta = \beta_\text{fit} + n_\text{min} / {\rm freq}. Args: curve_data: Formatted data to fit. Returns: The best fitting outcome with minimum reduced chi-squared value. """ fit_result = super()._run_curve_fit(curve_data) if fit_result and fit_result.params is not None: beta = fit_result.params["beta"] freq = fit_result.params["freq"] min_beta = ((beta + 1 / freq / 2) % (1 / freq)) - 1 / freq / 2 fit_result.params["beta"] = min_beta return fit_result def _evaluate_quality(self, fit_data: curve.CurveFitResult) -> Union[str, None]: """Algorithmic criteria for whether the fit is good or bad. A good fit has: - a reduced chi-squared lower than three and greater than zero, - a DRAG parameter value within the first period of the lowest number of repetitions, - an error on the drag beta smaller than the beta. """ fit_beta = fit_data.ufloat_params["beta"] fit_freq = fit_data.ufloat_params["freq"] criteria = [ 0 < fit_data.reduced_chisq < 3, abs(fit_beta.nominal_value) < 1 / fit_freq.nominal_value / 2, curve.utils.is_error_not_significant(fit_beta), ] if all(criteria): return "good" return "bad" def _initialize( self, experiment_data: ExperimentData, ): reps = set(d.get("metadata", None).get("nrep", None) for d in experiment_data.data()) if None in reps: reps.remove(None) if not reps: raise AnalysisError( f"{self.__class__.__name__} expects 'nrep' value in circuit metadata. " "Please setup your experiment circuits with proper metadata." ) reps = sorted(reps) # Model is initialized at runtime because # the experiment option "reps" can be changed before experiment run. models = [] data_subfit_map = {} for nrep in sorted(reps): name = f"nrep={nrep}" models.append( lmfit.models.ExpressionModel( expr=f"amp * cos(2 * pi * {nrep} * freq * (x - beta)) + base", name=name, ) ) data_subfit_map[name] = {"nrep": nrep} self._models = models self._options.data_subfit_map = data_subfit_map super()._initialize(experiment_data)