qiskit/pulse/pulse_lib/continuous.py
def drag(times: np.ndarray, amp: complex, center: float, sigma: float, beta: float,
         zeroed_width: Union[None, float] = None, rescale_amp: bool = False) -> np.ndarray:
    r"""Continuous Y-only correction DRAG pulse for standard nonlinear oscillator (SNO) [1].

    [1] Gambetta, J. M., Motzoi, F., Merkel, S. T. & Wilhelm, F. K.
        Analytic control methods for high-fidelity unitary operations
        in a weakly nonlinear oscillator. Phys. Rev. A 83, 012308 (2011).


    Args:
        times: Times to output pulse for.
        amp: Pulse amplitude at `center`.
        center: Center (mean) of pulse.
        sigma: Width (standard deviation) of pulse.
        beta: Y correction amplitude. For the SNO this is $\beta=-\frac{\lambda_1^2}{4\Delta_2}$.
            Where $\lambds_1$ is the relative coupling strength between the first excited and second
            excited states and $\Delta_2$ is the detuning between the resepective excited states.
        zeroed_width: Subtract baseline to gaussian pulses to make sure
                 $\Omega_g(center \pm zeroed_width/2)=0$ is satisfied. This is used to avoid
                 large discontinuities at the start of a gaussian pulse.
        rescale_amp: If `zeroed_width` is not `None` and `rescale_amp=True` the pulse will
                     be rescaled so that $\Omega_g(center)-\Omega_g(center\pm zeroed_width/2)=amp$.

    """
    gauss_deriv, gauss = gaussian_deriv(times, amp=amp, center=center, sigma=sigma,
                                        ret_gaussian=True)
    if zeroed_width is not None:
        gauss, scale_factor = _fix_gaussian_width(gauss, amp=amp, center=center, sigma=sigma,
                                                  zeroed_width=zeroed_width,
                                                  rescale_amp=rescale_amp,
                                                  ret_scale_factor=True)
        gauss_deriv *= scale_factor

    return gauss + 1j*beta*gauss_deriv
def drag(times: np.ndarray, amp: complex, center: float, sigma: float, beta: float,
         zeroed_width: Union[None, float] = None, rescale_amp: bool = False) -> np.ndarray:
    r"""Continuous Y-only correction DRAG pulse for standard nonlinear oscillator (SNO) [1].

    [1] Gambetta, J. M., Motzoi, F., Merkel, S. T. & Wilhelm, F. K.
        Analytic control methods for high-fidelity unitary operations
        in a weakly nonlinear oscillator. Phys. Rev. A 83, 012308 (2011).


    Args:
        times: Times to output pulse for.
        amp: Pulse amplitude at `center`.
        center: Center (mean) of pulse.
        sigma: Width (standard deviation) of pulse.
        beta: Y correction amplitude. For the SNO this is $\beta=-\frac{\lambda_1^2}{4\Delta_2}$.
            Where $\lambds_1$ is the relative coupling strength between the first excited and second
            excited states and $\Delta_2$ is the detuning between the resepective excited states.
        zeroed_width: Subtract baseline to gaussian pulses to make sure
                 $\Omega_g(center \pm zeroed_width/2)=0$ is satisfied. This is used to avoid
                 large discontinuities at the start of a gaussian pulse.
        rescale_amp: If `zeroed_width` is not `None` and `rescale_amp=True` the pulse will
                     be rescaled so that $\Omega_g(center)-\Omega_g(center\pm zeroed_width/2)=amp$.

    """
    gauss_deriv, gauss = gaussian_deriv(times, amp=amp, center=center, sigma=sigma,
                                        ret_gaussian=True)
    if zeroed_width is not None:
        gauss, scale_factor = _fix_gaussian_width(gauss, amp=amp, center=center, sigma=sigma,
                                                  zeroed_width=zeroed_width,
                                                  rescale_amp=rescale_amp,
                                                  ret_scale_factor=True)
        gauss_deriv *= scale_factor

    return gauss + 1j*beta*gauss_deriv
def drag ( times : np . ndarray , amp : complex , center : float , sigma : float , beta : float , zeroed_width : Union [ None , float ] = None , rescale_amp : bool = False ) -> np . ndarray : gauss_deriv , gauss = gaussian_deriv ( times , amp = amp , center = center , sigma = sigma , ret_gaussian = True ) if zeroed_width is not None : gauss , scale_factor = _fix_gaussian_width ( gauss , amp = amp , center = center , sigma = sigma , zeroed_width = zeroed_width , rescale_amp = rescale_amp , ret_scale_factor = True ) gauss_deriv *= scale_factor return gauss + 1j * beta * gauss_deriv
r"""Continuous Y-only correction DRAG pulse for standard nonlinear oscillator (SNO) [1].

    [1] Gambetta, J. M., Motzoi, F., Merkel, S. T. & Wilhelm, F. K.
        Analytic control methods for high-fidelity unitary operations
        in a weakly nonlinear oscillator. Phys. Rev. A 83, 012308 (2011).


    Args:
        times: Times to output pulse for.
        amp: Pulse amplitude at `center`.
        center: Center (mean) of pulse.
        sigma: Width (standard deviation) of pulse.
        beta: Y correction amplitude. For the SNO this is $\beta=-\frac{\lambda_1^2}{4\Delta_2}$.
            Where $\lambds_1$ is the relative coupling strength between the first excited and second
            excited states and $\Delta_2$ is the detuning between the resepective excited states.
        zeroed_width: Subtract baseline to gaussian pulses to make sure
                 $\Omega_g(center \pm zeroed_width/2)=0$ is satisfied. This is used to avoid
                 large discontinuities at the start of a gaussian pulse.
        rescale_amp: If `zeroed_width` is not `None` and `rescale_amp=True` the pulse will
                     be rescaled so that $\Omega_g(center)-\Omega_g(center\pm zeroed_width/2)=amp$.
r Continuous Y - only correction DRAG pulse for standard nonlinear oscillator ( SNO ) [ 1 ] .