pybaselines.Baseline.iasls
- Baseline.iasls(data, lam=1000000.0, p=0.01, lam_1=0.0001, max_iter=50, tol=0.001, weights=None, diff_order=2)[source]
Fits the baseline using the improved asymmetric least squares (IAsLS) algorithm.
The algorithm consideres both the first and second derivatives of the residual.
- Parameters:
- dataarray_like, shape (N,)
The y-values of the measured data, with N data points. Must not contain missing data (NaN) or Inf.
- lam
float, optional The smoothing parameter. Larger values will create smoother baselines. Default is 1e6.
- p
float, optional The penalizing weighting factor. Must be between 0 and 1. Values greater than the baseline will be given p weight, and values less than the baseline will be given 1 - p weight. Default is 1e-2.
- lam_1
float, optional The smoothing parameter for the first derivative of the residual. Default is 1e-4.
- max_iter
int, optional The max number of fit iterations. Default is 50.
- tol
float, optional The exit criteria. Default is 1e-3.
- weightsarray_like, shape (N,), optional
The weighting array. If None (default), then the initial weights will be set by fitting the data with a second order polynomial.
- diff_order
int, optional The order of the differential matrix. Must be greater than 1. Default is 2 (second order differential matrix). Typical values are 2 or 3.
- Returns:
- baseline
numpy.ndarray, shape (N,) The calculated baseline.
- params
dict A dictionary with the following items:
- 'weights': numpy.ndarray, shape (N,)
The weight array used for fitting the data.
- 'tol_history': numpy.ndarray
An array containing the calculated tolerance values for each iteration. The length of the array is the number of iterations completed. If the last value in the array is greater than the input tol value, then the function did not converge.
- baseline
- Raises:
ValueErrorRaised if p is not between 0 and 1 or if diff_order is less than 2.
References
He, S., et al. Baseline correction for raman spectra using an improved asymmetric least squares method, Analytical Methods, 2014, 6(12), 4402-4407.