Source code for coolest.api.util

__author__ = 'aymgal'


import os
import math
import numpy as np
# from astropy.coordinates import SkyCoord
from skimage import measure

from coolest.template.json import JSONSerializer


[docs] def convert_image_to_data_units(image, mag_tot, mag_zero_point=None, coolest_object=None): """ Rescale an image such that it has units of electrons per second (e/s), given a total magnitude and a magnitude zero-point. After rescaling, the total magnitude of the image_rescaled should corresponds to `-2.5 * np.log10(image_rescaled.sum()) + mag_zero_point = mag_tot` where `mag_zero_point` corresponds to the magnitude of 1 e/s. :param image: input image, as a 2D array. :param mag_tot: target total magnitude, integrated over the whole image :param mag_zero_point: magnitude zero point of the observation (that corresponds to 1 e/s). If coolest_object is not None, mag_zero_point is ignored. :param coolest_object: if given, will be used to retrieve the zero-point magnitude of the observation. """ if coolest_object is None and mag_zero_point is None: raise ValueError("Either a COOLEST object or a zero-point magnitude should be provided.") flux_tot = np.sum(image) image_unit_flux = image / flux_tot if coolest_object is not None: mag_zp = coolest.observation.mag_zero_point else: mag_zp = mag_zero_point delta_mag = mag_tot - mag_zp flux_unit_mag = 10 ** ( - delta_mag / 2.5 ) image_rescaled = image_unit_flux * flux_unit_mag return image_rescaled
[docs] def get_coolest_object(file_path, verbose=False, **kwargs_serializer): if not os.path.isabs(file_path): file_path = os.path.abspath(file_path) serializer = JSONSerializer(file_path, **kwargs_serializer) return serializer.load(verbose=verbose)
[docs] def get_coordinates(coolest_object, offset_x=0., offset_y=0.): from coolest.api.coordinates import Coordinates # prevents circular import errors nx, ny = coolest_object.observation.pixels.shape pix_scl = coolest_object.instrument.pixel_size half_size_x, half_size_y = nx * pix_scl / 2., ny * pix_scl / 2. x_at_ij_0 = - half_size_x + pix_scl / 2. # position of x=0 with respect to bottom left pixel y_at_ij_0 = - half_size_y + pix_scl / 2. # position of y=0 with respect to bottom left pixel matrix_pix2ang = pix_scl * np.eye(2) # transformation matrix pixel <-> angle return Coordinates(nx, ny, matrix_ij_to_xy=matrix_pix2ang, x_at_ij_0=x_at_ij_0 + offset_x, y_at_ij_0=y_at_ij_0 + offset_y)
[docs] def get_coordinates_from_regular_grid(field_of_view_x, field_of_view_y, num_pix_x, num_pix_y): from coolest.api.coordinates import Coordinates # prevents circular import errors pix_scl_x = np.abs(field_of_view_x[0] - field_of_view_x[1]) / num_pix_x pix_scl_y = np.abs(field_of_view_y[0] - field_of_view_y[1]) / num_pix_y matrix_pix2ang = np.array([[pix_scl_x, 0.], [0., pix_scl_y]]) x_at_ij_0 = field_of_view_x[0] + pix_scl_x / 2. y_at_ij_0 = field_of_view_y[0] + pix_scl_y / 2. return Coordinates( num_pix_x, num_pix_y, matrix_ij_to_xy=matrix_pix2ang, x_at_ij_0=x_at_ij_0, y_at_ij_0=y_at_ij_0, )
[docs] def get_coordinates_set(coolest_file_list, reference=0): coordinates_list = [] for coolest_file in coolest_file_list: # TODO: compute correct offsets when each file has # obs = self.coolest.observation # sky_coord = SkyCoord(obs.ra, obs.dec, frame='icrs') # ra, dec = sky_coord.to_string(style='hmsdms').split(' ') coordinates = get_coordinates(coolest_file) coordinates_list.append(coordinates) return coordinates_list
[docs] def array2image(array, nx=0, ny=0): """Convert a 1d array into a 2d array. Note: this only works when length of array is a perfect square, or else if nx and ny are provided :param array: image values :type array: array of size n**2 :returns: 2d array :raises: AttributeError, KeyError """ if nx == 0 or ny == 0: # Avoid turning n into a JAX-traced object with jax.numpy.sqrt n = int(np.sqrt(len(array))) if n**2 != len(array): err_msg = f"Input array size {len(array)} is not a perfect square." raise ValueError(err_msg) nx, ny = n, n image = array.reshape(int(nx), int(ny)) return image
[docs] def image2array(image): """Convert a 2d array into a 1d array. :param array: image values :type array: array of size (n,n) :returns: 1d array :raises: AttributeError, KeyError """ # nx, ny = image.shape # find the size of the array # imgh = np.reshape(image, nx * ny) # change the shape to be 1d # return imgh return image.ravel()
[docs] def downsampling(image, factor=1): if factor < 1: raise ValueError(f"Downscaling factor must be > 1") if factor == 1: return image f = int(factor) nx, ny = np.shape(image) if int(nx/f) == nx/f and int(ny/f) == ny/f: down = image.reshape([int(nx/f), f, int(ny/f), f]).mean(3).mean(1) return down else: raise ValueError(f"Downscaling factor {factor} is not possible with shape ({nx}, {ny})")
[docs] def effective_radius(light_map, x, y, outer_radius=10, initial_guess=1, initial_delta_pix=10, n_iter=10): """Computes the effective radius of the 2D surface brightness profile, based on a definition similar to the half-light radius. NOTE: This functions assumes that the profile is centered on the grid. Parameters ---------- light_map : ndarray 2D array of the light model x : ndarray x-coordinates associated to the light model y : ndarray y-coordinates associated to the light model outer_radius : int, optional outer limit of integration within which half the light is calculated to estimate the effective radius, by default 10 initial_guess : int, optional Initial guess for effective radius in arcsecond, by default 1 initial_delta_pix : int, optional Initial step size in pixels before shrinking in future iterations, by default 10 n_iter : int, optional Number of iterations, by default 5 Returns ------- (float, float) Effective radius and spacing of the coordinates grid (approximate accuracy) Raises ------ RuntimeError If integration loop exceeds outer bound before convergence. """ #initialize grid_res=np.abs(x[0,0]-x[0,1]) initial_delta=grid_res*initial_delta_pix #default inital step size is 10 pixels r_grid=np.hypot(x, y) total_light=np.sum(light_map[r_grid<outer_radius]) cumulative_light=np.sum(light_map[r_grid<initial_guess]) if cumulative_light < total_light/2: #move outward direction=1 elif cumulative_light > total_light/2: #move inward direction=-1 else: return initial_guess, grid_res r_eff=initial_guess delta=initial_delta loopcount=0 for n in range(n_iter): #overshoots, turn around and backtrack at higher precision while (total_light/2.-cumulative_light)*direction>0: if loopcount > 100: raise RuntimeError('Stuck in very long (possibly infinite) loop') r_eff=r_eff+delta*direction cumulative_light=np.sum(light_map[r_grid<r_eff]) loopcount+=1 direction=direction*-1 delta=delta/2. return r_eff, grid_res
[docs] def ellipticity_from_moments(light_map, pixel_size): # compute central momoments try: # scikit-image version 0.19.3 and older mu = measure.moments_central(light_map, order=2, spacing=(pixel_size, pixel_size)) except IndexError: # scikit-image version 0.20.0 and beyond mu = measure.moments_central(light_map, order=2, spacing=pixel_size) # use the moments to estimate orientation and ellipticity (https://en.wikipedia.org/wiki/Image_moment) mu_20_ = mu[2, 0] / mu[0, 0] mu_02_ = mu[0, 2] / mu[0, 0] mu_11_ = mu[1, 1] / mu[0, 0] lambda_1 = (mu_20_ + mu_02_) / 2. + np.sqrt(4*mu_11_**2 + (mu_20_ - mu_02_)**2) / 2. lambda_2 = (mu_20_ + mu_02_) / 2. - np.sqrt(4*mu_11_**2 + (mu_20_ - mu_02_)**2) / 2. q = np.sqrt(lambda_2 / lambda_1) # b/a, axis ratio phi = np.arctan(2. * mu_11_ / (mu_20_ - mu_02_)) / 2. # position angle if mu_02_ > mu_20_: phi += np.pi / 2. # makes it consistent angles conventions in COOLEST return phi, q
[docs] def azim_averaged_two_point_correlation(light_image, dpix, rmax, Nbins): """ The two point correlation function can be obtained from the covariance matrix of an image and the distances between its pixels. By binning the covariance matrix entries in distance (or radial) bins, one can obtain the 1D correlation function. There are two ways to obtain the covariance matrix: 1) it is equivalent to the inverse Fourier transform of the power spectrum, and 2) by calculating explicitly the covariance between any two pixels Here we use the first way. Parameters ---------- light_image : 2D ndarray Pixels of the image to analyse. dpix : float Pixel size Nbins : int, optional The number of radial bins to use for converting the 2D covariance matrix into a 1D correlation function. rmax : float, optional A value for the maximum extent of the radial bins. If none is given then it is equal to half the diagonal of the provided image. Returns ------- (array, array, array, array) The location, value, uncertainty and covariance matrix The covariance matrix here is the inverse of fourier transform of power spectrum) """ # Fourier transform image fouriertf = np.fft.fft2(light_image, norm='ortho') # Power spectrum (the square of the signal) absval2 = fouriertf.real**2 + fouriertf.imag**2 # Covariance matrix (the inverse fourier transform of the power spectrum) complex_cov = np.fft.fftshift(np.fft.ifft2(absval2, norm='ortho')) cov = complex_cov.real # Bin the 2D covariance matrix into radial bins rmin = 0.0 dr = (rmax-rmin)/Nbins bins = np.arange(rmin,rmax,dr) vals = [[] for _ in range(len(bins))] # Ni = Nj = the total number of pixels in the image Ni = cov.shape[1] Nj = cov.shape[0] for i in range(0,Ni): for j in range(0,Nj): r = np.hypot((j-Nj/2.0)*dpix,(i-Ni/2.0)*dpix) if r < rmax and i != j: index = int(np.floor(r/dr)) vals[index].append(cov[i][j]) means = np.zeros(len(bins)) sdevs = np.zeros(len(bins)) for i in range(0,len(bins)): if len(vals[i]) > 0: means[i] = np.mean(vals[i]) sdevs[i] = np.std(vals[i]) return bins, means, sdevs, cov
[docs] def lensing_information(data_lens_sub, x, y, theta_E, noise_map, center_x_lens=0, center_y_lens=0, a=16, b=0, arc_mask=None): """ Computes the 'lensing information' defined in Tan et al. 2023, Equations (8) and (9). https://ui.adsabs.harvard.edu/abs/2023arXiv231109307T/abstract Parameters ---------- data_lens_sub : np.ndarray Imaging data as a 2D array. It is assumed to contain no lens light. x : np.ndarray 2D array of x coordinates, in arcsec. y : np.ndarray 2D array of y coordinates, in arcsec. theta_E : float Einstein radius in arcsec, by default None noise_map : np.ndarray 2D array with 1-sigma noise level per pixel (same units as `data_lens_sub`), by default None center_x_lens : int, optional x coordinates of the center of the lens, by default 0 center_y_lens : int, optional y coordinates of the center of the lens, by default 0 a : int, optional Exponent in Eq. (9) from Yi Tan et al. 2023, by default 16 b : int, optional Exponent in Eq. (9) from Yi Tan et al. 2023, by default 0 arc_mask : np.ndarray, optional Binary 2D array with 1s where there is are lensed arcs, by default None Returns ------- 4-tuple Lensing information I, Einstein radius, reference azimuthal angle, total mask used for computing I """ if arc_mask is None: arc_mask = np.ones_like(data_lens_sub) # estimate background noise from one corner of the noise map sigma_bkg = np.mean(noise_map[:10, :10]) # build a mask to only consider pixels at least 3 times the background noise level snr_mask = np.where(data_lens_sub > 3.*sigma_bkg, 1., 0.) # combine user mask and SNR mask arc_mask_tot = snr_mask * arc_mask # shift coordinates so that lens is at (0, 0) theta_x, theta_y = x - center_x_lens, y - center_y_lens # compute polar coordinates centered on the lens theta_r = np.hypot(theta_x, theta_y) phi = np.arctan2(theta_y, theta_x) # find index of the brightest pixel (within the arc mask) max_idx = np.where(data_lens_sub == (data_lens_sub*arc_mask_tot).max()) # get azimuthal angle corresponding to the brightest pixel phi_ref = float(np.arctan2(theta_y[max_idx], theta_x[max_idx])) # compute the weights following Eq. (9) from Yi Tan et al. 2023 weights = ( 1. + np.abs(theta_r - theta_E) / theta_E * (1 + np.abs(phi - phi_ref) / phi_ref)**b )**a # compute the weighted sum numerator = np.sum(arc_mask_tot*weights*data_lens_sub) denominator = np.sqrt(np.sum(arc_mask_tot*noise_map**2)) lens_I = numerator / denominator return lens_I, theta_E, phi_ref, arc_mask_tot
[docs] def split_lens_source_params(coolest_list, name_list, lens_light=False): """ Read several json files already containing a model with the results of this model fitting INPUT ----- file_list: list, list of path or names of the file to read name_list: list, list of shorter names to distinguish the files lens_light: bool, if True, computes the lens light kwargs as well (not yet implemented) OUTPUT ------ param_all_lens, param_all_source: organized dictionaries readable by plotting function """ param_all_lens = {} param_all_source = {} for idx_file, file_name in enumerate(name_list): print(file_name) coolest_obj = coolest_list[idx_file] if coolest_obj.mode == 'MAP': print('LENS COOLEST : ', coolest_obj.mode) else: print('LENS COOLEST IS NOT MAP, BUT IS ', coolest_obj.mode) lensing_entities_list = coolest_obj.lensing_entities param_lens = {} param_source = {} if lensing_entities_list is not None: creation_lens_source_light = True idx_lens = 0 idx_lens_light = 0 idx_source = 0 idx_ps = 0 min_red = 0 max_red = 5 creation_red_list = True red_list = [] MultiPlane = False for lensing_entity in lensing_entities_list: red_list.append(lensing_entity.redshift) min_red = np.min(red_list) max_red = np.max(red_list) for lensing_entity in lensing_entities_list: if lensing_entity.type == "Galaxy": galac = lensing_entity if galac.redshift > min_red: # SOURCE OF LIGHT light_list = galac.light_model for light in light_list: if light.type == 'Sersic': read_sersic(light, param_source) idx_source += 1 else: print('Light Type ', light.type, ' not yet implemented.') if galac.redshift < max_red: # LENSING GALAXY if galac.redshift > min_red: MultiPlane = True print('Multiplane lensing to consider.') mass_list = galac.mass_model for mass in mass_list: if mass.type == 'PEMD': read_pemd(mass, param_lens) idx_lens += 1 elif mass.type == 'SIE': read_sie(mass, param_lens) idx_lens += 1 else: print('Mass Type ', mass.type, ' not yet implemented.') if (galac.redshift <= min_red) and (galac.redshift >= max_red): print('REDSHIFT ', galac.redshift, ' is not in the range ]', min_red, ',', max_red, '[') elif lensing_entity.type == "MassField": shear_list = lensing_entity.mass_model for shear_idx in shear_list: if shear_idx.type == 'ExternalShear': read_shear(shear_idx, param_lens) idx_lens += 1 else: print("type of Shear ", shear_idx.type, " not implemented") else: print("Lensing entity of type ", lensing_enity.type, " is unknown.") param_all_lens[name_list[idx_file]] = param_lens param_all_source[name_list[idx_file]] = param_source return param_all_lens, param_all_source
[docs] def read_shear(mass, param={}, prefix='SHEAR_0_'): """ Reads the parameters of a coolest.template.classes.profiles.mass.ExternalShear object INPUT ----- mass : coolest.template.classes.profiles.mass.ExternalShear object param : dict, already existing dictionnary with ordered parameters readable by plotting function prefix : str, prefix to use in saving parameters names OUTPUT ------ param : updated param """ for mass_name, mass_param in mass.parameters.items(): p = getattr(mass_param.point_estimate, 'value') p_84 = getattr(mass_param.posterior_stats, 'percentile_84th') p_16 = getattr(mass_param.posterior_stats, 'percentile_16th') p_med = getattr(mass_param.posterior_stats, 'median') p_mean = getattr(mass_param.posterior_stats, 'mean') latex_name = getattr(mass_param, 'latex_str') if mass_name == 'gamma_ext': param[prefix + 'gamma_ext'] = {'point_estimate': p, 'percentile_84th': p_84, 'percentile_16th': p_16, 'median': p_med, 'mean': p_mean, 'latex_str': latex_name} elif mass_name == 'phi_ext': param[prefix + 'phi_ext'] = {'point_estimate': p, 'percentile_84th': p_84, 'percentile_16th': p_16, 'median': p_med, 'mean': p_mean, 'latex_str': latex_name} else: print(shear_name, " not known") print('\t Shear correctly added') return param
[docs] def read_pemd(mass, param={}, prefix='PEMD_0_'): """ Reads the parameters of a coolest.template.classes.profiles.mass.PEMD object INPUT ----- mass : coolest.template.classes.profiles.mass.PEMD object param : dict, already existing dictionnary with ordered parameters readable by plotting function prefix : str, prefix to use in saving parameters names OUTPUT ------ param : updated param """ for mass_name, mass_param in mass.parameters.items(): p = getattr(mass_param.point_estimate, 'value') p_84 = getattr(mass_param.posterior_stats, 'percentile_84th') p_16 = getattr(mass_param.posterior_stats, 'percentile_16th') p_med = getattr(mass_param.posterior_stats, 'median') p_mean = getattr(mass_param.posterior_stats, 'mean') latex_name = getattr(mass_param, 'latex_str') if mass_name == 'theta_E': param[prefix + 'theta_E'] = {'point_estimate': p, 'percentile_84th': p_84, 'percentile_16th': p_16, 'median': p_med, 'mean': p_mean, 'latex_str': latex_name} elif mass_name == 'q': param[prefix + 'q'] = {'point_estimate': p, 'percentile_84th': p_84, 'percentile_16th': p_16, 'median': p_med, 'mean': p_mean, 'latex_str': latex_name} elif mass_name == 'phi': param[prefix + 'phi'] = {'point_estimate': p, 'percentile_84th': p_84, 'percentile_16th': p_16, 'median': p_med, 'mean': p_mean, 'latex_str': latex_name} elif mass_name == 'center_x': param[prefix + 'cx'] = {'point_estimate': p, 'percentile_84th': p_84, 'percentile_16th': p_16, 'median': p_med, 'mean': p_mean, 'latex_str': latex_name} elif mass_name == 'center_y': param[prefix + 'cy'] = {'point_estimate': p, 'percentile_84th': p_84, 'percentile_16th': p_16, 'median': p_med, 'mean': p_mean, 'latex_str': latex_name} elif mass_name == 'gamma': param[prefix + 'gamma'] = {'point_estimate': p, 'percentile_84th': p_84, 'percentile_16th': p_16, 'median': p_med, 'mean': p_mean, 'latex_str': latex_name} else: print(mass_name, " not known") print('\t PEMD correctly added') return param
[docs] def read_sie(mass, param={}, prefix='SIE_0_'): """ Reads the parameters of a coolest.template.classes.profiles.mass.SIE object INPUT ----- mass : coolest.template.classes.profiles.mass.SIE object param : dict, already existing dictionnary with ordered parameters readable by plotting function prefix : str, prefix to use in saving parameters names OUTPUT ------ param : updated param """ for mass_name, mass_param in mass.parameters.items(): p = getattr(mass_param.point_estimate, 'value') p_84 = getattr(mass_param.posterior_stats, 'percentile_84th') p_16 = getattr(mass_param.posterior_stats, 'percentile_16th') p_med = getattr(mass_param.posterior_stats, 'median') p_mean = getattr(mass_param.posterior_stats, 'mean') latex_name = getattr(mass_param, 'latex_str') if mass_name == 'theta_E': param[prefix + 'theta_E'] = {'point_estimate': p, 'percentile_84th': p_84, 'percentile_16th': p_16, 'median': p_med, 'mean': p_mean, 'latex_str': latex_name} elif mass_name == 'q': param[prefix + 'q'] = {'point_estimate': p, 'percentile_84th': p_84, 'percentile_16th': p_16, 'median': p_med, 'mean': p_mean, 'latex_str': latex_name} elif mass_name == 'phi': param[prefix + 'phi'] = {'point_estimate': p, 'percentile_84th': p_84, 'percentile_16th': p_16, 'median': p_med, 'mean': p_mean, 'latex_str': latex_name} elif mass_name == 'center_x': param[prefix + 'cx'] = {'point_estimate': p, 'percentile_84th': p_84, 'percentile_16th': p_16, 'median': p_med, 'mean': p_mean, 'latex_str': latex_name} elif mass_name == 'center_y': param[prefix + 'cy'] = {'point_estimate': p, 'percentile_84th': p_84, 'percentile_16th': p_16, 'median': p_med, 'mean': p_mean, 'latex_str': latex_name} else: print(mass_name, " not known") print('\t SIE correctly added') return param
[docs] def read_sersic(light, param={}, prefix='Sersic_0_'): """ Reads the parameters of a coolest.template.classes.profiles.light.Sersic object INPUT ----- mass : coolest.template.classes.profiles.light.Sersic object param : dict, already existing dictionnary with ordered parameters readable by plotting function prefix : str, prefix to use in saving parameters names OUTPUT ------ param : updated param """ for light_name, light_param in light.parameters.items(): p = getattr(light_param.point_estimate, 'value') p_84 = getattr(light_param.posterior_stats, 'percentile_84th') p_16 = getattr(light_param.posterior_stats, 'percentile_16th') p_med = getattr(light_param.posterior_stats, 'median') p_mean = getattr(light_param.posterior_stats, 'mean') latex_name = getattr(light_param, 'latex_str') if light_name == 'I_eff': param[prefix + 'A'] = {'point_estimate': p, 'percentile_84th': p_84, 'percentile_16th': p_16, 'median': p_med, 'mean': p_mean, 'latex_str': latex_name} elif light_name == 'n': param[prefix + 'n_sersic'] = {'point_estimate': p, 'percentile_84th': p_84, 'percentile_16th': p_16, 'median': p_med, 'mean': p_mean, 'latex_str': latex_name} elif light_name == 'theta_eff': param[prefix + 'R_sersic'] = {'point_estimate': p, 'percentile_84th': p_84, 'percentile_16th': p_16, 'median': p_med, 'mean': p_mean, 'latex_str': latex_name} elif light_name == 'q': param[prefix + 'q'] = {'point_estimate': p, 'percentile_84th': p_84, 'percentile_16th': p_16, 'median': p_med, 'mean': p_mean, 'latex_str': latex_name} elif light_name == 'phi': param[prefix + 'phi'] = {'point_estimate': p, 'percentile_84th': p_84, 'percentile_16th': p_16, 'median': p_med, 'mean': p_mean, 'latex_str': latex_name} elif light_name == 'center_x': param[prefix + 'cx'] = {'point_estimate': p, 'percentile_84th': p_84, 'percentile_16th': p_16, 'median': p_med, 'mean': p_mean, 'latex_str': latex_name} elif light_name == 'center_y': param[prefix + 'cy'] = {'point_estimate': p, 'percentile_84th': p_84, 'percentile_16th': p_16, 'median': p_med, 'mean': p_mean, 'latex_str': latex_name} else: print(light_name, " not known") print('\t Sersic correctly added') return param
[docs] def find_critical_lines(coordinates, mag_map): # invert and find contours corresponding to infinite magnification (i.e., changing sign) inv_mag = 1. / np.array(mag_map) contours = measure.find_contours(inv_mag, 0.) # convert to model coordinates lines = [] for contour in contours: curve_x, curve_y = coordinates.pixel_to_radec(contour[:, 1], contour[:, 0]) lines.append((np.array(curve_x), np.array(curve_y))) return lines
[docs] def find_caustics(crit_lines, composable_lens): """`composable_lens` can be an instance of `ComposableLens` or `ComposableMass`""" lines = [] for cline in crit_lines: cl_src_x, cl_src_y = composable_lens.ray_shooting(cline[0], cline[1]) lines.append((np.array(cl_src_x), np.array(cl_src_y))) return lines
[docs] def find_all_lens_lines(coordinates, composable_lens): """`composable_lens` can be an instance of `ComposableLens` or `ComposableMass`""" from coolest.api.composable_models import ComposableLensModel, ComposableMassModel # avoiding circular imports if isinstance(composable_lens, ComposableLensModel): mag_fn = composable_lens.lens_mass.evaluate_magnification elif isinstance(composable_lens, ComposableMassModel): mag_fn = composable_lens.evaluate_magnification else: raise ValueError("`composable_lens` must be a ComposableLensModel or a ComposableMassModel.") mag_map = mag_fn(*coordinates.pixel_coordinates) crit_lines = find_critical_lines(coordinates, mag_map) caustics = find_caustics(crit_lines, composable_lens) return crit_lines, caustics
[docs] def resample_multivariate_normal(samples, num_samples=5_000, **kwargs_cov): """Resample following multi-variate normal distribution""" mean = np.mean(samples, axis=0) cov = np.cov(samples.T, **kwargs_cov) num_params = samples.shape[1] resampled = np.random.multivariate_normal( mean=mean, cov=cov, size=(int(num_samples/num_params), num_params)).reshape((-1, num_params)) return resampled