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plotting.py
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plotting.py
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import numpy as np
import traceback
import itertools
from scipy.optimize import curve_fit
from scipy.special import erf
try:
import matplotlib.pyplot as plt
import seaborn as sns
except ModuleNotFoundError:
raise RuntimeError(
"ROC estimation can only be done when matplotlib and seaborn are installed."
)
sns.set(context="talk", style="ticks")
class ScoreHistogramFdr:
def __init__(self):
self.fig = plt.figure(figsize=(5 * 2, 5))
self.hist_ax = self.fig.add_subplot(1, 2, 1)
self.fdr_ax = self.fig.add_subplot(1, 2, 2)
def draw_histogram(self, scores, nbins=30, return_bins=False):
y, x_hist, _ = self.hist_ax.hist(
scores, bins=nbins, histtype="step", color="grey"
)
self.hist_ax.set_xlabel(r"${LCC}_{max}$")
self.hist_ax.set_xlim(x_hist[0], x_hist[-1])
self.hist_ax.set_ylabel("Frequency")
if return_bins:
return y, x_hist
def draw_bimodal(self, x, y1, y2, ymax=None):
# plot bimodal model and the gaussian particle population
self.hist_ax.plot(
x, y1, lw=3.5, alpha=0.9, color="tab:blue"
) # , label='Bimodal model')
self.hist_ax.plot(
x, y2, lw=4, alpha=0.9, color="tab:orange"
) # , label='True positives')
# population = params[2:5]
if ymax is not None:
self.hist_ax.set_ylim(0, ymax)
# self.hist_ax.legend(loc='upper right')
def draw_score_threshold(self, x, ymax):
self.hist_ax.vlines(
x, 0, ymax, linestyle="dashed", label=f"Cutoff: {x:.2f}", color="black"
)
self.hist_ax.legend(loc="upper right")
def draw_fdr_recall(self, fdr, recall, optimal_id, ruc):
self.fdr_ax.scatter(fdr, recall, facecolors="none", edgecolors="gray", s=25)
# add optimal threshold in green
self.fdr_ax.scatter(
fdr[optimal_id],
recall[optimal_id],
s=25,
color="black",
label=f"RUC: {ruc:.2f}",
)
self.fdr_ax.plot([0, 1], [0, 1], ls="--", c=".3", lw=1)
self.fdr_ax.set_xlabel("FDR")
self.fdr_ax.set_ylabel("Recall")
self.fdr_ax.set_xlim(0, 1)
self.fdr_ax.set_xticks([0, 0.2, 0.4, 0.6, 0.8, 1])
self.fdr_ax.set_ylim(0, 1)
self.fdr_ax.set_yticks([0, 0.2, 0.4, 0.6, 0.8, 1])
self.fdr_ax.legend(loc="lower right")
def write(self, filename, quality=300, transparency=False, bbox="tight"):
plt.tight_layout()
plt.savefig(filename, dpi=quality, transparent=transparency, bbox_inches=bbox)
def display(self):
plt.tight_layout()
plt.show()
def check_square_fdr(fdr, recall, epsilon=1e-3):
"""
@param fdr: list of fdr values
@type fdr: L{list}
@param recall: list of recall values
@type recall: L{list}
@param epsilon: tolerance for closeness to 0 and 1
@type epsilon: L{float}
@return: boolean of whether the FDR is almost square within tolerance
@rtype: L{bool}
@author: Marten Chaillet
"""
# fdr and recall should contain values very close to 0 and 1, respectively
# if function is square
union = [
(f, r)
for f, r in zip(fdr, recall)
if ((np.abs(0.0 - f) < epsilon) and (np.abs(1.0 - r) < epsilon))
]
return bool(union)
def distance_to_diag(fdr, recall):
"""
@param fdr: list of fdr values
@type fdr: L{list}
@param recall: list of recall values
@type recall: L{list}
@return: list of distance of each fdr, recall combination to diagonal line
@rtype: L{list}
@author: Marten Chaillet
"""
# two point on the diagonal to find the distance to
lp1, lp2 = (0, 0), (1, 1)
# list to hold distances
distance = []
for f, r in zip(fdr, recall):
d = np.abs(
(lp2[0] - lp1[0]) * (lp1[1] - r) - (lp1[0] - f) * (lp2[1] - lp1[1])
) / np.sqrt((lp2[0] - lp1[0]) ** 2 + (lp2[1] - lp1[1]) ** 2)
distance.append(d)
return distance
def calculate_histogram(scores, num_steps):
# construct x and y array according to the given peak index
# preferably input is already sorted
scores.sort() # this is sorted from lowest to highest
min = scores[0]
max = scores[-1]
step = (max - min) / num_steps
x = []
for i in range(num_steps):
x.append(min + i * step)
x.append(max)
y = []
for i in range(num_steps):
lower = x[i]
upper = x[i + 1]
n = len([v for v in scores if lower <= v <= upper])
y.append(n)
return x, y
def evaluate_estimates(estimated_positions, ground_truth_positions, tolerance):
"""
Estimated_positions numpy array, ground truth positions numpy array
:param estimated_positions:
:type estimated_positions:
:param ground_truth_positions:
:type ground_truth_positions:
:param tolerance:
:type tolerance:
:return:
:rtype:
"""
from scipy.spatial.distance import cdist
n_estimates = estimated_positions.shape[0]
matrix = cdist(estimated_positions, ground_truth_positions, metric="euclidean")
correct = [0] * n_estimates
for i in range(n_estimates):
if matrix[i].min() < tolerance:
correct[i] = 1
return correct
def fdr_recall(correct_particles, scores):
assert all(i > j for i, j in itertools.pairwise(scores)), print(
"Scores list should be decreasing."
)
n_true_positives = sum(correct_particles)
true_positives, false_positives = 0, 0
fdr, recall = [], []
for correct, score in zip(correct_particles, scores):
if correct:
true_positives += 1
else:
false_positives += 1
if n_true_positives == 0:
recall.append(0)
else:
recall.append(true_positives / n_true_positives)
fdr.append(false_positives / (true_positives + false_positives))
return fdr, recall
def get_distance(line, point):
a1, b1 = line
x, y = point
a2 = -(1 / a1)
b2 = y - a2 * x
x_int = (b2 - b1) / (a1 - a2)
y_int = a2 * x_int + b2
return np.sqrt((x_int - x) ** 2 + (y_int - y) ** 2)
def distance_to_random(fdr, recall):
auc = [0] * len(fdr)
for i in range(len(fdr)):
d = get_distance((1, 0), (fdr[i], recall[i])) # AUC should be 1 at most not 1/2
if recall[i] > fdr[i]:
auc[i] = d
else:
auc[i] = -d
return max(auc), np.argmax(auc)
# ========== functions for fitting ==========
# define gaussian function with parameters to fit
def gauss(x, mu, sigma, amp):
return amp * np.exp(-((x - mu) ** 2) / (2 * sigma**2))
# integral of gaussian with certain sigma and A
def gauss_integral(sigma, amp):
# mu does not influence the integral
return amp * np.abs(sigma) * np.sqrt(2 * np.pi)
# define bimodal function of two gaussians to fit both populations
def bimodal(x, mu1, sigma1, amp1, mu2, sigma2, amp2):
return gauss(x, mu1, sigma1, amp1) + gauss(x, mu2, sigma2, amp2)
def plist_quality_gaussian_fit(
lcc_max_values,
score_volume,
particle_peak_index,
force_peak=False,
output_figure_name=None,
crop_hist=False,
num_bins=30,
n_tomograms=1,
):
# read out the scores
correlation_scores = np.array(sorted(lcc_max_values, reverse=True))
# draw the histogram
plot = ScoreHistogramFdr()
y, x_hist = plot.draw_histogram(
correlation_scores, nbins=num_bins, return_bins=True
)
try:
# ===== fit bimodal distribution =====
# adjust x to center of each bin so len(x)==len(y)
x = (x_hist[1:] + x_hist[:-1]) / 2
hist_step = x_hist[1] - x_hist[0]
# noise gaussian std
# noise_sigma = np.sqrt((score_volume.std() ** 2) * n_tomograms)
# if n_tomograms > 1 else score_volume.std()
noise_sigma = score_volume.std()
noise_mean = score_volume.mean()
noise_size = score_volume.size * n_tomograms
# noise gaussian A value
noise_a = ((noise_size) / (noise_sigma * np.sqrt(2 * np.pi))) * hist_step
# expected values
# left gaussian expectation:
# score volume is skewed gaussian, fit only sigma with upper limit
# (skewed because it only contains highest score at each position)
# right gaussian expectation:
# mu ~ x[half] and A ~ y[half]
expected = (noise_sigma, x[particle_peak_index], 0.1, y[particle_peak_index])
# force peak of particle population to be at peak index
if force_peak:
bounds = (
[noise_sigma, x[particle_peak_index] - 0.01, 0, 0],
[noise_sigma * 1.5, x[particle_peak_index] + 0.01, 0.1, y[1]],
)
else:
bounds = (
[noise_sigma, x[int(len(x) * 0.25)], 0, 0],
[noise_sigma * 1.5, x[-1], 0.1, y[1]],
)
# TODO use lambda expression to fix mu_1 and sigma_1
# params_names = ['mu_1', 'sigma_1', 'A_1', 'mu_2', 'sigma_2', 'A_2']
params_names = ["sigma_1", "mu_2", "sigma_2", "A_2"]
# skip first position as the noise peak there is likely incorrect
params, cov = curve_fit(
lambda x, p1, p2, p3, p4: bimodal(x, noise_mean, p1, noise_a, p2, p3, p4),
x[1:],
y[1:],
p0=expected,
bounds=bounds,
maxfev=2000,
) # max iterations argument: maxfev=2000)
# give sigma of fit for each parameter
sigma = np.sqrt(np.diag(cov))
# print information about fit of the model
print("\nfit of the bimodal model:")
print("\testimated\t\tsigma")
for n, p, s in zip(params_names, params, sigma):
print(f"{n}\t{p:.3f}\t\t{s:.3f}")
print("\n")
noise, population = ((noise_mean, params[0], noise_a), tuple(params[1:4]))
y_bimodal = bimodal(x, *noise, *population)
y_gauss = gauss(x, *population)
if crop_hist:
plot.draw_bimodal(x, y_bimodal, y_gauss, ymax=3 * population[2])
else:
plot.draw_bimodal(x, y_bimodal, y_gauss)
# ===== Generate a ROC curve =====
roc_steps = 50
x_roc = np.flip(np.linspace(x[0], x[-1], roc_steps))
# find ratio of hist step vs roc step
roc_step = (x[-1] - x[0]) / roc_steps
delta = (
hist_step / roc_step
) # can be used to divide true/false positives by per roc step
# variable for total number of tp and fp
n_false_positives = 0.0
# list for storing probability of true positives and false positives
# for each cutoff
# recall = TP / (TP + FN); TP + FN is the full area under the Gaussian curve
recall = []
# false discovery rate = FP / (TP + FP); == 1 - TP / (TP + FP)
fdr = []
# find integral of gaussian particle population;
# NEED TO DIVIDE BY HISTOGRAM BIN STEP
population_integral = gauss_integral(population[1], population[2]) / hist_step
print(
f" - estimation total number of true positives: {population_integral:.1f}"
)
# should use CDF (cumulative distribution function) of Gaussian,
# gives probability from -infinity to x
def cdf(x):
return 0.5 * (1 + erf((x - population[0]) / (np.sqrt(2) * population[1])))
def gauss_noise(x):
return gauss(x, *noise)
for x_i in x_roc:
# calculate probability of true positives x_i
# n_true_positives += gauss_pop(x_i) / delta
n_true_positives = (1 - cdf(x_i)) * population_integral
# determine false positives up to this point, could also use CDF
n_false_positives += gauss_noise(x_i) / delta
# add probability
recall.append(n_true_positives / population_integral)
fdr.append(n_false_positives / (n_true_positives + n_false_positives))
# find best classifier by calculating the rectangle under the curve
# for each roc point
recall = np.array(recall)
fdr = np.array(fdr)
rectangles = recall * (1 - fdr)
cutoff, ruc = rectangles.argmax(), rectangles.max()
# plot the threshold on the distribution plot for visual inspection
plot.draw_score_threshold(x_roc[cutoff], max(y))
print(f" - optimal correlation coefficient threshold is {x_roc[cutoff]:.3f}")
print(
(
" - this threshold approximately selects "
f"{(1 - cdf(x_roc[cutoff])) * population_integral:.1f} particles",
)
)
# plot the fdr curve
plot.draw_fdr_recall(fdr, recall, cutoff, ruc)
print("Rectangle Under Curve (RUC): ", ruc)
except (RuntimeError, ValueError):
# runtime error is because the model could not be fit,
# in that case print error and continue with execution
traceback.print_exc()
if output_figure_name is None:
plot.display()
else:
if output_figure_name.suffix not in [".svg", ".png"]:
output_figure_name = output_figure_name + ".png"
plot.write(output_figure_name)