Examples with IterativeLegendreGaussIntegrator org.apache.commons.math3.analysis.integration.IterativeLegendreGaussIntegrator used on opensource projects

Example 1 with IterativeLegendreGaussIntegrator

use of org.apache.commons.math3.analysis.integration.IterativeLegendreGaussIntegrator in project GDSC-SMLM by aherbert.

the class PoissonGammaGaussianFunction method likelihood.

/**
	 * Compute the likelihood
	 * 
	 * @param o
	 *            The observed count
	 * @param e
	 *            The expected count
	 * @return The likelihood
	 */
public double likelihood(final double o, final double e) {
    // Use the same variables as the Python code
    final double cij = o;
    // convert to photons
    final double eta = alpha * e;
    if (sigma == 0) {
        // No convolution with a Gaussian. Simply evaluate for a Poisson-Gamma distribution.
        final double p;
        // Any observed count above zero
        if (cij > 0.0) {
            // The observed count converted to photons
            final double nij = alpha * cij;
            // The limit on eta * nij is therefore (709/2)^2 = 125670.25
            if (eta * nij > 10000) {
                // Approximate Bessel function i1(x) when using large x:
                // i1(x) ~ exp(x)/sqrt(2*pi*x)
                // However the entire equation is logged (creating transform),
                // evaluated then raised to e to prevent overflow error on 
                // large exp(x)
                final double transform = 0.5 * Math.log(alpha * eta / cij) - nij - eta + 2 * Math.sqrt(eta * nij) - Math.log(twoSqrtPi * Math.pow(eta * nij, 0.25));
                p = FastMath.exp(transform);
            } else {
                // Second part of equation 135
                p = Math.sqrt(alpha * eta / cij) * FastMath.exp(-nij - eta) * Bessel.I1(2 * Math.sqrt(eta * nij));
            }
        } else if (cij == 0.0) {
            p = FastMath.exp(-eta);
        } else {
            p = 0;
        }
        return (p > minimumProbability) ? p : minimumProbability;
    } else if (useApproximation) {
        return mortensenApproximation(cij, eta);
    } else {
        // This code is the full evaluation of equation 7 from the supplementary information  
        // of the paper Chao, et al (2013) Nature Methods 10, 335-338.
        // It is the full evaluation of a Poisson-Gamma-Gaussian convolution PMF. 
        // Read noise
        final double sk = sigma;
        // Gain
        final double g = 1.0 / alpha;
        // Observed pixel value
        final double z = o;
        // Expected number of photons
        final double vk = eta;
        // Compute the integral to infinity of:
        // exp( -((z-u)/(sqrt(2)*s)).^2 - u/g ) * sqrt(vk*u/g) .* besseli(1, 2 * sqrt(vk*u/g)) ./ u;
        // vk / g
        final double vk_g = vk * alpha;
        final double sqrt2sigma = Math.sqrt(2) * sk;
        // Specify the function to integrate
        UnivariateFunction f = new UnivariateFunction() {

            public double value(double u) {
                return eval(sqrt2sigma, z, vk_g, g, u);
            }
        };
        // Integrate to infinity is not necessary. The convolution of the function with the 
        // Gaussian should be adequately sampled using a nxSD around the maximum.
        // Find a bracket containing the maximum
        double lower, upper;
        double maxU = Math.max(1, o);
        double rLower = maxU;
        double rUpper = maxU + 1;
        double f1 = f.value(rLower);
        double f2 = f.value(rUpper);
        // Calculate the simple integral and the range
        double sum = f1 + f2;
        boolean searchUp = f2 > f1;
        if (searchUp) {
            while (f2 > f1) {
                f1 = f2;
                rUpper += 1;
                f2 = f.value(rUpper);
                sum += f2;
            }
            maxU = rUpper - 1;
        } else {
            // Ensure that u stays above zero
            while (f1 > f2 && rLower > 1) {
                f2 = f1;
                rLower -= 1;
                f1 = f.value(rLower);
                sum += f1;
            }
            maxU = (rLower > 1) ? rLower + 1 : rLower;
        }
        lower = Math.max(0, maxU - 5 * sk);
        upper = maxU + 5 * sk;
        if (useSimpleIntegration && lower > 0) {
            // remaining points in the range
            for (double u = rLower - 1; u >= lower; u -= 1) {
                sum += f.value(u);
            }
            for (double u = rUpper + 1; u <= upper; u += 1) {
                sum += f.value(u);
            }
        } else {
            // Use Legendre-Gauss integrator
            try {
                final double relativeAccuracy = 1e-4;
                final double absoluteAccuracy = 1e-8;
                final int minimalIterationCount = 3;
                final int maximalIterationCount = 32;
                final int integrationPoints = 16;
                // Use an integrator that does not use the boundary since u=0 is undefined (divide by zero)
                UnivariateIntegrator i = new IterativeLegendreGaussIntegrator(integrationPoints, relativeAccuracy, absoluteAccuracy, minimalIterationCount, maximalIterationCount);
                sum = i.integrate(2000, f, lower, upper);
            } catch (TooManyEvaluationsException ex) {
                return mortensenApproximation(cij, eta);
            }
        }
        // Compute the final probability
        //final double 
        f1 = z / sqrt2sigma;
        final double p = (FastMath.exp(-vk) / (sqrt2pi * sk)) * (FastMath.exp(-(f1 * f1)) + sum);
        return (p > minimumProbability) ? p : minimumProbability;
    }
}

Example 2 with IterativeLegendreGaussIntegrator

use of org.apache.commons.math3.analysis.integration.IterativeLegendreGaussIntegrator in project GDSC-SMLM by aherbert.

the class PeakResult method computeI1.

/**
	 * Compute the function I1 using numerical integration. See Mortensen, et al (2010) Nature Methods 7, 377-383), SI
	 * equation 43.
	 * 
	 * <pre>
	 * I1 = 1 + sum [ ln(t) / (1 + t/rho) ] dt
	 *    = - sum [ t * ln(t) / (t + rho) ] dt
	 * </pre>
	 * 
	 * Where sum is the integral between 0 and 1. In the case of rho=0 the function returns 1;
	 * 
	 * @param rho
	 * @param integrationPoints
	 *            the number of integration points for the LegendreGaussIntegrator
	 * @return the I1 value
	 */
private static double computeI1(final double rho, int integrationPoints) {
    if (rho == 0)
        return 1;
    final double relativeAccuracy = 1e-4;
    final double absoluteAccuracy = 1e-8;
    final int minimalIterationCount = 3;
    final int maximalIterationCount = 32;
    // Use an integrator that does not use the boundary since log(0) is undefined.
    UnivariateIntegrator i = new IterativeLegendreGaussIntegrator(integrationPoints, relativeAccuracy, absoluteAccuracy, minimalIterationCount, maximalIterationCount);
    // Specify the function to integrate
    UnivariateFunction f = new UnivariateFunction() {

        public double value(double x) {
            return x * Math.log(x) / (x + rho);
        }
    };
    final double i1 = -i.integrate(2000, f, 0, 1);
    return i1;
}