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Update app.py
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app.py
CHANGED
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@@ -4,12 +4,6 @@ import numpy as np
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import plotly.graph_objects as go
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from scipy.optimize import fsolve
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from scipy.stats import gaussian_kde
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import os
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import sys
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import tempfile
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import subprocess
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import importlib.util
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import shutil
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# Configure Streamlit for Hugging Face Spaces
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st.set_page_config(
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@@ -18,539 +12,6 @@ st.set_page_config(
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initial_sidebar_state="collapsed"
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)
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# Define C++ extension code as a string
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CPP_CODE = r'''
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#include <pybind11/pybind11.h>
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#include <pybind11/numpy.h>
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#include <pybind11/eigen.h>
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#include <Eigen/Dense>
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#include <vector>
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#include <cmath>
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#include <limits>
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namespace py = pybind11;
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// Compute the cubic discriminant
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double compute_discriminant(double z, double beta, double z_a, double y_effective) {
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double a = z * z_a;
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double b = z * z_a + z + z_a - z_a * y_effective;
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double c = z + z_a + 1 - y_effective * (beta * z_a + 1 - beta);
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double d = 1;
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// Symbolic expression for the cubic discriminant
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return std::pow((b*c)/(6*a*a) - std::pow(b, 3)/(27*std::pow(a, 3)) - d/(2*a), 2) +
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std::pow(c/(3*a) - std::pow(b, 2)/(9*std::pow(a, 2)), 3);
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}
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// Find z values where the discriminant equals zero
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std::vector<double> find_z_at_discriminant_zero(double z_a, double y, double beta,
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double z_min, double z_max, int steps) {
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// Apply the condition for y
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double y_effective = y > 1 ? y : 1/y;
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// Create z grid
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std::vector<double> z_grid(steps);
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double step_size = (z_max - z_min) / (steps - 1);
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for (int i = 0; i < steps; i++) {
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z_grid[i] = z_min + i * step_size;
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}
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// Calculate discriminant values
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std::vector<double> disc_vals(steps);
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for (int i = 0; i < steps; i++) {
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disc_vals[i] = compute_discriminant(z_grid[i], beta, z_a, y_effective);
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}
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// Find roots
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std::vector<double> roots_found;
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for (int i = 0; i < steps - 1; i++) {
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double f1 = disc_vals[i];
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double f2 = disc_vals[i+1];
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// Skip if NaN
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if (std::isnan(f1) || std::isnan(f2)) {
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continue;
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}
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// Check for exact zero
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if (f1 == 0.0) {
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roots_found.push_back(z_grid[i]);
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}
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else if (f2 == 0.0) {
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roots_found.push_back(z_grid[i+1]);
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}
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// Check for sign change
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else if (f1 * f2 < 0) {
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double zl = z_grid[i];
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double zr = z_grid[i+1];
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double f1_local = f1;
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double f2_local = f2;
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// Use binary search to refine the root
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for (int j = 0; j < 50; j++) {
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double mid = 0.5 * (zl + zr);
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double fm = compute_discriminant(mid, beta, z_a, y_effective);
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if (fm == 0) {
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zl = zr = mid;
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break;
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}
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if ((fm > 0 && f1_local > 0) || (fm < 0 && f1_local < 0)) {
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zl = mid;
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f1_local = fm;
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} else {
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zr = mid;
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f2_local = fm;
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}
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}
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roots_found.push_back(0.5 * (zl + zr));
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}
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}
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return roots_found;
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}
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// Sweep beta values and find z boundary values
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std::tuple<py::array_t<double>, py::array_t<double>, py::array_t<double>>
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sweep_beta_and_find_z_bounds(double z_a, double y, double z_min, double z_max, int beta_steps, int z_steps) {
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// Create beta values
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py::array_t<double> betas(beta_steps);
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auto betas_ptr = betas.mutable_data();
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double beta_step = 1.0 / (beta_steps - 1);
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for (int i = 0; i < beta_steps; i++) {
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betas_ptr[i] = i * beta_step;
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}
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// Initialize arrays for min and max z values
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py::array_t<double> z_min_values(beta_steps);
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py::array_t<double> z_max_values(beta_steps);
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auto z_min_ptr = z_min_values.mutable_data();
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auto z_max_ptr = z_max_values.mutable_data();
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for (int i = 0; i < beta_steps; i++) {
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double beta = betas_ptr[i];
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std::vector<double> roots = find_z_at_discriminant_zero(z_a, y, beta, z_min, z_max, z_steps);
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if (roots.size() == 0) {
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z_min_ptr[i] = std::numeric_limits<double>::quiet_NaN();
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z_max_ptr[i] = std::numeric_limits<double>::quiet_NaN();
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} else {
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// Find min and max roots
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double min_root = roots[0];
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double max_root = roots[0];
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for (size_t j = 1; j < roots.size(); j++) {
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if (roots[j] < min_root) min_root = roots[j];
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if (roots[j] > max_root) max_root = roots[j];
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}
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z_min_ptr[i] = min_root;
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z_max_ptr[i] = max_root;
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}
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}
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return std::make_tuple(betas, z_min_values, z_max_values);
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}
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// Compute High y Expression curve
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py::array_t<double> compute_high_y_curve(py::array_t<double> betas, double z_a, double y) {
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// Apply the condition for y
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double y_effective = y > 1 ? y : 1/y;
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auto betas_ptr = betas.data();
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size_t n = betas.size();
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py::array_t<double> result(n);
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auto result_ptr = result.mutable_data();
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double a = z_a;
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double denominator = 1 - 2*a;
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if (std::abs(denominator) < 1e-10) {
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for (size_t i = 0; i < n; i++) {
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result_ptr[i] = std::numeric_limits<double>::quiet_NaN();
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}
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} else {
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for (size_t i = 0; i < n; i++) {
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double beta = betas_ptr[i];
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double numerator = -4*a*(a-1)*y_effective*beta - 2*a*y_effective - 2*a*(2*a-1);
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result_ptr[i] = numerator/denominator;
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}
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}
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return result;
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}
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// Compute alternative low expression
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py::array_t<double> compute_alternate_low_expr(py::array_t<double> betas, double z_a, double y) {
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// Apply the condition for y
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double y_effective = y > 1 ? y : 1/y;
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auto betas_ptr = betas.data();
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size_t n = betas.size();
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py::array_t<double> result(n);
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auto result_ptr = result.mutable_data();
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for (size_t i = 0; i < n; i++) {
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double beta = betas_ptr[i];
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result_ptr[i] = (z_a * y_effective * beta * (z_a - 1) - 2*z_a*(1 - y_effective) - 2*z_a*z_a) / (2 + 2*z_a);
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}
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return result;
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}
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// Compute max k expression
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py::array_t<double> compute_max_k_expression(py::array_t<double> betas, double z_a, double y, int k_samples=1000) {
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// Apply the condition for y
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double y_effective = y > 1 ? y : 1/y;
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auto betas_ptr = betas.data();
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size_t n = betas.size();
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py::array_t<double> result(n);
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auto result_ptr = result.mutable_data();
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double a = z_a;
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// Sample k values on a logarithmic scale
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std::vector<double> k_values(k_samples);
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double log_min = -3;
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double log_max = 3;
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double log_step = (log_max - log_min) / (k_samples - 1);
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for (int j = 0; j < k_samples; j++) {
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k_values[j] = std::pow(10, log_min + j * log_step);
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}
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for (size_t i = 0; i < n; i++) {
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double beta = betas_ptr[i];
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std::vector<double> values(k_samples);
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for (int j = 0; j < k_samples; j++) {
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double k = k_values[j];
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double numerator = y_effective*beta*(a-1)*k + (a*k+1)*((y_effective-1)*k-1);
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double denominator = (a*k+1)*(k*k+k);
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if (std::abs(denominator) < 1e-10) {
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values[j] = std::numeric_limits<double>::quiet_NaN();
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} else {
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values[j] = numerator/denominator;
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}
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}
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// Find max value, ignoring NaNs
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double max_val = -std::numeric_limits<double>::infinity();
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bool found_valid = false;
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for (double val : values) {
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if (!std::isnan(val) && val > max_val) {
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max_val = val;
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found_valid = true;
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}
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}
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result_ptr[i] = found_valid ? max_val : std::numeric_limits<double>::quiet_NaN();
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}
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return result;
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}
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// Compute min t expression
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py::array_t<double> compute_min_t_expression(py::array_t<double> betas, double z_a, double y, int t_samples=1000) {
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// Apply the condition for y
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double y_effective = y > 1 ? y : 1/y;
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auto betas_ptr = betas.data();
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size_t n = betas.size();
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py::array_t<double> result(n);
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auto result_ptr = result.mutable_data();
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double a = z_a;
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if (a <= 0) {
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for (size_t i = 0; i < n; i++) {
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result_ptr[i] = std::numeric_limits<double>::quiet_NaN();
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}
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return result;
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}
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// Create t values from -1/a to 0
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double lower_bound = -1/a + 1e-10; // Avoid division by zero
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double step_size = (-1e-10 - lower_bound) / (t_samples - 1);
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std::vector<double> t_values(t_samples);
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for (int j = 0; j < t_samples; j++) {
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t_values[j] = lower_bound + j * step_size;
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}
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for (size_t i = 0; i < n; i++) {
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double beta = betas_ptr[i];
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std::vector<double> values(t_samples);
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for (int j = 0; j < t_samples; j++) {
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double t = t_values[j];
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double numerator = y_effective*beta*(a-1)*t + (a*t+1)*((y_effective-1)*t-1);
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double denominator = (a*t+1)*(t*t+t);
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if (std::abs(denominator) < 1e-10) {
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values[j] = std::numeric_limits<double>::quiet_NaN();
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} else {
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values[j] = numerator/denominator;
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}
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}
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// Find min value, ignoring NaNs
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double min_val = std::numeric_limits<double>::infinity();
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bool found_valid = false;
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for (double val : values) {
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if (!std::isnan(val) && val < min_val) {
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min_val = val;
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found_valid = true;
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}
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}
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result_ptr[i] = found_valid ? min_val : std::numeric_limits<double>::quiet_NaN();
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}
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return result;
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}
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// Compute eigenvalue support boundaries
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std::tuple<py::array_t<double>, py::array_t<double>>
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compute_eigenvalue_support_boundaries(double z_a, double y, py::array_t<double> beta_values,
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int n_samples = 100, int seeds = 5) {
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// Apply the condition for y
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double y_effective = y > 1 ? y : 1/y;
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auto beta_ptr = beta_values.data();
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size_t num_betas = beta_values.size();
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py::array_t<double> min_eigenvalues(num_betas);
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py::array_t<double> max_eigenvalues(num_betas);
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auto min_eig_ptr = min_eigenvalues.mutable_data();
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auto max_eig_ptr = max_eigenvalues.mutable_data();
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for (size_t i = 0; i < num_betas; i++) {
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double beta = beta_ptr[i];
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std::vector<double> min_vals;
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std::vector<double> max_vals;
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// Run multiple trials with different seeds
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for (int seed = 0; seed < seeds; seed++) {
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// Set random seed
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srand(seed * 100 + i);
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// Compute dimension p based on aspect ratio y
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int n = n_samples;
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int p = int(y_effective * n);
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// Constructing T_n (Population / Shape Matrix)
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int k = int(std::floor(beta * p));
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// Create diagonal entries
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std::vector<double> diag_entries(p);
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for (int j = 0; j < k; j++) {
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diag_entries[j] = z_a;
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}
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for (int j = k; j < p; j++) {
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diag_entries[j] = 1.0;
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}
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// Shuffle the diagonal entries (simple Fisher-Yates shuffle)
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for (int j = p-1; j > 0; j--) {
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int idx = rand() % (j+1);
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std::swap(diag_entries[j], diag_entries[idx]);
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}
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// Generate the data matrix X with i.i.d. standard normal entries
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std::vector<std::vector<double>> X(p, std::vector<double>(n));
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for (int row = 0; row < p; row++) {
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for (int col = 0; col < n; col++) {
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// Box-Muller transform to generate normal distribution
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double u1 = rand() / (RAND_MAX + 1.0);
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double u2 = rand() / (RAND_MAX + 1.0);
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if (u1 < 1e-10) u1 = 1e-10; // Avoid log(0)
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| 374 |
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double z = sqrt(-2.0 * log(u1)) * cos(2.0 * M_PI * u2);
|
| 375 |
-
X[row][col] = z;
|
| 376 |
-
}
|
| 377 |
-
}
|
| 378 |
-
|
| 379 |
-
// Compute the sample covariance matrix S_n = (1/n) * XX^T
|
| 380 |
-
std::vector<std::vector<double>> S_n(p, std::vector<double>(p, 0.0));
|
| 381 |
-
for (int row = 0; row < p; row++) {
|
| 382 |
-
for (int col = 0; col < p; col++) {
|
| 383 |
-
double sum = 0.0;
|
| 384 |
-
for (int k = 0; k < n; k++) {
|
| 385 |
-
sum += X[row][k] * X[col][k];
|
| 386 |
-
}
|
| 387 |
-
S_n[row][col] = sum / n;
|
| 388 |
-
}
|
| 389 |
-
}
|
| 390 |
-
|
| 391 |
-
// Compute B_n = S_n T_n
|
| 392 |
-
std::vector<std::vector<double>> B_n(p, std::vector<double>(p, 0.0));
|
| 393 |
-
for (int row = 0; row < p; row++) {
|
| 394 |
-
for (int col = 0; col < p; col++) {
|
| 395 |
-
B_n[row][col] = S_n[row][col] * diag_entries[col];
|
| 396 |
-
}
|
| 397 |
-
}
|
| 398 |
-
|
| 399 |
-
// Use Eigen library to compute eigenvalues
|
| 400 |
-
Eigen::MatrixXd B_n_eigen(p, p);
|
| 401 |
-
for (int row = 0; row < p; row++) {
|
| 402 |
-
for (int col = 0; col < p; col++) {
|
| 403 |
-
B_n_eigen(row, col) = B_n[row][col];
|
| 404 |
-
}
|
| 405 |
-
}
|
| 406 |
-
|
| 407 |
-
Eigen::SelfAdjointEigenSolver<Eigen::MatrixXd> solver(B_n_eigen);
|
| 408 |
-
Eigen::VectorXd eigenvalues = solver.eigenvalues();
|
| 409 |
-
|
| 410 |
-
// Find min and max eigenvalues
|
| 411 |
-
if (p > 0) {
|
| 412 |
-
min_vals.push_back(eigenvalues(0));
|
| 413 |
-
max_vals.push_back(eigenvalues(p-1));
|
| 414 |
-
}
|
| 415 |
-
}
|
| 416 |
-
|
| 417 |
-
// Average over seeds for stability
|
| 418 |
-
if (!min_vals.empty() && !max_vals.empty()) {
|
| 419 |
-
double min_sum = 0.0, max_sum = 0.0;
|
| 420 |
-
for (double val : min_vals) min_sum += val;
|
| 421 |
-
for (double val : max_vals) max_sum += val;
|
| 422 |
-
|
| 423 |
-
min_eig_ptr[i] = min_sum / min_vals.size();
|
| 424 |
-
max_eig_ptr[i] = max_sum / max_vals.size();
|
| 425 |
-
} else {
|
| 426 |
-
min_eig_ptr[i] = std::numeric_limits<double>::quiet_NaN();
|
| 427 |
-
max_eig_ptr[i] = std::numeric_limits<double>::quiet_NaN();
|
| 428 |
-
}
|
| 429 |
-
}
|
| 430 |
-
|
| 431 |
-
return std::make_tuple(min_eigenvalues, max_eigenvalues);
|
| 432 |
-
}
|
| 433 |
-
|
| 434 |
-
PYBIND11_MODULE(cubic_cpp, m) {
|
| 435 |
-
m.doc() = "C++ implementation of cubic root analysis functions";
|
| 436 |
-
|
| 437 |
-
m.def("sweep_beta_and_find_z_bounds", &sweep_beta_and_find_z_bounds,
|
| 438 |
-
"Sweep beta values and find z boundary values",
|
| 439 |
-
py::arg("z_a"), py::arg("y"), py::arg("z_min"), py::arg("z_max"),
|
| 440 |
-
py::arg("beta_steps"), py::arg("z_steps"));
|
| 441 |
-
|
| 442 |
-
m.def("compute_high_y_curve", &compute_high_y_curve,
|
| 443 |
-
"Compute High y Expression curve",
|
| 444 |
-
py::arg("betas"), py::arg("z_a"), py::arg("y"));
|
| 445 |
-
|
| 446 |
-
m.def("compute_alternate_low_expr", &compute_alternate_low_expr,
|
| 447 |
-
"Compute alternative low expression",
|
| 448 |
-
py::arg("betas"), py::arg("z_a"), py::arg("y"));
|
| 449 |
-
|
| 450 |
-
m.def("compute_max_k_expression", &compute_max_k_expression,
|
| 451 |
-
"Compute max k expression",
|
| 452 |
-
py::arg("betas"), py::arg("z_a"), py::arg("y"), py::arg("k_samples")=1000);
|
| 453 |
-
|
| 454 |
-
m.def("compute_min_t_expression", &compute_min_t_expression,
|
| 455 |
-
"Compute min t expression",
|
| 456 |
-
py::arg("betas"), py::arg("z_a"), py::arg("y"), py::arg("t_samples")=1000);
|
| 457 |
-
|
| 458 |
-
m.def("compute_eigenvalue_support_boundaries", &compute_eigenvalue_support_boundaries,
|
| 459 |
-
"Compute eigenvalue support boundaries",
|
| 460 |
-
py::arg("z_a"), py::arg("y"), py::arg("beta_values"),
|
| 461 |
-
py::arg("n_samples")=100, py::arg("seeds")=5);
|
| 462 |
-
}
|
| 463 |
-
'''
|
| 464 |
-
|
| 465 |
-
# Function to build and load the C++ extension
|
| 466 |
-
@st.cache_resource
|
| 467 |
-
def build_cpp_extension():
|
| 468 |
-
try:
|
| 469 |
-
# Create temporary directory
|
| 470 |
-
temp_dir = tempfile.mkdtemp()
|
| 471 |
-
|
| 472 |
-
# Write C++ code to a file
|
| 473 |
-
cpp_file = os.path.join(temp_dir, "cubic_cpp.cpp")
|
| 474 |
-
with open(cpp_file, "w") as f:
|
| 475 |
-
f.write(CPP_CODE)
|
| 476 |
-
|
| 477 |
-
# Check if pybind11 and Eigen are installed
|
| 478 |
-
try:
|
| 479 |
-
import pybind11
|
| 480 |
-
pybind11_include = pybind11.get_include()
|
| 481 |
-
except ImportError:
|
| 482 |
-
# Install pybind11 if not available
|
| 483 |
-
subprocess.check_call([sys.executable, "-m", "pip", "install", "pybind11"])
|
| 484 |
-
import pybind11
|
| 485 |
-
pybind11_include = pybind11.get_include()
|
| 486 |
-
|
| 487 |
-
# Try to find Eigen or download it
|
| 488 |
-
eigen_include = os.path.join(temp_dir, "eigen")
|
| 489 |
-
if not os.path.exists(eigen_include):
|
| 490 |
-
os.makedirs(eigen_include)
|
| 491 |
-
# Download Eigen headers (just the minimal required parts)
|
| 492 |
-
subprocess.check_call(["wget", "https://gitlab.com/libeigen/eigen/-/archive/3.4.0/eigen-3.4.0.tar.gz", "-O", os.path.join(temp_dir, "eigen.tar.gz")])
|
| 493 |
-
subprocess.check_call(["tar", "-xzf", os.path.join(temp_dir, "eigen.tar.gz"), "-C", temp_dir])
|
| 494 |
-
# Move Eigen headers to the include directory
|
| 495 |
-
eigen_src = os.path.join(temp_dir, "eigen-3.4.0")
|
| 496 |
-
for folder in ["Eigen", "unsupported"]:
|
| 497 |
-
if os.path.exists(os.path.join(eigen_src, folder)):
|
| 498 |
-
shutil.copytree(os.path.join(eigen_src, folder), os.path.join(eigen_include, folder))
|
| 499 |
-
|
| 500 |
-
# Build the extension module
|
| 501 |
-
setup_py = os.path.join(temp_dir, "setup.py")
|
| 502 |
-
with open(setup_py, "w") as f:
|
| 503 |
-
f.write(f'''
|
| 504 |
-
from setuptools import setup, Extension
|
| 505 |
-
import pybind11
|
| 506 |
-
import os
|
| 507 |
-
|
| 508 |
-
ext_modules = [
|
| 509 |
-
Extension(
|
| 510 |
-
'cubic_cpp',
|
| 511 |
-
['cubic_cpp.cpp'],
|
| 512 |
-
include_dirs=[
|
| 513 |
-
pybind11.get_include(),
|
| 514 |
-
os.path.dirname(os.path.abspath(__file__))
|
| 515 |
-
],
|
| 516 |
-
language='c++'
|
| 517 |
-
)
|
| 518 |
-
]
|
| 519 |
-
|
| 520 |
-
setup(
|
| 521 |
-
name='cubic_cpp',
|
| 522 |
-
ext_modules=ext_modules,
|
| 523 |
-
py_modules=[],
|
| 524 |
-
)
|
| 525 |
-
''')
|
| 526 |
-
|
| 527 |
-
# Build the extension in place
|
| 528 |
-
subprocess.check_call([sys.executable, setup_py, "build_ext", "--inplace"], cwd=temp_dir)
|
| 529 |
-
|
| 530 |
-
# Find the compiled module
|
| 531 |
-
extension_path = None
|
| 532 |
-
for file in os.listdir(temp_dir):
|
| 533 |
-
if file.startswith("cubic_cpp") and file.endswith(".so"):
|
| 534 |
-
extension_path = os.path.join(temp_dir, file)
|
| 535 |
-
break
|
| 536 |
-
|
| 537 |
-
if extension_path is None:
|
| 538 |
-
st.warning("Failed to find the compiled C++ extension")
|
| 539 |
-
return None
|
| 540 |
-
|
| 541 |
-
# Load the module
|
| 542 |
-
spec = importlib.util.spec_from_file_location("cubic_cpp", extension_path)
|
| 543 |
-
cubic_cpp = importlib.util.module_from_spec(spec)
|
| 544 |
-
spec.loader.exec_module(cubic_cpp)
|
| 545 |
-
|
| 546 |
-
return cubic_cpp
|
| 547 |
-
except Exception as e:
|
| 548 |
-
st.warning(f"Failed to build C++ extension: {str(e)}")
|
| 549 |
-
return None
|
| 550 |
-
|
| 551 |
-
# Try to build and load the C++ extension
|
| 552 |
-
cubic_cpp = build_cpp_extension()
|
| 553 |
-
|
| 554 |
def add_sqrt_support(expr_str):
|
| 555 |
"""Replace 'sqrt(' with 'sp.sqrt(' for sympy compatibility"""
|
| 556 |
return expr_str.replace('sqrt(', 'sp.sqrt(')
|
|
@@ -583,12 +44,6 @@ def find_z_at_discriminant_zero(z_a, y, beta, z_min, z_max, steps):
|
|
| 583 |
Scan z in [z_min, z_max] for sign changes in the discriminant,
|
| 584 |
and return approximated roots (where the discriminant is zero).
|
| 585 |
"""
|
| 586 |
-
# Use C++ implementation if available
|
| 587 |
-
if cubic_cpp is not None:
|
| 588 |
-
roots = np.array(cubic_cpp.find_z_at_discriminant_zero(z_a, y, beta, z_min, z_max, steps))
|
| 589 |
-
return roots
|
| 590 |
-
|
| 591 |
-
# Python fallback implementation
|
| 592 |
# Apply the condition for y
|
| 593 |
y_effective = y if y > 1 else 1/y
|
| 594 |
|
|
@@ -625,13 +80,6 @@ def sweep_beta_and_find_z_bounds(z_a, y, z_min, z_max, beta_steps, z_steps):
|
|
| 625 |
for which the discriminant is zero.
|
| 626 |
Returns: betas, lower z*(β) values, and upper z*(β) values.
|
| 627 |
"""
|
| 628 |
-
# Use C++ implementation if available
|
| 629 |
-
if cubic_cpp is not None:
|
| 630 |
-
betas, z_min_values, z_max_values = cubic_cpp.sweep_beta_and_find_z_bounds(
|
| 631 |
-
z_a, y, z_min, z_max, beta_steps, z_steps)
|
| 632 |
-
return np.array(betas), np.array(z_min_values), np.array(z_max_values)
|
| 633 |
-
|
| 634 |
-
# Python fallback implementation
|
| 635 |
betas = np.linspace(0, 1, beta_steps)
|
| 636 |
z_min_values = []
|
| 637 |
z_max_values = []
|
|
@@ -651,13 +99,6 @@ def compute_eigenvalue_support_boundaries(z_a, y, beta_values, n_samples=100, se
|
|
| 651 |
Compute the support boundaries of the eigenvalue distribution by directly
|
| 652 |
finding the minimum and maximum eigenvalues of B_n = S_n T_n for different beta values.
|
| 653 |
"""
|
| 654 |
-
# Use C++ implementation if available
|
| 655 |
-
if cubic_cpp is not None:
|
| 656 |
-
min_eigenvalues, max_eigenvalues = cubic_cpp.compute_eigenvalue_support_boundaries(
|
| 657 |
-
z_a, y, beta_values, n_samples, seeds)
|
| 658 |
-
return np.array(min_eigenvalues), np.array(max_eigenvalues)
|
| 659 |
-
|
| 660 |
-
# Python fallback implementation
|
| 661 |
# Apply the condition for y
|
| 662 |
y_effective = y if y > 1 else 1/y
|
| 663 |
|
|
@@ -725,12 +166,6 @@ def compute_high_y_curve(betas, z_a, y):
|
|
| 725 |
"""
|
| 726 |
Compute the "High y Expression" curve.
|
| 727 |
"""
|
| 728 |
-
# Use C++ implementation if available
|
| 729 |
-
if cubic_cpp is not None:
|
| 730 |
-
curve = cubic_cpp.compute_high_y_curve(betas, z_a, y)
|
| 731 |
-
return np.array(curve)
|
| 732 |
-
|
| 733 |
-
# Python fallback implementation
|
| 734 |
# Apply the condition for y
|
| 735 |
y_effective = y if y > 1 else 1/y
|
| 736 |
|
|
@@ -748,12 +183,6 @@ def compute_alternate_low_expr(betas, z_a, y):
|
|
| 748 |
Compute the alternate low expression:
|
| 749 |
(z_a*y*beta*(z_a-1) - 2*z_a*(1-y) - 2*z_a**2) / (2+2*z_a)
|
| 750 |
"""
|
| 751 |
-
# Use C++ implementation if available
|
| 752 |
-
if cubic_cpp is not None:
|
| 753 |
-
curve = cubic_cpp.compute_alternate_low_expr(betas, z_a, y)
|
| 754 |
-
return np.array(curve)
|
| 755 |
-
|
| 756 |
-
# Python fallback implementation
|
| 757 |
# Apply the condition for y
|
| 758 |
y_effective = y if y > 1 else 1/y
|
| 759 |
|
|
@@ -765,12 +194,6 @@ def compute_max_k_expression(betas, z_a, y, k_samples=1000):
|
|
| 765 |
"""
|
| 766 |
Compute max_{k ∈ (0,∞)} (y*beta*(a-1)*k + (a*k+1)*((y-1)*k-1)) / ((a*k+1)*(k^2+k))
|
| 767 |
"""
|
| 768 |
-
# Use C++ implementation if available
|
| 769 |
-
if cubic_cpp is not None:
|
| 770 |
-
curve = cubic_cpp.compute_max_k_expression(betas, z_a, y, k_samples)
|
| 771 |
-
return np.array(curve)
|
| 772 |
-
|
| 773 |
-
# Python fallback implementation
|
| 774 |
# Apply the condition for y
|
| 775 |
y_effective = y if y > 1 else 1/y
|
| 776 |
|
|
@@ -802,12 +225,6 @@ def compute_min_t_expression(betas, z_a, y, t_samples=1000):
|
|
| 802 |
"""
|
| 803 |
Compute min_{t ∈ (-1/a, 0)} (y*beta*(a-1)*t + (a*t+1)*((y-1)*t-1)) / ((a*t+1)*(t^2+t))
|
| 804 |
"""
|
| 805 |
-
# Use C++ implementation if available
|
| 806 |
-
if cubic_cpp is not None:
|
| 807 |
-
curve = cubic_cpp.compute_min_t_expression(betas, z_a, y, t_samples)
|
| 808 |
-
return np.array(curve)
|
| 809 |
-
|
| 810 |
-
# Python fallback implementation
|
| 811 |
# Apply the condition for y
|
| 812 |
y_effective = y if y > 1 else 1/y
|
| 813 |
|
|
@@ -1071,126 +488,905 @@ def generate_z_vs_beta_plot(z_a, y, z_min, z_max, beta_steps, z_steps,
|
|
| 1071 |
)
|
| 1072 |
return fig
|
| 1073 |
|
| 1074 |
-
|
| 1075 |
-
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
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|
|
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|
|
|
|
|
|
|
|
|
|
| 1076 |
|
| 1077 |
-
|
| 1078 |
-
|
| 1079 |
-
|
|
|
|
|
|
|
|
|
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|
|
|
|
|
|
| 1080 |
|
| 1081 |
-
|
| 1082 |
-
|
|
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|
|
|
|
|
| 1083 |
|
| 1084 |
-
|
| 1085 |
-
|
| 1086 |
-
|
|
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|
|
|
|
| 1087 |
|
| 1088 |
-
|
| 1089 |
-
|
| 1090 |
-
|
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|
|
|
|
| 1091 |
|
| 1092 |
-
|
| 1093 |
-
|
| 1094 |
-
|
| 1095 |
-
[
|
| 1096 |
-
|
| 1097 |
-
|
|
|
|
|
|
|
|
|
|
|
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|
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|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
| 1098 |
|
| 1099 |
-
|
| 1100 |
-
|
| 1101 |
-
|
| 1102 |
-
|
| 1103 |
-
|
| 1104 |
-
|
| 1105 |
-
|
| 1106 |
-
|
| 1107 |
-
|
| 1108 |
-
|
| 1109 |
-
|
| 1110 |
-
|
| 1111 |
-
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
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|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
| 1112 |
|
| 1113 |
-
|
| 1114 |
-
|
| 1115 |
-
|
| 1116 |
-
|
| 1117 |
-
|
| 1118 |
-
|
| 1119 |
-
|
| 1120 |
-
show_low_y = st.checkbox("Show Low y Expression", value=False, key="show_low_y")
|
| 1121 |
-
show_min_t = st.checkbox("Show Min t Expression", value=True, key="show_min_t")
|
| 1122 |
|
| 1123 |
-
#
|
| 1124 |
-
|
| 1125 |
-
|
| 1126 |
-
|
| 1127 |
-
|
| 1128 |
-
|
| 1129 |
-
|
| 1130 |
-
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
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|
|
|
|
|
| 1131 |
|
| 1132 |
-
|
| 1133 |
-
|
| 1134 |
-
|
| 1135 |
-
|
| 1136 |
-
|
|
|
|
|
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|
|
|
|
| 1137 |
|
| 1138 |
-
|
| 1139 |
-
|
| 1140 |
-
|
|
|
|
|
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|
|
|
|
| 1141 |
|
| 1142 |
-
|
| 1143 |
-
|
| 1144 |
-
|
| 1145 |
-
|
| 1146 |
-
|
| 1147 |
-
|
| 1148 |
-
|
| 1149 |
-
|
| 1150 |
-
|
| 1151 |
-
|
|
|
|
|
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|
|
| 1152 |
else:
|
| 1153 |
-
|
| 1154 |
-
|
| 1155 |
-
|
| 1156 |
-
|
|
|
|
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|
|
| 1157 |
|
| 1158 |
-
if
|
| 1159 |
-
|
|
|
|
|
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|
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|
|
|
|
|
| 1160 |
|
| 1161 |
-
#
|
| 1162 |
-
|
| 1163 |
-
|
| 1164 |
-
|
| 1165 |
-
|
| 1166 |
-
|
| 1167 |
-
|
| 1168 |
-
|
| 1169 |
-
|
| 1170 |
-
|
| 1171 |
-
|
| 1172 |
-
|
| 1173 |
-
|
| 1174 |
-
|
| 1175 |
-
|
| 1176 |
-
|
| 1177 |
-
|
| 1178 |
-
|
| 1179 |
-
|
| 1180 |
-
|
| 1181 |
-
|
| 1182 |
-
|
| 1183 |
-
|
| 1184 |
-
|
| 1185 |
-
|
| 1186 |
-
|
| 1187 |
-
|
| 1188 |
-
|
| 1189 |
-
|
| 1190 |
-
|
|
|
|
|
|
|
|
|
|
|
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|
|
|
|
|
| 1191 |
|
| 1192 |
-
#
|
| 1193 |
-
|
| 1194 |
-
st.
|
| 1195 |
-
|
| 1196 |
-
|
|
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|
| 4 |
import plotly.graph_objects as go
|
| 5 |
from scipy.optimize import fsolve
|
| 6 |
from scipy.stats import gaussian_kde
|
|
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|
| 7 |
|
| 8 |
# Configure Streamlit for Hugging Face Spaces
|
| 9 |
st.set_page_config(
|
|
|
|
| 12 |
initial_sidebar_state="collapsed"
|
| 13 |
)
|
| 14 |
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| 15 |
def add_sqrt_support(expr_str):
|
| 16 |
"""Replace 'sqrt(' with 'sp.sqrt(' for sympy compatibility"""
|
| 17 |
return expr_str.replace('sqrt(', 'sp.sqrt(')
|
|
|
|
| 44 |
Scan z in [z_min, z_max] for sign changes in the discriminant,
|
| 45 |
and return approximated roots (where the discriminant is zero).
|
| 46 |
"""
|
|
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|
| 47 |
# Apply the condition for y
|
| 48 |
y_effective = y if y > 1 else 1/y
|
| 49 |
|
|
|
|
| 80 |
for which the discriminant is zero.
|
| 81 |
Returns: betas, lower z*(β) values, and upper z*(β) values.
|
| 82 |
"""
|
|
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|
| 83 |
betas = np.linspace(0, 1, beta_steps)
|
| 84 |
z_min_values = []
|
| 85 |
z_max_values = []
|
|
|
|
| 99 |
Compute the support boundaries of the eigenvalue distribution by directly
|
| 100 |
finding the minimum and maximum eigenvalues of B_n = S_n T_n for different beta values.
|
| 101 |
"""
|
|
|
|
|
|
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|
| 102 |
# Apply the condition for y
|
| 103 |
y_effective = y if y > 1 else 1/y
|
| 104 |
|
|
|
|
| 166 |
"""
|
| 167 |
Compute the "High y Expression" curve.
|
| 168 |
"""
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
| 169 |
# Apply the condition for y
|
| 170 |
y_effective = y if y > 1 else 1/y
|
| 171 |
|
|
|
|
| 183 |
Compute the alternate low expression:
|
| 184 |
(z_a*y*beta*(z_a-1) - 2*z_a*(1-y) - 2*z_a**2) / (2+2*z_a)
|
| 185 |
"""
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
| 186 |
# Apply the condition for y
|
| 187 |
y_effective = y if y > 1 else 1/y
|
| 188 |
|
|
|
|
| 194 |
"""
|
| 195 |
Compute max_{k ∈ (0,∞)} (y*beta*(a-1)*k + (a*k+1)*((y-1)*k-1)) / ((a*k+1)*(k^2+k))
|
| 196 |
"""
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
| 197 |
# Apply the condition for y
|
| 198 |
y_effective = y if y > 1 else 1/y
|
| 199 |
|
|
|
|
| 225 |
"""
|
| 226 |
Compute min_{t ∈ (-1/a, 0)} (y*beta*(a-1)*t + (a*t+1)*((y-1)*t-1)) / ((a*t+1)*(t^2+t))
|
| 227 |
"""
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
| 228 |
# Apply the condition for y
|
| 229 |
y_effective = y if y > 1 else 1/y
|
| 230 |
|
|
|
|
| 488 |
)
|
| 489 |
return fig
|
| 490 |
|
| 491 |
+
def compute_cubic_roots(z, beta, z_a, y):
|
| 492 |
+
"""
|
| 493 |
+
Compute the roots of the cubic equation for given parameters using SymPy for maximum accuracy.
|
| 494 |
+
"""
|
| 495 |
+
# Apply the condition for y
|
| 496 |
+
y_effective = y if y > 1 else 1/y
|
| 497 |
+
|
| 498 |
+
# Import SymPy functions
|
| 499 |
+
from sympy import symbols, solve, im, re, N, Poly
|
| 500 |
+
|
| 501 |
+
# Create a symbolic variable for the equation
|
| 502 |
+
s = symbols('s')
|
| 503 |
+
|
| 504 |
+
# Coefficients in the form as^3 + bs^2 + cs + d = 0
|
| 505 |
+
a = z * z_a
|
| 506 |
+
b = z * z_a + z + z_a - z_a*y_effective
|
| 507 |
+
c = z + z_a + 1 - y_effective*(beta*z_a + 1 - beta)
|
| 508 |
+
d = 1
|
| 509 |
+
|
| 510 |
+
# Handle special cases
|
| 511 |
+
if abs(a) < 1e-10:
|
| 512 |
+
if abs(b) < 1e-10: # Linear case
|
| 513 |
+
roots = np.array([-d/c, 0, 0], dtype=complex)
|
| 514 |
+
else: # Quadratic case
|
| 515 |
+
quad_roots = np.roots([b, c, d])
|
| 516 |
+
roots = np.append(quad_roots, 0).astype(complex)
|
| 517 |
+
return roots
|
| 518 |
+
|
| 519 |
+
try:
|
| 520 |
+
# Create the cubic polynomial
|
| 521 |
+
cubic_eq = Poly(a*s**3 + b*s**2 + c*s + d, s)
|
| 522 |
+
|
| 523 |
+
# Solve the equation symbolically
|
| 524 |
+
symbolic_roots = solve(cubic_eq, s)
|
| 525 |
+
|
| 526 |
+
# Convert symbolic roots to complex numbers with high precision
|
| 527 |
+
numerical_roots = []
|
| 528 |
+
for root in symbolic_roots:
|
| 529 |
+
# Use SymPy's N function with high precision
|
| 530 |
+
numerical_root = complex(N(root, 30))
|
| 531 |
+
numerical_roots.append(numerical_root)
|
| 532 |
+
|
| 533 |
+
# If we got fewer than 3 roots (due to multiplicity), pad with zeros
|
| 534 |
+
while len(numerical_roots) < 3:
|
| 535 |
+
numerical_roots.append(0j)
|
| 536 |
+
|
| 537 |
+
return np.array(numerical_roots, dtype=complex)
|
| 538 |
+
|
| 539 |
+
except Exception as e:
|
| 540 |
+
# Fallback to numpy if SymPy has issues
|
| 541 |
+
coeffs = [a, b, c, d]
|
| 542 |
+
return np.roots(coeffs)
|
| 543 |
|
| 544 |
+
def track_roots_consistently(z_values, all_roots):
|
| 545 |
+
"""
|
| 546 |
+
Ensure consistent tracking of roots across z values by minimizing discontinuity.
|
| 547 |
+
"""
|
| 548 |
+
n_points = len(z_values)
|
| 549 |
+
n_roots = all_roots[0].shape[0]
|
| 550 |
+
tracked_roots = np.zeros((n_points, n_roots), dtype=complex)
|
| 551 |
+
tracked_roots[0] = all_roots[0]
|
| 552 |
+
|
| 553 |
+
for i in range(1, n_points):
|
| 554 |
+
prev_roots = tracked_roots[i-1]
|
| 555 |
+
current_roots = all_roots[i]
|
| 556 |
+
|
| 557 |
+
# For each previous root, find the closest current root
|
| 558 |
+
assigned = np.zeros(n_roots, dtype=bool)
|
| 559 |
+
assignments = np.zeros(n_roots, dtype=int)
|
| 560 |
+
|
| 561 |
+
for j in range(n_roots):
|
| 562 |
+
distances = np.abs(current_roots - prev_roots[j])
|
| 563 |
+
|
| 564 |
+
# Find the closest unassigned root
|
| 565 |
+
while True:
|
| 566 |
+
best_idx = np.argmin(distances)
|
| 567 |
+
if not assigned[best_idx]:
|
| 568 |
+
assignments[j] = best_idx
|
| 569 |
+
assigned[best_idx] = True
|
| 570 |
+
break
|
| 571 |
+
else:
|
| 572 |
+
# Mark as infinite distance and try again
|
| 573 |
+
distances[best_idx] = np.inf
|
| 574 |
+
|
| 575 |
+
# Safety check if all are assigned (shouldn't happen)
|
| 576 |
+
if np.all(distances == np.inf):
|
| 577 |
+
assignments[j] = j # Default to same index
|
| 578 |
+
break
|
| 579 |
+
|
| 580 |
+
# Reorder current roots based on assignments
|
| 581 |
+
tracked_roots[i] = current_roots[assignments]
|
| 582 |
+
|
| 583 |
+
return tracked_roots
|
| 584 |
|
| 585 |
+
def generate_cubic_discriminant(z, beta, z_a, y_effective):
|
| 586 |
+
"""
|
| 587 |
+
Calculate the cubic discriminant using the standard formula.
|
| 588 |
+
For a cubic ax^3 + bx^2 + cx + d:
|
| 589 |
+
Δ = 18abcd - 27a^2d^2 + b^2c^2 - 2b^3d - 9ac^3
|
| 590 |
+
"""
|
| 591 |
+
a = z * z_a
|
| 592 |
+
b = z * z_a + z + z_a - z_a*y_effective
|
| 593 |
+
c = z + z_a + 1 - y_effective*(beta*z_a + 1 - beta)
|
| 594 |
+
d = 1
|
| 595 |
+
|
| 596 |
+
# Standard formula for cubic discriminant
|
| 597 |
+
discriminant = (18*a*b*c*d - 27*a**2*d**2 + b**2*c**2 - 2*b**3*d - 9*a*c**3)
|
| 598 |
+
return discriminant
|
| 599 |
|
| 600 |
+
def generate_root_plots(beta, y, z_a, z_min, z_max, n_points):
|
| 601 |
+
"""
|
| 602 |
+
Generate Im(s) and Re(s) vs. z plots with improved accuracy using SymPy.
|
| 603 |
+
"""
|
| 604 |
+
if z_a <= 0 or y <= 0 or z_min >= z_max:
|
| 605 |
+
st.error("Invalid input parameters.")
|
| 606 |
+
return None, None, None
|
| 607 |
+
|
| 608 |
+
# Apply the condition for y
|
| 609 |
+
y_effective = y if y > 1 else 1/y
|
| 610 |
+
|
| 611 |
+
z_points = np.linspace(z_min, z_max, n_points)
|
| 612 |
+
|
| 613 |
+
# Collect all roots first
|
| 614 |
+
all_roots = []
|
| 615 |
+
discriminants = []
|
| 616 |
+
|
| 617 |
+
# Progress indicator
|
| 618 |
+
progress_bar = st.progress(0)
|
| 619 |
+
status_text = st.empty()
|
| 620 |
|
| 621 |
+
for i, z in enumerate(z_points):
|
| 622 |
+
# Update progress
|
| 623 |
+
progress_bar.progress((i + 1) / n_points)
|
| 624 |
+
status_text.text(f"Computing roots for z = {z:.3f} ({i+1}/{n_points})")
|
| 625 |
+
|
| 626 |
+
# Calculate roots using SymPy
|
| 627 |
+
roots = compute_cubic_roots(z, beta, z_a, y)
|
| 628 |
+
|
| 629 |
+
# Initial sorting to help with tracking
|
| 630 |
+
roots = sorted(roots, key=lambda x: (abs(x.imag), x.real))
|
| 631 |
+
all_roots.append(roots)
|
| 632 |
+
|
| 633 |
+
# Calculate discriminant
|
| 634 |
+
disc = generate_cubic_discriminant(z, beta, z_a, y_effective)
|
| 635 |
+
discriminants.append(disc)
|
| 636 |
+
|
| 637 |
+
# Clear progress indicators
|
| 638 |
+
progress_bar.empty()
|
| 639 |
+
status_text.empty()
|
| 640 |
+
|
| 641 |
+
all_roots = np.array(all_roots)
|
| 642 |
+
discriminants = np.array(discriminants)
|
| 643 |
+
|
| 644 |
+
# Track roots consistently across z values
|
| 645 |
+
tracked_roots = track_roots_consistently(z_points, all_roots)
|
| 646 |
+
|
| 647 |
+
# Extract imaginary and real parts
|
| 648 |
+
ims = np.imag(tracked_roots)
|
| 649 |
+
res = np.real(tracked_roots)
|
| 650 |
+
|
| 651 |
+
# Create figure for imaginary parts
|
| 652 |
+
fig_im = go.Figure()
|
| 653 |
+
for i in range(3):
|
| 654 |
+
fig_im.add_trace(go.Scatter(x=z_points, y=ims[:, i], mode="lines", name=f"Im{{s{i+1}}}",
|
| 655 |
+
line=dict(width=2)))
|
| 656 |
+
|
| 657 |
+
# Add vertical lines at discriminant zero crossings
|
| 658 |
+
disc_zeros = []
|
| 659 |
+
for i in range(len(discriminants)-1):
|
| 660 |
+
if discriminants[i] * discriminants[i+1] <= 0: # Sign change
|
| 661 |
+
zero_pos = z_points[i] + (z_points[i+1] - z_points[i]) * (0 - discriminants[i]) / (discriminants[i+1] - discriminants[i])
|
| 662 |
+
disc_zeros.append(zero_pos)
|
| 663 |
+
fig_im.add_vline(x=zero_pos, line=dict(color="red", width=1, dash="dash"))
|
| 664 |
+
|
| 665 |
+
fig_im.update_layout(title=f"Im{{s}} vs. z (β={beta:.3f}, y={y:.3f}, z_a={z_a:.3f})",
|
| 666 |
+
xaxis_title="z", yaxis_title="Im{s}", hovermode="x unified")
|
| 667 |
|
| 668 |
+
# Create figure for real parts
|
| 669 |
+
fig_re = go.Figure()
|
| 670 |
+
for i in range(3):
|
| 671 |
+
fig_re.add_trace(go.Scatter(x=z_points, y=res[:, i], mode="lines", name=f"Re{{s{i+1}}}",
|
| 672 |
+
line=dict(width=2)))
|
| 673 |
+
|
| 674 |
+
# Add vertical lines at discriminant zero crossings
|
| 675 |
+
for zero_pos in disc_zeros:
|
| 676 |
+
fig_re.add_vline(x=zero_pos, line=dict(color="red", width=1, dash="dash"))
|
| 677 |
+
|
| 678 |
+
fig_re.update_layout(title=f"Re{{s}} vs. z (β={beta:.3f}, y={y:.3f}, z_a={z_a:.3f})",
|
| 679 |
+
xaxis_title="z", yaxis_title="Re{s}", hovermode="x unified")
|
| 680 |
+
|
| 681 |
+
# Create discriminant plot
|
| 682 |
+
fig_disc = go.Figure()
|
| 683 |
+
fig_disc.add_trace(go.Scatter(x=z_points, y=discriminants, mode="lines",
|
| 684 |
+
name="Cubic Discriminant", line=dict(color="black", width=2)))
|
| 685 |
+
fig_disc.add_hline(y=0, line=dict(color="red", width=1, dash="dash"))
|
| 686 |
+
|
| 687 |
+
fig_disc.update_layout(title=f"Cubic Discriminant vs. z (β={beta:.3f}, y={y:.3f}, z_a={z_a:.3f})",
|
| 688 |
+
xaxis_title="z", yaxis_title="Discriminant", hovermode="x unified")
|
| 689 |
+
|
| 690 |
+
return fig_im, fig_re, fig_disc
|
| 691 |
|
| 692 |
+
def analyze_complex_root_structure(beta_values, z, z_a, y):
|
| 693 |
+
"""
|
| 694 |
+
Analyze when the cubic equation switches between having all real roots
|
| 695 |
+
and having a complex conjugate pair plus one real root.
|
| 696 |
+
|
| 697 |
+
Returns:
|
| 698 |
+
- transition_points: beta values where the root structure changes
|
| 699 |
+
- structure_types: list indicating whether each interval has all real roots or complex roots
|
| 700 |
+
"""
|
| 701 |
+
# Apply the condition for y
|
| 702 |
+
y_effective = y if y > 1 else 1/y
|
| 703 |
+
|
| 704 |
+
transition_points = []
|
| 705 |
+
structure_types = []
|
| 706 |
+
|
| 707 |
+
previous_type = None
|
| 708 |
+
|
| 709 |
+
for beta in beta_values:
|
| 710 |
+
roots = compute_cubic_roots(z, beta, z_a, y)
|
| 711 |
+
|
| 712 |
+
# Check if all roots are real (imaginary parts close to zero)
|
| 713 |
+
is_all_real = all(abs(root.imag) < 1e-10 for root in roots)
|
| 714 |
+
|
| 715 |
+
current_type = "real" if is_all_real else "complex"
|
| 716 |
+
|
| 717 |
+
if previous_type is not None and current_type != previous_type:
|
| 718 |
+
# Found a transition point
|
| 719 |
+
transition_points.append(beta)
|
| 720 |
+
structure_types.append(previous_type)
|
| 721 |
+
|
| 722 |
+
previous_type = current_type
|
| 723 |
+
|
| 724 |
+
# Add the final interval type
|
| 725 |
+
if previous_type is not None:
|
| 726 |
+
structure_types.append(previous_type)
|
| 727 |
+
|
| 728 |
+
return transition_points, structure_types
|
| 729 |
|
| 730 |
+
def generate_roots_vs_beta_plots(z, y, z_a, beta_min, beta_max, n_points):
|
| 731 |
+
"""
|
| 732 |
+
Generate Im(s) and Re(s) vs. β plots with improved accuracy using SymPy.
|
| 733 |
+
"""
|
| 734 |
+
if z_a <= 0 or y <= 0 or beta_min >= beta_max:
|
| 735 |
+
st.error("Invalid input parameters.")
|
| 736 |
+
return None, None, None
|
|
|
|
|
|
|
| 737 |
|
| 738 |
+
# Apply the condition for y
|
| 739 |
+
y_effective = y if y > 1 else 1/y
|
| 740 |
+
|
| 741 |
+
beta_points = np.linspace(beta_min, beta_max, n_points)
|
| 742 |
+
|
| 743 |
+
# Collect all roots first
|
| 744 |
+
all_roots = []
|
| 745 |
+
discriminants = []
|
| 746 |
+
|
| 747 |
+
# Progress indicator
|
| 748 |
+
progress_bar = st.progress(0)
|
| 749 |
+
status_text = st.empty()
|
| 750 |
+
|
| 751 |
+
for i, beta in enumerate(beta_points):
|
| 752 |
+
# Update progress
|
| 753 |
+
progress_bar.progress((i + 1) / n_points)
|
| 754 |
+
status_text.text(f"Computing roots for β = {beta:.3f} ({i+1}/{n_points})")
|
| 755 |
+
|
| 756 |
+
# Calculate roots using SymPy
|
| 757 |
+
roots = compute_cubic_roots(z, beta, z_a, y)
|
| 758 |
+
|
| 759 |
+
# Initial sorting to help with tracking
|
| 760 |
+
roots = sorted(roots, key=lambda x: (abs(x.imag), x.real))
|
| 761 |
+
all_roots.append(roots)
|
| 762 |
+
|
| 763 |
+
# Calculate discriminant
|
| 764 |
+
disc = generate_cubic_discriminant(z, beta, z_a, y_effective)
|
| 765 |
+
discriminants.append(disc)
|
| 766 |
+
|
| 767 |
+
# Clear progress indicators
|
| 768 |
+
progress_bar.empty()
|
| 769 |
+
status_text.empty()
|
| 770 |
+
|
| 771 |
+
all_roots = np.array(all_roots)
|
| 772 |
+
discriminants = np.array(discriminants)
|
| 773 |
+
|
| 774 |
+
# Track roots consistently across beta values
|
| 775 |
+
tracked_roots = track_roots_consistently(beta_points, all_roots)
|
| 776 |
+
|
| 777 |
+
# Extract imaginary and real parts
|
| 778 |
+
ims = np.imag(tracked_roots)
|
| 779 |
+
res = np.real(tracked_roots)
|
| 780 |
+
|
| 781 |
+
# Create figure for imaginary parts
|
| 782 |
+
fig_im = go.Figure()
|
| 783 |
+
for i in range(3):
|
| 784 |
+
fig_im.add_trace(go.Scatter(x=beta_points, y=ims[:, i], mode="lines", name=f"Im{{s{i+1}}}",
|
| 785 |
+
line=dict(width=2)))
|
| 786 |
+
|
| 787 |
+
# Add vertical lines at discriminant zero crossings
|
| 788 |
+
disc_zeros = []
|
| 789 |
+
for i in range(len(discriminants)-1):
|
| 790 |
+
if discriminants[i] * discriminants[i+1] <= 0: # Sign change
|
| 791 |
+
zero_pos = beta_points[i] + (beta_points[i+1] - beta_points[i]) * (0 - discriminants[i]) / (discriminants[i+1] - discriminants[i])
|
| 792 |
+
disc_zeros.append(zero_pos)
|
| 793 |
+
fig_im.add_vline(x=zero_pos, line=dict(color="red", width=1, dash="dash"))
|
| 794 |
+
|
| 795 |
+
fig_im.update_layout(title=f"Im{{s}} vs. β (z={z:.3f}, y={y:.3f}, z_a={z_a:.3f})",
|
| 796 |
+
xaxis_title="β", yaxis_title="Im{s}", hovermode="x unified")
|
| 797 |
|
| 798 |
+
# Create figure for real parts
|
| 799 |
+
fig_re = go.Figure()
|
| 800 |
+
for i in range(3):
|
| 801 |
+
fig_re.add_trace(go.Scatter(x=beta_points, y=res[:, i], mode="lines", name=f"Re{{s{i+1}}}",
|
| 802 |
+
line=dict(width=2)))
|
| 803 |
+
|
| 804 |
+
# Add vertical lines at discriminant zero crossings
|
| 805 |
+
for zero_pos in disc_zeros:
|
| 806 |
+
fig_re.add_vline(x=zero_pos, line=dict(color="red", width=1, dash="dash"))
|
| 807 |
+
|
| 808 |
+
fig_re.update_layout(title=f"Re{{s}} vs. β (z={z:.3f}, y={y:.3f}, z_a={z_a:.3f})",
|
| 809 |
+
xaxis_title="β", yaxis_title="Re{s}", hovermode="x unified")
|
| 810 |
+
|
| 811 |
+
# Create discriminant plot
|
| 812 |
+
fig_disc = go.Figure()
|
| 813 |
+
fig_disc.add_trace(go.Scatter(x=beta_points, y=discriminants, mode="lines",
|
| 814 |
+
name="Cubic Discriminant", line=dict(color="black", width=2)))
|
| 815 |
+
fig_disc.add_hline(y=0, line=dict(color="red", width=1, dash="dash"))
|
| 816 |
+
|
| 817 |
+
fig_disc.update_layout(title=f"Cubic Discriminant vs. β (z={z:.3f}, y={y:.3f}, z_a={z_a:.3f})",
|
| 818 |
+
xaxis_title="β", yaxis_title="Discriminant", hovermode="x unified")
|
| 819 |
+
|
| 820 |
+
return fig_im, fig_re, fig_disc
|
| 821 |
|
| 822 |
+
def generate_phase_diagram(z_a, y, beta_min=0.0, beta_max=1.0, z_min=-10.0, z_max=10.0,
|
| 823 |
+
beta_steps=100, z_steps=100):
|
| 824 |
+
"""
|
| 825 |
+
Generate a phase diagram showing regions of complex and real roots.
|
| 826 |
+
|
| 827 |
+
Returns a heatmap where:
|
| 828 |
+
- Value 1 (red): Region with all real roots
|
| 829 |
+
- Value -1 (blue): Region with complex roots
|
| 830 |
+
"""
|
| 831 |
+
# Apply the condition for y
|
| 832 |
+
y_effective = y if y > 1 else 1/y
|
| 833 |
+
|
| 834 |
+
beta_values = np.linspace(beta_min, beta_max, beta_steps)
|
| 835 |
+
z_values = np.linspace(z_min, z_max, z_steps)
|
| 836 |
+
|
| 837 |
+
# Initialize phase map
|
| 838 |
+
phase_map = np.zeros((z_steps, beta_steps))
|
| 839 |
+
|
| 840 |
+
# Progress tracking
|
| 841 |
+
progress_bar = st.progress(0)
|
| 842 |
+
status_text = st.empty()
|
| 843 |
+
|
| 844 |
+
for i, z in enumerate(z_values):
|
| 845 |
+
# Update progress
|
| 846 |
+
progress_bar.progress((i + 1) / len(z_values))
|
| 847 |
+
status_text.text(f"Analyzing phase at z = {z:.2f} ({i+1}/{len(z_values)})")
|
| 848 |
+
|
| 849 |
+
for j, beta in enumerate(beta_values):
|
| 850 |
+
roots = compute_cubic_roots(z, beta, z_a, y)
|
| 851 |
+
|
| 852 |
+
# Check if all roots are real (imaginary parts close to zero)
|
| 853 |
+
is_all_real = all(abs(root.imag) < 1e-10 for root in roots)
|
| 854 |
+
|
| 855 |
+
phase_map[i, j] = 1 if is_all_real else -1
|
| 856 |
+
|
| 857 |
+
# Clear progress indicators
|
| 858 |
+
progress_bar.empty()
|
| 859 |
+
status_text.empty()
|
| 860 |
+
|
| 861 |
+
# Create heatmap
|
| 862 |
+
fig = go.Figure(data=go.Heatmap(
|
| 863 |
+
z=phase_map,
|
| 864 |
+
x=beta_values,
|
| 865 |
+
y=z_values,
|
| 866 |
+
colorscale=[[0, 'blue'], [0.5, 'white'], [1.0, 'red']],
|
| 867 |
+
zmin=-1,
|
| 868 |
+
zmax=1,
|
| 869 |
+
showscale=True,
|
| 870 |
+
colorbar=dict(
|
| 871 |
+
title="Root Type",
|
| 872 |
+
tickvals=[-1, 1],
|
| 873 |
+
ticktext=["Complex Roots", "All Real Roots"]
|
| 874 |
+
)
|
| 875 |
+
))
|
| 876 |
+
|
| 877 |
+
fig.update_layout(
|
| 878 |
+
title=f"Phase Diagram: Root Structure (y={y:.3f}, z_a={z_a:.3f})",
|
| 879 |
+
xaxis_title="β",
|
| 880 |
+
yaxis_title="z",
|
| 881 |
+
hovermode="closest"
|
| 882 |
+
)
|
| 883 |
+
|
| 884 |
+
return fig
|
| 885 |
|
| 886 |
+
@st.cache_data
|
| 887 |
+
def generate_eigenvalue_distribution(beta, y, z_a, n=1000, seed=42):
|
| 888 |
+
"""
|
| 889 |
+
Generate the eigenvalue distribution of B_n = S_n T_n as n→∞
|
| 890 |
+
"""
|
| 891 |
+
# Apply the condition for y
|
| 892 |
+
y_effective = y if y > 1 else 1/y
|
| 893 |
+
|
| 894 |
+
# Set random seed
|
| 895 |
+
np.random.seed(seed)
|
| 896 |
+
|
| 897 |
+
# Compute dimension p based on aspect ratio y
|
| 898 |
+
p = int(y_effective * n)
|
| 899 |
+
|
| 900 |
+
# Constructing T_n (Population / Shape Matrix) - using the approach from the second script
|
| 901 |
+
k = int(np.floor(beta * p))
|
| 902 |
+
diag_entries = np.concatenate([
|
| 903 |
+
np.full(k, z_a),
|
| 904 |
+
np.full(p - k, 1.0)
|
| 905 |
+
])
|
| 906 |
+
np.random.shuffle(diag_entries)
|
| 907 |
+
T_n = np.diag(diag_entries)
|
| 908 |
+
|
| 909 |
+
# Generate the data matrix X with i.i.d. standard normal entries
|
| 910 |
+
X = np.random.randn(p, n)
|
| 911 |
+
|
| 912 |
+
# Compute the sample covariance matrix S_n = (1/n) * XX^T
|
| 913 |
+
S_n = (1 / n) * (X @ X.T)
|
| 914 |
+
|
| 915 |
+
# Compute B_n = S_n T_n
|
| 916 |
+
B_n = S_n @ T_n
|
| 917 |
+
|
| 918 |
+
# Compute eigenvalues of B_n
|
| 919 |
+
eigenvalues = np.linalg.eigvalsh(B_n)
|
| 920 |
+
|
| 921 |
+
# Use KDE to compute a smooth density estimate
|
| 922 |
+
kde = gaussian_kde(eigenvalues)
|
| 923 |
+
x_vals = np.linspace(min(eigenvalues), max(eigenvalues), 500)
|
| 924 |
+
kde_vals = kde(x_vals)
|
| 925 |
+
|
| 926 |
+
# Create figure
|
| 927 |
+
fig = go.Figure()
|
| 928 |
+
|
| 929 |
+
# Add histogram trace
|
| 930 |
+
fig.add_trace(go.Histogram(x=eigenvalues, histnorm='probability density',
|
| 931 |
+
name="Histogram", marker=dict(color='blue', opacity=0.6)))
|
| 932 |
+
|
| 933 |
+
# Add KDE trace
|
| 934 |
+
fig.add_trace(go.Scatter(x=x_vals, y=kde_vals, mode="lines",
|
| 935 |
+
name="KDE", line=dict(color='red', width=2)))
|
| 936 |
+
|
| 937 |
+
fig.update_layout(
|
| 938 |
+
title=f"Eigenvalue Distribution for B_n = S_n T_n (y={y:.1f}, β={beta:.2f}, a={z_a:.1f})",
|
| 939 |
+
xaxis_title="Eigenvalue",
|
| 940 |
+
yaxis_title="Density",
|
| 941 |
+
hovermode="closest",
|
| 942 |
+
showlegend=True
|
| 943 |
+
)
|
| 944 |
+
|
| 945 |
+
return fig, eigenvalues
|
| 946 |
+
|
| 947 |
+
# ----------------- Streamlit UI -----------------
|
| 948 |
+
st.title("Cubic Root Analysis")
|
| 949 |
+
|
| 950 |
+
# Define three tabs
|
| 951 |
+
tab1, tab2, tab3 = st.tabs(["z*(β) Curves", "Complex Root Analysis", "Differential Analysis"])
|
| 952 |
+
|
| 953 |
+
# ----- Tab 1: z*(β) Curves -----
|
| 954 |
+
with tab1:
|
| 955 |
+
st.header("Eigenvalue Support Boundaries")
|
| 956 |
+
|
| 957 |
+
# Cleaner layout with better column organization
|
| 958 |
+
col1, col2, col3 = st.columns([1, 1, 2])
|
| 959 |
+
|
| 960 |
+
with col1:
|
| 961 |
+
z_a_1 = st.number_input("z_a", value=1.0, key="z_a_1")
|
| 962 |
+
y_1 = st.number_input("y", value=1.0, key="y_1")
|
| 963 |
+
|
| 964 |
+
with col2:
|
| 965 |
+
z_min_1 = st.number_input("z_min", value=-10.0, key="z_min_1")
|
| 966 |
+
z_max_1 = st.number_input("z_max", value=10.0, key="z_max_1")
|
| 967 |
+
|
| 968 |
+
with col1:
|
| 969 |
+
method_type = st.radio(
|
| 970 |
+
"Calculation Method",
|
| 971 |
+
["Eigenvalue Method", "Discriminant Method"],
|
| 972 |
+
index=0 # Default to eigenvalue method
|
| 973 |
+
)
|
| 974 |
+
|
| 975 |
+
# Advanced settings in collapsed expanders
|
| 976 |
+
with st.expander("Method Settings", expanded=False):
|
| 977 |
+
if method_type == "Eigenvalue Method":
|
| 978 |
+
beta_steps = st.slider("β steps", min_value=21, max_value=101, value=51, step=10,
|
| 979 |
+
key="beta_steps_eigen")
|
| 980 |
+
n_samples = st.slider("Matrix size (n)", min_value=100, max_value=2000, value=1000,
|
| 981 |
+
step=100)
|
| 982 |
+
seeds = st.slider("Number of seeds", min_value=1, max_value=10, value=5, step=1)
|
| 983 |
else:
|
| 984 |
+
beta_steps = st.slider("β steps", min_value=51, max_value=501, value=201, step=50,
|
| 985 |
+
key="beta_steps")
|
| 986 |
+
z_steps = st.slider("z grid steps", min_value=1000, max_value=100000, value=50000,
|
| 987 |
+
step=1000, key="z_steps")
|
| 988 |
+
|
| 989 |
+
# Curve visibility options
|
| 990 |
+
with st.expander("Curve Visibility", expanded=False):
|
| 991 |
+
col_vis1, col_vis2 = st.columns(2)
|
| 992 |
+
with col_vis1:
|
| 993 |
+
show_high_y = st.checkbox("Show High y Expression", value=False, key="show_high_y")
|
| 994 |
+
show_max_k = st.checkbox("Show Max k Expression", value=True, key="show_max_k")
|
| 995 |
+
with col_vis2:
|
| 996 |
+
show_low_y = st.checkbox("Show Low y Expression", value=False, key="show_low_y")
|
| 997 |
+
show_min_t = st.checkbox("Show Min t Expression", value=True, key="show_min_t")
|
| 998 |
+
|
| 999 |
+
# Custom expressions collapsed by default
|
| 1000 |
+
with st.expander("Custom Expression 1 (s-based)", expanded=False):
|
| 1001 |
+
st.markdown("""Enter expressions for s = numerator/denominator
|
| 1002 |
+
(using variables `y`, `beta`, `z_a`, and `sqrt()`)""")
|
| 1003 |
+
st.latex(r"\text{This s will be inserted into:}")
|
| 1004 |
+
st.latex(r"\frac{y\beta(z_a-1)\underline{s}+(a\underline{s}+1)((y-1)\underline{s}-1)}{(a\underline{s}+1)(\underline{s}^2 + \underline{s})}")
|
| 1005 |
+
s_num = st.text_input("s numerator", value="", key="s_num")
|
| 1006 |
+
s_denom = st.text_input("s denominator", value="", key="s_denom")
|
| 1007 |
+
|
| 1008 |
+
with st.expander("Custom Expression 2 (direct z(β))", expanded=False):
|
| 1009 |
+
st.markdown("""Enter direct expression for z(β) = numerator/denominator
|
| 1010 |
+
(using variables `y`, `beta`, `z_a`, and `sqrt()`)""")
|
| 1011 |
+
z_num = st.text_input("z(β) numerator", value="", key="z_num")
|
| 1012 |
+
z_denom = st.text_input("z(β) denominator", value="", key="z_denom")
|
| 1013 |
+
|
| 1014 |
+
# Move show_derivatives to main UI level for better visibility
|
| 1015 |
+
with col2:
|
| 1016 |
+
show_derivatives = st.checkbox("Show derivatives", value=False)
|
| 1017 |
+
|
| 1018 |
+
# Compute button
|
| 1019 |
+
if st.button("Compute Curves", key="tab1_button"):
|
| 1020 |
+
with col3:
|
| 1021 |
+
use_eigenvalue_method = (method_type == "Eigenvalue Method")
|
| 1022 |
+
if use_eigenvalue_method:
|
| 1023 |
+
fig = generate_z_vs_beta_plot(z_a_1, y_1, z_min_1, z_max_1, beta_steps, None,
|
| 1024 |
+
s_num, s_denom, z_num, z_denom, show_derivatives,
|
| 1025 |
+
show_high_y, show_low_y, show_max_k, show_min_t,
|
| 1026 |
+
use_eigenvalue_method=True, n_samples=n_samples,
|
| 1027 |
+
seeds=seeds)
|
| 1028 |
+
else:
|
| 1029 |
+
fig = generate_z_vs_beta_plot(z_a_1, y_1, z_min_1, z_max_1, beta_steps, z_steps,
|
| 1030 |
+
s_num, s_denom, z_num, z_denom, show_derivatives,
|
| 1031 |
+
show_high_y, show_low_y, show_max_k, show_min_t,
|
| 1032 |
+
use_eigenvalue_method=False)
|
| 1033 |
+
|
| 1034 |
+
if fig is not None:
|
| 1035 |
+
st.plotly_chart(fig, use_container_width=True)
|
| 1036 |
+
|
| 1037 |
+
# Curve explanations in collapsed expander
|
| 1038 |
+
with st.expander("Curve Explanations", expanded=False):
|
| 1039 |
+
if use_eigenvalue_method:
|
| 1040 |
+
st.markdown("""
|
| 1041 |
+
- **Upper/Lower Bounds** (Blue): Maximum/minimum eigenvalues of B_n = S_n T_n
|
| 1042 |
+
- **Shaded Region**: Eigenvalue support region
|
| 1043 |
+
- **High y Expression** (Green): Asymptotic approximation for high y values
|
| 1044 |
+
- **Low Expression** (Orange): Alternative asymptotic expression
|
| 1045 |
+
- **Max k Expression** (Red): $\\max_{k \\in (0,\\infty)} \\frac{y\\beta (a-1)k + \\bigl(ak+1\\bigr)\\bigl((y-1)k-1\\bigr)}{(ak+1)(k^2+k)}$
|
| 1046 |
+
- **Min t Expression** (Purple): $\\min_{t \\in \\left(-\\frac{1}{a},\\, 0\\right)} \\frac{y\\beta (a-1)t + \\bigl(at+1\\bigr)\\bigl((y-1)t-1\\bigr)}{(at+1)(t^2+t)}$
|
| 1047 |
+
- **Custom Expression 1** (Magenta): Result from user-defined s substituted into the main formula
|
| 1048 |
+
- **Custom Expression 2** (Brown): Direct z(β) expression
|
| 1049 |
+
""")
|
| 1050 |
+
else:
|
| 1051 |
+
st.markdown("""
|
| 1052 |
+
- **Upper z*(β)** (Blue): Maximum z value where discriminant is zero
|
| 1053 |
+
- **Lower z*(β)** (Blue): Minimum z value where discriminant is zero
|
| 1054 |
+
- **High y Expression** (Green): Asymptotic approximation for high y values
|
| 1055 |
+
- **Low Expression** (Orange): Alternative asymptotic expression
|
| 1056 |
+
- **Max k Expression** (Red): $\\max_{k \\in (0,\\infty)} \\frac{y\\beta (a-1)k + \\bigl(ak+1\\bigr)\\bigl((y-1)k-1\\bigr)}{(ak+1)(k^2+k)}$
|
| 1057 |
+
- **Min t Expression** (Purple): $\\min_{t \\in \\left(-\\frac{1}{a},\\, 0\\right)} \\frac{y\\beta (a-1)t + \\bigl(at+1\\bigr)\\bigl((y-1)t-1\\bigr)}{(at+1)(t^2+t)}$
|
| 1058 |
+
- **Custom Expression 1** (Magenta): Result from user-defined s substituted into the main formula
|
| 1059 |
+
- **Custom Expression 2** (Brown): Direct z(β) expression
|
| 1060 |
+
""")
|
| 1061 |
+
if show_derivatives:
|
| 1062 |
+
st.markdown("""
|
| 1063 |
+
Derivatives are shown as:
|
| 1064 |
+
- Dashed lines: First derivatives (d/dβ)
|
| 1065 |
+
- Dotted lines: Second derivatives (d²/dβ²)
|
| 1066 |
+
""")
|
| 1067 |
+
|
| 1068 |
+
# ----- Tab 2: Complex Root Analysis -----
|
| 1069 |
+
with tab2:
|
| 1070 |
+
st.header("Complex Root Analysis")
|
| 1071 |
+
|
| 1072 |
+
# Create tabs within the page for different plots
|
| 1073 |
+
plot_tabs = st.tabs(["Im{s} vs. z", "Im{s} vs. β", "Phase Diagram", "Eigenvalue Distribution"])
|
| 1074 |
+
|
| 1075 |
+
# Tab for Im{s} vs. z plot
|
| 1076 |
+
with plot_tabs[0]:
|
| 1077 |
+
col1, col2 = st.columns([1, 2])
|
| 1078 |
+
with col1:
|
| 1079 |
+
beta_z = st.number_input("β", value=0.5, min_value=0.0, max_value=1.0, key="beta_tab2_z")
|
| 1080 |
+
y_z = st.number_input("y", value=1.0, key="y_tab2_z")
|
| 1081 |
+
z_a_z = st.number_input("z_a", value=1.0, key="z_a_tab2_z")
|
| 1082 |
+
z_min_z = st.number_input("z_min", value=-10.0, key="z_min_tab2_z")
|
| 1083 |
+
z_max_z = st.number_input("z_max", value=10.0, key="z_max_tab2_z")
|
| 1084 |
+
with st.expander("Resolution Settings", expanded=False):
|
| 1085 |
+
z_points = st.slider("z grid points", min_value=100, max_value=2000, value=500, step=100, key="z_points_z")
|
| 1086 |
+
if st.button("Compute Complex Roots vs. z", key="tab2_button_z"):
|
| 1087 |
+
with col2:
|
| 1088 |
+
fig_im, fig_re, fig_disc = generate_root_plots(beta_z, y_z, z_a_z, z_min_z, z_max_z, z_points)
|
| 1089 |
+
if fig_im is not None and fig_re is not None and fig_disc is not None:
|
| 1090 |
+
st.plotly_chart(fig_im, use_container_width=True)
|
| 1091 |
+
st.plotly_chart(fig_re, use_container_width=True)
|
| 1092 |
+
st.plotly_chart(fig_disc, use_container_width=True)
|
| 1093 |
+
|
| 1094 |
+
with st.expander("Root Structure Analysis", expanded=False):
|
| 1095 |
+
st.markdown("""
|
| 1096 |
+
### Root Structure Explanation
|
| 1097 |
+
|
| 1098 |
+
The red dashed vertical lines mark the points where the cubic discriminant equals zero.
|
| 1099 |
+
At these points, the cubic equation's root structure changes:
|
| 1100 |
+
|
| 1101 |
+
- When the discriminant is positive, the cubic has three distinct real roots.
|
| 1102 |
+
- When the discriminant is negative, the cubic has one real root and two complex conjugate roots.
|
| 1103 |
+
- When the discriminant is exactly zero, the cubic has at least two equal roots.
|
| 1104 |
+
|
| 1105 |
+
These transition points align perfectly with the z*(β) boundary curves from the first tab,
|
| 1106 |
+
which represent exactly these transitions in the (β,z) plane.
|
| 1107 |
+
""")
|
| 1108 |
+
|
| 1109 |
+
# New tab for Im{s} vs. β plot
|
| 1110 |
+
with plot_tabs[1]:
|
| 1111 |
+
col1, col2 = st.columns([1, 2])
|
| 1112 |
+
with col1:
|
| 1113 |
+
z_beta = st.number_input("z", value=1.0, key="z_tab2_beta")
|
| 1114 |
+
y_beta = st.number_input("y", value=1.0, key="y_tab2_beta")
|
| 1115 |
+
z_a_beta = st.number_input("z_a", value=1.0, key="z_a_tab2_beta")
|
| 1116 |
+
beta_min = st.number_input("β_min", value=0.0, min_value=0.0, max_value=1.0, key="beta_min_tab2")
|
| 1117 |
+
beta_max = st.number_input("β_max", value=1.0, min_value=0.0, max_value=1.0, key="beta_max_tab2")
|
| 1118 |
+
with st.expander("Resolution Settings", expanded=False):
|
| 1119 |
+
beta_points = st.slider("β grid points", min_value=100, max_value=1000, value=500, step=100, key="beta_points")
|
| 1120 |
+
if st.button("Compute Complex Roots vs. β", key="tab2_button_beta"):
|
| 1121 |
+
with col2:
|
| 1122 |
+
fig_im_beta, fig_re_beta, fig_disc = generate_roots_vs_beta_plots(
|
| 1123 |
+
z_beta, y_beta, z_a_beta, beta_min, beta_max, beta_points)
|
| 1124 |
+
|
| 1125 |
+
if fig_im_beta is not None and fig_re_beta is not None and fig_disc is not None:
|
| 1126 |
+
st.plotly_chart(fig_im_beta, use_container_width=True)
|
| 1127 |
+
st.plotly_chart(fig_re_beta, use_container_width=True)
|
| 1128 |
+
st.plotly_chart(fig_disc, use_container_width=True)
|
| 1129 |
+
|
| 1130 |
+
# Add analysis of transition points
|
| 1131 |
+
transition_points, structure_types = analyze_complex_root_structure(
|
| 1132 |
+
np.linspace(beta_min, beta_max, beta_points), z_beta, z_a_beta, y_beta)
|
| 1133 |
+
|
| 1134 |
+
if transition_points:
|
| 1135 |
+
st.subheader("Root Structure Transition Points")
|
| 1136 |
+
for i, beta in enumerate(transition_points):
|
| 1137 |
+
prev_type = structure_types[i]
|
| 1138 |
+
next_type = structure_types[i+1] if i+1 < len(structure_types) else "unknown"
|
| 1139 |
+
st.markdown(f"- At β = {beta:.6f}: Transition from {prev_type} roots to {next_type} roots")
|
| 1140 |
+
else:
|
| 1141 |
+
st.info("No transitions detected in root structure across this β range.")
|
| 1142 |
+
|
| 1143 |
+
# Explanation
|
| 1144 |
+
with st.expander("Analysis Explanation", expanded=False):
|
| 1145 |
+
st.markdown("""
|
| 1146 |
+
### Interpreting the Plots
|
| 1147 |
+
|
| 1148 |
+
- **Im{s} vs. β**: Shows how the imaginary parts of the roots change with β. When all curves are at Im{s}=0, all roots are real.
|
| 1149 |
+
- **Re{s} vs. β**: Shows how the real parts of the roots change with β.
|
| 1150 |
+
- **Discriminant Plot**: The cubic discriminant changes sign at points where the root structure changes.
|
| 1151 |
+
- When discriminant < 0: The cubic has one real root and two complex conjugate roots.
|
| 1152 |
+
- When discriminant > 0: The cubic has three distinct real roots.
|
| 1153 |
+
- When discriminant = 0: The cubic has multiple roots (at least two roots are equal).
|
| 1154 |
+
|
| 1155 |
+
The vertical red dashed lines mark the transition points where the root structure changes.
|
| 1156 |
+
""")
|
| 1157 |
+
|
| 1158 |
+
# Tab for Phase Diagram
|
| 1159 |
+
with plot_tabs[2]:
|
| 1160 |
+
col1, col2 = st.columns([1, 2])
|
| 1161 |
+
with col1:
|
| 1162 |
+
z_a_phase = st.number_input("z_a", value=1.0, key="z_a_phase")
|
| 1163 |
+
y_phase = st.number_input("y", value=1.0, key="y_phase")
|
| 1164 |
+
beta_min_phase = st.number_input("β_min", value=0.0, min_value=0.0, max_value=1.0, key="beta_min_phase")
|
| 1165 |
+
beta_max_phase = st.number_input("β_max", value=1.0, min_value=0.0, max_value=1.0, key="beta_max_phase")
|
| 1166 |
+
z_min_phase = st.number_input("z_min", value=-10.0, key="z_min_phase")
|
| 1167 |
+
z_max_phase = st.number_input("z_max", value=10.0, key="z_max_phase")
|
| 1168 |
+
|
| 1169 |
+
with st.expander("Resolution Settings", expanded=False):
|
| 1170 |
+
beta_steps_phase = st.slider("β grid points", min_value=20, max_value=200, value=100, step=20, key="beta_steps_phase")
|
| 1171 |
+
z_steps_phase = st.slider("z grid points", min_value=20, max_value=200, value=100, step=20, key="z_steps_phase")
|
| 1172 |
|
| 1173 |
+
if st.button("Generate Phase Diagram", key="tab2_button_phase"):
|
| 1174 |
+
with col2:
|
| 1175 |
+
st.info("Generating phase diagram. This may take a while depending on resolution...")
|
| 1176 |
+
fig_phase = generate_phase_diagram(
|
| 1177 |
+
z_a_phase, y_phase, beta_min_phase, beta_max_phase, z_min_phase, z_max_phase,
|
| 1178 |
+
beta_steps_phase, z_steps_phase)
|
| 1179 |
+
|
| 1180 |
+
if fig_phase is not None:
|
| 1181 |
+
st.plotly_chart(fig_phase, use_container_width=True)
|
| 1182 |
+
|
| 1183 |
+
with st.expander("Phase Diagram Explanation", expanded=False):
|
| 1184 |
+
st.markdown("""
|
| 1185 |
+
### Understanding the Phase Diagram
|
| 1186 |
+
|
| 1187 |
+
This heatmap shows the regions in the (β, z) plane where:
|
| 1188 |
+
|
| 1189 |
+
- **Red Regions**: The cubic equation has all real roots
|
| 1190 |
+
- **Blue Regions**: The cubic equation has one real root and two complex conjugate roots
|
| 1191 |
+
|
| 1192 |
+
The boundaries between these regions represent values where the discriminant is zero,
|
| 1193 |
+
which are the exact same curves as the z*(β) boundaries in the first tab. This phase
|
| 1194 |
+
diagram provides a comprehensive view of the eigenvalue support structure.
|
| 1195 |
+
""")
|
| 1196 |
+
|
| 1197 |
+
# Eigenvalue distribution tab
|
| 1198 |
+
with plot_tabs[3]:
|
| 1199 |
+
st.subheader("Eigenvalue Distribution for B_n = S_n T_n")
|
| 1200 |
+
with st.expander("Simulation Information", expanded=False):
|
| 1201 |
+
st.markdown("""
|
| 1202 |
+
This simulation generates the eigenvalue distribution of B_n as n→∞, where:
|
| 1203 |
+
- B_n = (1/n)XX^T with X being a p×n matrix
|
| 1204 |
+
- p/n → y as n→∞
|
| 1205 |
+
- The diagonal entries of T_n follow distribution β·δ(z_a) + (1-β)·δ(1)
|
| 1206 |
+
""")
|
| 1207 |
+
|
| 1208 |
+
col_eigen1, col_eigen2 = st.columns([1, 2])
|
| 1209 |
+
with col_eigen1:
|
| 1210 |
+
beta_eigen = st.number_input("β", value=0.5, min_value=0.0, max_value=1.0, key="beta_eigen")
|
| 1211 |
+
y_eigen = st.number_input("y", value=1.0, key="y_eigen")
|
| 1212 |
+
z_a_eigen = st.number_input("z_a", value=1.0, key="z_a_eigen")
|
| 1213 |
+
n_samples = st.slider("Number of samples (n)", min_value=100, max_value=2000, value=1000, step=100)
|
| 1214 |
+
sim_seed = st.number_input("Random seed", min_value=1, max_value=1000, value=42, step=1)
|
| 1215 |
|
| 1216 |
+
# Add comparison option
|
| 1217 |
+
show_theoretical = st.checkbox("Show theoretical boundaries", value=True)
|
| 1218 |
+
show_empirical_stats = st.checkbox("Show empirical statistics", value=True)
|
| 1219 |
+
|
| 1220 |
+
if st.button("Generate Eigenvalue Distribution", key="tab2_eigen_button"):
|
| 1221 |
+
with col_eigen2:
|
| 1222 |
+
# Generate the eigenvalue distribution
|
| 1223 |
+
fig_eigen, eigenvalues = generate_eigenvalue_distribution(beta_eigen, y_eigen, z_a_eigen, n=n_samples, seed=sim_seed)
|
| 1224 |
+
|
| 1225 |
+
# If requested, compute and add theoretical boundaries
|
| 1226 |
+
if show_theoretical:
|
| 1227 |
+
# Calculate min and max eigenvalues using the support boundary functions
|
| 1228 |
+
betas = np.array([beta_eigen])
|
| 1229 |
+
min_eig, max_eig = compute_eigenvalue_support_boundaries(z_a_eigen, y_eigen, betas, n_samples=n_samples, seeds=5)
|
| 1230 |
+
|
| 1231 |
+
# Add vertical lines for boundaries
|
| 1232 |
+
fig_eigen.add_vline(
|
| 1233 |
+
x=min_eig[0],
|
| 1234 |
+
line=dict(color="red", width=2, dash="dash"),
|
| 1235 |
+
annotation_text="Min theoretical",
|
| 1236 |
+
annotation_position="top right"
|
| 1237 |
+
)
|
| 1238 |
+
fig_eigen.add_vline(
|
| 1239 |
+
x=max_eig[0],
|
| 1240 |
+
line=dict(color="red", width=2, dash="dash"),
|
| 1241 |
+
annotation_text="Max theoretical",
|
| 1242 |
+
annotation_position="top left"
|
| 1243 |
+
)
|
| 1244 |
+
|
| 1245 |
+
# Display the plot
|
| 1246 |
+
st.plotly_chart(fig_eigen, use_container_width=True)
|
| 1247 |
+
|
| 1248 |
+
# Add comparison of empirical vs theoretical bounds
|
| 1249 |
+
if show_theoretical and show_empirical_stats:
|
| 1250 |
+
empirical_min = eigenvalues.min()
|
| 1251 |
+
empirical_max = eigenvalues.max()
|
| 1252 |
+
|
| 1253 |
+
st.markdown("### Comparison of Empirical vs Theoretical Bounds")
|
| 1254 |
+
col1, col2, col3 = st.columns(3)
|
| 1255 |
+
with col1:
|
| 1256 |
+
st.metric("Theoretical Min", f"{min_eig[0]:.4f}")
|
| 1257 |
+
st.metric("Theoretical Max", f"{max_eig[0]:.4f}")
|
| 1258 |
+
st.metric("Theoretical Width", f"{max_eig[0] - min_eig[0]:.4f}")
|
| 1259 |
+
with col2:
|
| 1260 |
+
st.metric("Empirical Min", f"{empirical_min:.4f}")
|
| 1261 |
+
st.metric("Empirical Max", f"{empirical_max:.4f}")
|
| 1262 |
+
st.metric("Empirical Width", f"{empirical_max - empirical_min:.4f}")
|
| 1263 |
+
with col3:
|
| 1264 |
+
st.metric("Min Difference", f"{empirical_min - min_eig[0]:.4f}")
|
| 1265 |
+
st.metric("Max Difference", f"{empirical_max - max_eig[0]:.4f}")
|
| 1266 |
+
st.metric("Width Difference", f"{(empirical_max - empirical_min) - (max_eig[0] - min_eig[0]):.4f}")
|
| 1267 |
+
|
| 1268 |
+
# Display additional statistics
|
| 1269 |
+
if show_empirical_stats:
|
| 1270 |
+
st.markdown("### Eigenvalue Statistics")
|
| 1271 |
+
col1, col2 = st.columns(2)
|
| 1272 |
+
with col1:
|
| 1273 |
+
st.metric("Mean", f"{np.mean(eigenvalues):.4f}")
|
| 1274 |
+
st.metric("Median", f"{np.median(eigenvalues):.4f}")
|
| 1275 |
+
with col2:
|
| 1276 |
+
st.metric("Standard Deviation", f"{np.std(eigenvalues):.4f}")
|
| 1277 |
+
st.metric("Interquartile Range", f"{np.percentile(eigenvalues, 75) - np.percentile(eigenvalues, 25):.4f}")
|
| 1278 |
|
| 1279 |
+
# ----- Tab 3: Differential Analysis -----
|
| 1280 |
+
with tab3:
|
| 1281 |
+
st.header("Differential Analysis vs. β")
|
| 1282 |
+
with st.expander("Description", expanded=False):
|
| 1283 |
+
st.markdown("This page shows the difference between the Upper (blue) and Lower (lightblue) z*(β) curves, along with their first and second derivatives with respect to β.")
|
| 1284 |
+
|
| 1285 |
+
col1, col2 = st.columns([1, 2])
|
| 1286 |
+
with col1:
|
| 1287 |
+
z_a_diff = st.number_input("z_a", value=1.0, key="z_a_diff")
|
| 1288 |
+
y_diff = st.number_input("y", value=1.0, key="y_diff")
|
| 1289 |
+
z_min_diff = st.number_input("z_min", value=-10.0, key="z_min_diff")
|
| 1290 |
+
z_max_diff = st.number_input("z_max", value=10.0, key="z_max_diff")
|
| 1291 |
+
|
| 1292 |
+
diff_method_type = st.radio(
|
| 1293 |
+
"Boundary Calculation Method",
|
| 1294 |
+
["Eigenvalue Method", "Discriminant Method"],
|
| 1295 |
+
index=0,
|
| 1296 |
+
key="diff_method_type"
|
| 1297 |
+
)
|
| 1298 |
+
|
| 1299 |
+
with st.expander("Resolution Settings", expanded=False):
|
| 1300 |
+
if diff_method_type == "Eigenvalue Method":
|
| 1301 |
+
beta_steps_diff = st.slider("β steps", min_value=21, max_value=101, value=51, step=10,
|
| 1302 |
+
key="beta_steps_diff_eigen")
|
| 1303 |
+
diff_n_samples = st.slider("Matrix size (n)", min_value=100, max_value=2000, value=1000,
|
| 1304 |
+
step=100, key="diff_n_samples")
|
| 1305 |
+
diff_seeds = st.slider("Number of seeds", min_value=1, max_value=10, value=5, step=1,
|
| 1306 |
+
key="diff_seeds")
|
| 1307 |
+
else:
|
| 1308 |
+
beta_steps_diff = st.slider("β steps", min_value=51, max_value=501, value=201, step=50,
|
| 1309 |
+
key="beta_steps_diff")
|
| 1310 |
+
z_steps_diff = st.slider("z grid steps", min_value=1000, max_value=100000, value=50000,
|
| 1311 |
+
step=1000, key="z_steps_diff")
|
| 1312 |
+
|
| 1313 |
+
# Add options for curve selection
|
| 1314 |
+
st.subheader("Curves to Analyze")
|
| 1315 |
+
analyze_upper_lower = st.checkbox("Upper-Lower Difference", value=True)
|
| 1316 |
+
analyze_high_y = st.checkbox("High y Expression", value=False)
|
| 1317 |
+
analyze_alt_low = st.checkbox("Low y Expression", value=False)
|
| 1318 |
+
|
| 1319 |
+
if st.button("Compute Differentials", key="tab3_button"):
|
| 1320 |
+
with col2:
|
| 1321 |
+
use_eigenvalue_method_diff = (diff_method_type == "Eigenvalue Method")
|
| 1322 |
+
|
| 1323 |
+
if use_eigenvalue_method_diff:
|
| 1324 |
+
betas_diff = np.linspace(0, 1, beta_steps_diff)
|
| 1325 |
+
st.info("Computing eigenvalue support boundaries. This may take a moment...")
|
| 1326 |
+
lower_vals, upper_vals = compute_eigenvalue_support_boundaries(
|
| 1327 |
+
z_a_diff, y_diff, betas_diff, diff_n_samples, diff_seeds)
|
| 1328 |
+
else:
|
| 1329 |
+
betas_diff, lower_vals, upper_vals = sweep_beta_and_find_z_bounds(
|
| 1330 |
+
z_a_diff, y_diff, z_min_diff, z_max_diff, beta_steps_diff, z_steps_diff)
|
| 1331 |
+
|
| 1332 |
+
# Create figure
|
| 1333 |
+
fig_diff = go.Figure()
|
| 1334 |
+
|
| 1335 |
+
if analyze_upper_lower:
|
| 1336 |
+
diff_curve = upper_vals - lower_vals
|
| 1337 |
+
d1 = np.gradient(diff_curve, betas_diff)
|
| 1338 |
+
d2 = np.gradient(d1, betas_diff)
|
| 1339 |
+
|
| 1340 |
+
fig_diff.add_trace(go.Scatter(x=betas_diff, y=diff_curve, mode="lines",
|
| 1341 |
+
name="Upper-Lower Difference", line=dict(color="magenta", width=2)))
|
| 1342 |
+
fig_diff.add_trace(go.Scatter(x=betas_diff, y=d1, mode="lines",
|
| 1343 |
+
name="Upper-Lower d/dβ", line=dict(color="magenta", dash='dash')))
|
| 1344 |
+
fig_diff.add_trace(go.Scatter(x=betas_diff, y=d2, mode="lines",
|
| 1345 |
+
name="Upper-Lower d²/dβ²", line=dict(color="magenta", dash='dot')))
|
| 1346 |
+
|
| 1347 |
+
if analyze_high_y:
|
| 1348 |
+
high_y_curve = compute_high_y_curve(betas_diff, z_a_diff, y_diff)
|
| 1349 |
+
d1 = np.gradient(high_y_curve, betas_diff)
|
| 1350 |
+
d2 = np.gradient(d1, betas_diff)
|
| 1351 |
+
|
| 1352 |
+
fig_diff.add_trace(go.Scatter(x=betas_diff, y=high_y_curve, mode="lines",
|
| 1353 |
+
name="High y", line=dict(color="green", width=2)))
|
| 1354 |
+
fig_diff.add_trace(go.Scatter(x=betas_diff, y=d1, mode="lines",
|
| 1355 |
+
name="High y d/dβ", line=dict(color="green", dash='dash')))
|
| 1356 |
+
fig_diff.add_trace(go.Scatter(x=betas_diff, y=d2, mode="lines",
|
| 1357 |
+
name="High y d²/dβ²", line=dict(color="green", dash='dot')))
|
| 1358 |
+
|
| 1359 |
+
if analyze_alt_low:
|
| 1360 |
+
alt_low_curve = compute_alternate_low_expr(betas_diff, z_a_diff, y_diff)
|
| 1361 |
+
d1 = np.gradient(alt_low_curve, betas_diff)
|
| 1362 |
+
d2 = np.gradient(d1, betas_diff)
|
| 1363 |
+
|
| 1364 |
+
fig_diff.add_trace(go.Scatter(x=betas_diff, y=alt_low_curve, mode="lines",
|
| 1365 |
+
name="Low y", line=dict(color="orange", width=2)))
|
| 1366 |
+
fig_diff.add_trace(go.Scatter(x=betas_diff, y=d1, mode="lines",
|
| 1367 |
+
name="Low y d/dβ", line=dict(color="orange", dash='dash')))
|
| 1368 |
+
fig_diff.add_trace(go.Scatter(x=betas_diff, y=d2, mode="lines",
|
| 1369 |
+
name="Low y d²/dβ²", line=dict(color="orange", dash='dot')))
|
| 1370 |
+
|
| 1371 |
+
fig_diff.update_layout(
|
| 1372 |
+
title="Differential Analysis vs. β" +
|
| 1373 |
+
(" (Eigenvalue Method)" if use_eigenvalue_method_diff else " (Discriminant Method)"),
|
| 1374 |
+
xaxis_title="β",
|
| 1375 |
+
yaxis_title="Value",
|
| 1376 |
+
hovermode="x unified",
|
| 1377 |
+
showlegend=True,
|
| 1378 |
+
legend=dict(
|
| 1379 |
+
yanchor="top",
|
| 1380 |
+
y=0.99,
|
| 1381 |
+
xanchor="left",
|
| 1382 |
+
x=0.01
|
| 1383 |
+
)
|
| 1384 |
+
)
|
| 1385 |
+
st.plotly_chart(fig_diff, use_container_width=True)
|
| 1386 |
+
|
| 1387 |
+
with st.expander("Curve Types", expanded=False):
|
| 1388 |
+
st.markdown("""
|
| 1389 |
+
- Solid lines: Original curves
|
| 1390 |
+
- Dashed lines: First derivatives (d/dβ)
|
| 1391 |
+
- Dotted lines: Second derivatives (d²/dβ²)
|
| 1392 |
+
""")
|