import streamlit as st
import sympy as sp
import numpy as np
import plotly.graph_objects as go
from scipy.optimize import fsolve
from scipy.stats import gaussian_kde
import os
import tempfile
import subprocess
import sys
import importlib.util
import time
from datetime import timedelta

# Configure Streamlit for Hugging Face Spaces
st.set_page_config(
    page_title="Cubic Root Analysis (C++ Accelerated)",
    layout="wide",
    initial_sidebar_state="collapsed"
)

# Create a class for advanced progress tracking
class AdvancedProgressBar:
    def __init__(self, total_steps, description="Processing", auto_refresh=True):
        self.total_steps = total_steps
        self.current_step = 0
        self.start_time = time.time()
        self.description = description
        self.auto_refresh = auto_refresh
        
        # Create UI elements
        self.status_container = st.empty()
        self.progress_bar = st.progress(0)
        self.metrics_cols = st.columns(4)
        self.step_metric = self.metrics_cols[0].empty()
        self.percent_metric = self.metrics_cols[1].empty()
        self.elapsed_metric = self.metrics_cols[2].empty()
        self.eta_metric = self.metrics_cols[3].empty()
        
        # Initialize with starting values
        self.update_status(f"Starting {self.description}...")
        self.update(0)
    
    def update(self, step=None, description=None):
        if step is not None:
            self.current_step = step
        else:
            self.current_step += 1
            
        if description:
            self.description = description
            
        # Calculate progress percentage
        progress = min(self.current_step / self.total_steps, 1.0)
        
        # Update progress bar
        self.progress_bar.progress(progress)
        
        # Update metrics
        elapsed = time.time() - self.start_time
        elapsed_str = str(timedelta(seconds=int(elapsed)))
        
        if progress > 0:
            eta = elapsed * (1 - progress) / progress
            eta_str = str(timedelta(seconds=int(eta)))
        else:
            eta_str = "Calculating..."
            
        step_text = f"{self.current_step}/{self.total_steps}"
        percent_text = f"{progress*100:.1f}%"
        
        self.step_metric.metric("Steps", step_text)
        self.percent_metric.metric("Progress", percent_text)
        self.elapsed_metric.metric("Elapsed", elapsed_str)
        self.eta_metric.metric("ETA", eta_str)
        
        # Update status text
        self.update_status(f"{self.description} - Step {self.current_step} of {self.total_steps}")
    
    def update_status(self, text):
        self.status_container.text(text)
    
    def complete(self, success=True):
        if success:
            self.progress_bar.progress(1.0)
            self.update_status(f"✅ {self.description} completed successfully!")
        else:
            self.update_status(f"❌ {self.description} failed or was interrupted.")
        
        elapsed = time.time() - self.start_time
        elapsed_str = str(timedelta(seconds=int(elapsed)))
        self.elapsed_metric.metric("Total Time", elapsed_str)
        self.eta_metric.metric("ETA", "Completed")
        
        # Add small delay to show completion
        time.sleep(0.5)
    
    def clear(self):
        self.status_container.empty()
        self.progress_bar.empty()
        self.step_metric.empty()
        self.percent_metric.empty()
        self.elapsed_metric.empty()
        self.eta_metric.empty()

# Initialize sympy precision settings for higher accuracy
# With these lines:
import mpmath
mpmath.mp.dps = 50  # Set decimal precision to 50 digits

# Check if C++ module is already compiled, otherwise compile it
cpp_compiled = False

def compile_cpp_module():
    progress = AdvancedProgressBar(5, "Compiling C++ module")
    
    # Define C++ code as a string
    cpp_code = """
    #include <pybind11/pybind11.h>
    #include <pybind11/numpy.h>
    #include <pybind11/stl.h>
    #include <Eigen/Dense>
    #include <Eigen/Eigenvalues>
    #include <complex>
    #include <vector>
    #include <random>
    #include <cmath>
    #include <algorithm>
    #include <omp.h>

    namespace py = pybind11;
    using namespace Eigen;

    // Fast discriminant computation function
    double compute_discriminant_fast(double z, double beta, double z_a, double y) {
        double a = z * z_a;
        double b = z * z_a + z + z_a - z_a*y;
        double c = z + z_a + 1 - y*(beta*z_a + 1 - beta);
        double d = 1.0;
        
        // Standard formula for cubic discriminant
        return 18*a*b*c*d - 27*a*a*d*d + b*b*c*c - 2*b*b*b*d - 9*a*c*c*c;
    }

    // Batch computation of discriminant for array of z values
    py::array_t<double> discriminant_array(double beta, double z_a, double y, py::array_t<double> z_values) {
        auto z_buf = z_values.request();
        auto result = py::array_t<double>(z_buf.size);
        auto result_buf = result.request();
        
        double* z_ptr = static_cast<double*>(z_buf.ptr);
        double* result_ptr = static_cast<double*>(result_buf.ptr);
        
        #pragma omp parallel for
        for (size_t i = 0; i < z_buf.size; i++) {
            result_ptr[i] = compute_discriminant_fast(z_ptr[i], beta, z_a, y);
        }
        
        return result;
    }

    // Find zeros of discriminant function
    std::tuple<py::array_t<double>, py::array_t<double>, py::array_t<double>> 
    find_discriminant_zeros(double z_a, double y, double z_min, double z_max, int beta_steps, int z_steps) {
        // Create beta grid
        auto betas = py::array_t<double>(beta_steps);
        auto betas_buf = betas.request();
        double* betas_ptr = static_cast<double*>(betas_buf.ptr);
        
        for (int i = 0; i < beta_steps; i++) {
            betas_ptr[i] = static_cast<double>(i) / (beta_steps - 1);
        }
        
        // Arrays for results
        auto z_mins = py::array_t<double>(beta_steps);
        auto z_maxs = py::array_t<double>(beta_steps);
        auto z_mins_buf = z_mins.request();
        auto z_maxs_buf = z_maxs.request();
        double* z_mins_ptr = static_cast<double*>(z_mins_buf.ptr);
        double* z_maxs_ptr = static_cast<double*>(z_maxs_buf.ptr);
        
        // Apply condition for y
        double y_effective = y > 1.0 ? y : 1.0/y;
        
        // Create z grid
        std::vector<double> z_grid(z_steps);
        for (int i = 0; i < z_steps; i++) {
            z_grid[i] = z_min + (z_max - z_min) * static_cast<double>(i) / (z_steps - 1);
        }
        
        // For each beta value, find min and max z where discriminant is zero
        #pragma omp parallel for
        for (int b_idx = 0; b_idx < beta_steps; b_idx++) {
            double beta = betas_ptr[b_idx];
            std::vector<double> roots_found;
            
            // Calculate discriminant for all z values
            std::vector<double> disc_vals(z_steps);
            for (int i = 0; i < z_steps; i++) {
                disc_vals[i] = compute_discriminant_fast(z_grid[i], beta, z_a, y_effective);
            }
            
            // Find sign changes (zeros of discriminant)
            for (int i = 0; i < z_steps - 1; i++) {
                double f1 = disc_vals[i];
                double f2 = disc_vals[i+1];
                
                if (std::isnan(f1) || std::isnan(f2)) {
                    continue;
                }
                
                if (f1 == 0.0) {
                    roots_found.push_back(z_grid[i]);
                } else if (f2 == 0.0) {
                    roots_found.push_back(z_grid[i+1]);
                } else if (f1 * f2 < 0) {
                    // Binary search for more accurate root
                    double zl = z_grid[i], zr = z_grid[i+1];
                    for (int j = 0; j < 50; j++) {
                        double mid = 0.5 * (zl + zr);
                        double fm = compute_discriminant_fast(mid, beta, z_a, y_effective);
                        
                        if (fm == 0) {
                            zl = zr = mid;
                            break;
                        }
                        
                        if ((fm > 0 && f1 > 0) || (fm < 0 && f1 < 0)) {
                            zl = mid;
                            f1 = fm;
                        } else {
                            zr = mid;
                            f2 = fm;
                        }
                    }
                    roots_found.push_back(0.5 * (zl + zr));
                }
            }
            
            // Store min and max roots if any found
            if (roots_found.empty()) {
                z_mins_ptr[b_idx] = std::numeric_limits<double>::quiet_NaN();
                z_maxs_ptr[b_idx] = std::numeric_limits<double>::quiet_NaN();
            } else {
                double min_root = *std::min_element(roots_found.begin(), roots_found.end());
                double max_root = *std::max_element(roots_found.begin(), roots_found.end());
                
                z_mins_ptr[b_idx] = min_root;
                z_maxs_ptr[b_idx] = max_root;
            }
        }
        
        return std::make_tuple(betas, z_mins, z_maxs);
    }

    // Compute eigenvalue support boundaries
    std::tuple<py::array_t<double>, py::array_t<double>> 
    compute_eigenvalue_boundaries(double z_a, double y, py::array_t<double> beta_values, int n_samples, int seeds) {
        auto beta_buf = beta_values.request();
        int beta_steps = beta_buf.size;
        
        // Results arrays
        auto min_eigenvalues = py::array_t<double>(beta_steps);
        auto max_eigenvalues = py::array_t<double>(beta_steps);
        auto min_buf = min_eigenvalues.request();
        auto max_buf = max_eigenvalues.request();
        double* min_ptr = static_cast<double*>(min_buf.ptr);
        double* max_ptr = static_cast<double*>(max_buf.ptr);
        double* beta_ptr = static_cast<double*>(beta_buf.ptr);
        
        // Apply condition for y
        double y_effective = y > 1.0 ? y : 1.0/y;
        
        // Compute eigenvalues for each beta value
        #pragma omp parallel for
        for (int i = 0; i < beta_steps; i++) {
            double beta = beta_ptr[i];
            
            std::vector<double> min_vals;
            std::vector<double> max_vals;
            
            // Run multiple trials with different seeds
            for (int seed = 0; seed < seeds; seed++) {
                // Set random seed
                std::mt19937 gen(seed * 100 + i);
                std::normal_distribution<double> normal_dist(0.0, 1.0);
                
                // Compute dimension p based on aspect ratio y
                int p = static_cast<int>(y_effective * n_samples);
                
                // Constructing T_n (Population / Shape Matrix)
                int k = static_cast<int>(std::floor(beta * p));
                
                // Create diagonal entries
                std::vector<double> diag_entries(p);
                std::fill_n(diag_entries.begin(), k, z_a);
                std::fill_n(diag_entries.begin() + k, p - k, 1.0);
                
                // Shuffle the diagonal entries
                std::shuffle(diag_entries.begin(), diag_entries.end(), gen);
                
                // Create T_n matrix
                MatrixXd T_n = MatrixXd::Zero(p, p);
                for (int j = 0; j < p; j++) {
                    T_n(j, j) = diag_entries[j];
                }
                
                // Generate random data matrix X with standard normal entries
                MatrixXd X(p, n_samples);
                for (int r = 0; r < p; r++) {
                    for (int c = 0; c < n_samples; c++) {
                        X(r, c) = normal_dist(gen);
                    }
                }
                
                // Compute sample covariance matrix S_n = (1/n) * XX^T
                MatrixXd S_n = (1.0 / n_samples) * (X * X.transpose());
                
                // Compute B_n = S_n T_n
                MatrixXd B_n = S_n * T_n;
                
                // Compute eigenvalues
                SelfAdjointEigenSolver<MatrixXd> solver(B_n);
                VectorXd eigenvalues = solver.eigenvalues();
                
                // Store min and max eigenvalues
                min_vals.push_back(eigenvalues.minCoeff());
                max_vals.push_back(eigenvalues.maxCoeff());
            }
            
            // Compute averages
            double min_avg = 0.0, max_avg = 0.0;
            for (double val : min_vals) min_avg += val;
            for (double val : max_vals) max_avg += val;
            
            min_ptr[i] = min_avg / seeds;
            max_ptr[i] = max_avg / seeds;
        }
        
        return std::make_tuple(min_eigenvalues, max_eigenvalues);
    }

    // Compute cubic roots using fast C++ implementation
    py::array_t<std::complex<double>> compute_cubic_roots_cpp(double z, double beta, double z_a, double y) {
        // Apply the condition for y
        double y_effective = y > 1.0 ? y : 1.0/y;
        
        // Coefficients in the form as³ + bs² + cs + d = 0
        double a = z * z_a;
        double b = z * z_a + z + z_a - z_a*y_effective;
        double c = z + z_a + 1 - y_effective*(beta*z_a + 1 - beta);
        double d = 1.0;
        
        // Handle special cases
        if (std::abs(a) < 1e-10) {
            // Create result array
            auto result = py::array_t<std::complex<double>>(3);
            auto buf = result.request();
            std::complex<double>* ptr = static_cast<std::complex<double>*>(buf.ptr);
            
            if (std::abs(b) < 1e-10) {  // Linear case
                ptr[0] = std::complex<double>(-d/c, 0.0);
                ptr[1] = std::complex<double>(0.0, 0.0);
                ptr[2] = std::complex<double>(0.0, 0.0);
            } else {  // Quadratic case
                double discriminant = c*c - 4*b*d;
                if (discriminant >= 0) {
                    double sqrt_disc = std::sqrt(discriminant);
                    ptr[0] = std::complex<double>((-c + sqrt_disc) / (2*b), 0.0);
                    ptr[1] = std::complex<double>((-c - sqrt_disc) / (2*b), 0.0);
                } else {
                    double sqrt_disc = std::sqrt(-discriminant);
                    ptr[0] = std::complex<double>(-c/(2*b), sqrt_disc/(2*b));
                    ptr[1] = std::complex<double>(-c/(2*b), -sqrt_disc/(2*b));
                }
                ptr[2] = std::complex<double>(0.0, 0.0);
            }
            return result;
        }
        
        // For better numerical stability, normalize the equation: x³ + px² + qx + r = 0
        double p = b / a;
        double q = c / a;
        double r = d / a;
        
        // Depressed cubic: t³ + pt + q = 0 where x = t - p/3
        double p_prime = q - p*p/3.0;
        double q_prime = r - p*q/3.0 + 2.0*p*p*p/27.0;
        
        // Compute discriminant
        double discriminant = 4.0*p_prime*p_prime*p_prime/27.0 + q_prime*q_prime;
        
        // Create result array
        auto result = py::array_t<std::complex<double>>(3);
        auto buf = result.request();
        std::complex<double>* ptr = static_cast<std::complex<double>*>(buf.ptr);
        
        // Calculate roots based on discriminant
        if (std::abs(discriminant) < 1e-10) {  // Discriminant ≈ 0
            if (std::abs(q_prime) < 1e-10) {  // Triple root
                ptr[0] = ptr[1] = ptr[2] = std::complex<double>(-p/3.0, 0.0);
            } else {  // One simple, one double root
                double u = std::cbrt(-q_prime/2.0);
                ptr[0] = std::complex<double>(2*u - p/3.0, 0.0);
                ptr[1] = ptr[2] = std::complex<double>(-u - p/3.0, 0.0);
            }
        } else if (discriminant > 0) {  // One real, two complex conjugate roots
            double sqrt_disc = std::sqrt(discriminant);
            std::complex<double> u = std::pow(std::complex<double>(-q_prime/2.0 + sqrt_disc/2.0, 0.0), 1.0/3.0);
            std::complex<double> v = std::pow(std::complex<double>(-q_prime/2.0 - sqrt_disc/2.0, 0.0), 1.0/3.0);
            
            ptr[0] = std::complex<double>(std::real(u + v) - p/3.0, 0.0);
            
            std::complex<double> omega(-0.5, 0.866025403784439);  // -1/2 + i*√3/2
            std::complex<double> omega2(-0.5, -0.866025403784439); // -1/2 - i*√3/2
            
            ptr[1] = omega * u + omega2 * v - std::complex<double>(p/3.0, 0.0);
            ptr[2] = omega2 * u + omega * v - std::complex<double>(p/3.0, 0.0);
        } else {  // Three distinct real roots
            double sqrt_disc = std::sqrt(-discriminant);
            double theta = std::atan2(sqrt_disc, -2.0*q_prime);
            double r_prime = std::pow(q_prime*q_prime + discriminant/4.0, 1.0/6.0);
            
            ptr[0] = std::complex<double>(2.0*r_prime*std::cos(theta/3.0) - p/3.0, 0.0);
            ptr[1] = std::complex<double>(2.0*r_prime*std::cos((theta + 2.0*M_PI)/3.0) - p/3.0, 0.0);
            ptr[2] = std::complex<double>(2.0*r_prime*std::cos((theta + 4.0*M_PI)/3.0) - p/3.0, 0.0);
        }
        
        return result;
    }

    // Compute high y curve
    py::array_t<double> compute_high_y_curve(py::array_t<double> betas, double z_a, double y) {
        auto beta_buf = betas.request();
        auto result = py::array_t<double>(beta_buf.size);
        auto result_buf = result.request();
        
        double* beta_ptr = static_cast<double*>(beta_buf.ptr);
        double* result_ptr = static_cast<double*>(result_buf.ptr);
        
        // Apply the condition for y
        double y_effective = y > 1.0 ? y : 1.0/y;
        
        double a = z_a;
        double denominator = 1.0 - 2.0*a;
        
        #pragma omp parallel for
        for (size_t i = 0; i < beta_buf.size; i++) {
            if (std::abs(denominator) < 1e-10) {
                result_ptr[i] = std::numeric_limits<double>::quiet_NaN();
                continue;
            }
            
            double beta = beta_ptr[i];
            double numerator = -4.0*a*(a-1.0)*y_effective*beta - 2.0*a*y_effective - 2.0*a*(2.0*a-1.0);
            result_ptr[i] = numerator/denominator;
        }
        
        return result;
    }

    // Compute alternate low expression
    py::array_t<double> compute_alternate_low_expr(py::array_t<double> betas, double z_a, double y) {
        auto beta_buf = betas.request();
        auto result = py::array_t<double>(beta_buf.size);
        auto result_buf = result.request();
        
        double* beta_ptr = static_cast<double*>(beta_buf.ptr);
        double* result_ptr = static_cast<double*>(result_buf.ptr);
        
        // Apply the condition for y
        double y_effective = y > 1.0 ? y : 1.0/y;
        
        #pragma omp parallel for
        for (size_t i = 0; i < beta_buf.size; i++) {
            double beta = beta_ptr[i];
            result_ptr[i] = (z_a * y_effective * beta * (z_a - 1.0) - 2.0*z_a*(1.0 - y_effective) - 2.0*z_a*z_a) / (2.0 + 2.0*z_a);
        }
        
        return result;
    }

    // Compute max k expression
    py::array_t<double> compute_max_k_expression(py::array_t<double> betas, double z_a, double y, int k_samples=1000) {
        auto beta_buf = betas.request();
        auto result = py::array_t<double>(beta_buf.size);
        auto result_buf = result.request();
        
        double* beta_ptr = static_cast<double*>(beta_buf.ptr);
        double* result_ptr = static_cast<double*>(result_buf.ptr);
        
        // Apply the condition for y
        double y_effective = y > 1.0 ? y : 1.0/y;
        
        double a = z_a;
        // Sample k values on a logarithmic scale
        std::vector<double> k_values(k_samples);
        for (int j = 0; j < k_samples; j++) {
            k_values[j] = std::pow(10.0, -3.0 + 6.0 * static_cast<double>(j) / (k_samples - 1));
        }
        
        #pragma omp parallel for
        for (size_t i = 0; i < beta_buf.size; i++) {
            double beta = beta_ptr[i];
            std::vector<double> values(k_samples);
            
            // Compute expression value for each k
            for (int j = 0; j < k_samples; j++) {
                double k = k_values[j];
                double numerator = y_effective*beta*(a-1.0)*k + (a*k+1.0)*((y_effective-1.0)*k-1.0);
                double denominator = (a*k+1.0)*(k*k+k);
                
                if (std::abs(denominator) < 1e-10) {
                    values[j] = std::numeric_limits<double>::quiet_NaN();
                } else {
                    values[j] = numerator/denominator;
                }
            }
            
            // Find maximum value (excluding NaNs)
            double max_val = -std::numeric_limits<double>::infinity();
            bool has_valid = false;
            
            for (double val : values) {
                if (!std::isnan(val)) {
                    max_val = std::max(max_val, val);
                    has_valid = true;
                }
            }
            
            result_ptr[i] = has_valid ? max_val : std::numeric_limits<double>::quiet_NaN();
        }
        
        return result;
    }

    // Compute min t expression
    py::array_t<double> compute_min_t_expression(py::array_t<double> betas, double z_a, double y, int t_samples=1000) {
        auto beta_buf = betas.request();
        auto result = py::array_t<double>(beta_buf.size);
        auto result_buf = result.request();
        
        double* beta_ptr = static_cast<double*>(beta_buf.ptr);
        double* result_ptr = static_cast<double*>(result_buf.ptr);
        
        // Apply the condition for y
        double y_effective = y > 1.0 ? y : 1.0/y;
        
        double a = z_a;
        if (a <= 0) {
            for (size_t i = 0; i < beta_buf.size; i++) {
                result_ptr[i] = std::numeric_limits<double>::quiet_NaN();
            }
            return result;
        }
        
        double lower_bound = -1.0/a + 1e-10;  // Avoid division by zero
        
        #pragma omp parallel for
        for (size_t i = 0; i < beta_buf.size; i++) {
            double beta = beta_ptr[i];
            
            // Sample t values
            std::vector<double> t_values(t_samples);
            for (int j = 0; j < t_samples; j++) {
                t_values[j] = lower_bound + (-1e-10 - lower_bound) * static_cast<double>(j) / (t_samples - 1);
            }
            
            std::vector<double> values(t_samples);
            
            // Compute expression value for each t
            for (int j = 0; j < t_samples; j++) {
                double t = t_values[j];
                double numerator = y_effective*beta*(a-1.0)*t + (a*t+1.0)*((y_effective-1.0)*t-1.0);
                double denominator = (a*t+1.0)*(t*t+t);
                
                if (std::abs(denominator) < 1e-10) {
                    values[j] = std::numeric_limits<double>::quiet_NaN();
                } else {
                    values[j] = numerator/denominator;
                }
            }
            
            // Find minimum value (excluding NaNs)
            double min_val = std::numeric_limits<double>::infinity();
            bool has_valid = false;
            
            for (double val : values) {
                if (!std::isnan(val)) {
                    min_val = std::min(min_val, val);
                    has_valid = true;
                }
            }
            
            result_ptr[i] = has_valid ? min_val : std::numeric_limits<double>::quiet_NaN();
        }
        
        return result;
    }

    // Generate eigenvalue distribution
    std::tuple<py::array_t<double>, py::array_t<double>> 
    generate_eigenvalue_distribution_cpp(double beta, double y, double z_a, int n, int seed) {
        // Apply the condition for y
        double y_effective = y > 1.0 ? y : 1.0/y;
        
        // Set random seed
        std::mt19937 gen(seed);
        std::normal_distribution<double> normal_dist(0.0, 1.0);
        
        // Compute dimension p based on aspect ratio y
        int p = static_cast<int>(y_effective * n);
        
        // Constructing T_n (Population / Shape Matrix)
        int k = static_cast<int>(std::floor(beta * p));
        
        // Create diagonal entries
        std::vector<double> diag_entries(p);
        std::fill_n(diag_entries.begin(), k, z_a);
        std::fill_n(diag_entries.begin() + k, p - k, 1.0);
        
        // Shuffle the diagonal entries
        std::shuffle(diag_entries.begin(), diag_entries.end(), gen);
        
        // Create T_n matrix
        MatrixXd T_n = MatrixXd::Zero(p, p);
        for (int i = 0; i < p; i++) {
            T_n(i, i) = diag_entries[i];
        }
        
        // Generate random data matrix X with standard normal entries
        MatrixXd X(p, n);
        for (int r = 0; r < p; r++) {
            for (int c = 0; c < n; c++) {
                X(r, c) = normal_dist(gen);
            }
        }
        
        // Compute sample covariance matrix S_n = (1/n) * XX^T
        MatrixXd S_n = (1.0 / n) * (X * X.transpose());
        
        // Compute B_n = S_n T_n
        MatrixXd B_n = S_n * T_n;
        
        // Compute eigenvalues
        SelfAdjointEigenSolver<MatrixXd> solver(B_n);
        VectorXd eigenvalues = solver.eigenvalues();
        
        // Return eigenvalues as numpy array
        auto result = py::array_t<double>(p);
        auto result_buf = result.request();
        double* result_ptr = static_cast<double*>(result_buf.ptr);
        
        for (int i = 0; i < p; i++) {
            result_ptr[i] = eigenvalues(i);
        }
        
        // Create x grid for KDE estimation (done in Python)
        auto x_grid = py::array_t<double>(500);
        auto x_grid_buf = x_grid.request();
        double* x_grid_ptr = static_cast<double*>(x_grid_buf.ptr);
        
        double min_eig = eigenvalues.minCoeff();
        double max_eig = eigenvalues.maxCoeff();
        
        for (int i = 0; i < 500; i++) {
            x_grid_ptr[i] = min_eig + (max_eig - min_eig) * static_cast<double>(i) / 499.0;
        }
        
        return std::make_tuple(result, x_grid);
    }

    // Generate phase diagram
    py::array_t<int> generate_phase_diagram_cpp(
        double z_a, double y, double beta_min, double beta_max, 
        double z_min, double z_max, int beta_steps, int z_steps) {
        
        // Apply the condition for y
        double y_effective = y > 1.0 ? y : 1.0/y;
        
        // Create result array
        auto result = py::array_t<int>({z_steps, beta_steps});
        auto result_buf = result.request();
        int* result_ptr = static_cast<int*>(result_buf.ptr);
        
        // Create beta and z grids
        std::vector<double> beta_values(beta_steps);
        std::vector<double> z_values(z_steps);
        
        for (int i = 0; i < beta_steps; i++) {
            beta_values[i] = beta_min + (beta_max - beta_min) * static_cast<double>(i) / (beta_steps - 1);
        }
        
        for (int i = 0; i < z_steps; i++) {
            z_values[i] = z_min + (z_max - z_min) * static_cast<double>(i) / (z_steps - 1);
        }
        
        // Analyze roots for each (z, beta) point
        #pragma omp parallel for collapse(2)
        for (int i = 0; i < z_steps; i++) {
            for (int j = 0; j < beta_steps; j++) {
                double z = z_values[i];
                double beta = beta_values[j];
                
                // Coefficients for cubic equation
                double a = z * z_a;
                double b = z * z_a + z + z_a - z_a*y_effective;
                double c = z + z_a + 1 - y_effective*(beta*z_a + 1 - beta);
                double d = 1.0;
                
                // Calculate discriminant
                double discriminant = 18*a*b*c*d - 27*a*a*d*d + b*b*c*c - 2*b*b*b*d - 9*a*c*c*c;
                
                // Set result based on sign of discriminant
                // 1 for all real roots (discriminant > 0), -1 for complex roots (discriminant < 0)
                result_ptr[i * beta_steps + j] = (discriminant > 0) ? 1 : -1;
            }
        }
        
        return result;
    }

    PYBIND11_MODULE(cubic_cpp, m) {
        m.doc() = "C++ accelerated cubic root analysis";
        
        // Expose all the C++ functions to Python
        m.def("discriminant_array", &discriminant_array, "Compute cubic discriminant for array of z values");
        m.def("find_discriminant_zeros", &find_discriminant_zeros, "Find zeros of the discriminant function");
        m.def("compute_eigenvalue_boundaries", &compute_eigenvalue_boundaries, "Compute eigenvalue boundaries");
        m.def("compute_cubic_roots_cpp", &compute_cubic_roots_cpp, "Compute cubic roots");
        m.def("compute_high_y_curve", &compute_high_y_curve, "Compute high y curve");
        m.def("compute_alternate_low_expr", &compute_alternate_low_expr, "Compute alternate low expression");
        m.def("compute_max_k_expression", &compute_max_k_expression, "Compute max k expression");
        m.def("compute_min_t_expression", &compute_min_t_expression, "Compute min t expression");
        m.def("generate_eigenvalue_distribution_cpp", &generate_eigenvalue_distribution_cpp, "Generate eigenvalue distribution");
        m.def("generate_phase_diagram_cpp", &generate_phase_diagram_cpp, "Generate phase diagram");
    }
    """
    
    progress.update(1, "Creating temporary directory for compilation")
    
    # Create a temporary directory to compile the C++ code
    with tempfile.TemporaryDirectory() as tmpdirname:
        # Write C++ code to file
        progress.update(2, "Writing C++ code to temporary file")
        with open(os.path.join(tmpdirname, "cubic_cpp.cpp"), "w") as f:
            f.write(cpp_code)
        
        # Write setup.py for compiling with pybind11
        progress.update(3, "Creating setup.py file")
        setup_py = """
from setuptools import setup, Extension
from pybind11.setup_helpers import Pybind11Extension, build_ext

ext_modules = [
    Pybind11Extension(
        "cubic_cpp",
        ["cubic_cpp.cpp"],
        include_dirs=["/usr/include/eigen3"],
        extra_compile_args=["-fopenmp", "-O3", "-march=native", "-ffast-math"],
        extra_link_args=["-fopenmp"],
        cxx_std=17,
    ),
]

setup(
    name="cubic_cpp",
    ext_modules=ext_modules,
    cmdclass={"build_ext": build_ext},
)
        """
        
        with open(os.path.join(tmpdirname, "setup.py"), "w") as f:
            f.write(setup_py)
        
        # Compile the module
        progress.update(4, "Running compilation process")
        try:
            result = subprocess.run(
                [sys.executable, "setup.py", "build_ext", "--inplace"],
                cwd=tmpdirname,
                capture_output=True,
                text=True,
                check=True
            )
            
            # Get the compiled module path
            module_path = None
            for file in os.listdir(tmpdirname):
                if file.startswith("cubic_cpp") and file.endswith(".so"):
                    module_path = os.path.join(tmpdirname, file)
                    break
            
            if not module_path:
                progress.complete(False)
                st.error("Failed to find compiled module.")
                st.code(result.stdout)
                st.code(result.stderr)
                return False
            
            # Import the module
            progress.update(5, "Importing compiled module")
            spec = importlib.util.spec_from_file_location("cubic_cpp", module_path)
            cubic_cpp = importlib.util.module_from_spec(spec)
            spec.loader.exec_module(cubic_cpp)
            
            # Make functions available globally
            globals()["discriminant_array"] = cubic_cpp.discriminant_array
            globals()["find_discriminant_zeros"] = cubic_cpp.find_discriminant_zeros
            globals()["compute_eigenvalue_boundaries"] = cubic_cpp.compute_eigenvalue_boundaries
            globals()["compute_cubic_roots_cpp"] = cubic_cpp.compute_cubic_roots_cpp
            globals()["compute_high_y_curve"] = cubic_cpp.compute_high_y_curve
            globals()["compute_alternate_low_expr"] = cubic_cpp.compute_alternate_low_expr
            globals()["compute_max_k_expression"] = cubic_cpp.compute_max_k_expression
            globals()["compute_min_t_expression"] = cubic_cpp.compute_min_t_expression
            globals()["generate_eigenvalue_distribution_cpp"] = cubic_cpp.generate_eigenvalue_distribution_cpp
            globals()["generate_phase_diagram_cpp"] = cubic_cpp.generate_phase_diagram_cpp
            
            progress.complete(True)
            return True
            
        except subprocess.CalledProcessError as e:
            progress.complete(False)
            st.error(f"Compilation failed: {e}")
            st.code(e.stdout)
            st.code(e.stderr)
            return False

# Try to compile the C++ module
cpp_compiled = compile_cpp_module()

# Python fallback functions if C++ compilation failed
def add_sqrt_support(expr_str):
    """Replace 'sqrt(' with 'sp.sqrt(' for sympy compatibility"""
    return expr_str.replace('sqrt(', 'sp.sqrt(')

@st.cache_data
def find_z_at_discriminant_zero(z_a, y, beta, z_min, z_max, steps):
    """
    Scan z in [z_min, z_max] for sign changes in the discriminant,
    and return approximated roots (where the discriminant is zero).
    """
    # Create progress bar
    progress = AdvancedProgressBar(steps, "Finding discriminant zeros")
    
    # Apply the condition for y
    y_effective = y if y > 1 else 1/y
    
    # Symbolic variables for the cubic discriminant with higher precision
    z_sym, beta_sym, z_a_sym, y_sym = sp.symbols("z beta z_a y", real=True, positive=True)
    
    # Define coefficients a, b, c, d in terms of z_sym, beta_sym, z_a_sym, y_sym
    a_sym = z_sym * z_a_sym
    b_sym = z_sym * z_a_sym + z_sym + z_a_sym - z_a_sym*y_sym
    c_sym = z_sym + z_a_sym + 1 - y_sym*(beta_sym*z_a_sym + 1 - beta_sym)
    d_sym = 1
    
    # Symbolic expression for the cubic discriminant using standard form
    Delta_expr = 18*a_sym*b_sym*c_sym*d_sym - 27*a_sym**2*d_sym**2 + b_sym**2*c_sym**2 - 2*b_sym**3*d_sym - 9*a_sym*c_sym**3
    
    # Fast numeric function for the discriminant
    discriminant_func = sp.lambdify((z_sym, beta_sym, z_a_sym, y_sym), Delta_expr, "mpmath")
    
    z_grid = np.linspace(z_min, z_max, steps)
    disc_vals = []
    
    # Calculate discriminant values with progress tracking
    for i, z in enumerate(z_grid):
        progress.update(i+1, f"Computing discriminant at z = {z:.4f}")
        disc_vals.append(float(discriminant_func(z, beta, z_a, y_effective)))
    
    disc_vals = np.array(disc_vals)
    roots_found = []
    
    # Find sign changes with high-precision refinement
    progress.update_status("Finding and refining discriminant zero locations")
    for i in range(len(z_grid) - 1):
        f1, f2 = disc_vals[i], disc_vals[i+1]
        if np.isnan(f1) or np.isnan(f2):
            continue
        if abs(f1) < 1e-12:
            roots_found.append(z_grid[i])
        elif abs(f2) < 1e-12:
            roots_found.append(z_grid[i+1])
        elif f1 * f2 < 0:
            # High-precision binary search for more accurate root
            zl, zr = z_grid[i], z_grid[i+1]
            f1 = discriminant_func(zl, beta, z_a, y_effective)
            f2 = discriminant_func(zr, beta, z_a, y_effective)
            
            for _ in range(50):
                mid = sp.Float(0.5) * (zl + zr)
                fm = discriminant_func(mid, beta, z_a, y_effective)
                if abs(fm) < 1e-15:
                    zl = zr = mid
                    break
                if fm * f1 > 0:
                    zl, f1 = mid, fm
                else:
                    zr, f2 = mid, fm
            
            # Convert back to float for NumPy compatibility
            roots_found.append(float(0.5 * (zl + zr)))
    
    progress.complete()
    return np.array(roots_found)

@st.cache_data
def sweep_beta_and_find_z_bounds(z_a, y, z_min, z_max, beta_steps, z_steps):
    """
    Python fallback. For each beta in [0,1] (with beta_steps points), find the minimum and maximum z 
    for which the discriminant is zero.
    Returns: betas, lower z*(β) values, and upper z*(β) values.
    """
    if cpp_compiled:
        return find_discriminant_zeros(z_a, y, z_min, z_max, beta_steps, z_steps)
    
    # Create progress tracking
    progress = AdvancedProgressBar(beta_steps, "Computing discriminant zeros across β values")
    
    betas = np.linspace(0, 1, beta_steps)
    z_min_values = []
    z_max_values = []
    
    for i, b in enumerate(betas):
        progress.update(i+1, f"Processing β = {b:.4f}")
        roots = find_z_at_discriminant_zero(z_a, y, b, z_min, z_max, z_steps)
        if len(roots) == 0:
            z_min_values.append(np.nan)
            z_max_values.append(np.nan)
        else:
            z_min_values.append(np.min(roots))
            z_max_values.append(np.max(roots))
    
    progress.complete()
    return betas, np.array(z_min_values), np.array(z_max_values)

@st.cache_data
def compute_eigenvalue_support_boundaries(z_a, y, beta_values, n_samples=100, seeds=5):
    """
    Python fallback. Compute the support boundaries of the eigenvalue distribution by directly
    finding the minimum and maximum eigenvalues of B_n = S_n T_n for different beta values.
    """
    if cpp_compiled:
        return compute_eigenvalue_boundaries(z_a, y, beta_values, n_samples, seeds)
    
    # Create progress tracking
    progress = AdvancedProgressBar(len(beta_values), "Computing eigenvalue support boundaries")
    
    # Apply the condition for y
    y_effective = y if y > 1 else 1/y
    
    min_eigenvalues = np.zeros_like(beta_values)
    max_eigenvalues = np.zeros_like(beta_values)
    
    for i, beta in enumerate(beta_values):
        # Update progress
        progress.update(i+1, f"Processing β = {beta:.4f}")
            
        min_vals = []
        max_vals = []
        
        # Run multiple trials with different seeds for more stable results
        for seed in range(seeds):
            # Set random seed
            np.random.seed(seed * 100 + i)
            
            # Compute dimension p based on aspect ratio y
            n = n_samples
            p = int(y_effective * n)
            
            # Constructing T_n (Population / Shape Matrix)
            k = int(np.floor(beta * p))
            diag_entries = np.concatenate([
                np.full(k, z_a),
                np.full(p - k, 1.0)
            ])
            np.random.shuffle(diag_entries)
            T_n = np.diag(diag_entries)
            
            # Generate the data matrix X with i.i.d. standard normal entries
            X = np.random.randn(p, n)
            
            # Compute the sample covariance matrix S_n = (1/n) * XX^T
            S_n = (1 / n) * (X @ X.T)
            
            # Compute B_n = S_n T_n
            B_n = S_n @ T_n
            
            # Compute eigenvalues of B_n
            eigenvalues = np.linalg.eigvalsh(B_n)
            
            # Find minimum and maximum eigenvalues
            min_vals.append(np.min(eigenvalues))
            max_vals.append(np.max(eigenvalues))
        
        # Average over seeds for stability
        min_eigenvalues[i] = np.mean(min_vals)
        max_eigenvalues[i] = np.mean(max_vals)
    
    progress.complete()
    return min_eigenvalues, max_eigenvalues

@st.cache_data
def compute_high_y_curve(betas, z_a, y):
    """
    Compute the "High y Expression" curve with high precision.
    """
    if cpp_compiled:
        return compute_high_y_curve(betas, z_a, y)
    
    # Create progress tracking
    progress = AdvancedProgressBar(1, "Computing high y expression")
    
    # Apply the condition for y
    y_effective = y if y > 1 else 1/y
    
    # Use SymPy for higher precision
    beta_sym, z_a_sym, y_sym = sp.symbols("beta z_a y", positive=True)
    a = z_a_sym
    denominator = 1 - 2*a
    numerator = -4*a*(a-1)*y_sym*beta_sym - 2*a*y_sym - 2*a*(2*a-1)
    
    # Create the high precision expression
    expr = numerator / denominator
    
    # Convert to a high-precision numeric function
    func = sp.lambdify((beta_sym, z_a_sym, y_sym), expr, "mpmath")
    
    # Compute values with high precision
    result = np.zeros_like(betas)
    if abs(float(denominator.subs(z_a_sym, z_a))) < 1e-12:
        result.fill(np.nan)
    else:
        for i, beta in enumerate(betas):
            result[i] = float(func(beta, z_a, y_effective))
    
    progress.complete()
    return result

@st.cache_data
def compute_alternate_low_expr(betas, z_a, y):
    """
    Compute the alternate low expression with high precision.
    """
    if cpp_compiled:
        return compute_alternate_low_expr(betas, z_a, y)
    
    # Create progress tracking
    progress = AdvancedProgressBar(1, "Computing low y expression")
    
    # Apply the condition for y
    y_effective = y if y > 1 else 1/y
    
    # Use SymPy for higher precision
    beta_sym, z_a_sym, y_sym = sp.symbols("beta z_a y", positive=True)
    expr = (z_a_sym * y_sym * beta_sym * (z_a_sym - 1) - 
            2*z_a_sym*(1 - y_sym) - 2*z_a_sym**2) / (2 + 2*z_a_sym)
    
    # Convert to a high-precision numeric function
    func = sp.lambdify((beta_sym, z_a_sym, y_sym), expr, "mpmath")
    
    # Compute values with high precision
    result = np.zeros_like(betas)
    for i, beta in enumerate(betas):
        result[i] = float(func(beta, z_a, y_effective))
    
    progress.complete()
    return result

@st.cache_data
def compute_max_k_expression(betas, z_a, y, k_samples=1000):
    """
    Compute max_{k ∈ (0,∞)} (y*beta*(a-1)*k + (a*k+1)*((y-1)*k-1)) / ((a*k+1)*(k^2+k))
    with high precision.
    """
    if cpp_compiled:
        return compute_max_k_expression(betas, z_a, y, k_samples)
    
    # Create progress tracking
    progress = AdvancedProgressBar(len(betas), "Computing max k expression")
    
    # Apply the condition for y
    y_effective = y if y > 1 else 1/y
    
    # Use SymPy for symbolic expression
    k_sym, beta_sym, z_a_sym, y_sym = sp.symbols("k beta z_a y", positive=True)
    a = z_a_sym
    numerator = y_sym*beta_sym*(a-1)*k_sym + (a*k_sym+1)*((y_sym-1)*k_sym-1)
    denominator = (a*k_sym+1)*(k_sym**2+k_sym)
    expr = numerator / denominator
    
    # Convert to high-precision function
    func = sp.lambdify((k_sym, beta_sym, z_a_sym, y_sym), expr, "mpmath")
    
    # Sample k values on a logarithmic scale
    k_values = np.logspace(-3, 3, k_samples)
    
    max_vals = np.zeros_like(betas)
    for i, beta in enumerate(betas):
        progress.update(i+1, f"Processing β = {beta:.4f}")
        
        values = np.zeros_like(k_values)
        for j, k in enumerate(k_values):
            try:
                val = float(func(k, beta, z_a, y_effective))
                if np.isfinite(val):
                    values[j] = val
                else:
                    values[j] = np.nan
            except (ZeroDivisionError, OverflowError):
                values[j] = np.nan
        
        valid_indices = ~np.isnan(values)
        if np.any(valid_indices):
            max_vals[i] = np.max(values[valid_indices])
        else:
            max_vals[i] = np.nan
    
    progress.complete()
    return max_vals

@st.cache_data
def compute_min_t_expression(betas, z_a, y, t_samples=1000):
    """
    Compute min_{t ∈ (-1/a, 0)} (y*beta*(a-1)*t + (a*t+1)*((y-1)*t-1)) / ((a*t+1)*(t^2+t))
    with high precision.
    """
    if cpp_compiled:
        return compute_min_t_expression(betas, z_a, y, t_samples)
    
    # Create progress tracking
    progress = AdvancedProgressBar(len(betas), "Computing min t expression")
    
    # Apply the condition for y
    y_effective = y if y > 1 else 1/y
    
    # Use SymPy for symbolic expression
    t_sym, beta_sym, z_a_sym, y_sym = sp.symbols("t beta z_a y")
    a = z_a_sym
    numerator = y_sym*beta_sym*(a-1)*t_sym + (a*t_sym+1)*((y_sym-1)*t_sym-1)
    denominator = (a*t_sym+1)*(t_sym**2+t_sym)
    expr = numerator / denominator
    
    # Convert to high-precision function
    func = sp.lambdify((t_sym, beta_sym, z_a_sym, y_sym), expr, "mpmath")
    
    a = z_a
    if a <= 0:
        progress.complete(False)
        return np.full_like(betas, np.nan)
        
    lower_bound = -1/a + 1e-10  # Avoid division by zero
    t_values = np.linspace(lower_bound, -1e-10, t_samples)
    
    min_vals = np.zeros_like(betas)
    for i, beta in enumerate(betas):
        progress.update(i+1, f"Processing β = {beta:.4f}")
        
        values = np.zeros_like(t_values)
        for j, t in enumerate(t_values):
            try:
                val = float(func(t, beta, z_a, y_effective))
                if np.isfinite(val):
                    values[j] = val
                else:
                    values[j] = np.nan
            except (ZeroDivisionError, OverflowError):
                values[j] = np.nan
        
        valid_indices = ~np.isnan(values)
        if np.any(valid_indices):
            min_vals[i] = np.min(values[valid_indices])
        else:
            min_vals[i] = np.nan
    
    progress.complete()
    return min_vals

@st.cache_data
def compute_derivatives(curve, betas):
    """Compute first and second derivatives of a curve using SymPy for accuracy."""
    # Create a spline representation for smoother derivatives
    from scipy.interpolate import CubicSpline
    
    # Filter out NaN values
    valid_idx = ~np.isnan(curve)
    if not np.any(valid_idx):
        return np.full_like(betas, np.nan), np.full_like(betas, np.nan)
    
    valid_betas = betas[valid_idx]
    valid_curve = curve[valid_idx]
    
    if len(valid_betas) < 4:  # Need at least 4 points for cubic spline
        # Fall back to numpy gradient
        d1 = np.gradient(curve, betas)
        d2 = np.gradient(d1, betas)
        return d1, d2
    
    # Create cubic spline for smoother derivatives
    cs = CubicSpline(valid_betas, valid_curve)
    
    # Evaluate first and second derivatives
    d1 = np.zeros_like(betas)
    d2 = np.zeros_like(betas)
    
    for i, beta in enumerate(betas):
        if np.isnan(curve[i]):
            d1[i] = np.nan
            d2[i] = np.nan
        else:
            d1[i] = cs(beta, 1)  # First derivative
            d2[i] = cs(beta, 2)  # Second derivative
    
    return d1, d2

def compute_all_derivatives(betas, z_mins, z_maxs, low_y_curve, high_y_curve, alt_low_expr, custom_curve1=None, custom_curve2=None):
    """Compute derivatives for all curves"""
    progress = AdvancedProgressBar(7, "Computing derivatives")
    
    derivatives = {}
    
    # Upper z*(β)
    progress.update(1, "Computing upper z*(β) derivatives")
    derivatives['upper'] = compute_derivatives(z_maxs, betas)
    
    # Lower z*(β)
    progress.update(2, "Computing lower z*(β) derivatives")
    derivatives['lower'] = compute_derivatives(z_mins, betas)
    
    # Low y Expression (only if provided)
    if low_y_curve is not None:
        progress.update(3, "Computing low y expression derivatives")
        derivatives['low_y'] = compute_derivatives(low_y_curve, betas)
    else:
        progress.update(3, "Skipping low y expression (not provided)")
    
    # High y Expression
    if high_y_curve is not None:
        progress.update(4, "Computing high y expression derivatives")
        derivatives['high_y'] = compute_derivatives(high_y_curve, betas)
    else:
        progress.update(4, "Skipping high y expression (not provided)")
    
    # Alternate Low Expression
    if alt_low_expr is not None:
        progress.update(5, "Computing alternate low expression derivatives")
        derivatives['alt_low'] = compute_derivatives(alt_low_expr, betas)
    else:
        progress.update(5, "Skipping alternate low expression (not provided)")
    
    # Custom Expression 1 (if provided)
    if custom_curve1 is not None:
        progress.update(6, "Computing custom expression 1 derivatives")
        derivatives['custom1'] = compute_derivatives(custom_curve1, betas)
    else:
        progress.update(6, "Skipping custom expression 1 (not provided)")

    # Custom Expression 2 (if provided)
    if custom_curve2 is not None:
        progress.update(7, "Computing custom expression 2 derivatives")
        derivatives['custom2'] = compute_derivatives(custom_curve2, betas)
    else:
        progress.update(7, "Skipping custom expression 2 (not provided)")
    
    progress.complete()
    return derivatives

def compute_custom_expression(betas, z_a, y, s_num_expr, s_denom_expr, is_s_based=True):
    """
    Compute custom curve with high precision using SymPy.
    If is_s_based=True, compute using s substitution. Otherwise, compute direct z(β) expression.
    """
    progress = AdvancedProgressBar(4, "Computing custom expression")
    
    # Apply the condition for y
    y_effective = y if y > 1 else 1/y
    
    # Create SymPy symbols
    beta_sym, z_a_sym, y_sym = sp.symbols("beta z_a y", positive=True)
    local_dict = {"beta": beta_sym, "z_a": z_a_sym, "y": y_sym, "sp": sp}
    
    try:
        # Add sqrt support
        progress.update(1, "Parsing expression")
        s_num_expr = add_sqrt_support(s_num_expr)
        s_denom_expr = add_sqrt_support(s_denom_expr)
        
        num_expr = sp.sympify(s_num_expr, locals=local_dict)
        denom_expr = sp.sympify(s_denom_expr, locals=local_dict)
        
        if is_s_based:
            # Compute s and substitute into main expression
            progress.update(2, "Computing s-based expression")
            s_expr = num_expr / denom_expr
            a = z_a_sym
            numerator = y_sym*beta_sym*(z_a_sym-1)*s_expr + (a*s_expr+1)*((y_sym-1)*s_expr-1)
            denominator = (a*s_expr+1)*(s_expr**2 + s_expr)
            final_expr = numerator/denominator
        else:
            # Direct z(β) expression
            progress.update(2, "Computing direct z(β) expression")
            final_expr = num_expr / denom_expr
            
    except sp.SympifyError as e:
        progress.complete(False)
        st.error(f"Error parsing expressions: {e}")
        return np.full_like(betas, np.nan)
    
    progress.update(3, "Creating lambda function")
    
    # Convert to high-precision numeric function
    final_func = sp.lambdify((beta_sym, z_a_sym, y_sym), final_expr, modules=["mpmath"])
    
    progress.update(4, "Evaluating expression")
    
    # Compute values for each beta
    result = np.zeros_like(betas)
    
    for i, beta in enumerate(betas):
        try:
            # Calculate with high precision
            val = final_func(beta, z_a, y_effective)
            # Convert to float for compatibility
            result[i] = float(val)
        except Exception as e:
            result[i] = np.nan
    
    progress.complete()
    return result

def compute_cubic_roots(z, beta, z_a, y):
    """
    Compute the roots of the cubic equation for given parameters with high precision using SymPy.
    """
    if cpp_compiled:
        roots = compute_cubic_roots_cpp(z, beta, z_a, y)
        return roots
    
    # Apply the condition for y
    y_effective = y if y > 1 else 1/y
    
    # Create a symbolic variable for the equation
    s = sp.Symbol('s')
    
    # Coefficients in the form as^3 + bs^2 + cs + d = 0
    a = z * z_a
    b = z * z_a + z + z_a - z_a*y_effective
    c = z + z_a + 1 - y_effective*(beta*z_a + 1 - beta)
    d = 1
    
    # Handle special cases
    if abs(a) < 1e-12:
        if abs(b) < 1e-12:  # Linear case
            roots = np.array([-d/c, 0, 0], dtype=complex)
        else:  # Quadratic case
            # Use SymPy for higher precision
            quad_eq = b*s**2 + c*s + d
            symbolic_roots = sp.solve(quad_eq, s)
            numerical_roots = [complex(float(sp.N(root.evalf(50)).real), 
                               float(sp.N(root.evalf(50)).imag)) for root in symbolic_roots]
            roots = np.array(numerical_roots + [0], dtype=complex)
        return roots
    
    try:
        # Create the cubic equation with high precision
        cubic_eq = a*s**3 + b*s**2 + c*s + d
        
        # Solve using SymPy's solver with high precision
        symbolic_roots = sp.solve(cubic_eq, s)
        
        # Convert to high-precision complex numbers
        numerical_roots = []
        for root in symbolic_roots:
            # Use SymPy's N function with high precision (50 digits)
            high_prec_root = root.evalf(50)
            numerical_root = complex(float(sp.re(high_prec_root)), float(sp.im(high_prec_root)))
            numerical_roots.append(numerical_root)
        
        # If we got fewer than 3 roots (due to multiplicity), pad with zeros
        while len(numerical_roots) < 3:
            numerical_roots.append(0j)
            
        return np.array(numerical_roots, dtype=complex)
        
    except Exception as e:
        # Fallback to numpy if SymPy has issues
        coeffs = [a, b, c, d]
        return np.roots(coeffs)

def track_roots_consistently(z_values, all_roots):
    """
    Ensure consistent tracking of roots across z values by minimizing discontinuity.
    """
    n_points = len(z_values)
    n_roots = all_roots[0].shape[0]
    tracked_roots = np.zeros((n_points, n_roots), dtype=complex)
    tracked_roots[0] = all_roots[0]
    
    for i in range(1, n_points):
        prev_roots = tracked_roots[i-1]
        current_roots = all_roots[i]
        
        # For each previous root, find the closest current root
        assigned = np.zeros(n_roots, dtype=bool)
        assignments = np.zeros(n_roots, dtype=int)
        
        for j in range(n_roots):
            distances = np.abs(current_roots - prev_roots[j])
            
            # Find the closest unassigned root
            while True:
                best_idx = np.argmin(distances)
                if not assigned[best_idx]:
                    assignments[j] = best_idx
                    assigned[best_idx] = True
                    break
                else:
                    # Mark as infinite distance and try again
                    distances[best_idx] = np.inf
                    
                # Safety check if all are assigned (shouldn't happen)
                if np.all(distances == np.inf):
                    assignments[j] = j  # Default to same index
                    break
        
        # Reorder current roots based on assignments
        tracked_roots[i] = current_roots[assignments]
    
    return tracked_roots

def generate_cubic_discriminant(z, beta, z_a, y_effective):
    """
    Calculate the cubic discriminant with high precision using SymPy's standard formula.
    For a cubic ax^3 + bx^2 + cx + d: Δ = 18abcd - 27a^2d^2 + b^2c^2 - 2b^3d - 9ac^3
    """
    # Create symbolic variables for more accurate calculation
    z_sym, beta_sym, z_a_sym, y_sym = sp.symbols("z beta z_a y", real=True)
    
    # Define coefficients with symbols
    a_sym = z_sym * z_a_sym
    b_sym = z_sym * z_a_sym + z_sym + z_a_sym - z_a_sym*y_sym
    c_sym = z_sym + z_a_sym + 1 - y_sym*(beta_sym*z_a_sym + 1 - beta_sym)
    d_sym = 1
    
    # Standard formula for cubic discriminant
    discriminant_expr = (
        18*a_sym*b_sym*c_sym*d_sym - 
        27*a_sym**2*d_sym**2 + 
        b_sym**2*c_sym**2 - 
        2*b_sym**3*d_sym - 
        9*a_sym*c_sym**3
    )
    
    # Create a high-precision lambda function
    discriminant_func = sp.lambdify(
        (z_sym, beta_sym, z_a_sym, y_sym), 
        discriminant_expr, 
        modules="mpmath"
    )
    
    # Evaluate with high precision
    return float(discriminant_func(z, beta, z_a, y_effective))

def generate_root_plots(beta, y, z_a, z_min, z_max, n_points):
    """
    Generate Im(s) and Re(s) vs. z plots with improved accuracy using SymPy.
    """
    if z_a <= 0 or y <= 0 or z_min >= z_max:
        st.error("Invalid input parameters.")
        return None, None, None

    # Apply the condition for y
    y_effective = y if y > 1 else 1/y
    
    # Create progress bar
    progress = AdvancedProgressBar(n_points, "Computing cubic roots vs. z")
    
    z_points = np.linspace(z_min, z_max, n_points)
    
    # Collect all roots first
    all_roots = []
    discriminants = []
    
    for i, z in enumerate(z_points):
        # Update progress
        progress.update(i+1, f"Computing roots for z = {z:.3f}")
        
        # Calculate roots using SymPy
        roots = compute_cubic_roots(z, beta, z_a, y)
        
        # Initial sorting to help with tracking
        roots = sorted(roots, key=lambda x: (abs(x.imag), x.real))
        all_roots.append(roots)
        
        # Calculate discriminant with high precision
        disc = generate_cubic_discriminant(z, beta, z_a, y_effective)
        discriminants.append(disc)
    
    progress.complete()
    
    # Create secondary progress bar for root tracking
    track_progress = AdvancedProgressBar(1, "Tracking roots consistently across z values")
    
    all_roots = np.array(all_roots)
    discriminants = np.array(discriminants)
    
    # Track roots consistently across z values
    tracked_roots = track_roots_consistently(z_points, all_roots)
    
    track_progress.complete()
    
    # Extract imaginary and real parts
    ims = np.imag(tracked_roots)
    res = np.real(tracked_roots)
    
    # Create figure for imaginary parts
    fig_im = go.Figure()
    for i in range(3):
        fig_im.add_trace(go.Scatter(x=z_points, y=ims[:, i], mode="lines", name=f"Im{{s{i+1}}}",
                                    line=dict(width=2)))
    
    # Add vertical lines at discriminant zero crossings
    disc_zeros = []
    for i in range(len(discriminants)-1):
        if discriminants[i] * discriminants[i+1] <= 0:  # Sign change
            zero_pos = z_points[i] + (z_points[i+1] - z_points[i]) * (0 - discriminants[i]) / (discriminants[i+1] - discriminants[i])
            disc_zeros.append(zero_pos)
            fig_im.add_vline(x=zero_pos, line=dict(color="red", width=1, dash="dash"))
    
    fig_im.update_layout(title=f"Im{{s}} vs. z (β={beta:.3f}, y={y:.3f}, z_a={z_a:.3f})",
                         xaxis_title="z", yaxis_title="Im{s}", hovermode="x unified")

    # Create figure for real parts
    fig_re = go.Figure()
    for i in range(3):
        fig_re.add_trace(go.Scatter(x=z_points, y=res[:, i], mode="lines", name=f"Re{{s{i+1}}}",
                                    line=dict(width=2)))
    
    # Add vertical lines at discriminant zero crossings
    for zero_pos in disc_zeros:
        fig_re.add_vline(x=zero_pos, line=dict(color="red", width=1, dash="dash"))
    
    fig_re.update_layout(title=f"Re{{s}} vs. z (β={beta:.3f}, y={y:.3f}, z_a={z_a:.3f})",
                         xaxis_title="z", yaxis_title="Re{s}", hovermode="x unified")
    
    # Create discriminant plot
    fig_disc = go.Figure()
    fig_disc.add_trace(go.Scatter(x=z_points, y=discriminants, mode="lines", 
                                 name="Cubic Discriminant", line=dict(color="black", width=2)))
    fig_disc.add_hline(y=0, line=dict(color="red", width=1, dash="dash"))
    
    fig_disc.update_layout(title=f"Cubic Discriminant vs. z (β={beta:.3f}, y={y:.3f}, z_a={z_a:.3f})",
                          xaxis_title="z", yaxis_title="Discriminant", hovermode="x unified")
    
    return fig_im, fig_re, fig_disc

def generate_roots_vs_beta_plots(z, y, z_a, beta_min, beta_max, n_points):
    """
    Generate Im(s) and Re(s) vs. β plots with improved accuracy using SymPy.
    """
    if z_a <= 0 or y <= 0 or beta_min >= beta_max:
        st.error("Invalid input parameters.")
        return None, None, None

    # Apply the condition for y
    y_effective = y if y > 1 else 1/y
    
    # Create progress bar
    progress = AdvancedProgressBar(n_points, "Computing cubic roots vs. β")
    
    beta_points = np.linspace(beta_min, beta_max, n_points)
    
    # Collect all roots first
    all_roots = []
    discriminants = []
    
    for i, beta in enumerate(beta_points):
        # Update progress
        progress.update(i+1, f"Computing roots for β = {beta:.3f}")
        
        # Calculate roots using SymPy for higher precision
        roots = compute_cubic_roots(z, beta, z_a, y)
        
        # Initial sorting to help with tracking
        roots = sorted(roots, key=lambda x: (abs(x.imag), x.real))
        all_roots.append(roots)
        
        # Calculate discriminant with high precision
        disc = generate_cubic_discriminant(z, beta, z_a, y_effective)
        discriminants.append(disc)
    
    progress.complete()
    
    # Create secondary progress bar for root tracking
    track_progress = AdvancedProgressBar(1, "Tracking roots consistently across β values")
    
    all_roots = np.array(all_roots)
    discriminants = np.array(discriminants)
    
    # Track roots consistently across beta values
    tracked_roots = track_roots_consistently(beta_points, all_roots)
    
    track_progress.complete()
    
    # Extract imaginary and real parts
    ims = np.imag(tracked_roots)
    res = np.real(tracked_roots)
    
    # Create figure for imaginary parts
    fig_im = go.Figure()
    for i in range(3):
        fig_im.add_trace(go.Scatter(x=beta_points, y=ims[:, i], mode="lines", name=f"Im{{s{i+1}}}",
                                    line=dict(width=2)))
    
    # Add vertical lines at discriminant zero crossings
    disc_zeros = []
    for i in range(len(discriminants)-1):
        if discriminants[i] * discriminants[i+1] <= 0:  # Sign change
            zero_pos = beta_points[i] + (beta_points[i+1] - beta_points[i]) * (0 - discriminants[i]) / (discriminants[i+1] - discriminants[i])
            disc_zeros.append(zero_pos)
            fig_im.add_vline(x=zero_pos, line=dict(color="red", width=1, dash="dash"))
    
    fig_im.update_layout(title=f"Im{{s}} vs. β (z={z:.3f}, y={y:.3f}, z_a={z_a:.3f})",
                         xaxis_title="β", yaxis_title="Im{s}", hovermode="x unified")

    # Create figure for real parts
    fig_re = go.Figure()
    for i in range(3):
        fig_re.add_trace(go.Scatter(x=beta_points, y=res[:, i], mode="lines", name=f"Re{{s{i+1}}}",
                                    line=dict(width=2)))
    
    # Add vertical lines at discriminant zero crossings
    for zero_pos in disc_zeros:
        fig_re.add_vline(x=zero_pos, line=dict(color="red", width=1, dash="dash"))
    
    fig_re.update_layout(title=f"Re{{s}} vs. β (z={z:.3f}, y={y:.3f}, z_a={z_a:.3f})",
                         xaxis_title="β", yaxis_title="Re{s}", hovermode="x unified")
    
    # Create discriminant plot
    fig_disc = go.Figure()
    fig_disc.add_trace(go.Scatter(x=beta_points, y=discriminants, mode="lines", 
                                 name="Cubic Discriminant", line=dict(color="black", width=2)))
    fig_disc.add_hline(y=0, line=dict(color="red", width=1, dash="dash"))
    
    fig_disc.update_layout(title=f"Cubic Discriminant vs. β (z={z:.3f}, y={y:.3f}, z_a={z_a:.3f})",
                          xaxis_title="β", yaxis_title="Discriminant", hovermode="x unified")
    
    return fig_im, fig_re, fig_disc

def generate_phase_diagram(z_a, y, beta_min=0.0, beta_max=1.0, z_min=-10.0, z_max=10.0, 
                          beta_steps=100, z_steps=100):
    """
    Generate a phase diagram showing regions of complex and real roots with high precision.
    """
    if cpp_compiled:
        phase_map = generate_phase_diagram_cpp(z_a, y, beta_min, beta_max, z_min, z_max, beta_steps, z_steps)
        beta_values = np.linspace(beta_min, beta_max, beta_steps)
        z_values = np.linspace(z_min, z_max, z_steps)
    else:
        # Create progress tracking
        progress = AdvancedProgressBar(z_steps, "Generating phase diagram")
        
        # Apply the condition for y
        y_effective = y if y > 1 else 1/y
        
        beta_values = np.linspace(beta_min, beta_max, beta_steps)
        z_values = np.linspace(z_min, z_max, z_steps)
        
        # Initialize phase map
        phase_map = np.zeros((z_steps, beta_steps))
        
        for i, z in enumerate(z_values):
            # Update progress
            progress.update(i+1, f"Analyzing z = {z:.2f}")
            
            for j, beta in enumerate(beta_values):
                # Calculate discriminant with high precision
                disc = generate_cubic_discriminant(z, beta, z_a, y_effective)
                
                # Set result based on sign of discriminant
                # 1 for all real roots (discriminant > 0), -1 for complex roots (discriminant < 0)
                phase_map[i, j] = 1 if disc > 0 else -1
        
        progress.complete()
    
    # Create heatmap
    fig = go.Figure(data=go.Heatmap(
        z=phase_map,
        x=beta_values,
        y=z_values,
        colorscale=[[0, 'blue'], [0.5, 'white'], [1.0, 'red']],
        zmin=-1,
        zmax=1,
        showscale=True,
        colorbar=dict(
            title="Root Type",
            tickvals=[-1, 1],
            ticktext=["Complex Roots", "All Real Roots"]
        )
    ))
    
    fig.update_layout(
        title=f"Phase Diagram: Root Structure (y={y:.3f}, z_a={z_a:.3f})",
        xaxis_title="β",
        yaxis_title="z",
        hovermode="closest"
    )
    
    return fig

def generate_eigenvalue_distribution(beta, y, z_a, n=1000, seed=42):
    """
    Generate the eigenvalue distribution of B_n = S_n T_n as n→∞
    with high precision.
    """
    # Create progress tracking
    progress = AdvancedProgressBar(7, "Computing eigenvalue distribution")
    
    if cpp_compiled:
        progress.update(1, "Using C++ accelerated implementation")
        eigenvalues, x_vals = generate_eigenvalue_distribution_cpp(beta, y, z_a, n, seed)
        progress.update(6, "Eigenvalues computed successfully")
    else:
        # Apply the condition for y
        y_effective = y if y > 1 else 1/y
        
        # Set random seed
        progress.update(1, "Setting up random seed")
        np.random.seed(seed)
        
        # Compute dimension p based on aspect ratio y
        progress.update(2, "Initializing matrices")
        p = int(y_effective * n)
        
        # Constructing T_n (Population / Shape Matrix)
        k = int(np.floor(beta * p))
        diag_entries = np.concatenate([
            np.full(k, z_a),
            np.full(p - k, 1.0)
        ])
        np.random.shuffle(diag_entries)
        T_n = np.diag(diag_entries)
        
        # Generate the data matrix X with i.i.d. standard normal entries
        progress.update(3, "Generating random data matrix")
        X = np.random.randn(p, n)
        
        # Compute the sample covariance matrix S_n = (1/n) * XX^T
        progress.update(4, "Computing sample covariance matrix")
        S_n = (1 / n) * (X @ X.T)
        
        # Compute B_n = S_n T_n
        progress.update(5, "Computing B_n matrix")
        B_n = S_n @ T_n
        
        # Compute eigenvalues of B_n with high precision
        progress.update(6, "Computing eigenvalues")
        eigenvalues = np.linalg.eigvalsh(B_n)
        
        # Generate x values for KDE
        x_vals = np.linspace(min(eigenvalues), max(eigenvalues), 500)
    
    # Use KDE to compute a smooth density estimate
    progress.update(7, "Computing kernel density estimate")
    kde = gaussian_kde(eigenvalues)
    kde_vals = kde(x_vals)
    
    progress.complete()
    
    # Create figure
    fig = go.Figure()
    
    # Add histogram trace
    fig.add_trace(go.Histogram(x=eigenvalues, histnorm='probability density', 
                              name="Histogram", marker=dict(color='blue', opacity=0.6)))
    
    # Add KDE trace
    fig.add_trace(go.Scatter(x=x_vals, y=kde_vals, mode="lines", 
                            name="KDE", line=dict(color='red', width=2)))
    
    fig.update_layout(
        title=f"Eigenvalue Distribution for B_n = S_n T_n (y={y:.1f}, β={beta:.2f}, a={z_a:.1f})",
        xaxis_title="Eigenvalue",
        yaxis_title="Density",
        hovermode="closest",
        showlegend=True
    )
    
    return fig, eigenvalues

def generate_z_vs_beta_plot(z_a, y, z_min, z_max, beta_steps, z_steps,
                          s_num_expr=None, s_denom_expr=None, 
                          z_num_expr=None, z_denom_expr=None,
                          show_derivatives=False,
                          show_high_y=False,
                          show_low_y=False,
                          show_max_k=True,
                          show_min_t=True,
                          use_eigenvalue_method=True,
                          n_samples=1000,
                          seeds=5):
    """
    Generate z vs beta plot with high precision calculations.
    """
    # Create main progress tracking
    main_progress = AdvancedProgressBar(5, "Computing z*(β) curves")
    
    if z_a <= 0 or y <= 0 or z_min >= z_max:
        main_progress.complete(False)
        st.error("Invalid input parameters.")
        return None

    main_progress.update(1, "Creating β grid")
    betas = np.linspace(0, 1, beta_steps)
    
    if use_eigenvalue_method:
        # Use the eigenvalue method to compute boundaries
        main_progress.update(2, "Computing eigenvalue support boundaries")
        min_eigs, max_eigs = compute_eigenvalue_support_boundaries(z_a, y, betas, n_samples, seeds)
        z_mins, z_maxs = min_eigs, max_eigs
    else:
        # Use the original discriminant method
        main_progress.update(2, "Computing discriminant zeros")
        betas, z_mins, z_maxs = sweep_beta_and_find_z_bounds(z_a, y, z_min, z_max, beta_steps, z_steps)
    
    main_progress.update(3, "Computing additional curves")
    
    # Compute additional curves
    high_y_curve = compute_high_y_curve(betas, z_a, y) if show_high_y else None
    alt_low_expr = compute_alternate_low_expr(betas, z_a, y) if show_low_y else None
    
    # Compute the max/min expressions
    max_k_curve = compute_max_k_expression(betas, z_a, y) if show_max_k else None
    min_t_curve = compute_min_t_expression(betas, z_a, y) if show_min_t else None
    
    # Compute both custom curves
    custom_curve1 = None
    custom_curve2 = None
    if s_num_expr and s_denom_expr:
        custom_curve1 = compute_custom_expression(betas, z_a, y, s_num_expr, s_denom_expr, True)
    if z_num_expr and z_denom_expr:
        custom_curve2 = compute_custom_expression(betas, z_a, y, z_num_expr, z_denom_expr, False)

    # Compute derivatives if needed
    if show_derivatives:
        main_progress.update(4, "Computing derivatives")
        derivatives = compute_all_derivatives(betas, z_mins, z_maxs, None, high_y_curve, 
                                           alt_low_expr, custom_curve1, custom_curve2)
        # Calculate derivatives for max_k and min_t curves if they exist
        if show_max_k and max_k_curve is not None:
            max_k_derivatives = compute_derivatives(max_k_curve, betas)
        if show_min_t and min_t_curve is not None:
            min_t_derivatives = compute_derivatives(min_t_curve, betas)
    
    main_progress.update(5, "Creating plot")

    fig = go.Figure()
    
    # Original curves
    if use_eigenvalue_method:
        fig.add_trace(go.Scatter(x=betas, y=z_maxs, mode="markers+lines", 
                                name="Upper Bound (Max Eigenvalue)", line=dict(color='blue')))
        fig.add_trace(go.Scatter(x=betas, y=z_mins, mode="markers+lines", 
                                name="Lower Bound (Min Eigenvalue)", line=dict(color='blue')))
        # Add shaded region between curves
        fig.add_trace(go.Scatter(
            x=np.concatenate([betas, betas[::-1]]),
            y=np.concatenate([z_maxs, z_mins[::-1]]),
            fill='toself',
            fillcolor='rgba(0,0,255,0.2)',
            line=dict(color='rgba(255,255,255,0)'),
            showlegend=False,
            hoverinfo='skip'
        ))
    else:
        fig.add_trace(go.Scatter(x=betas, y=z_maxs, mode="markers+lines", 
                                name="Upper z*(β)", line=dict(color='blue')))
        fig.add_trace(go.Scatter(x=betas, y=z_mins, mode="markers+lines", 
                                name="Lower z*(β)", line=dict(color='blue')))

    # Add High y Expression only if selected
    if show_high_y and high_y_curve is not None:
        fig.add_trace(go.Scatter(x=betas, y=high_y_curve, mode="markers+lines", 
                                name="High y Expression", line=dict(color='green')))
    
    # Add Low Expression only if selected
    if show_low_y and alt_low_expr is not None:
        fig.add_trace(go.Scatter(x=betas, y=alt_low_expr, mode="markers+lines", 
                                name="Low Expression", line=dict(color='orange')))
    
    # Add the max/min curves if selected
    if show_max_k and max_k_curve is not None:
        fig.add_trace(go.Scatter(x=betas, y=max_k_curve, mode="lines", 
                                name="Max k Expression", line=dict(color='red', width=2)))
    
    if show_min_t and min_t_curve is not None:
        fig.add_trace(go.Scatter(x=betas, y=min_t_curve, mode="lines", 
                                name="Min t Expression", line=dict(color='purple', width=2)))
    
    if custom_curve1 is not None:
        fig.add_trace(go.Scatter(x=betas, y=custom_curve1, mode="markers+lines", 
                                name="Custom 1 (s-based)", line=dict(color='magenta')))
    if custom_curve2 is not None:
        fig.add_trace(go.Scatter(x=betas, y=custom_curve2, mode="markers+lines", 
                                name="Custom 2 (direct)", line=dict(color='brown')))

    if show_derivatives:
        # First derivatives
        curve_info = [
            ('upper', 'Upper Bound' if use_eigenvalue_method else 'Upper z*(β)', 'blue'),
            ('lower', 'Lower Bound' if use_eigenvalue_method else 'Lower z*(β)', 'lightblue'),
        ]
        
        if show_high_y and high_y_curve is not None:
            curve_info.append(('high_y', 'High y', 'green'))
        if show_low_y and alt_low_expr is not None:
            curve_info.append(('alt_low', 'Alt Low', 'orange'))
        
        if custom_curve1 is not None:
            curve_info.append(('custom1', 'Custom 1', 'magenta'))
        if custom_curve2 is not None:
            curve_info.append(('custom2', 'Custom 2', 'brown'))

        for key, name, color in curve_info:
            if key in derivatives:
                fig.add_trace(go.Scatter(x=betas, y=derivatives[key][0], mode="lines", 
                                        name=f"{name} d/dβ", line=dict(color=color, dash='dash')))
                fig.add_trace(go.Scatter(x=betas, y=derivatives[key][1], mode="lines", 
                                        name=f"{name} d²/dβ²", line=dict(color=color, dash='dot')))
        
        # Add derivatives for max_k and min_t curves if they exist
        if show_max_k and max_k_curve is not None and 'max_k_derivatives' in locals():
            fig.add_trace(go.Scatter(x=betas, y=max_k_derivatives[0], mode="lines", 
                                    name="Max k d/dβ", line=dict(color='red', dash='dash')))
            fig.add_trace(go.Scatter(x=betas, y=max_k_derivatives[1], mode="lines", 
                                    name="Max k d²/dβ²", line=dict(color='red', dash='dot')))
        
        if show_min_t and min_t_curve is not None and 'min_t_derivatives' in locals():
            fig.add_trace(go.Scatter(x=betas, y=min_t_derivatives[0], mode="lines", 
                                    name="Min t d/dβ", line=dict(color='purple', dash='dash')))
            fig.add_trace(go.Scatter(x=betas, y=min_t_derivatives[1], mode="lines", 
                                    name="Min t d²/dβ²", line=dict(color='purple', dash='dot')))

    fig.update_layout(
        title="Curves vs β: Eigenvalue Support Boundaries and Asymptotic Expressions" if use_eigenvalue_method 
              else "Curves vs β: z*(β) Boundaries and Asymptotic Expressions",
        xaxis_title="β",
        yaxis_title="Value",
        hovermode="x unified",
        showlegend=True,
        legend=dict(
            yanchor="top",
            y=0.99,
            xanchor="left",
            x=0.01
        )
    )
    
    main_progress.complete()
    return fig

def analyze_complex_root_structure(beta_values, z, z_a, y):
    """
    Analyze when the cubic equation switches between having all real roots
    and having a complex conjugate pair plus one real root.
    
    Returns:
    - transition_points: beta values where the root structure changes
    - structure_types: list indicating whether each interval has all real roots or complex roots
    """
    # Create progress tracking
    progress = AdvancedProgressBar(len(beta_values), "Analyzing root structure")
    
    # Apply the condition for y
    y_effective = y if y > 1 else 1/y
    
    transition_points = []
    structure_types = []
    
    previous_type = None
    
    for i, beta in enumerate(beta_values):
        progress.update(i+1, f"Analyzing root structure at β = {beta:.4f}")
        
        roots = compute_cubic_roots(z, beta, z_a, y)
        
        # Check if all roots are real (imaginary parts close to zero)
        is_all_real = all(abs(root.imag) < 1e-10 for root in roots)
        
        current_type = "real" if is_all_real else "complex"
        
        if previous_type is not None and current_type != previous_type:
            # Found a transition point
            transition_points.append(beta)
            structure_types.append(previous_type)
        
        previous_type = current_type
    
    # Add the final interval type
    if previous_type is not None:
        structure_types.append(previous_type)
    
    progress.complete()
    return transition_points, structure_types

# ----------------- Streamlit UI -----------------
st.title("Cubic Root Analysis (C++ Accelerated)")

# Add a note about C++ acceleration and high precision
if cpp_compiled:
    st.success("✅ C++ acceleration module loaded successfully. Calculations will run faster!")
else:
    st.warning("⚠️ C++ module compilation failed. Falling back to Python implementations with high precision SymPy calculations.")

st.info(f"Using SymPy with {sp.mpmath.mp.dps} decimal digits of precision for accurate calculations.")

# Define three tabs
tab1, tab2, tab3 = st.tabs(["z*(β) Curves", "Complex Root Analysis", "Differential Analysis"])

# ----- Tab 1: z*(β) Curves -----
with tab1:
    st.header("Eigenvalue Support Boundaries")
    
    # Cleaner layout with better column organization
    col1, col2, col3 = st.columns([1, 1, 2])
    
    with col1:
        z_a_1 = st.number_input("z_a", value=1.0, key="z_a_1")
        y_1 = st.number_input("y", value=1.0, key="y_1")
        
    with col2:
        z_min_1 = st.number_input("z_min", value=-10.0, key="z_min_1")
        z_max_1 = st.number_input("z_max", value=10.0, key="z_max_1")
    
    with col1:
        method_type = st.radio(
            "Calculation Method",
            ["Eigenvalue Method", "Discriminant Method"],
            index=0  # Default to eigenvalue method
        )
    
    # Advanced settings in collapsed expanders
    with st.expander("Method Settings", expanded=False):
        if method_type == "Eigenvalue Method":
            beta_steps = st.slider("β steps", min_value=21, max_value=101, value=51, step=10, 
                                  key="beta_steps_eigen")
            n_samples = st.slider("Matrix size (n)", min_value=100, max_value=2000, value=1000, 
                                step=100)
            seeds = st.slider("Number of seeds", min_value=1, max_value=10, value=5, step=1)
        else:
            beta_steps = st.slider("β steps", min_value=51, max_value=501, value=201, step=50, 
                                  key="beta_steps")
            z_steps = st.slider("z grid steps", min_value=1000, max_value=100000, value=50000, 
                              step=1000, key="z_steps")
    
    # Curve visibility options
    with st.expander("Curve Visibility", expanded=False):
        col_vis1, col_vis2 = st.columns(2)
        with col_vis1:
            show_high_y = st.checkbox("Show High y Expression", value=False, key="show_high_y")
            show_max_k = st.checkbox("Show Max k Expression", value=True, key="show_max_k")
        with col_vis2:
            show_low_y = st.checkbox("Show Low y Expression", value=False, key="show_low_y")
            show_min_t = st.checkbox("Show Min t Expression", value=True, key="show_min_t")
    
    # Custom expressions collapsed by default
    with st.expander("Custom Expression 1 (s-based)", expanded=False):
        st.markdown("""Enter expressions for s = numerator/denominator 
                    (using variables `y`, `beta`, `z_a`, and `sqrt()`)""")
        st.latex(r"\text{This s will be inserted into:}")
        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})}")
        s_num = st.text_input("s numerator", value="", key="s_num")
        s_denom = st.text_input("s denominator", value="", key="s_denom")

    with st.expander("Custom Expression 2 (direct z(β))", expanded=False):
        st.markdown("""Enter direct expression for z(β) = numerator/denominator 
                    (using variables `y`, `beta`, `z_a`, and `sqrt()`)""")
        z_num = st.text_input("z(β) numerator", value="", key="z_num")
        z_denom = st.text_input("z(β) denominator", value="", key="z_denom")

    # Move show_derivatives to main UI level for better visibility
    with col2:
        show_derivatives = st.checkbox("Show derivatives", value=False)

    # Compute button
    if st.button("Compute Curves", key="tab1_button"):
        with col3:
            use_eigenvalue_method = (method_type == "Eigenvalue Method")
            if use_eigenvalue_method:
                fig = generate_z_vs_beta_plot(z_a_1, y_1, z_min_1, z_max_1, beta_steps, None,
                                            s_num, s_denom, z_num, z_denom, show_derivatives, 
                                            show_high_y, show_low_y, show_max_k, show_min_t,
                                            use_eigenvalue_method=True, n_samples=n_samples, 
                                            seeds=seeds)
            else:
                fig = generate_z_vs_beta_plot(z_a_1, y_1, z_min_1, z_max_1, beta_steps, z_steps,
                                            s_num, s_denom, z_num, z_denom, show_derivatives,
                                            show_high_y, show_low_y, show_max_k, show_min_t,
                                            use_eigenvalue_method=False)
            
            if fig is not None:
                st.plotly_chart(fig, use_container_width=True)
                
                # Curve explanations in collapsed expander
                with st.expander("Curve Explanations", expanded=False):
                    if use_eigenvalue_method:
                        st.markdown("""
                        - **Upper/Lower Bounds** (Blue): Maximum/minimum eigenvalues of B_n = S_n T_n
                        - **Shaded Region**: Eigenvalue support region
                        - **High y Expression** (Green): Asymptotic approximation for high y values
                        - **Low Expression** (Orange): Alternative asymptotic expression
                        - **Max k Expression** (Red): $\\max_{k \\in (0,\\infty)} \\frac{y\\beta (a-1)k + \\bigl(ak+1\\bigr)\\bigl((y-1)k-1\\bigr)}{(ak+1)(k^2+k)}$
                        - **Min t Expression** (Purple): $\\min_{t \\in \\left(-\\frac{1}{a},\\, 0\\right)} \\frac{y\\beta (a-1)t + \\bigl(at+1\\bigr)\\bigl((y-1)t-1\\bigr)}{(at+1)(t^2+t)}$
                        - **Custom Expression 1** (Magenta): Result from user-defined s substituted into the main formula
                        - **Custom Expression 2** (Brown): Direct z(β) expression
                        """)
                    else:
                        st.markdown("""
                        - **Upper z*(β)** (Blue): Maximum z value where discriminant is zero
                        - **Lower z*(β)** (Blue): Minimum z value where discriminant is zero
                        - **High y Expression** (Green): Asymptotic approximation for high y values
                        - **Low Expression** (Orange): Alternative asymptotic expression
                        - **Max k Expression** (Red): $\\max_{k \\in (0,\\infty)} \\frac{y\\beta (a-1)k + \\bigl(ak+1\\bigr)\\bigl((y-1)k-1\\bigr)}{(ak+1)(k^2+k)}$
                        - **Min t Expression** (Purple): $\\min_{t \\in \\left(-\\frac{1}{a},\\, 0\\right)} \\frac{y\\beta (a-1)t + \\bigl(at+1\\bigr)\\bigl((y-1)t-1\\bigr)}{(at+1)(t^2+t)}$
                        - **Custom Expression 1** (Magenta): Result from user-defined s substituted into the main formula
                        - **Custom Expression 2** (Brown): Direct z(β) expression
                        """)
                    if show_derivatives:
                        st.markdown("""
                        Derivatives are shown as:
                        - Dashed lines: First derivatives (d/dβ)
                        - Dotted lines: Second derivatives (d²/dβ²)
                        """)

# ----- Tab 2: Complex Root Analysis -----
with tab2:
    st.header("Complex Root Analysis")
    
    # Create tabs within the page for different plots
    plot_tabs = st.tabs(["Im{s} vs. z", "Im{s} vs. β", "Phase Diagram", "Eigenvalue Distribution"])
    
    # Tab for Im{s} vs. z plot
    with plot_tabs[0]:
        col1, col2 = st.columns([1, 2])
        with col1:
            beta_z = st.number_input("β", value=0.5, min_value=0.0, max_value=1.0, key="beta_tab2_z")
            y_z = st.number_input("y", value=1.0, key="y_tab2_z")
            z_a_z = st.number_input("z_a", value=1.0, key="z_a_tab2_z")
            z_min_z = st.number_input("z_min", value=-10.0, key="z_min_tab2_z")
            z_max_z = st.number_input("z_max", value=10.0, key="z_max_tab2_z")
            with st.expander("Resolution Settings", expanded=False):
                z_points = st.slider("z grid points", min_value=100, max_value=2000, value=500, step=100, key="z_points_z")
        if st.button("Compute Complex Roots vs. z", key="tab2_button_z"):
            with col2:
                fig_im, fig_re, fig_disc = generate_root_plots(beta_z, y_z, z_a_z, z_min_z, z_max_z, z_points)
                if fig_im is not None and fig_re is not None and fig_disc is not None:
                    st.plotly_chart(fig_im, use_container_width=True)
                    st.plotly_chart(fig_re, use_container_width=True)
                    st.plotly_chart(fig_disc, use_container_width=True)
                    
                    with st.expander("Root Structure Analysis", expanded=False):
                        st.markdown("""
                        ### Root Structure Explanation
                        
                        The red dashed vertical lines mark the points where the cubic discriminant equals zero.
                        At these points, the cubic equation's root structure changes:
                        
                        - When the discriminant is positive, the cubic has three distinct real roots.
                        - When the discriminant is negative, the cubic has one real root and two complex conjugate roots.
                        - When the discriminant is exactly zero, the cubic has at least two equal roots.
                        
                        These transition points align perfectly with the z*(β) boundary curves from the first tab,
                        which represent exactly these transitions in the (β,z) plane.
                        """)

    # New tab for Im{s} vs. β plot
    with plot_tabs[1]:
        col1, col2 = st.columns([1, 2])
        with col1:
            z_beta = st.number_input("z", value=1.0, key="z_tab2_beta")
            y_beta = st.number_input("y", value=1.0, key="y_tab2_beta")
            z_a_beta = st.number_input("z_a", value=1.0, key="z_a_tab2_beta")
            beta_min = st.number_input("β_min", value=0.0, min_value=0.0, max_value=1.0, key="beta_min_tab2")
            beta_max = st.number_input("β_max", value=1.0, min_value=0.0, max_value=1.0, key="beta_max_tab2")
            with st.expander("Resolution Settings", expanded=False):
                beta_points = st.slider("β grid points", min_value=100, max_value=1000, value=500, step=100, key="beta_points")
        if st.button("Compute Complex Roots vs. β", key="tab2_button_beta"):
            with col2:
                fig_im_beta, fig_re_beta, fig_disc = generate_roots_vs_beta_plots(
                    z_beta, y_beta, z_a_beta, beta_min, beta_max, beta_points)
                
                if fig_im_beta is not None and fig_re_beta is not None and fig_disc is not None:
                    st.plotly_chart(fig_im_beta, use_container_width=True)
                    st.plotly_chart(fig_re_beta, use_container_width=True)
                    st.plotly_chart(fig_disc, use_container_width=True)
                    
                    # Add analysis of transition points
                    transition_points, structure_types = analyze_complex_root_structure(
                        np.linspace(beta_min, beta_max, beta_points), z_beta, z_a_beta, y_beta)
                    
                    if transition_points:
                        st.subheader("Root Structure Transition Points")
                        for i, beta in enumerate(transition_points):
                            prev_type = structure_types[i]
                            next_type = structure_types[i+1] if i+1 < len(structure_types) else "unknown"
                            st.markdown(f"- At β = {beta:.6f}: Transition from {prev_type} roots to {next_type} roots")
                    else:
                        st.info("No transitions detected in root structure across this β range.")
                    
                    # Explanation
                    with st.expander("Analysis Explanation", expanded=False):
                        st.markdown("""
                        ### Interpreting the Plots
                        
                        - **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.
                        - **Re{s} vs. β**: Shows how the real parts of the roots change with β.
                        - **Discriminant Plot**: The cubic discriminant changes sign at points where the root structure changes.
                          - When discriminant < 0: The cubic has one real root and two complex conjugate roots.
                          - When discriminant > 0: The cubic has three distinct real roots.
                          - When discriminant = 0: The cubic has multiple roots (at least two roots are equal).
                        
                        The vertical red dashed lines mark the transition points where the root structure changes.
                        """)
    
    # Tab for Phase Diagram
    with plot_tabs[2]:
        col1, col2 = st.columns([1, 2])
        with col1:
            z_a_phase = st.number_input("z_a", value=1.0, key="z_a_phase")
            y_phase = st.number_input("y", value=1.0, key="y_phase")
            beta_min_phase = st.number_input("β_min", value=0.0, min_value=0.0, max_value=1.0, key="beta_min_phase")
            beta_max_phase = st.number_input("β_max", value=1.0, min_value=0.0, max_value=1.0, key="beta_max_phase")
            z_min_phase = st.number_input("z_min", value=-10.0, key="z_min_phase")
            z_max_phase = st.number_input("z_max", value=10.0, key="z_max_phase")
            
            with st.expander("Resolution Settings", expanded=False):
                beta_steps_phase = st.slider("β grid points", min_value=20, max_value=200, value=100, step=20, key="beta_steps_phase")
                z_steps_phase = st.slider("z grid points", min_value=20, max_value=200, value=100, step=20, key="z_steps_phase")
        
        if st.button("Generate Phase Diagram", key="tab2_button_phase"):
            with col2:
                st.info("Generating phase diagram. This may take a while depending on resolution...")
                fig_phase = generate_phase_diagram(
                    z_a_phase, y_phase, beta_min_phase, beta_max_phase, z_min_phase, z_max_phase, 
                    beta_steps_phase, z_steps_phase)
                
                if fig_phase is not None:
                    st.plotly_chart(fig_phase, use_container_width=True)
                    
                    with st.expander("Phase Diagram Explanation", expanded=False):
                        st.markdown("""
                        ### Understanding the Phase Diagram
                        
                        This heatmap shows the regions in the (β, z) plane where:
                        
                        - **Red Regions**: The cubic equation has all real roots
                        - **Blue Regions**: The cubic equation has one real root and two complex conjugate roots
                        
                        The boundaries between these regions represent values where the discriminant is zero,
                        which are the exact same curves as the z*(β) boundaries in the first tab. This phase
                        diagram provides a comprehensive view of the eigenvalue support structure.
                        """)

    # Eigenvalue distribution tab
    with plot_tabs[3]:
        st.subheader("Eigenvalue Distribution for B_n = S_n T_n")
        with st.expander("Simulation Information", expanded=False):
            st.markdown("""
            This simulation generates the eigenvalue distribution of B_n as n→∞, where:
            - B_n = (1/n)XX^T with X being a p×n matrix
            - p/n → y as n→∞
            - The diagonal entries of T_n follow distribution β·δ(z_a) + (1-β)·δ(1)
            """)
        
        col_eigen1, col_eigen2 = st.columns([1, 2])
        with col_eigen1:
            beta_eigen = st.number_input("β", value=0.5, min_value=0.0, max_value=1.0, key="beta_eigen")
            y_eigen = st.number_input("y", value=1.0, key="y_eigen")
            z_a_eigen = st.number_input("z_a", value=1.0, key="z_a_eigen")
            n_samples = st.slider("Number of samples (n)", min_value=100, max_value=2000, value=1000, step=100)
            sim_seed = st.number_input("Random seed", min_value=1, max_value=1000, value=42, step=1)
            
            # Add comparison option
            show_theoretical = st.checkbox("Show theoretical boundaries", value=True)
            show_empirical_stats = st.checkbox("Show empirical statistics", value=True)

        if st.button("Generate Eigenvalue Distribution", key="tab2_eigen_button"):
            with col_eigen2:
                # Generate the eigenvalue distribution
                fig_eigen, eigenvalues = generate_eigenvalue_distribution(beta_eigen, y_eigen, z_a_eigen, n=n_samples, seed=sim_seed)
                
                # If requested, compute and add theoretical boundaries
                if show_theoretical:
                    # Calculate min and max eigenvalues using the support boundary functions
                    betas = np.array([beta_eigen])
                    min_eig, max_eig = compute_eigenvalue_support_boundaries(z_a_eigen, y_eigen, betas, n_samples=n_samples, seeds=5)
                    
                    # Add vertical lines for boundaries
                    fig_eigen.add_vline(
                        x=min_eig[0], 
                        line=dict(color="red", width=2, dash="dash"),
                        annotation_text="Min theoretical",
                        annotation_position="top right"
                    )
                    fig_eigen.add_vline(
                        x=max_eig[0], 
                        line=dict(color="red", width=2, dash="dash"),
                        annotation_text="Max theoretical",
                        annotation_position="top left"
                    )
                
                # Display the plot
                st.plotly_chart(fig_eigen, use_container_width=True)
                
                # Add comparison of empirical vs theoretical bounds
                if show_theoretical and show_empirical_stats:
                    empirical_min = eigenvalues.min()
                    empirical_max = eigenvalues.max()
                    
                    st.markdown("### Comparison of Empirical vs Theoretical Bounds")
                    col1, col2, col3 = st.columns(3)
                    with col1:
                        st.metric("Theoretical Min", f"{min_eig[0]:.6f}")
                        st.metric("Theoretical Max", f"{max_eig[0]:.6f}")
                        st.metric("Theoretical Width", f"{max_eig[0] - min_eig[0]:.6f}")
                    with col2:
                        st.metric("Empirical Min", f"{empirical_min:.6f}")
                        st.metric("Empirical Max", f"{empirical_max:.6f}")
                        st.metric("Empirical Width", f"{empirical_max - empirical_min:.6f}")
                    with col3:
                        st.metric("Min Difference", f"{empirical_min - min_eig[0]:.6f}")
                        st.metric("Max Difference", f"{empirical_max - max_eig[0]:.6f}")
                        st.metric("Width Difference", f"{(empirical_max - empirical_min) - (max_eig[0] - min_eig[0]):.6f}")
                
                # Display additional statistics
                if show_empirical_stats:
                    st.markdown("### Eigenvalue Statistics")
                    col1, col2 = st.columns(2)
                    with col1:
                        st.metric("Mean", f"{np.mean(eigenvalues):.6f}")
                        st.metric("Median", f"{np.median(eigenvalues):.6f}")
                    with col2:
                        st.metric("Standard Deviation", f"{np.std(eigenvalues):.6f}")
                        st.metric("Interquartile Range", f"{np.percentile(eigenvalues, 75) - np.percentile(eigenvalues, 25):.6f}")

# ----- Tab 3: Differential Analysis -----
with tab3:
    st.header("Differential Analysis vs. β")
    with st.expander("Description", expanded=False):
        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.")
    
    col1, col2 = st.columns([1, 2])
    with col1:
        z_a_diff = st.number_input("z_a", value=1.0, key="z_a_diff")
        y_diff = st.number_input("y", value=1.0, key="y_diff")
        z_min_diff = st.number_input("z_min", value=-10.0, key="z_min_diff")
        z_max_diff = st.number_input("z_max", value=10.0, key="z_max_diff")
        
        diff_method_type = st.radio(
            "Boundary Calculation Method",
            ["Eigenvalue Method", "Discriminant Method"],
            index=0,
            key="diff_method_type"
        )
        
        with st.expander("Resolution Settings", expanded=False):
            if diff_method_type == "Eigenvalue Method":
                beta_steps_diff = st.slider("β steps", min_value=21, max_value=101, value=51, step=10, 
                                         key="beta_steps_diff_eigen")
                diff_n_samples = st.slider("Matrix size (n)", min_value=100, max_value=2000, value=1000, 
                                        step=100, key="diff_n_samples")
                diff_seeds = st.slider("Number of seeds", min_value=1, max_value=10, value=5, step=1,
                                     key="diff_seeds")
            else:
                beta_steps_diff = st.slider("β steps", min_value=51, max_value=501, value=201, step=50, 
                                         key="beta_steps_diff")
                z_steps_diff = st.slider("z grid steps", min_value=1000, max_value=100000, value=50000, 
                                      step=1000, key="z_steps_diff")
        
        # Add options for curve selection
        st.subheader("Curves to Analyze")
        analyze_upper_lower = st.checkbox("Upper-Lower Difference", value=True)
        analyze_high_y = st.checkbox("High y Expression", value=False)
        analyze_alt_low = st.checkbox("Low y Expression", value=False)

    if st.button("Compute Differentials", key="tab3_button"):
        with col2:
            use_eigenvalue_method_diff = (diff_method_type == "Eigenvalue Method")
            
            # Create a progress tracker
            progress = AdvancedProgressBar(5, "Computing differential analysis")
            
            progress.update(1, "Setting up β grid")
            if use_eigenvalue_method_diff:
                betas_diff = np.linspace(0, 1, beta_steps_diff)
                progress.update(2, "Computing eigenvalue support boundaries")
                lower_vals, upper_vals = compute_eigenvalue_support_boundaries(
                    z_a_diff, y_diff, betas_diff, diff_n_samples, diff_seeds)
            else:
                progress.update(2, "Computing discriminant zeros")
                betas_diff, lower_vals, upper_vals = sweep_beta_and_find_z_bounds(
                    z_a_diff, y_diff, z_min_diff, z_max_diff, beta_steps_diff, z_steps_diff)
            
            # Create figure
            progress.update(3, "Creating plot")
            fig_diff = go.Figure()
            
            progress.update(4, "Computing derivatives")
            if analyze_upper_lower:
                diff_curve = upper_vals - lower_vals
                d1 = np.gradient(diff_curve, betas_diff)
                d2 = np.gradient(d1, betas_diff)
                
                fig_diff.add_trace(go.Scatter(x=betas_diff, y=diff_curve, mode="lines", 
                                name="Upper-Lower Difference", line=dict(color="magenta", width=2)))
                fig_diff.add_trace(go.Scatter(x=betas_diff, y=d1, mode="lines", 
                                name="Upper-Lower d/dβ", line=dict(color="magenta", dash='dash')))
                fig_diff.add_trace(go.Scatter(x=betas_diff, y=d2, mode="lines", 
                                name="Upper-Lower d²/dβ²", line=dict(color="magenta", dash='dot')))

            if analyze_high_y:
                high_y_curve = compute_high_y_curve(betas_diff, z_a_diff, y_diff)
                d1 = np.gradient(high_y_curve, betas_diff)
                d2 = np.gradient(d1, betas_diff)
                
                fig_diff.add_trace(go.Scatter(x=betas_diff, y=high_y_curve, mode="lines", 
                                name="High y", line=dict(color="green", width=2)))
                fig_diff.add_trace(go.Scatter(x=betas_diff, y=d1, mode="lines", 
                                name="High y d/dβ", line=dict(color="green", dash='dash')))
                fig_diff.add_trace(go.Scatter(x=betas_diff, y=d2, mode="lines", 
                                name="High y d²/dβ²", line=dict(color="green", dash='dot')))

            if analyze_alt_low:
                alt_low_curve = compute_alternate_low_expr(betas_diff, z_a_diff, y_diff)
                d1 = np.gradient(alt_low_curve, betas_diff)
                d2 = np.gradient(d1, betas_diff)
                
                fig_diff.add_trace(go.Scatter(x=betas_diff, y=alt_low_curve, mode="lines", 
                                name="Low y", line=dict(color="orange", width=2)))
                fig_diff.add_trace(go.Scatter(x=betas_diff, y=d1, mode="lines", 
                                name="Low y d/dβ", line=dict(color="orange", dash='dash')))
                fig_diff.add_trace(go.Scatter(x=betas_diff, y=d2, mode="lines", 
                                name="Low y d²/dβ²", line=dict(color="orange", dash='dot')))

            progress.update(5, "Finalizing plot")
            fig_diff.update_layout(
                title="Differential Analysis vs. β" + 
                      (" (Eigenvalue Method)" if use_eigenvalue_method_diff else " (Discriminant Method)"),
                xaxis_title="β",
                yaxis_title="Value",
                hovermode="x unified",
                showlegend=True,
                legend=dict(
                    yanchor="top",
                    y=0.99,
                    xanchor="left",
                    x=0.01
                )
            )
            
            progress.complete()
            st.plotly_chart(fig_diff, use_container_width=True)
            
            with st.expander("Curve Types", expanded=False):
                st.markdown("""
                - Solid lines: Original curves
                - Dashed lines: First derivatives (d/dβ)
                - Dotted lines: Second derivatives (d²/dβ²)
                """)