Statistics & Probability / Metropolis-Hastings MCMC
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LABORATORY 41 · STATISTICS & PROBABILITY

Metropolis-Hastings MCMC lab report

A worked metropolis-hastings mcmc lab report with sample observation tables, regression plots, calculations, and error analysis.

WORKED EXAMPLE · BENCHMARK OBSERVATIONS

A complete example laboratory report.

Simulated demonstration data.

This report illustrates formal statistical analysis, sampling error tracking, and parameter estimation. Replace its observations with your own empirical telemetry when preparing a practical submission.

Student: __________________Student ID: __________________Course: __________________Date: __________________Partner: __________________Instructor: __________________

1. Title and aim

Metropolis-Hastings Algorithm, Markov Chain Monte Carlo (MCMC), and Acceptance Dynamics. Implement the Metropolis-Hastings Markov Chain Monte Carlo (MCMC) algorithm, construct Gaussian random walk proposals, evaluate acceptance probability ratios, verify detailed balance, and quantify Monte Carlo error attenuation.

2. Abstract

Six statistical trials were executed across standardized inputs Iterations N = 10.0 to Iterations N = 320.0 for Metropolis-Hastings Algorithm, Markov Chain Monte Carlo (MCMC), and Acceptance Dynamics. An ordinary least-squares regression yielded an empirical MCMC Error Attenuation Exponent α of -0.500 (difference from theoretical reference = 0.0004%). The empirical telemetry conclusively validates the theoretical statistical law and asymptotic behavior with R² = 1.000000. The investigation demonstrates stable convergence across all observation stages with minimal residual variance. Data generated through systematic pseudo-random sampling exhibited strict conformity with theoretical density profiles, illustrating key principles of sampling variability, asymptotic normality, and unbiased estimation in empirical data analysis. The experimental design effectively mitigates numerical artifacts and validates the central mathematical assertions of the curriculum.

3. Apparatus and fixed settings

4. Theory and graph choice

The Metropolis-Hastings algorithm is the bedrock of modern Bayesian computation and computational statistical physics. By constructing an ergodic Markov chain whose stationary equilibrium matches the unnormalized posterior density, it circumvents the curse of dimensionality and the intractability of high-dimensional normalizing integrals. In this laboratory, we implement random walk Metropolis sampling, analyze acceptance probability dynamics, track burn-in trajectories, compute autocorrelation times, and confirm the universal Monte Carlo error attenuation rate α = -0.500. In mathematical statistics, empirical data science, and modern computational engineering, understanding the asymptotic sampling properties and theoretical behavior of Metropolis-Hastings Algorithm, Markov Chain Monte Carlo (MCMC), and Acceptance Dynamics provides crucial guarantees. Rigorous experimental validation connects foundational probability laws with observable empirical phenomena, ensuring that statistical inference remains valid under finite sample sizes and real-world data collection constraints.

ln(SE) = -0.5000 · ln(N) + 1.2000

The statistical relationship was linearized into the standard regression form y = mx + b. Here, the independent variable x represents Log Sample Size ln(N), and the dependent variable y represents Log Monte Carlo Standard Error ln(SE). The slope m directly extracts MCMC Error Attenuation Exponent α, while the intercept b accounts for residual baseline offsets. Linear transformation allows robust parameter estimation via ordinary least squares without non-linear solver bias. Plotting transformed observation pairs highlights distribution scale factors and rate parameters directly as slope gradients. This linear graphical formulation provides an immediate visual check of homoscedasticity, linearity, and potential outlier leverage across the experimental domain, verifying that the empirical variance matches theoretical bounds.

5. Method

  1. Set target density to standard normal p(x) ∝ e^(-x^2/2) with proposal standard deviation σ_prop = 1.0 on the MCMC interface.
  2. Initialize chain at X_0 = 5.0. Draw proposal Y ~ N(X_t, 1.0) and accept with probability α = min(1, p(Y)/p(X_t)). Record 2,000 steps.
  3. Inspect trace plot trajectory as X_t migrates from extreme start X_0 = 5.0 down into the high-density target region around 0. Discard initial 500 burn-in steps.
  4. Compute empirical acceptance rate, verifying that for Gaussian proposals σ_prop ≈ 1.0, acceptance rate aligns with optimal Roberts-Gelman efficiency (~44%).
  5. Increment MCMC sample sizes across standardized geometric steps N ∈ {10, 20, 40, 80, 160, 320}, recording empirical Monte Carlo standard error SE.
  6. Fit a linear regression model y = mx + b to coordinates (x = ln(N), y = ln(SE)). Confirm that empirical slope m = -0.5000 validates N^(-1/2) convergence.

6. Observations and calculation table

All statistical observations use strictly controlled 64-bit IEEE 754 precision buffers. Residuals are computed relative to the ordinary least-squares regression line.

Table 1. Six simulated observations; x and y represent transformed statistical metrics.
No.MCMC Sample Iteration Count N (samples)Empirical Monte Carlo Standard Error SE(θ̂) (Std Error SE)Log Sample Size ln(N)Log Monte Carlo Standard Error ln(SE)Fitted yResidual
110.01.049912.30260.04870.0487-0.0000
220.00.742452.9957-0.2978-0.29780.0000
340.00.524983.6889-0.6444-0.64440.0000
480.00.371214.3820-0.9910-0.9910-0.0000
5160.00.262475.0752-1.3376-1.3376-0.0000
6320.00.185615.7683-1.6841-1.68410.0000

Download the sample observations (CSV) ↓

7. Worked calculation for one observation

For input Iterations N = 10.0: Measured Empirical Monte Carlo Standard Error SE(θ̂) = 1.0499. Transformed coordinates: independent x = 2.3026, dependent y = 0.0487.

8. Graph, gradient and final calculation

-1.941.89-1.382.96-0.824.04-0.255.110.316.18Log Sample Size ln(N)Log Monte Carlo Standard Error ln(SE)

Circular markers represent empirical statistical observations. The solid line represents the ordinary least-squares linear fit.

x̄ = 4.0354; ȳ = -0.8177
Σ(x − x̄)² = 8.4079
Σ(x − x̄)(y − ȳ) = -4.2039
m = Σ(x − x̄)(y − ȳ) / Σ(x − x̄)² = -0.49999794
b = ȳ − mx̄ = 1.20001668
y = -0.5000 · x + 1.2000 ⟹ Target = -0.500 (theoretical = -0.500)

9. Uncertainty and comparison

Percentage difference = |estimate − theoretical value| / |theoretical value| × 100 = 0.0004%.

For n = 6 observations, Σresidual² = 3.714e-09; s² = Σresidual²/(n − 2). Gradient standard error = √[s²/Σ(x − x̄)²] = 1.051e-05. Intercept standard error = √[s²(1/n + x̄²/Σ(x − x̄)²)] = 4.420e-05.

Propagating the fit parameters yields a fit standard error of 1.051e-05 , with an ideal coefficient of determination R² = 1.000000.

In mathematical statistics, empirical uncertainty stems from finite sample variance, stochastic resampling dispersion, and numerical floating-point discretization (IEEE 754 precision). The ordinary least-squares regression across n = 6 standardized observations yields unbiased standard errors for the gradient and intercept. Because the underlying mathematical expectation follows rigorous statistical distributions, residual deviations are tightly bounded, yielding a coefficient of determination R² ≥ 0.999999 and confirming the theoretical probabilistic model. Moreover, potential sources of experimental bias—including pseudo-random generator cycle length, initial seed dependency, and boundary edge effects in discrete approximations—have been minimized through large Monte Carlo trial repetition. Standard deviations are propagated using first-order Taylor expansion approximations (delta method) where non-linear transformations are applied. The resulting confidence intervals asymptotically converge to the nominal 95% coverage rate under standard regularity conditions. Residual diagnostics demonstrate homoscedasticity across the entire observation domain without systematic bias.

10. Result and discussion

MCMC Error Attenuation Exponent α = -0.500
Theoretical reference value: -0.500

The empirical benchmark observations provide rigorous quantitative verification of Metropolis-Hastings Algorithm, Markov Chain Monte Carlo (MCMC), and Acceptance Dynamics. In mathematical statistics, data analytics, and computational probability, statistical models are characterized by their sampling distributions, estimators, and asymptotic rates. Across all six observations, the empirical slope m = -0.5000 confirms the theoretical model with near-zero residual variance. Furthermore, comparison with classical parametric and non-parametric benchmarks underscores critical principles of bias-variance trade-offs, sampling efficiency, and hypothesis test power. The empirical telemetry confirms the predictions established by statistical literature. Residual analysis reveals homoscedastic dispersion without systematic non-linear patterning, validating the underlying model assumptions. Confidence intervals calculated via asymptotic standard errors align with theoretical quantiles, indicating that finite-sample distortions remain negligible under controlled conditions. The experimental protocol confirms the robustness of the estimator against sampling fluctuations, reinforcing the theoretical foundations articulated by Devore, Ross, and Montgomery & Runger. The convergence of empirical metrics toward theoretical limits provides unambiguous confirmation of the asymptotic properties under study.

11. Precautions and limitations

Random walk Metropolis can become trapped in local modes when sampling from multi-modal distributions with deep valleys. The log-log regression of Monte Carlo standard error against sample size confirms the square-root convergence law with slope m = -0.5000 and R² = 1.000000.

12. Conclusion

This laboratory investigation quantitatively verified the mathematical formulation and sampling behavior of Metropolis-Hastings Algorithm, Markov Chain Monte Carlo (MCMC), and Acceptance Dynamics. Through rigorous tracking across six observation points, we confirmed an empirical MCMC Error Attenuation Exponent α of -0.500 matching the theoretical reference -0.500 within 0.0004% error. The investigation demonstrates why this statistical method serves as a fundamental foundation in data science and empirical inquiry. The verified convergence rates and parameter estimates demonstrate the practical efficacy of probabilistic modelling and mathematical statistics in modern scientific workflows, providing students and researchers with reliable quantitative verification tools.