We'll use a few pictures to compare these two methods, specifically in learning about the variance hyperparameter tau. Here's the exact MCMC method:
1. We write a function defining the log posterior of mu and log tau.
2. We simulate from (mu, log tau) using the function rwmetrop.R in the LearnBayes package. We choose a suitable proposal function from output from the laplace.R function. The acceptance rate of this random walk algorithm is 20%. We sample for 10,000 iterations, saving the draws of log tau in a vector.
We then run the Gibbs sampler for 10,000 iterations, also saving the draws of log tau.
DENSITY PLOTS. We first compare density estimates of the simulated samples of log tau using the two methods. The two estimates seem pretty similar. The density estimate for the Gibbs sampling draws looks smoother, but that doesn't mean this sample is a better estimate of the posterior of log tau.
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TRACE PLOTS. We compare trace plots of the two sets of simulated draws. They look pretty similar, but there are differences in closer inspection. The draws from the Gibbs sampling run look more irregular, or perhaps they have more of a "snake-like" appearance.
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AUTOCORRELATION PLOTS. A autocorrelation plot is a graph of the autocorrelations
corr (theta(j), theta(j-g))
graphed against the lag g. For most MCMC runs, the values of the stream of simulated draws will show positive autocorrelation, but hopefully the autocorrelation values decrease quickly as the lag increases. It is pretty obvious that the lag autocorrelation values drop off slower for method 2 (Gibbs sampling); in contrast, the lag autocorrelations decrease to zero for method 1 (Exact MCMC) for values of the lag from 1 to 15.
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