Put . The log-likelihood for the Laplace distribution is
For the derivative is positive for and negative for , so the unique maximum-likelihood estimator is
The exceptional data set has probability zero; there the likelihood has its supremum at the excluded boundary . For the Fisher information, has exponential density for , hence mean . Since ,
This also follows from the score variance, because .
The absolute observations are independent exponential random variables with mean and variance . Applying the central limit theorem directly to their average proves
Thus the large-sample approximation is , consistent with inverse Fisher information. Also in probability by the weak law of large numbers, so in the standard error can be replaced by through Slutsky's theorem.
Let , where . By the preceding asymptotic normality and Slutsky's theorem, is approximately standard normal. Inverting gives the Wald confidence interval
Its coverage approaches as . The interpretation of the confidence interval is repeated-sample coverage of the fixed parameter; it does not assign a posterior probability to .
Let . The Bernoulli distribution likelihood is proportional to . Multiplication by the beta distribution prior gives
Normalizing with the beta function therefore gives
The parameters remain positive. This is Beta-binomial conjugacy: successes add to the first shape parameter and failures to the second.
A credible set is a measurable subset with posterior probability :
In ordinary language, given the observed data and the chosen prior model, the probability that the parameter lies in this set is . Such a set need not be an interval or be unique; its defining requirement is posterior mass.
Let denote the distribution function of the posterior beta distribution, with and . This distribution is continuous with positive density on . Its equal-tailed credible interval is
Compute the two quantiles by solving and . Each excluded tail has mass , leaving posterior mass between the endpoints.
The further observation is independent of the earlier observations conditional on . Integrate its conditional success probability against the posterior:
The given factorial formula for the beta function gives this ratio as . Thus the posterior predictive probability is
It is the posterior mean of the Bernoulli success parameter. Independence here is conditional: sharing the uncertain parameter generally makes past and future observations dependent before conditioning on it.

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