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Suppose we observe an unknown amplitude in white Gaussian noise with unknown variance: , where are independent and identically distributed. We would like to estimate by computing the MLE. Differentiating the log-likelihood gives Equating with zero and solving gives us our MLEs: and
As an exercise, try the following problem:
Suppose we observe a random sample of Poisson measurements with intensity : , . Find the MLE for .
Let denote an IID sample of size , and each sample is distributed according to . Let denote the MLE based on a sample .
If the likelihood satisfies certain "regularity" conditions
Since the mean of the MLE tends to the true parameter value, we say the MLE is asymptotically unbiased . Since the covariance tends to the inverse Fisher information matrix, we saythe MLE is asymptotically efficient .
In general, the rate at which the mean-squared error converges to zero is not known. It is possible that for small samplesizes, some other estimator may have a smaller MSE.The proof of consistency is an application of the weak law of largenumbers. Derivation of the asymptotic distribution relies on the central limit theorem. The theorem is also true in moregeneral settings (e.g., dependent samples). See, Kay, Vol. I, Ch. 7 for further discussion.
In some cases, the MLE is efficient, not just asymptotically efficient. In fact, when an efficient estimator exists, itmust be the MLE, as described by the following result:
If is an efficient estimator, and the Fisher information matrix is positive definite for all , then maximizes the likelihood.
Recall the is efficient (meaning it is unbiased and achieves the Cramer-Rao lower bound) if and only if for all and . Since is assumed to be efficient, this equation holds, and in particular it holds when . But then the derivative of the log-likelihood is zero at . Thus, is a critical point of the likelihood. Since the Fisher information matrix, which is the negative ofthe matrix of second order derivatives of the log-likelihood, is positive definite, must be a maximum of the likelihood.
An important case where this happens is described in the following subsection.
If the observed data are described by where is with full rank, is , and , then the MLE of is This can be established in two ways. The first is to compute the CRLB for . It turns out that the condition for equality in the bound is satisfied, and can be read off from that condition.
The second way is to maximize the likelihood directly. Equivalently, we must minimize with respect to . Since is positive definite, we can write , where , where is an orthogonal matrix whose columns are eigenvectors of , and is a diagonal matrix with positive diagonal entries. Thus, we must minimize But this is a linear least squares problem, so the solution is given by the pseudoinverse of :
Consider , where is a unknown signal, and is known. Express the data in the linear model and find the MLE for the signal.
Suppose we wish to estimate the function and not itself. To use the maximum likelihood approach for estimating , we need an expression for the likelihood . In other words, we would need to be able to parameterize thedistribution of the data by . If is not a one-to-one function, however, this may not be possible. Therefore, we define the induced likelihood The MLE is defined to be the value of that maximizes the induced likelihood. With this definition, the following invarianceprinciple is immediate.
Let denote the MLE of . Then is the MLE of .
The proof follows directly from the definitions of and . As an exercise, work through the logical steps of the proof on your own.
Let where Given , find the MLE of the probability that exceeds the mean .
where . The MLE of is where is the MLE of :
Be aware that the MLE of a transformed parameter does not necessarily satisfy the asymptotic properties discussed earlier.
Consider observations ,, , where is a -dimensional vector of the form where is an unknown signal and are independent realizations of white Gaussian noise: Find the maximum likelihood estimate of the energy of the unknown signal.
The likelihood principle states that information broughtby an observation about is entirely contained in the likelihood function . The maximum likelihood estimator is one effective implementation of the likelihood principle. In some cases, the MLE can be computedexactly, using calculus and linear algebra, but at other times iterative numerical algorithms are needed. The MLE has severaldesireable properties:
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