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Dc level in white guassian noise

Suppose we observe an unknown amplitude in white Gaussian noise with unknown variance: x n A w n n 0 1 N 1 , where w n 0 2 are independent and identically distributed. We would like to estimate A 2 by computing the MLE. Differentiating the log-likelihood gives A p x 1 2 n 1 N x n A 2 p x N 2 1 2 4 n 1 N x n A 2 Equating with zero and solving gives us our MLEs: A 1 N n 1 N x n and 2 1 N n 1 N x n A 2

2 is biased!

As an exercise, try the following problem:

Suppose we observe a random sample x x 1 x N of Poisson measurements with intensity : x i n n n , n 0 1 2 . Find the MLE for .

Unfortunately, this approach is only feasible for the most elementarypdfs and pmfs. In general, we may have to resort to more advanced numerical maximization techniques:
  • Newton-Raphson iteration
  • Iteration by the Scoring Method
  • Expectation-Maximization Algorithm
All of these are iterative techniques which posit some initial guess at the MLE, and then incrementally update thatguess. The iteration procedes until a local maximum of the likelihood is attained, although in the case of the first twomethods, such convergence is not guaranteed. The EM algorithm has the advantage that the likelihood is always increased ateach iteration, and so convergence to at least a local maximum is guaranteed (assuming a bounded likelihood). For eachalgorithm, the final estimate is highly dependent on the initial guess, and so it is customary to try several differentstarting values. For details on these algorithms, see Kay, Vol. I .

Asymptotic properties of the mle

Let x x 1 x N denote an IID sample of size N , and each sample is distributed according to p x . Let N denote the MLE based on a sample x .

Asymptotic properties of mle

If the likelihood x p x satisfies certain "regularity" conditions

The regularity conditions are essentially the same as those assumed for the Cramer-Rao lower bound : the log-likelihood must be twice differentiable, and theexpected value of the first derivative of the log-likelihood must be zero.
, then the MLE N is consistent , and moreover, N converges in probability to , where I where I is the Fisher Information matrix evaluated at the true value of .

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.

The mle and efficiency

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 I 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 p x I for all and x . Since is assumed to be efficient, this equation holds, and in particular it holds when x . But then the derivative of the log-likelihood is zero at x . 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.

Optimality of mle for linear statistical model

If the observed data x are described by x H w where H is N p with full rank, is p 1 , and w 0 C , then the MLE of is H C H H C x 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 x H C x H with respect to . Since C is positive definite, we can write C U U D D , where D 1 2 U , where U is an orthogonal matrix whose columns are eigenvectors of C , and is a diagonal matrix with positive diagonal entries. Thus, we must minimize D x D H D x D H But this is a linear least squares problem, so the solution is given by the pseudoinverse of D H :

D H D H D H D x H C H H C x

Consider X 1 , , X N s 2 I , where s is a p 1 unknown signal, and 2 is known. Express the data in the linear model and find the MLE s for the signal.

Invariance of mle

Suppose we wish to estimate the function w W and not itself. To use the maximum likelihood approach for estimating w , we need an expression for the likelihood x w p w x . In other words, we would need to be able to parameterize thedistribution of the data by w . If W is not a one-to-one function, however, this may not be possible. Therefore, we define the induced likelihood x w W w x The MLE w is defined to be the value of w that maximizes the induced likelihood. With this definition, the following invarianceprinciple is immediate.

Let denote the MLE of . Then w W is the MLE of w W .

The proof follows directly from the definitions of and w . As an exercise, work through the logical steps of the proof on your own.

Let x x 1 x N where x i Poisson Given x , find the MLE of the probability that x Poisson exceeds the mean .

W x n 1 n n where z largest integer z . The MLE of w is w n 1 n n where is the MLE of : 1 N n 1 N x n

Be aware that the MLE of a transformed parameter does not necessarily satisfy the asymptotic properties discussed earlier.

Consider observations x 1 ,, x N , where x i is a p -dimensional vector of the form x i s w i where s is an unknown signal and w i are independent realizations of white Gaussian noise: w i 0 2 I p p Find the maximum likelihood estimate of the energy E s s of the unknown signal.

Summary of mle

The likelihood principle states that information broughtby an observation x about is entirely contained in the likelihood function p x . 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:

  • It is consistent and asymptotically efficient (as N we are doing as well as MVUE).
  • When an efficient estimator exists, it is the MLE.
  • The MLE is invariant to reparameterization.

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Source:  OpenStax, Statistical signal processing. OpenStax CNX. Jun 14, 2004 Download for free at http://cnx.org/content/col10232/1.1
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