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When we know the density of , the likelihood function can be expressed as p r i r p r i r p and the likelihood ratio in the random parameter case becomes r p r i r p p r i r p Unfortunately, there are many examples where either the integrals involved are intractable or the sufficient statisticis virtually the same as the likelihood ratio, which can be difficult to compute.

A simple, but interesting, example that results in a computable answer occurs when the mean of Gaussian randomvariables is either zero (model 0) or is m with equal probability (hypothesis 1). The second hypothesis means that a non-zero mean is present, but its sign is notknown. We are therefore stating that if hypothesis one is in fact valid, the mean has fixed sign for each observation -what is random is its a priori value. As before, L statistically independent observations are made. 0 : r 0 2 I 1 : r m 2 I m m m 1 2 m m 1 2 The numerator of the likelihood ratio is the sum of two Gaussian densities weighted by 1 2 (the a priori probability values), one having a positive mean, the other negative. The likelihood ratio,after simple cancellation of common terms, becomes r 1 2 2 m l 0 L 1 r l L m 2 2 2 1 2 -2 m l 0 L 1 r l L m 2 2 2 and the decision rule takes the form m 2 l 0 L 1 r l 0 1 L m 2 2 2 where x is the hyperbolic cosine given simply as x x 2 . As this quantity is an even function, the sign of its argument has no effect on the result. The decision rulecan be written more simply as l 0 L 1 r l 0 1 2 m L m 2 2 2 The sufficient statistic equals the magnitude of the sum of the observations in this case. While the right side of this expression, whichequals , is complicated, it need only be computed once. Calculation of the performanceprobabilities can be complicated; in this case, the false-alarm probability is easy to find and the others moredifficult.

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Source:  OpenStax, Signal and information processing for sonar. OpenStax CNX. Dec 04, 2007 Download for free at http://cnx.org/content/col10422/1.5
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