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6. Sufficiency, Completeness, and Ancillarity  301

                           situations separately. The notion of the information about an unknown param-
                           eter θ contained in the data was introduced by F. Y. Edgeworth in a series of
                           papers, published in the J. Roy. Statist. Soc., during 1908-1909. Fisher (1922)
                           articulated the systematic development of this concept. The reader is referred
                           to Efron’s (1998, p.101) recent commentaries on (Fisher) information.

                           6.4.1   One-parameter Situation
                           Suppose that X is an observable real valued random variable with the pmf or
                           pdf f (x; θ) where the unknown parameter θ ∈ Θ, an open subinterval of ℜ,
                           while the χ space is assumed not to depend upon θ. We assume throughout
                           that the partial derivative    (x; θ) is finite for all x ∈ χ, θ ∈ Θ. We also
                           assume that we can interchange the derivative (with respect to θ) and the
                           integral (with respect to x).
                              Definition 6.4.1 The Fisher information or simply the information about
                           θ, contained in the data, is given by




                              Example 6.4.1 Let X be Poisson(λ), λ > 0. Now,




                           which implies that                     . Thus, we have





                           since E [(X – λ) ] = V(X) = λ. That is, as we contemplate having larger and
                                         2
                                 λ
                           larger values of λ, the variability built in X increases, and hence it seems
                           natural that the information about the unknown parameter λ contained in the
                           data X will go down further and further.
                              Example 6.4.2 Let X be N(µ, σ ) where µ ∈ (–∞, ∞) is the unknown pa-
                                                         2
                           rameter. Here, σ ∈ (0, ∞) is assumed known. Now,




                           which implies that                     . Thus we have
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