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Mathematical Methods for Physics and Engineering - Matematica.NET

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31.4 SOME BASIC ESTIMATORSwhere s 4 is given bys 4 =[ ∑i x2 iN( ∑− i x ) ] 2 2iN= (∑ i x2 i )2− 2 (∑ i x2 i )(∑ i x i) 2+ (∑ i x i) 4. (31.45)N 2 N 3 N 4We will consider in turn each of the three terms on the RHS. In the first term, the sum( ∑ i x2 i )2 can be written as( ) 2∑x 2 i = ∑ x 4 i + ∑ x 2 i x 2 j ,iii,jj≠iwhere the first sum contains N terms <strong>and</strong> the second contains N(N − 1) terms. Since thesample elements x i <strong>and</strong> x j are assumed independent, we have E[x 2 i x2 j ]=E[x2 i ]E[x2 j ]=µ2 2 ,<strong>and</strong> so⎡( ) ⎤ 2∑E ⎣ x 2 ⎦i = Nµ 4 + N(N − 1)µ 2 2.iTurning to the second term on the RHS of (31.45),( )( ) 2∑ ∑x 2 i x i = ∑ x 4 i + ∑ x 3 i x j + ∑ x 2 i x 2 j + ∑ x 2 i x j x k .iiii,ji,ji,j,kj≠ij≠ik≠j≠iSince the mean of the population has been assumed to equal zero, the expectation valuesof the second <strong>and</strong> fourth sums on the RHS vanish. The first <strong>and</strong> third sums contain N<strong>and</strong> N(N − 1) terms respectively, <strong>and</strong> so⎡( )( ) ⎤ 2∑ ∑E ⎣ x 2 i x i⎦ = Nµ 4 + N(N − 1)µ 2 2.iiFinally, we consider the third term on the RHS of (31.45), <strong>and</strong> write( ) 4∑x i = ∑ x 4 i + ∑ x 3 i x j + ∑ x 2 i x 2 j + ∑ x 2 i x j x k + ∑ x i x j x k x l .iii,ji,ji,j,ki,j,k,lj≠ij≠ik≠j≠il≠k≠j≠iThe expectation values of the second, fourth <strong>and</strong> fifth sums are zero, <strong>and</strong> the first <strong>and</strong> thirdsums contain N <strong>and</strong> 3N(N − 1) terms respectively (<strong>for</strong> the third sum, there are N(N − 1)/2ways of choosing i <strong>and</strong> j, <strong>and</strong> the multinomial coefficient of x 2 i x 2 j is 4!/(2!2!) = 6). Thus⎡( ) ⎤ 4∑E ⎣ x i⎦ = Nµ 4 +3N(N − 1)µ 2 2.iCollecting together terms, we there<strong>for</strong>e obtainE[s 4 (N − 1)2]= µN 3 4 + (N − 1)(N2 − 2N +3)µ 2N2, (31.46)3which, together with the result (31.43), may be substituted into (31.44) to obtain finallyV [s 2 (N − 1)2 (N − 1)(N − 3)]= µN 3 4 − µ 2N 3 2= N − 1 [(N − 1)νN 3 4 − (N − 3)ν2], 2 (31.47)1247

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