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Monte Carlo Particle Transport Methods: Neutron and Photon - gnssn

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509where, according to Equation (7.62)K, K|P.OO = E k)p(kjk;) = V k)(D;) !1•(I - td«Now, for the elementary properties of the binomial distributionp 0(k;) = I, p,(k|) - k|t, = (k,_,n, + j)t,<strong>and</strong>p 2(k[) = k;V + k;t,(i - Uwhere, from Equation (7.60), we havek[ = k,_ ,n, + jInserting this expression, together with that of TR(JJk 1.,) in Equation (7.61), into Equation(A.2), the moments become = 1= S t-,(K-n + K,.,V 1)P 1. ,(K,..,) = tMK-,) (A3)ki-i<strong>and</strong>KJ _ i J = O[(k 2^n| + 2k,.Aj + f)t 2 + (k,..,n, + J)I 1(I - I 1VJP 1.,(k,.,)= 2Wi k >-i( n i + 2n,v, E v 2 ) + ^.,V 1(I - V 1)k]-i+ t,(i - ^,.,^,.,(k,.,)= t 2 a 2 (k 2 _,) + [tj(l - t,)a, + tfv,(l - V 1)Kk 1.,) (A.4)REFERENCES1. Bending, R. C, Direction dependent exponential biassing, in Proc. NEACRP Meeting of a <strong>Monte</strong> <strong>Carlo</strong>Study Group, ANL-75-2 Report, Argonne National Laboratory, 1974, 295.2. Booth, T. E., Automatic importance estimation in forward <strong>Monte</strong> <strong>Carlo</strong>, Trans. Am. Nucl. Soc., 41, 308,1982.3. Booth, T. E. <strong>and</strong> Hendricks, J. S., Deep penetration by <strong>Monte</strong> <strong>Carlo</strong>, Trans. Am. Nucl. Soc. 43, 609,1982.4. Booth, T. E. <strong>and</strong> Hendricks, J. S., Importance estimation in forward <strong>Monte</strong> <strong>Carlo</strong> calculations, Nucl.Technol. Fusion, 5, 90, 1984.5. Burgart, C. E. <strong>and</strong> Stevens, P. N., A general method of importance sampling the angle of scattering in<strong>Monte</strong> <strong>Carlo</strong> calculations, Nucl. Sci. Eng.. 42, 306, 1970.

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