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Library of Congress Cataloging-in-P
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III. Statistical Considerations •
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IV. Further Generalizations — 183
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Appendix 6A:Unbiased Estimation of
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2 Monte Carlo Particle Transport Me
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Chapter 2INTRODUCTIONWhen we starte
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thus,As it is proved" — and is so
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9B. THE PROBABILITY MIXING METHODTh
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11It is easy to prove 15by summing
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13but the most probable values:x, =
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ISand give a random sign (by the us
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441Chapter 7OPTIMIZATION OF EFFICIE
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443estimated be the number of parti
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445and on the optical thickness X.
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447The variance of the escape rate
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449In view of Equation (7.15) and (
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451The solution of this equation go
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453formation can be chosen asb(x) =
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455or, equivalently, the stretched
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457andH(x,y) = y/(l + xy)The qualit
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459is w 2w,/n, and the expected sco
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461.where the parameter b is for th
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463An easy-to-use direct statistica
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465with a probabilityTR(JIk 1-,) =
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46?moment of the score isM 2= Mf[I
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469fact, the number of fragments ar
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471As for the first question, let u
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473of Equations (7.82) and (7.83) a
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475In the equation above we have in
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479importance function. Accordingly
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481- ---!'M + (I - i) - M + (i)l +
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mi-11.5A 3.- QUALJTY FACTOR INLEAKA
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487due to a starter in a region is
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489of the directional dependence 41
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49!whereT(P,P') = j dto-sr 4 to,R)t
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493both sides of the equality byT(P
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495Comparing this kernel to the tra
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497expected score is put into the f
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499The constant A follows from the
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SOlform isQ(x,|x,E)8(x)Q E(E)1 cx(x
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