Exact(1)
For the cases (iv - vi) iv - vie 2, the quantine funcTableQ X (u) is in closed form, so the n th moment of the random variable X may be obtained from ( {E}_Xleft[{X}^nright]={int}_0^1{left[{Q}_X(u)right]}^n du. ) The following Theorem 3 derives an approximation for computing the n th moment of a member, Uniform-R{GL} of case (i).
Similar(59)
In this paper we present a new approximation for computing lower bound for the fixed charge transportation problem (FCTP).
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In order to avoid the computational complexity associated with the BCJR algorithm (or the max-log MAP or SOMA approximations), we consider two reduced-complexity approximations for computing the APPs.
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