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A fast and accurate method for evaluating joint second-order PMD ...

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FORESTIERI: A FAST AND ACCURATE METHOD FOR EVALUATING JOINT SECOND-ORDER <strong>PMD</strong> STATISTICS 2949<br />

Evaluation of the inner integral in (10) is the most<br />

critical, as it is to be evaluated with very high accuracy <strong>for</strong> the<br />

tails of the <strong>joint</strong> pdf, <strong>and</strong> we had to use a value <strong>for</strong> accuracy<br />

as small as in the numerical integration <strong>method</strong> described<br />

at the end of Section II to obtain reliable values down to<br />

. We also noticed that the higher the accuracy in <strong>evaluating</strong><br />

, the lesser the number of times that step size<br />

in (33) is to be halved to achieve a given number of reliable<br />

digits <strong>for</strong> the <strong>joint</strong> pdf. The very high accuracy needed <strong>for</strong><br />

is easily <strong>and</strong> efficiently achieved through the expansions<br />

reported in Sections II–IV. Until a closed-<strong>for</strong>m expression<br />

is not available, a <strong>fast</strong> <strong>and</strong> <strong>accurate</strong> <strong>method</strong> <strong>for</strong> <strong>evaluating</strong> the<br />

<strong>joint</strong> <strong>second</strong>-<strong>order</strong> <strong>PMD</strong> statistics is a prerequisite <strong>for</strong> a full analytical<br />

evaluation of the <strong>PMD</strong> impact on the per<strong>for</strong>mance of<br />

compensated systems <strong>and</strong> may also be a useful tool <strong>for</strong> validating<br />

IS techniques (see Appendix C).<br />

APPENDIX A<br />

In this appendix, we show the derivation of (9), (11), <strong>and</strong> (22)<br />

mentioned in the paper. The exact expression <strong>for</strong><br />

can be obtained by direct antitrans<strong>for</strong>mation of (7) as<br />

(A1)<br />

where is as in (8). Changing to spherical polar coordinates<br />

yields<br />

(A2)<br />

<strong>and</strong> the integral with respect to is easily per<strong>for</strong>med, yielding<br />

(A3)<br />

From (A3), we obtain the <strong>joint</strong> pdf of <strong>and</strong><br />

as<br />

(A4)<br />

from which, by the change of variable <strong>and</strong> after some<br />

algebra, we obtain (9).<br />

By using the expansion , the integral<br />

in (10) can be evaluated as<br />

Letting <strong>and</strong> as in (12), we start from [20, eq. 6.677.6]<br />

<strong>and</strong>, by repeated differentiation with respect to , obtain<br />

(A5)<br />

(A6)<br />

(A7)<br />

which, substituted in (A5), gives (11).<br />

Thus, we simply need an explicit expression <strong>for</strong> the<br />

right-h<strong>and</strong>-side term in (A7). To obtain it, we use the rule<br />

<strong>for</strong> the th derivative of a composite function. Letting<br />

(such that ), if<br />

, then [20]<br />

where<br />

(A8)<br />

(A9)<br />

Given , where<br />

, , we apply the previous rule<br />

to obtain the th derivative of as<br />

where<br />

By using the <strong>for</strong>mula [20]<br />

(A10)<br />

(A11)<br />

(A12)<br />

where denotes the Pochhammer’s symbol, defined as [21]<br />

(A13)

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