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Note that (X X)(X X )T is a real Lt Lt matrix whose ij th element is the correlation of the i th and the complex conjugate of the j th rows of the symbol error matrix X X. Thus, if the rows of X X are orthogonal (as can be the case for certain error paths in the trellis), then (X X)(X X ) T will be an Lt Lt diagonal matrix and the matrix ILt Lt s(X X)(X X ) T { s /[2 (1 + K)]} will likewise be diagonal with elements 1 s s 2 (1 + K)

Resnick, R., D. Halliday, and K. S. Krane. Physics, 4th ed., Wiley, New York, 1992. Meyerhof, W. E. Elements of Nuclear Physics, McGraw-Hill, New York, 1967. Myers, W. D. and W. J. Swiatecki. Nucl. Phys. 81, 1 (1966).

They can also be set for a particular processing run to provide special handling for certain data..

xR 2 (1, ) = 0

4-20 1 &40

Message queues are not necessarily accessed in FIFO data structures. System V UNIXstyle message queues are, but POSIX message queues enable readers to pull messages out of a queue in an arbitrary order.

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These nancial statements generally must conform to the rules set by the FASB. The SEC generally defers to industry rule-making bodies but nevertheless imposes additional requirements. The AICPA also promulgates rules de ning acceptable disclosure. These rules, along with custom and practice, de ne generally accepted accounting principles. Auditors check statements prior to publication and certify compliance with GAAP. Outside of the United States, the most widely recognized standard for accounting procedures is the International Financial Reporting Standards (IFRS) promulgated by the International Accounting Standards Board (IASB). Global accounting standards have become more consistent in recent years.

2 2 2 2 1 2 Y1 Y2 + (1 ) Y1 Y2 Y1 + Y2 sin d 2 2 2 2 Y1 + 2 Y1 Y2 sin + Y2 Y1 + 2 Y1 Y2 sin + Y2 The complement of the region just considered is where Y2 > Y1 or equivalently Y2 > Y1 . Here, however, we can have either Y2 > Y1 or Y1 < Y2 < Y1 . Thus, two separate subcases must be considered. For the rst subcase where Y2 > Y1 , we would certainly also have Y2 > Y1 , and thus for both Marcum Q-function terms in (6.5), the second argument is greater than the rst argument. Thus, substituting Eq. (4.42) in both of these terms, we obtain after much simpli 2 cation the identical result of (6.6) except that the second term, namely, exp Y2 , 2 now becomes exp Y1 . Finally, for the second subcase where Y1 < Y2 < Y1 , 2 once again (6.6) is appropriate with, however, the second term, exp Y2 , now 2 2 replaced by exp Y1 + exp Y2 . What remains is to evaluate the bivariate Rayleigh CDF at the endpoints between the regions where one must make use of the relation in (4.40). When this is done, the following results are obtained for the second term in (6.6). When Y2 = Y1 , use 1 2 2 2 2 Y2 , use 1 exp Y2 + exp Y2 . 2 exp Y1 + exp Y1 , and when Y1 = 2 Summarizing, the bivariate Rayleigh can be expressed in the form of a single integral with nite limits and an integrand composed of elementary functions as follows: PR1 ,R2 (r1 ,

(9.89)

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