CROSS-REF in .NET

Integrated Data Matrix 2d barcode in .NET CROSS-REF

For the TRX signalling, estimation of the total signalling load per TRX can be performed. In case of using A-bis pool, dimensioning of the A-bis pool size for a required maximum

246. J. L. Wardell, in Comprehensive Organometallic Chemistry, Vol. 1, G. Wilkinson, F. G. A. Stone, and E. W. Abel, eds., Pergamon Press, Oxford, 1982, 2, p. 54. 247. J. L. Wardell, in The Chemistry of the Metal-Carbon Bond, Vol. 4, F. R. Hartley, ed., Wiley, Chichester, 1987, 1, p. 27. 248. W. E. Lindsell, in Comprehensive Organometallic Chemistry, Vol. 1, G. Wilkinson, F. G. A. Stone, and E. W. Abel, eds., Pergamon Press, Oxford, 1982, 4, p. 163. 249. L. Lochmann, J. Pospisil, and D. Lim, Tetrahedron Lett. 257 (1966). 250. M. Schlosser, J. Organomet. Chem. 8, 9 (1967). 251. M. Schlosser, Pure Appl. Chem. 60, 1627 (1988). 252. A. Mordini, Adv. Carbanion Chem. 1, 1 (1992). 253. J. Hartmann and M. Schlosser, Helv. Chim. Acta 59, 453 (1976). 254. M. Schlosser, Angew. Chem., Int. Ed. Engl. 13, 701 (1974). 255. M. Schlosser and J. Hartmann, J. Am. Chem. Soc. 98,4674 (1976). 256. M. Schlosser, J. Hartmann, and V. David, Helv. Chim. Acta 57, 1567 (1974). 257. P. A. A. Klusener, H. H. Hommes, H. D. Verkruijsse, and L. Brandsma, J. Chem. Soc., Chem. Commun. 1677 (1985). 258. P. A. A. Klusener, W. Kulik, and L. Brandsma, J. Org. Chem. 52,5261 (1987). 259. G. B. Trimitsis, A. Tuncay, R. D. Beyer, and K. J. Ketterman, J. Org. Chem. 38, 1491 (1973). 260. V. R. Sandel and H. H. Freedman, J. Am. Chem. Soc. 85, 2328 (1963). 261. R. B. Bates and C. A. Ogle, J. Org. Chem. 47, 3949 (1982). 262. C. D. Broaddus, J. Org. Chem. 29, 2689 (1964). 263. M. Schlosser and S. Strunk, Tetrahedron Lett. 25, 741 (1984). 264. H. Hommes, H. D. Verkruijsse, and L. Brandsma, J. Chem. Soc., Chem. Commun. 366 (1981). 265. L. Brandsma, H. Hommes, H. D. Verkruijsse, and R. L. P. de Jong, Reel. Trav. Chim. Pays-Bas 104,226 (1985). 266. D. A. Ben-Efraim, in The Chemistry of the Carbon-Carbon Triple Bond, S. Patai, ed., Wiley, Chichester, 1978, 18, p. 790. 267. A. J. Quillinan and F. Scheinmann, Org. Synth., Coli. Vol. 6, 595 (1988). 268. S. Bhanu and F. Scheinmann, J. Chem. Soc., Perkin Trans. 1 1218 (1979). 269. T. Koerts, P. A. Leclercq, and R. A. van Santen, J. Am. Chem. Soc. 114, 7272 (1992). 270. A. M. Browstein, in Catalysis of Organic Recations, W. R. Moser, ed., Marcel Dekker, New York, 1981, p. 3. 271. H. Itoh, T. Hattori, K. Suzuki, and Y. Murakami, J. Catal. 79, 21 (1983). 272. Yu. N. Sidorenko, P. N. Galich, V. S. Gutyrya, V. G. I1'in, and 1. E. Neimark, Dokl. Akad. Nauk, SSSR 173, 132 (1967). 273. T. Yashima, K. Sato, T. Hayasaka, and N. Hara, J. Catal. 26, 303 (1972). 274. M. D. Sefcik, J. Am. Chem. Soc. 101,2164 (1979). 275. M. L. Unland and G. E. Barker, in Catalysis of Organic Recations, W. R. Moser, ed., Marcel Dekker, New York, 1981, p. 51. 276. C. Yang and Z. Meng, Appl. Catal. 71, 45 (1991). 277. R. E. Payne, Petrol. Refiner 37(9),316 (1958).

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A number x is smooth relative to a bound N if the prime factorization of x pn1 pn2. . . pns 1 2 s involves only prime numbers satisfying pi N. Proposition 14.2 (Adelman s Algorithm for the Discrete Logarithm Problem): Given: p a prime, q a primitive root of p, and x q k (modulo p), A bound N( p) and primes p1 , p2 , , pm N( p); Find: k. S1. Find an integer R by random sampling such that B is smooth relative to N( p) B (n1 , n2 , . . . , nm ) B xR (modulo p) pn1 pn2 . . . pnm m 1 2 1 gcd{R, p 1} S2. Find integers Ri for 1 N( p). and the vectors i m by random sampling such that Ai is smooth relative to

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number of fermion operator permutations has been required, in which case it is -1. By virtue of the discussion in 53.3, a n operator product is in normal order if in a Fourier decomposition its positive-frequency parts stand to the right of its negative-frequency parts. From the definitions of the time-ordered and normal products we also have the properties

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Equation (1.1) needs to be adapted differently if more complicated arrangements of charges are involved, for instance if a xed dipole and a monopole are allowed to interact in a vacuum separated by a distance r. We usually de ne a dipole as two opposite point charges, for instance q1 and q1 , separated by a distance l (Figure 1.96). In this case the electrostatic in uence of the dipole is described in terms of a dipole moment: 1 = q 1l (1.3)