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22 Nov 2006: HMM ML – 29.4 27.3C-Aug ML CML 24.2 –. HMM MMI – 25.3 24.8C-Aug MMI CML 23.4 –. Table 2. Classification error on the TIMIT core test ... A point of particular interest is that despite poorer statesegmentation—the sufficient statistics fix the

26 Apr 2006: 1.0 [24]. The slope of the linethrough data set (h), for silicon carbide particles in a succino-nitrile melt, is! ... Azouni, W. Kalita, M. Yemmou, J. Crystal Growth. 99 (1990) 201.[24] S.

16 Jun 2006: Science (Wash. DC). 208:1454-1457. 24. Ross, M. J., M. W. Klymkowsky, D. ... J. Ultrastruct. R e s 24:454-564. 27. Ziogsheim, H.-P., D.-C. Neugehauer, F.

23 Jul 2006: MP3. 44100 Hz. 123.64 MB. Date: July 24, 2006. Speakers: Revd Michael Roberts.

14 Jun 2006: Mentalizing X 3 53 24 M 5.29. Harrington, D. L., et al. ... 2004). Journal of Neuroscience, 24, 3917–3925 Episodic Retrieval 35 60 14 L 4.25.

21 Dec 2006: q 26%). b, X-ray rapper ensemble (q 24%). c, The published NMR ensemble(q 14%). ... Biochemistry 24, 3831–3841 (1984). 27. Best, R. B., Clarke, J. & Karplus, M.

26 Apr 2006: Using equations (3) and (22)–(24), it is possibleto calculate _h, S0 and T0 in terms of far-field properties T1and S1 by eliminating two of the unknowns to obtain aquadratic ... For this simula-tion we used again the values given in Table 1 and Si =

15 Sep 2006: There is also. [Journal of Petrologf, Vol. 29, P t n 3, pp 599-«24, 1988] Oxford Umvcroty Prcu 19S8. ... FJH,. (24). We determined numerical solutions of (15)—(18) in addition to either (19)—(23) or merely (24).The differences were negligible.

30 May 2006: r 2 ) ( r < 1) 2.94 0.93 1.27 1.00 {(‘i ( r > 1 ). - I Cylindrical Gaussian e-T2 ( f < 00) 3.13 1-12 2.24 0.86. ... If h,R-l > Fmin (2.24) t It is interesting to compare these values with the relationship h0R-l = 2 deduced by.

5 May 2006: We areinterested in cases with small C2H because otherwise the distance of propagation issmall, see (3.24), and no real gravity current appears. ... Using the approximations (3.19)–(3.24), we find: (i) for S < 1.