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27 Apr 2006: As a result of the crystalli- zation and different fluid dynamical processes op- erating in each of the described experiments, the concentration of the input fluid is considerably reduced before it

20 Nov 2006: indirect op-tical transitionssX point phonons in cubic BNd, "vd is theenergy of the direct band gap, and"vl the laser energy. ... III. The peak at 2940 cm1 slabeled overb. in Fig. 4d is asso-ciated with the overbending of the in-plane longitudinal

19 Apr 2006: "! $#&%(')! ,.-/%103246587797: 0<;=>&?%/3#60A@ B4%)CD0CEGFHI6KJ&0ML80ONPRQ8%S 4T0. UWVYXOZ [MV6]AXV_ba c&dfehgjiZ k.l<]m.XOV$c=nPo$Zpp.V6qUhal VC]rsZ qoftuvxw=y"z. {}|x|C) 9(A6Wf69O6AR.E&RAAA9E9 //.¡¢E£¤E(¥ª«¢¥ª<E4OP/GK=. |Y|&µEºA)»|&{f|

21 Nov 2006: In these situations, an op-timal hyperplane is found to minimise the probabilityof error, averaged over the training set.

14 Sep 2006: Now the problem of finding an op-timal replacement of pixels in patch p′ from those in patch m′ is equivalent to finding apath in the graph such that the error

12 Oct 2006: 20. 0 120 1. 2 h0 1 2 h0 1. – –––. – –. KO. PS. -2/K. OP. S-0. Time (h). 5′3′ 5′.

4 Dec 2006: op--o. --. rg. 1 A. M. Liu and M. L. Cohen, Science24, 841 1989!; Phys.

19 Apr 2006: 4.2. Modelingg the SED. The spectral energy distribution (SED) of Corvi from op-tical to submillimeter wavelengths is plotted in Figure 4.

19 Mar 2006: The optimal. values were found to be2.3 and6.2 for visual data; the op-timal filter for thermal data was found to be alow-passfilterwith W2 = 2.8 (i.e.

22 Nov 2006: Theseallow high-dimensional kernel feature-spaces to be de-fined and calculated using only simple transducer op-erations on discrete sequences (or lattices) of observa-tions.