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9 Aug 2005: $#%#&"'$#%"()!#%" #% ,. 15 20 25 30 35 40 45 50 55 6025. ... 20. 15. 10. 5. 0. 5. 10Initial projection step. first eigenvector depending on τ.

21 Sep 2005: 2,. 20. 6 Estimation of trend and seasonality. 6.1 Moving averages. Consider a decomposition into trend, seasonal, cyclic and residual components. ... 20 by fitting a regression line, Xt = β̂0 β̂1t, to the first few points of the.

27 Sep 2005: WHITEGenre and Period: Nerval. (20 Oct.). 4. DR A. MARTINGenre and Period: Diderot.

30 Sep 2005: 2.5.1 Constructing the Solutions 20. 2.6 What Became of Instantons 22. ... d. dx6 iA6 i(Xi ri)σi (2.51). – 20 –. where we’ve reintroduced the spatial coordinates ri into the game.

19 Sep 2005: is. ω2 = f2 gHk2, i.e. ω = (f2 gHk2)1/2. (3.20). The two branches of the dispersion relation correspond to waves with phase propagationin two different directions. ... ithou. t per. mis. sion. P.H.Haynes Mathematics III Atmosphere-Ocean Dynamics

15 Aug 2005: v2 hA(. h. 2, e. h2A(0,Y0)Y0. )= [2](h) O(h3). Y1 = ev2 Y0, (20). ... Now [1] can be approximated with Euler and [2](h) with the midpoint rule, eq.(20),.

27 Jul 2005: 2001). Given that the brain may consume as much as 20%of the oxygen we extract from the air that we breathe (Raichle et al. ... occur (after a delay, and on 20% of trials), and participants had thechance to respond to them (“execution” condition).

1 Apr 2005: Training Data %WERdev03 eval03 dev04f. bntr04-750h 16/7k 13.4 12.1 –bntr04-750h 32/7k 12.8 11.8 21.6bntr04-1050h 32/9k 12.2 11.4

9 Aug 2005: 0 5 10 15 20 25 300. 0.02. 0.04. 0.06. 0.08. ... 0 5 10 15 20 25 30 35 400. 0.02. 0.04.

23 Nov 2005: M4WM4H. ). 1 4M2W. M2H. 20 Calculate the rate for the decay of the Higgs boson into a fermion-antifermion pair:.