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30 Sep 2008: with width 1/σ (See figure (13)) We will now evaluate the resulting wave-function bysubstituting (24) for A in (23),. ... ψ|2U. 0x0(t). Figure 24: Initial state of wavepacket. x. |ψ|2U. 0.

20 Feb 2008: Proof. When N = G this is follows from [13, Theorem 7.24]; see also [1, Lemma3.11]. ... Lemma. The quotient category Fd/Fd1 is equivalent to M(Q(kG)). Proof. This follows from [24, Propositions XI.3.4(a) and XI.6.4], with appropriatemodifications to

11 Nov 2008: 24 h after transfection cells were serum-starved for 16 h and then stimulated with 20 ng/ml TNF-α. ... 24. 26. 28. 30. 32. 34. 36. 38. 40. 42. inte.

20 Oct 2008: for further N2 addi-tion up to 20%;22,24 ii electron mobility increases slightlywith N2 10%–20%;. ... 0 TM1/2, following Ref. 24, with VRH0 independent of TM. However, the slopes for.

16 Jan 2008: 2.2.2 Hidden conditional random fields (HCRFs). 24. 2.2.3 Parameter estimation for conditional models.

8 Jul 2008: Rather the dust distribution seen at 24 and 70 µm extendsout to 800 AU [73]. ... Wyatt. Eridani disk which is a narrow ring at 60 AU with a well resolved inner hole[24].

3 Jul 2008: 1 |φn |2)p2 d x (24). and1. 4π. jφp(x)d x = limn1. ... Ann. Math. 113, 1–24 (1981)22. Schoen, R., Uhlenbeck, K.: Boundary regularity and the Dirichlet problem for harmonic maps.

16 Feb 2008: 20. 21. 22. 23. 24. 25. Coverage. eval02eval03eval04. 1 2 3 4 523.2. ... 23.4. 23.6. 23.8. 24. 24.2. 24.4. 24.6. 24.8. 25. 25.2. BLEU.

31 Jul 2008: 9.3.9]:. u0(t) = 1, u1(t) =3t 5t3. 24, u2(t) =. 81t2 462t4 385t61152. , ... 9.6.24]. Kν (νz) =1. 2. eνφ(v) dv, φ(v) = z cosh v v.

1 Jul 2008: The Riemann–Hilbert factorization problem underlies this approachto integrability: it appears in classical solution generating techniques such as dressingtransformations [18], as well as in the twistor treatment of ASDYM [24]. ... Math. Phys. 7