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25 Sep 2008: while the kinematic equation yieldsu = @x@t ; v = @y@t : (20)Van Dommelen & Shen (1980) made the key observation that (19) de-pends only on x and u, and hence that ... 19) and the rst of (20) can besolved independently of the equations governing y and v.

30 Sep 2008: ψ(x, t) = χ(x) exp. (. iEt. ). (20). Substituting for (20) for ψ in the Schrödinger equation yields the time-independent. ... States of the special form (20) are known as stationary states.

29 Jan 2008: The results were staggering,especially the minimization of a periodic function F (x), x Rn, with 100 vari-ables, although problems with n = 20 were considered large at that time. ... The average values of these counts with m = 2n1 are 931, 1809,3159 and

5 Dec 2008: 20. Cop. yrig. ht. 200. 8 U. nive. rsity. of C.

3 Jul 2008: Now consider the integrated form of the first equation of (1.20) (i.e. ... and corresponding Sobolev norms ‖ ‖Hs on the space of sections defined as in [20].

23 Sep 2008: JOURNAL OF GEOPHYSICAL RESEARCH, VOL. 94, NO. D12, PAGES 14,617-14,628, OCTOBER 20, 1989. ... r {-«Z3m a(sin Zm - Zm cos Zm)} (20). lfOZm AA = • -(z 2 - a 2 sin 2 z)dz - 3 -- •Zm q- «a2(zm- sinzm coszm)} (21).

8 Apr 2008: 19. 2.2 Supersymmetry - Algebra. 20. 2.2.1 History of Supersymmetry. 20. ... century. It has been carefully experimentally verified in many ways, especially during the past 20 years,.

3 Jul 2008: 11.27). From (11.21) and (11.27) inequality (11.20) follows.Now (11.13), (11.18), (11.19) and (11.20) imply. ... Introduce the majorant. m(t) := sup[0,t]. (1 s)3/2‖η(s)‖Lβ, t t1. 20.

17 Jan 2008: whenever this limit exists. Remarks. • It follows from (1.20) and the definition of a partial deriva-tive (1.14) that. ... To derive (1.52) start from the definition of a directional derivative (1.20), and use the definition of.

24 Apr 2008: 1.4 The ADHM Construction 20. 1.4.1 The Metric on the Higgs Branch 23. ... 20 –. of the D(p 4)-brane [3, 5]. They are the same object!