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2 Jan 2007: z =x iy. 2, z̄ =. x iy2. , (24). =12. (.

3 Sep 2007: uncorrected. Results are displayed on axialslices (z 24) of the participants’ mean normalized structural image.

3 Sep 2007: One study examined memoryover three intervals including 24 hours and 7 days(Kopelman, 1985). ... Degenszajn et al. (2001) found thatpatients with mild to moderate AD and matchedcontrols showed a similar rate of forgetting at 30minutes and 24 hours after

10 Oct 2007: 040. A09. E23. 9.1. 38.1. 24.1. 37.1. 31. 1.14. 1.52. 3.79. ... 2.3. 23.7. 1.0. 310. 24. 12. 3. No. te:A. llin. tera.

10 Oct 2007: satellites in BBM-1, 34 in BBM-2, and 24 in BBM-3); any 2populations share on average 21 7.0 polymorphic microsa-tellites. ... 2004)found that the number of linkage groups dropped from 32(with 297 markers) to 24 (with 541 markers).

10 Oct 2007: Earth and Plan-. etary Science Letters, 220, 3–24. Mitchell, B.L. (1980) Report on a survey of the termites of.

9 Oct 2007: pseudoobscura [24]. DNA Sequence DataPCR primers were designed from the published or preliminary ge-nome sequences of D. ... 24. Richards, S., Liu, Y., Bettencourt, B.R., Hradecky, P., Letovsky,S., Nielsen, R., Thornton, K., Hubisz, M.J., Chen, R., Meisel

9 Oct 2007: Intron 503 12 11 1.02 0.84. GNBP3 mele Coding 1470 12 24 0.55 0.18 1.73 9.61 0.54.

9 Oct 2007: this left us with three markers. The first was a 24 bp INDEL. ... Kenya, 24 isofemale lines from Zimbabwe and 23. isofemale lines from The Netherlands.

9 Oct 2007: Immunity 24, 363–366. Insect Immunity: The Post-Genomic Era. Outline placeholder. Introduction.

25 Jan 2007: E. Huppert. Parameter Value Units. a (5.0+ 0.24( T- 20)) x U 0.015 cm2 s-' CC 4.14 J O C - '. 2.66 J cm-3 O C - '

25 Jan 2007: 0.01 (for Ra, = lo@), convection continues in the melt until t = 0.24, by which time the system is about 40% solidified.

16 Jan 2007: J. Fluid M e c h. (1990). vol. 212, p p. 209-240. Printed in Great Britain 209. The fluid mechanics of solidification. By H E R B E R T E. H U P P E R T Institute of Theoretical Geophysics and Department of Applied Mathematics and Theoretical.

25 Jan 2007: J. Fluid Mech. (1989), voZ. 198, p p. 293-319. Printed in Great Britain. 293. Phase changes following the initiation of a hot turbulent flow over a cold solid surface. By HERBERT E. HUPPERT Department of Applied Mathematics and Theoretical Physics,

25 Jan 2007: Substituting (18), (19) and (24) into (21), we obtain the following implicit relationship between T and Tl :. ( 2 5 ). Substituting (20) and (21) into ( 2 2 ) , and using (23a, c ) in ... a = pcDH;' (To--T). (24). Tl = Tmp2c2k' D J H i l ( T o - T ) (T-T,

16 Jan 2007: expressed as wt.%, as a function of the amount of K2CO 3 or NaNO 3 present in solution at 24.2C. ... Lower and upper layer properties were: initial temperatures 46 and 15C; initial concentrations 37 and 24%; initial densities 1.26 and 1.23 g cm 3; and

13 Nov 2007: Method. Glass beads 24 Rotating drume. 0.25–0.35 24 Smooth inclined planef. ... 0.5 0.04 24–31 Rough inclined planeg. 1.26 9–11 Shear gauge, smooth chute flowh.

8 May 2007: 2(m2 1). 2u. XY= Mm2h2. (2.24). We posit a solution in the form. ... 4.1) for openchannel flow is replaced by 24/105 = 0.229 for a circular constraining geometry andK/m = 0.137m2/(1 m2) for a V-shaped constrainer.

22 Jan 2007: Inserting equations (2.23) and (2.24) into equations (2.12)–(2.16) andlinearizing in the perturbed quantities leads to the following nonlinear ordinarydifferential equation for the disturbance amplitude:.

6 Nov 2007: A =. kT log 2 1β. log[. 1 β2(qJM h)2/2 β4(qJM h)4/24. ]. ... hA1/24. |A2|3/2. A4 is not particularly interesting: the denominator |A2| is the interesting part.