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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.

5 Feb 2007: L. Jaffe, Phys. Today 48N9, 24 (1995). [15] D. B. Renner et al.

19 Jun 2007: 1. e2=. x6 ls2gs. (3.24). where ls is the string length, and gs the string coupling. ... with worldvolume 039, as shown in figure 6 [24]. The x3.

19 Jun 2007: d4x Tr (δAµ δAµ) = 2Sinst ρ2 (1.24). Note that, unlike the others, this component of the metric depends on the collective. ... theory [22, 23, 24]. We’ll do things the simple way. The brane construction is another place.

19 Oct 2007: dxδ(x) = 1 (1.24). The Fourier transform of the delta-function provides a useful representation that we.

10 Oct 2007: Consider the action for a real scalar. field given by. S =. d4x1. 2µφ. µφ 1. 2m2φ2 gφp (24). Find the scaling dimension D such that the derivative terms remain invariant.

2 Nov 2007: "# $%& '&(),#-.(/ 0&&1&. 243563798:3<;>=?A@CBD7FEG. HJICKMLONCPRQOLSUT#VXWJYJZ[]_]_Facb dMefWhgi]jDbkbCW1limCend_bk[oefoXpqb d_]rq[DpXb sCtendbk[oO]efZW#mX]_Wpud_[W1vkmXt1bkpCendWwpXb

19 Oct 2007: subtraction,r = 1, with 12, 24, 48 and 96 terms respectively. ... 24. Huybrechs, D. & Vandewalle, S. (2006), ‘On the evaluation ofhighly oscillatory integrals byanalytic continuation’,SIAM J.

13 Apr 2007: The second inclusion follows by Theorem VIII.24 ([RS72], p. 290)if we can show that PnAPn A in the strong resolvent sense. ... PROOF. Now, (i) follows from the fact that A1,n A strongly (see Theorem VIII.24 in[RS72], p.

15 Feb 2007: rkxj (1)αj erkxj ] = 2ν. k=1. a[αj ,sj ]k cosh(rkxj ). Likewise,. Sα[2s1x f](1) =d. j12sjxj [e. xj (1)αj exj ]g(0). 24.

10 Oct 2007: Intl. J. Approx. Reasoning, 34,3–24, 2003. Warwick, K., March of the Machines: Why the New Raceof Robots will Rule the World.

5 Dec 2007: Conditions in the outer flow, including the boundary conditions, can be chosen in a special way (Warn & Warn 1978, 56; (2.24) below) such that the changes induced in the outer ... 2.24) jl,n being the nth zero of the Bessel function J1.

7 May 2007: 24 = 1 and find its degree. By calculating. Tr((dg g1)3) at the point on S3 where x4 = 1, or otherwise deduce that the formula.

16 Feb 2007: uthor for correspondence (m.dunajski@damtp.cam.ac.uk). eived 13 June 2006epted 24 November 2006 945 This journal is q 2007 The Royal Society.

27 Jul 2007: Digital Object Identifier (DOI) 10.1007/s00220-007-0208-4Commun. Math. Phys. 272, 85–118 (2007) Communications in. MathematicalPhysics. Anti-self-dual Conformal Structures with Null KillingVectors from Projective Structures. Maciej Dunajski, Simon

17 Apr 2007: IOP PUBLISHING CLASSICAL AND QUANTUM GRAVITY. Class. Quantum Grav. 24 (2007) 1841–1862 doi:10.1088/0264-9381/24/7/010. ... An early example of this technique in gravityis the slow motion of Majumdar–Papepetrou black holes [24].

25 May 2007: Let us concentrate on instantons, in which case [24]. Q = 2π N , (3.6). ... B 272. (1986) 322–328.[24] W.J. Zakrzewski, Low-Dimensional Sigma Models, Adam Hilger, 1989.

5 Sep 2007: Anal. Priloz. 21,. 81–82 1987.24 Ovsienko, V. and Rogers, C., “Deforming the Lie algebra of vector fields on S1 inside the Poisson algebra on ṪS1,”.

24 Jun 2007: Could generalise to F theory with ds2 = g(2,2) dx82. Dunajski (DAMTP, Cambridge) ASD in ( ) 27 March 2007 24 / 26.

21 Jun 2007: The Mathematical Institute, 24{29 St Giles’, Oxford OX1 3LB, UK(dunajski@maths.ox.ac.uk). Received 4 June 2001; accepted 21 September 2001; published online 28 March 2002.

27 Nov 2007: Instead, one uses a space oftempered distributions). 24. Example 6.1.2 H = L2(Rn) (where n = 1, 2, 3 are important cases) is a space of complex-valued functions such ... Ĥ =. 3j=1 P̂. 2j. 2m+ V (X̂j) =. 2. 2m2 V (xj) (6.24).

19 Nov 2007: Logarithmic approach to long-time:. value depends on initial condition. Pipemix - Nottingham 2007 – p.24/25.

29 Sep 2007: In axoneme, dynein motors arspaced every 24 nm along the microtubules.

25 Jan 2007: ithou. t per. mis. sion. where D = 0E; H = 10B: (24)The latter vectors are used to describe non-trivial electrical and magnetic properties ofmedia for which and are callled permittivity ... We might ask: can we obtain an understanding of the elementary

25 Jan 2007: Geodesic Deviation (23). Eij = j gi. Tidal Tensor (24). Now the gravitational field is conservative, curl g = 0, and so we may introducethe Newtonian Potential by. ... 24. Cop. yrig. ht. 200. 6 U. nive. rsity. of C.

25 Jan 2007: iqt qxx 2rq2 = 0irt rxx 2r2q = 0. (4.3.24). The reduction r = σq̄, σ = 1, yields the celebrated NLS equation (1.2). ... 24. Cop. yrig. ht. 200. 7 U. nive. rsity. of C.

25 Jan 2007: mis. sion. P.H.Haynes Mathematics IA Algebra and Geometry Michaelmas Term 2002 24.

24 Apr 2007: of conformations [23,24,25]. The success of this approach. relies on the ability of the conformational sampling to. ... states [24,26,27]. In a series of recent studies, NMR. chemical shift information has been used to restrain.

23 Jan 2007: Trends Biochem. Sci. 24, 329–332. Dobson, C. M. 2001 The structural basis of protein folding and its links with human disease.Phil.

24 Apr 2007: Trends. Biochem. Sci. 24, 329–3326 Lansbury, P.T. and Lashuel, H.A. (2006) A century old debate on.

14 Feb 2007: Proteins 24, 145–151. Bai, Y.W., Milne, J.S., Mayne, L., and Englander, S.W.