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4 Dec 2017: 24.11 brief comms NEW 17/11/05 5:21 PM Page 441. Nature Publishing Group 2005. ... INSECT COMMUNICATION. ‘No entry’ signal in ant foraging. 24.11 brief comms NEW 17/11/05 5:21 PM Page 442.

14 Jun 2017: Michaelmas Term 2016. 24 lectures:. Mondays, Wednesdays and Fridays at 9 am, starting Friday 7 October 2016. ... Thursday 10 November 2016, 2:00-3:00 pm, room MR13. Thursday 24 November 2016, 2:00-3:00 pm, room MR13.

20 Jan 2017: Lent Term 2017. 24 lectures:. Tuesdays, Thursdays and Saturdays at 11 am, starting Thursday 19 January.

23 Nov 2017: LecturesSeptember 17-24, 2011 - Maratea (Italy). LecturesSao Paulo, Brazil, April 4-14, 2011.

25 Oct 2017: 24.1", "babel-preset-react": "6.24.1", "babel-preset-stage-2": "6.24.1", "volleyball": "1.4.1", "webpack": "3.5.5" } }.

2 May 2017: Ann travels at a speed given byβ u/c = 24/25 in the x direction for seven years and then comes back at the samespeed, while Bob stays at home.

26 Feb 2017: Cop. yrig. ht. 201. 7 U. nive. rsity. of C. ambr. idge. Not. to b. e qu. oted. or. repr. oduc. ed w. ithou. t per. mis. sion. Quantum Fluids: Example Sheet 2. Problem 1. Mixtures of condensates. Consider a mixture of two different species ofbosons

27 Oct 2017: Old people in Cambridgeshire. 2012 2030? Over 65 96,000 17%. 135,000 24%.

22 Aug 2017: PS-Adobe-2.0 %%Creator: dvips(k) 5.993 Copyright 2013 Radical Eye Software %%Title: GeomTriCents021214.dvi %%CreationDate: Tue Aug 22 13:48:50 2017 %%Pages: 24 %%PageOrder: Ascend %%BoundingBox: 0 ... begin /FontType 1 def /FontMatrix [0.001 0 0 0.001 0

4 May 2017: Thank you! 24/24. Conclusion. Approximation theory with convexity. Approach extends to other operator concave functions via their integralrepresentation (Löwner theorem). ... Thank you! 24/24.

11 May 2017: For finite action solutions to the Euler Lagrange equations (II.24), the fields |B|,|DΦ| and. ... 0. (iii) a(; z) and φ(, z) solve the Euler Lagrange equations (II.24) at λ = 1.

22 Nov 2017: Ð L0 k. 2(s, t)ds, with a vanishing intrinsic curvature[24], thus neglecting shearing stresses.

6 Jul 2017: While thesubject of sparse quasi-Newton methods was eventually developed mostly by Toint,it also involved Mike in three interesting contributions [24, 26, 31], the first of whichis an extension to

13 Oct 2017: ON THE STABLE SAMPLING RATE FOR BINARY MEASUREMENTS AND WAVELETRECONSTRUCTION. A. C. HANSEN AND L. TERHAAR. ABSTRACT. This paper is concerned with the problem of reconstructing an infinite-dimensional signal from alimited amount of linear

13 Oct 2017: In the last example we used the code from [24] and consider reconstructionof images from Fourier samples. ... J. Amer. Math. Soc., 24(1):81–124, 2011. [30] A. C. Hansen and L.

16 Oct 2017: homozygotes and the microtubules continue to grow at 0.24 mm/sec (Figure 7A).

3 Oct 2017: ζ0. ψ(h,ζ,ξ) dξ dζ = 0, (2.24). lending an extra power of h to terms featuring Λ [ψ]a,b(h).

15 Feb 2017: A , [B, [A , C ]]] = 0, [B, [A , [B, G ]]] = 0, [C , [A , [C , E ]]] = 0, (3.24)[A , [B, [A , E ]]] = 0, [B, [B, [B, C ]]] = 0, [C , [A , [C , G ]]] =

9 Jul 2017: Thus we have a time quasicrys-tal, in analog of a conventional spatial quasicrystal [24].The persistent rotation of trapped ions can be detected. ... 24] D. Levine and P. J. Steinhardt, Phys. Rev. B 34, 596(1986).

13 Oct 2017: ON THE STABLE SAMPLING RATE FOR BINARY MEASUREMENTS AND WAVELETRECONSTRUCTION. A. C. HANSEN AND L. TERHAAR. ABSTRACT. This paper is concerned with the problem of reconstructing an infinite-dimensional signal from alimited amount of linear

19 Dec 2017: y(J) (r I,t l,r2,t2,r3,t3). == ( - i) (T{n(rl,tl)n (r2,t2)n(r3,t3)}), (2.24 ) as the time-order expectation of the electron ... This in tum gives. 24. k = 81T,Be2A i 3XI-'(0), (5.8).

4 Sep 2017: β. IL. βI. Lβ. IL. βI. Lβ. IL. β. β = 0.44ν = 1.24. ... 24] We note that this phase is related to the π spin glass phase[10,13] and is referred to as a Floquet time crystal in [11].

13 Feb 2017: Askey. 24. Jin, S., Markowich, P. & Sparber, C. (2011), ‘Mathematical and computational meth-ods for semiclassical Schrödinger equations’, Acta Numer.

29 Jul 2017: 24. 2.4 Canonical connections. 31. 2.4.1 The Ξ-connection. 32. 2.4.2 The torsion Ξ-connection. ... in [24]. Note that theorem 2.3.3 is a different construction of 4n-dimensional moduli spaces to.

1 Dec 2017: T(η,ω,X) = TabcηaωbXc. (2.24). This formula generalizes in the obvious way to a (r,s) tensor. ... Thisis easiest to demonstrate with an example. Part 3 GR December 1, 2017 24 H.S.

4 Sep 2017: 10]) that, forcontinuous time-translation symmetry, TTSB is impossibleso long as the eigenstate thermalization hypothesis [21–24] issatisfied.However,wecanbuilduponrecentdevelopmentsinthe study of Floquet-many-body-localized (Floquet-MBL)systems

11 Dec 2017: ahX=0-07 exp (V/20), (23)and II V301). Ph --Jrx 10 I(24). 516. ... h=1/(exp V30 1). (24). Equation (26) is derived simply from eqns.

20 Jan 2017: A 24.6 25.5 1.403 4 — 5.3 10.7 5.2B 43.6 24.7 1.4 4.7 20 6.3 13.3 3.4C 36.6

30 Apr 2017: 2.5 -. 8. Douady. 2.0 4 I 23 24 25 26 21 28 29 30 31 32. ... Figure 24 presents a study of the mode n = 9, around 20 Hz.

22 Nov 2017: Proc. Nat. Acad. Sci. USA 74, 2397–2401 (1977)24. LeBret, M.: Catastrophic variations of twist and writhing of circular DNA with constraint? ... Math. Methods Appl. Sci. 24, 1325–1335 (2001)37. Goriely, A., Tabor, M.: Nonlinear dynamics of filaments.

3 Dec 2017: Received 16 July 2015; revised manuscript received 24 March 2016; published 12 May 2016). ... 24)See the right panel of Fig. 4. Again, F [rf ](ω) denotes theFourier amplitude at frequency ω.

22 Aug 2017: PS-Adobe-2.0 %%Creator: dvips(k) 5.993 Copyright 2013 Radical Eye Software %%Title: 12pointTriangle12052017.dvi %%CreationDate: Tue Aug 22 13:40:04 2017 %%Pages: 21 %%PageOrder: Ascend %%BoundingBox: 0 0 596 842 %%DocumentFonts: CMBX12 CMR7 CMSL10

8 Dec 2017: for16-24 year-olds.

29 May 2017: DOI: 10.1039/c6sm02649d. rsc.li/soft-matter-journal. Soft Matter. PAPER. Publ. ishe. d on. 24. ... L. Ekiel-Jeżewska and E. Wajnryb, J. Chem. Phys., 2015, 142, 214902.24 B.

20 Jan 2017: Accepted article online 24 JUN 2016. Published online 13 JUL 2016.

3 Dec 2017: Oecologia118, 132–143. 24 Beyschlag, W. and Pfanz, H. (1992) A fast method to detect the occurrence ofnonhomogenous distribution of stomatal aperture in heterobaric plant leaves.Experiments with Arbutus unedoL.

20 Jan 2017: Note that (2.24) implies thatui is independent of z in the interior of each isopycnal layer, hi1 < z < hi. ... interior of each layer, @ui/@z = 0,as implied by (2.24).

8 Nov 2017: Chlamydomonas is a pulleron average but in fact oscillates between instantaneouspusher and puller behaviours [24], potentially interferingwith the development of an instability. ... Rev. FluidMech., 24 (1992) 313. [20] Jibuti L., Qi L., Misbah C.,

19 Dec 2017: Quality of life 16-24 year-olds complain of not enough to do, and that the events and.

9 Jul 2017: Received 28 March 2015; published 24 June 2015). In analogy with crystalline solids around us, Wilczek recently proposed the idea of “time crystals” asphases that spontaneously break the continuous time translation

4 Dec 2017: When the nutrient is essential for life, suchas oxygen for obligate aerobes, f (c) may vanish below somec [24,25]. ... μ̄ = 1λ. λ0. dx y(c)cb. (24). 022701-5. FRANÇOIS J. PEAUDECERF AND RAYMOND E.

19 Dec 2017: PHYSICAL REVIEW A VOLUME 40, NUMBER 2 JULY 15, 1989. Structural phase transitions of interacting membranes. Raymond E. Goldstein and Stanislas LeiblerService de Physique Theorique, Centre d'Etudes Nucleaires de Saclay, F 911-91 Gif sur Yue-tte CEDEX,

4 Sep 2017: Refael, and V. Galitski, Nat. Phys. 7, 490(2011). [24] T. Kitagawa, E.

11 Mar 2017: In this regime, MBL is expected to persist even in the presence of long-range interactions23,24. ... Phys. Rev. B 92, 104428 (2015). 24. Yao, N. Y. et al.

11 Mar 2017: of novel, out-of-equilibrium quantum phases3,5,24. ... LETTER RESEARCH. 24. Abanin, D. A., De Roeck, W. & Huveneers, F.

4 Apr 2017: S i m i l a r l y k is the t r u e coefficient o f diffusion, a b o u t 0"24 c m? /

2 Oct 2017: Naeh Aufgiessen reinen Wassers erschienen dann schon innerhalb 24 Stunden sowohl die gewShnlichen grossen wie die kleinsten beweglichen Zustnde wieder.

25 Nov 2017: Current chips measure 24 32 mm, and today’sproduction processes are aiming to print 50-nm features.

7 Apr 2017: k. , sin a 1 (24) = - t v " 1 , 3 0 9 " l o g n a t '. Soll W g l e i e h W sein, so f o l ... g t d u r c h G l e i c h s e t z e n v o n (23) u n d (24).

23 Apr 2017: Pi[Vr/(r, - a)]2 = 277a2D2/rl(r1 - a)4. (24)The volume involved is approximately 8irr 2(r, - a), so the total stirring power ex-pended in this region