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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.

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" } }.

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,

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.

25 Oct 2017: 6.24.1", "babel-messages": "6.23.0", "babel-register": "6.26.0", "babel-runtime": "6.26.0", "babel-template": "6.26.0", "babel-traverse": "6.26.0", "babel-types": ... 5.7", "resolved": "https://registry.npmjs.org/source-map/-/source-map-0.5.7.tgz",

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

21 Feb 2017: 24 FEBRUARY 2017. 0031-9007=17=118(8)=088001(5) 088001-1 Published by the American Physical Society. ... 24 FEBRUARY 2017. 088001-3. freezing [Fig. 4(a)], a strong experimental signature of theformation of rotator phase next to the perimeter [3].

8 Nov 2017: This technique allows theasymptotic exploration of a range of ribbon structures, such asartificial microswimmers comprising a magnetic head and aribbon tail.22–24. ... 24 L. Zhang, K. E. Peyer and B. J. Nelson, Lab Chip, 2010, 10,2203–2215.

8 Nov 2017: I 1. 2ezez. ). (I ezez) = I, (24). and we further note that ξ/4πµ 1/ln(1/ϵa) [9]. ... Rev. Lett., 96 (2006). 058102.[24] Guirao B. and Joanny J. F., Biophys.

2 Oct 2017: Rev. 35 415–24[8] Grant M A, Waclaw B, Allen R J and Cicuta P 2014 J. ... Rev. Lett. 109 168105[24] Ravnik M and Yeomans J M 2013 Phys.

4 Sep 2017: One can also combine MBL with the above quantumorders to obtain MBL phases in which individual highly ex-cited eigenstates show SSB, SPT, or topological order [19–24].

7 Nov 2017: The collective behaviour of Bacillus subtilis swarms and theirinteractions has been shown to depend on the geometry of the enclosing cavities [24]. ... Rev. Fluid Mech. 24. 313–58[5] Guasto J S, Rusconi R and Stocker R 2012 Fluid mechanics of

12 Jul 2017: 25 and 38 have gas fractions 26–55%; the gratings in ref.24 have g '1 mm). ... Phys Fluids 24:112003. 24. Bolognesi G, Cottin-Bizonne C, Pirat C (2014) Evidence of slippage breakdown for asuperhydrophobic microchannel.

13 Mar 2017: 2′. n=0 fn d. 2. 2(U α β). (24). Finally, to determine U , we impose that the force on the torus must vanish. ... 100 100.5 101. 0.24. 0.245. 0.25. s0. |U|. 0.8 1 1.2Concentration.

8 Nov 2017: At large times, clearlythe time-independent terms in (24) can be neglected comparedto the logarithmic term. ... J. E 29, 27 (2009).[24] J. Brady, J. Fluid Mech. 667, 216 (2011).[25] B.

26 Jan 2017: where. û1(λ) eiλN1l=0. [iλal1P̂l(λ) b. l1P̂l(λ). ],. 24. û2(λ) eλN1l=0. [λal2P̂l(iλ) bl2P̂l(iλ). ],. ... Appl. Math. 24 (2013), no. 6, 857–886, DOI10.1017/S0956792513000223. MR3181485. [24] B.

23 Aug 2017: T =AreaN8π2. Σ. [2. ȧwȧw Cφ̇φ̇]ωΣ, (3.24). F Contatto and M Dunajski J. ... WN} is, from (3.24),. AreaN8π. Ni,j=1. ((Wk)δij 2Wi bj) dWidW j,.

8 Nov 2017: and on the interaction between the surface of the particle and its physico-chemical environment (M)24. ... Designing phoretic micro- and nano-swimmers. New J. Phys. 9, 126 (2007).24.

7 Nov 2017: small-amplitude perturbations of Taylor’s swimming sheet[24] and squirming motion on a spherical surface [26]. ... 15) in any shear-thinning fluid model. We choosethe Carreau model, which is a good fit to many shear-thinningfluids [24,52] and in

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

8 Nov 2017: Phys. Fluids 24, 081703.LAUGA, E. 2007 Propulsion in a viscoelastic fluid. ... 2012 Self-propulsion in viscoelastic fluids: pushers vs. pullers.Phys. Fluids 24, 051902.

10 Jan 2017: where ξa are local coordinates on the fibres of M, and 24 is the Ricci scalar.

3 Dec 2017: L. Kuzemsky, Int. J. Mod. Phys. B 24, 835 (2010). [7] H.

11 Dec 2017: 93, 26.617. 93.710.26. 2.523. 20'. 22211480. 93.18.08—1. 93.6 93.710.68 10.72. 24. ... 24, 575-587 (1924},Eq. {13}. H. Fricke, The electric capacity of suspensions with special reference to blood,Jour.

3 May 2017: 8 24.2Re(c2) Re(c1) 93 96 40 12.3 7.5 3.2. ... In (a) Re = 21.7and (b) Re = 24.0, Re(c1) < Re < Re(c2), and a constant steady-state lift force is observed.In (c) Re=25.3 and (d)

23 Nov 2017: 8.17) dictates that. V#̇ : ûdV = 0, (8.24). and so the velocity of the swimmer, as given by Eq. ... experimental measurement of the swimming kinematics ofdeforming bodies [24] based on theory proposed by Khair and Squires [23].

3 Dec 2017: 1990 The American Physical Society 2953. VOLUME 64, NUMBER 24 PHYSICAL REVIEW LETTERS 11 JUNE 1990. ... Temperature: 7'C. 2954. VOLUME 64, NUMBER 24 PHYSICAL REVIEW LETTERS 11 JUNE 1990.

19 Dec 2017: T(x) = —', p(x)[1 —xp(x)][1 ——,'p(x)]. 1/2. (23). (24). (25). (26).

9 Jul 2017: I; Xi. miR2. 1. hðiÞ;i. 1. ðiÞ;. 1. þ ðĥ2i; ĥi2;Þ > 0; (24). ... Phys. 5, 56 (2003).[24] I. Bloch, J. Dalibard, and W. Zwerger, Rev.

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

7 Nov 2017: This understanding has then prompted the scientificcommunity to create artificial microswimmers [22–24]. ... 24)The above force exhibits a structure 1/[ln(/b) ξ ], where ξ is some constant, very similar to theforces exerted by a thin prolate ellipsoid

11 Jan 2017: X = tp 12t2[p,k] 1. 6t3[k, [p,k]] t4. (1. 24[p.[p, [p.k]]] 1. ... 24[k, [k, [p,k]]]. )(20)265. t5(. 7. 360[k, [p, [p, [p,k]]]] 1.

20 Jan 2017: x = h(y) = 16 y3 c1y c2, (4.24)where c1 and c2 are constants. ... angles. SIAM J. Appl. Math. 49, 1009–1028. (doi:10.1137/0149061)24. Vogel TI. 2013 Liquid bridges between balls: the small volume instability.

14 Jun 2017: ckBλ ,1(ck,t)dt, (23) ck1. ck. t1ck. [Bλ ,1(ck,t2),Bλ ,1(ck,t1). ]dt2dt1, (24) ck1. ... of (24)to local order 8 is equivalent to quadrature of (35) to local order 3,. –

11 Dec 2017: r 24 25 26 21.28.29.30.31. 22.23 24 25 26 21. 28 29. ... z2.1 o. r-. o or5. 12. %. 6. 022. 23 24 25 26 27 28 29.

9 Oct 2017: 3.24)The solution of Eq. (3.23) with initial condition uµ = uµ(0) at τ = 0 is. ... 4.24) by a term. 1µ0c. αAµFνα = 1. µ0cα (AµF. να) , (4.45).

7 Nov 2017: 0.95 3.58–3.68 14.5 μm (1.9–4.3) 103U/U0 0.99 6.24–6.30 25 μm (1.3–2.6) 104U/U0 0.999 ... 0.049U/U0 0.95 3.58–4.04 15.2 μm 0.0020–0.022U/U0 0.99 6.24–6.91 26.3 μm (0.34–4.2)

10 Aug 2017: Clement, and R. Soto, Phys. Fluids 24,. 011901 (2012).[6] S. E. ... 24] H. Wioland, F. G. Woodhouse, J. Dunkel, and R. E.

20 Jan 2017: Received 24 June 2015; revised manuscript received 1 January 2016; published 24 February 2016). ... 24)] while the effective permeability decreases like H1(cf. (22)). The porosity also approaches an asymptotic profilewith φ0 0 as H.

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.

12 Jul 2017: water and the microbeadsuspension were made of glass and polytetrafluoroethylene andfitted with stainless steel needles (24-gauge injection needles;Carl Roth GmbH), and the inlet and outlet reservoirs were madeof glass. ... 4 A, B, and D), at a frame

23 Apr 2017: 23). From (22) and (23)PJL. For a given power P and frequency / , equation (24) gives a maximum value ofuwhen ,X. ... the observed value is 24/14.

11 Dec 2017: By this agent the height was depressed to 24, which shows th a t the tension of a surface of soapy water is much less than the combined tensions of a

10 Nov 2017: These range over geometry in the study of hyper-Kähler manifolds[14,19–23], conformal, Cauchy–Riemann CR and projective structures [24–36], exoticholonomy [37–40], in representation theory [12,41], ... See [41] for details of these constructions,

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.

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