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14 Jun 2021: Slide 21. Slide 22. Slide 23. Slide 24. Slide 25. Slide 26.

13 May 2021: ACE Memory 25.0 (1.50) 25.1 (1.00) 24.7 (1.53). ROCF immediate 33.3 (2.59) 31.8 (2.69) 32.0 (2.65).

19 May 2021: mis. sion. 4 Surfaces and Surface Integrals 24. 4.1 Surfaces and Normals 24. ... 24 –. Cop. yrig. ht. 201. 6 U. nive. rsity.

12 Jun 2021: perpendicular to B. In the last line, we’ve used the equation (2.24). ... oscillating with frequency! = qB/m. However, because of the constraint (2.24), the.

12 Jun 2021: anti-clockwise in the Southern hemisphere. Notice that the period of rotation is not 24. ... hours unless the pendulum is suspended at the poles. Instead the period is 24/ sin.

12 Jun 2021: 7. Special Relativity. Although Newtonian mechanics gives an excellent description of Nature, it is not uni-. versally valid. When we reach extreme conditions — the very small, the very heavy or. the very fast — the Newtonian Universe that

12 Jun 2021: S T)µ1.µp1.r1.q1.s. = Sµ1.µp1.qT1.r. 1.s (2.24). Given an (r, s) tensor T , we can also construct a tensor of lower rank (r

14 Jun 2021: 6. Black Holes. Black holes are among the most enigmatic objects in the universe. They are described. by deceptively simple solutions to the Einstein equations, yet hold a host of insights. and surprises, from the meaning of causal structure, to

21 May 2021: 01/01/17-. 31/12/18). ;. the Governance Review Working Group. (24/04/17-. 31/12/20. );. the Pensions Advisory Group. (May 2017 onwards, also October 2010 - December 2014).

23 Jul 2021: Demonstration of convergence. 24 THE BARRIERS OF DEEP LEARNING AND SMALE’S 18TH PROBLEM.

22 Jul 2021: Demonstration of convergence. 24 THE BARRIERS OF DEEP LEARNING AND SMALE’S 18TH PROBLEM.

26 May 2021: Demonstration of convergence. 24 THE BARRIERS OF DEEP LEARNING AND SMALE’S 18TH PROBLEM.

14 Jul 2021: 1.29:. 1.28:. 1.27:. 1.26:. 1.25:. 1.24:. 1.23:. 1.22:. 1.21:. 1.20:. 1.19:. ... 0.31:. 0.30:. 0.29:. 0.28:. 0.27:. 0.26:. 0.25:. 0.24:. 0.23:. 0.22:. 0.21:.

11 Jun 2021: Demonstration of convergence. 24 THE BARRIERS OF DEEP LEARNING AND SMALE’S 18TH PROBLEM.

31 Jul 2021: tomodel the effects of the porous plate, where 𝜇 = 𝛼𝐻𝐾𝑅/(𝜋𝑟2) is the porosity parameter [23, 24]. ... 723, 2013, pp. 456–479. [24] Howe,M.S., Scott,M. I., andSipcic, S.R., “The influenceof tangentialmeanflowon theRayleigh

20 Jul 2021: RESEARCH ARTICLE. Hydrodynamics and direction change of. tumbling bacteria. Mariia DvoriashynaID, Eric LaugaID. Department of Applied Mathematics and Theoretical Physics, University of Cambridge, Cambridge, United. Kingdom. e.lauga@damtp.cam.ac.uk.

8 Jul 2021: 𝑝(𝑧) = 𝑟𝑅𝑢𝑟(𝑅, 𝑧). (24). Kinematics based model. The kinematic based model was postulated from the system’s bound-ary conditions.

8 Jul 2021: cells swim [24–28]. Absolute pressure [29], pH [30] and even magnetic field [31] have also. ... Bi = 0.11 0.06 (n = 2),hB/Li = 0.63 0.24 (n = 9)).

8 Jul 2021: B. Microsphere motion. The dynamics of a microsphere forced by an optical trap whose position is laterally oscillated isa well-studied problem [24]. ... Phys. 1, 28 (2018).[24] K. C. Neuman and S. M. Block, Optical trapping, Rev.

8 Jul 2021: Cells interact with their surroundingsthrough complex hydrodynamic and steric interactions.21,22 Rigidboundaries, free surfaces and other obstacles in suspensions areknown to strongly affect swimming behaviour.23,24 Relevantcomplex media include

8 Jul 2021: While recent numerical work reported that the elasticstresses in the wake of rigid cylinders depend on the orientation of the cylinder relative to its velocity[24], the dependence of the drag ... symmetry breaking, Phys. Fluids 24, 103102 (2012).[19] J. A

8 Jul 2021: Received 13 May 2020; revised 18 February 2021; accepted 24 February 2021). ... Ω. , (2.23). where. A = 6ζ‖ 4Δζ (φ21 φ22 ) O(φ4), (2.24)B = 4Δζ (φ1 φ2) 83 Δζ (φ31 φ32 ) O(φ4), (2.25).

8 Jul 2021: For larger ciliatedcells [24], or for multicellular aquatic organisms equippedwith many short flagella [25], the synchronization dynamicstakes the form of metachronal waves, akin to spectator wavesin sport stadiums. ... p = p1 O(2 ), (24). σ = σ1 O(2 ).

8 Jul 2021: 19]. Ex-perimental work on bacteria in their swimming [20–24]or swarming states [25,26], algae [27,28] and sperma-tozoa [29,30] provide diverse examples of correlated,collective dynamics ... 23] Wolgemuth C. W., Biophys. J., 95 (2008) 1564.[24] Sokolov

8 Jul 2021: Since all the prefactors in Eq. (24), including r2and 〈y1, y2〉, are positive numbers, the phase difference (2)0 isthe linearly stable solution to Eq. ... 24) is not entirelyequivalent to the Adler’s equation. It is important to note thatboth r2 and.

8 Jul 2021: of Bristol, 24 Tyndall Avenue, Bristol BS8 1TQ, UK. ... uθ = cΩ I1(κr)K1(κ) K1(κr)I1(κ)I1(κc)K1(κ) K1(κc)I1(κ), (4.24)where. α0 = cκΩ. I1(κ)I1(κc)K1(κ)

27 May 2021: B. Microsphere motion. The dynamics of a microsphere forced by an optical trap whose position is laterally oscillated isa well-studied problem [24]. ... Phys. 1, 28 (2018).[24] K. C. Neuman and S. M. Block, Optical trapping, Rev.

9 Jun 2021: activator” [24,25], the com-plicated instability conditions for N > 2 [26] do not lendthemselves to analytical progress.Here, we analyze the diffusive threshold for Turing. ... Natl. Acad. Sci. U.S.A.115, 6572 (2018). [24] A. J. Koch and H.

18 May 2021: 24 CHAPTER 2. GENERALISED SOLUTIONS. The representation (2.8) makes it clear again that the Moore-Penrose inverse is un-bounded if R(A) is infinite dimensional.

11 Jun 2021: 24. Fancy dress must not interfere with the operation of lifejackets or cause any other safety concerns.

8 May 2021: 1. The in-plane elastic-plastic response of an incompressible, filled hexagonal honeycomb. H Tankasala, V S Deshpande+ and N A Fleck+. Now at School of Mechanical, Aerospace & Automotive Engineering, Coventry University,. Priory Street, Coventry CV1

9 Jun 2021: Au/WS2/P ZT/Au 24.3 3.5 0 µA / 0 µW 0.15 µA / 0.53 µW 10 S36.

18 Jun 2021: Sel. Top. Quantum Electron. 24, 1–12 (2018).16. Nagarajan, R. et al. ... Nat. Photonics 7, 883–887 (2013).24. Wang, X., Cheng, Z., Xu, K., Tsang, H.

16 Jun 2021: S12), from which we extract τs =24.24.0 ns and τl =3.530.09 µs (red), τs =104.6 2.7ns. ... This is in agreement with. Refs. [24, 25]. We extract and show in Supplementary Fig.

16 Jun 2021: ount. s). 0. 6. 12. 18. 24. x20. x4. x1. Fig. ... Nat. Mater. 13, 247–252 (2013). 24. Byrnes, T. et al. Exciton-polariton condensates.

9 Jun 2021: Graphene-basedoptoelectronic devices are compatible with Si platforms16,24–27.Therefore, graphene-based OEMs could combine telecomoperation and CMOS compatibility. ... 24. Pospischil, A. et al. CMOS-compatible graphene photodetector covering alloptical

4 Aug 2021: Second, GO can be prepared inexpensively via LPE. Spray-coating allows conformal coverage surfaces with complex shapes.[24] This approach is very attrac-tive from an industrial point of view. ... Park, M.-J. Park, J.-S. Lee, Adv. Funct. Mater. 2018, 28,

9 Jun 2021: We perform Raman mea-surements at 785 nm, the available Raman wavelength closest tothat used in HAMR (830 nm25,55), with a spot size 1.24 μm, asdetermined by the razor ... 75 on a 0.24 cm2. area, is investigated using an electrochemical corrosionmethod51

22 Jul 2021: German translations are kept true-cased. Corpus Task #Sentences. TED-LIUM3 [23] ASR 268kWMT17-P En-De [24] MT 400kMuST-C En-De [25] ST 229k. ... E2E - - 19.29Casc 9.60 16.56 20.54EP 7.97 18.84 22.56. EP-J 9.60 16.24 23.25.

28 Jun 2021: These include accurate 3Ddeformable template models [23] generated from real human scans, 3D motioncapture datasets [11, 24] and large 2D datasets [22, 12, 4] which provide keypointand silhouette annotations. ... In: Proceedings of the British Machine

28 Jun 2021: weak supervision from stereo [17], weakly-aligned map la-. bels [24] or synth-to-real domain transfer [24, 21]. ... ing and 24 validation sequences captured in two cities, Mi-. ami and Pittsburg, using a range of sensors including seven.

28 Jun 2021: al [25] 15.919 24.85 8.68 16.48 2.98Logothetis et. al [16] 16.07 28.53 6.32 16.97 2.75. ... 24] Y. Quéau and J.-D. Durou. Edge-preserving integration of a normal field:Weighted least squares, TV and L1 approaches.

28 Jun 2021: large-scale environments [24, 21]. Nevertheless, recent advances in deep learn-ing particularly improve upon localization with challenging lighting, appearancechanges and in run-time performance [19, 10, 14]. ... 2019) 3302–3312. 24. Sattler, T., Torii,

28 Jun 2021: Torii, A., Arandjelović, R., Sivic, J., Okutomi, M., Pajdla, T.: 24/7 place recogni-tion by view synthesis. ... IEEE TPAMI (2011). 24. Sattler, T., Leibe, B., Kobbelt, L.: Fast image-based localization using direct 2D-to-3D matching.

28 Jun 2021: 24], expressing changesin foot shape based on 10 PCA parameters. The foot mesh is composed of1602 vertices. ... 2010) 17–22. 6. Precision3D: Fotoscan 3D Foot Scanner. (accessed 24/05/2020) http://www.precision3d.co.uk/fs.htm.

28 Jun 2021: Object navigationgoals can be represented with images [19], [22] or semantics [8],[23], [24]. ... 2, APRIL 2021. or as a target label [24]. Language instructions (e.g.

28 Jun 2021: These include accurate 3Ddeformable template models [23] generated from real human scans, 3D motioncapture datasets [11, 24] and large 2D datasets [22, 12, 4] which provide keypointand silhouette annotations. ... In: Proceedings of the British Machine

28 Jun 2021: weak supervision from stereo [17], weakly-aligned map la-. bels [24] or synth-to-real domain transfer [24, 21]. ... ing and 24 validation sequences captured in two cities, Mi-. ami and Pittsburg, using a range of sensors including seven.

28 Jun 2021: al [25] 15.919 24.85 8.68 16.48 2.98Logothetis et. al [16] 16.07 28.53 6.32 16.97 2.75. ... 24] Y. Quéau and J.-D. Durou. Edge-preserving integration of a normal field:Weighted least squares, TV and L1 approaches.

28 Jun 2021: large-scale environments [24, 21]. Nevertheless, recent advances in deep learn-ing particularly improve upon localization with challenging lighting, appearancechanges and in run-time performance [19, 10, 14]. ... 2019) 3302–3312. 24. Sattler, T., Torii,