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3 Oct 2016: b) A membrane extension drawn from afluctuating vesicle using optical tweezers (830 nm single-moddiode, 200 mW).

12 Aug 2016: 200. 220. 240. 260. 280. 300. 320. 340. 0 50 100 150 200 25010-12. ... 10-5. 10-4. 10-3. 10-2. 10-1. 100. 0 50 100 150 200 250 300time (D/U).

12 Aug 2016: For the Earth,. 115. 1 200. R, = 4 x 10 - << q x - << 1,.

22 Jan 2016: v p(µ. m/s. )0 100 200. Area (µm2 ). 0. 10.

24 May 2016: Selective deformation of soft continuous microscale bodiesWe fabricate LCE microrobots in the form of long cylinders (about1 mm in length and 200–300µm in diameter), and flat discs (50µmthick and either ... Themixture is then ultraviolet-cured

25 Feb 2016: PHYSICS OF FLUIDS 28, 013101 (2016). Slender-ribbon theoryLyndon Koens. a). and Eric Lauga. b). Department of Applied Mathematics and Theoretical Physics, University of Cambridge,Wilberforce Road, Cambridge CB3 0WA, United Kingdom. (Received 20 May

1 Oct 2016: Other measurements reports significantly larger sizes, withwidths that can range 100–300 µm and length 200–500 µm[21, 23, 24]. ... pp. 1171–200. 26. Berdyyeva TK, Woodworth CD, Sokolov I. Human epithelial cells increase.

6 Oct 2016: For differentvalues of |K| (number of attacked sensors) and |L| (numberof attacked actuators), we ran the decoder on 200 differentinitial conditions and attack sets and we recorded the successrate of the

6 Oct 2016: For this. 0 5 10 15 200. 0.2. 0.4. 0.6. 0.8. ... Fordifferent values of q between 1 and 34, we ran 200 simulationswith different sets of attacked sensors K of cardinality q, anddifferent initial conditions x(0).

6 Oct 2016: I Used 1/2 decoder. 0 5 10 15 200. 0.2. 0.4. ... For each value of q, 200 simulations were carried out. with different initial conditions and different sets of attacked sensors.