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5 Feb 2015: 174.3860 212.0221 183.4615 275.1014 184.2850 184.2154 184.4135 244.6897 187.3142 70.22635 190.3387 94.84615 197.1700 121.0863 200.5851

4 Oct 2015: 200 100 0 100 2000. 0.2. 0.4. 0.6. 0.8. 1. ... For a complete picture of the spectrum consult Figure 7. Notice that the smaller featuresshown here are over 200 times smaller than the elastic peak.

17 Sep 2015: Electrodes were aligned in asquare array, spaced 200 um apart.). 1.

1 Oct 2015: ty w. ith N. orm. al F. it. 0.000.050.100.150.200.25. 60 65 70 75 80. ... Alto 1. Soprano 2. 60 65 70 75 80. 0.000.050.100.150.200.25. Soprano 1.

3 Jun 2015: 200. 0. 200. 100. 0. colonyaxis. uÒtur. uq. t = 0 ms 6 ms 12 ms 18 ms 24 ms. ... beats0 200 400 600. no. beats. no. beats0 10 20 30 40 50 0 20 40 60 80 100.

1 May 2015: b) Poly(ethyleneglycol) cylinder at 5, 150, 200, and 250 min. Individual image size: 14cm 4 cm.

24 Mar 2015: Comput. Phys. 200, 299 (2004). [12] D. Leppinen and J. R.

16 May 2015: eH. uH. uyej. 400. 0.5. 0.006 200. –200. –400. 0. 60. ... x (µm)–400 –200 200 4000. –1. 1. –10 –5 0. z (mm).

4 Oct 2015: 200 100 0 100 2000. 0.2. 0.4. 0.6. 0.8. 1. ... For a complete picture of the spectrum consult Figure 7. Notice that the smaller featuresshown here are over 200 times smaller than the elastic peak.

4 Aug 2015: Two additional large connections arepositioned 200 μm away from the narrow channelsallowing pressure equalization between the two reservoirs.For the fabrication of the chips, we use focused ion beam,photolithography, and

4 Aug 2015: Cðx;ZÞð Þdsðx;ZÞ:. (8). The upper and lower boundaries of the domain are discretizedinto 200 straight-line segments, and C and dC/dn are assumedconstant over each element.

25 Sep 2015: r. Ω (r. ad/s. ). ω (rad/s). r. 1 mm. 200 μm. ... 200 μm. 200 μm. AverageInfalling dataSingularity model. t. Figure 6(a) Observations of the hydrodynamic bound state of Volvox.

22 Apr 2015: For instance, even with A 200 and a 0.8, if a sphericalswimmer is initially placed parallel to the surface, the initialdistance from the colloid below which the body is trapped ... 0. A threshold of r 1.5 is chosen in the. Fig. 13 Trapping times Th (with

3 Apr 2015: is 8.14 1017 and for N = 200 the norm is2.211033) and has not been displayed in the figure. ... For N = 200 we have. 21. Option α ‖x̃x‖L1 6.22333 105 1.29 105R1 9.78111 106 7.71 106L2 9.96161 106 7.80 106R2 5.07442 105

4 Aug 2015: Thediameter of the particle (Xanthan gum in the experiment ofRef. [42]) is about 200 μm.

21 Jan 2015: J. Fluid Mech. (2014), vol. 745, pp. 592–620. c Cambridge University Press 2014doi:10.1017/jfm.2014.76. 592. Fluid injection into a confined porous layer. Samuel S. Pegler1,†, Herbert E. Huppert1,2,3 and Jerome A. Neufeld1,4. 1Institute of

21 Jan 2015: J. Fluid Mech. (2014), vol. 757, pp. 330–353. c Cambridge University Press 2014doi:10.1017/jfm.2014.469. 330. Fluid migration between confined aquifers. Samuel S. Pegler1,†, Herbert E. Huppert1,2,3 and Jerome A. Neufeld1,4. 1Institute of

23 Sep 2015: elifesciences.org. RESEARCH ARTICLE. Cortical microtubule nucleation canorganise the cytoskeleton of Drosophilaoocytes to define the anteroposterior axisPhilipp Khuc Trong1,2, Hélène Doerflinger3, Jörn Dunkel1,4, Daniel St Johnston3,Raymond E

15 Jul 2015: CORONAL LOOP VII WORKSHOP Cambridge 21 – 23 July 2015. ABSTRACTS. SESSION 1: Coronal Heating: Global Active Region Models and. Mechanisms. INVITED TALKS. IT1.1 Mahboubeh Asgari-Targhi. Title - Heating Mechanisms (Reconnections vs Waves) Authors:

21 Jan 2015: roughly 1–5 m deep) than the formation itself (roughly 200 mdeep) (Bickle et al.

8 Nov 2015: On the Solvability Complexity Index, the n-Pseudospectrumand Approximations of Spectra of Operators. ANDERS C. HANSENApplied and Computational Mathematics, California Institute of Technology,. hansen@acm.caltech.edu. Abstract. We show that it is

8 Nov 2015: On the Solvability Complexity Index, the n-Pseudospectrumand Approximations of Spectra of Operators. ANDERS C. HANSENApplied and Computational Mathematics, California Institute of Technology,. hansen@acm.caltech.edu. Abstract. We show that it is