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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.

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].

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.

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.

18 Dec 2017: µ = 0. (3.24). This ensures that (3.3) implies. MµνΦϕ = LµνΦϕ , PµΦϕ = µΦϕ. ... Θµν =1. z. (µΦϕ νΦϕ. 1. 2δµν λΦϕ λΦϕ. d 24(d 1). (

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.