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28 Oct 2010: This isremarkable since localizing a nanopore would require tag-ging with fluorescent dyes, measuring the scattered lightfrom the nanopore edge in an optical microscope, or usingscanning ion conductance microscopy.23,24. ... preparation. The buffer can

22 Nov 2010: 12 16 20 24 28 32 360.00. 0.05. 0.10. 0.15. 0.20. ... 15+ 16+ 17+ 18+ 19+ 20+ 21+ 22+ 23+ 24+ 25+ 26+ 27+ 28+.

12 Nov 2010: Spectral theory of large Wiener–Hopf operators with. complex-symmetric kernels and rational symbols. Albrecht Böttcher Sergei Grudsky Arieh Iserles. November 12, 2010. AbstractThis paper is devoted to the asymptotic behaviour of individual

22 Oct 2010: J. 80, 3009–3018 (2001). 24. Garcia, R. & Perez, R. Dynamic atomic force microscopy methods.

22 Jul 2010: 2 4 ) (2.24 b - d ). - - - a= = a , " = vL, DLo, = DLTp. ... It is closely related t o the approximate equation (24) of Dewar (1970); i t also contains Bretherton’s form of Kelvin’s circulation theorem, and indeed the details of

13 Nov 2010: of the complexes (18, 85), probe local molecular conformations of DNA by use of specific anti- bodies (55), and follow protein-nucleic acid interactions in buffer (24).

18 Nov 2010: Quarterly Reviews of Biophysics 25, 2 (1992), pp. 171-204 171Printed in Great Britain. Problems and prospects in the theory of gelelectrophoresis of D N A. BRUNO H. ZIMM AND STEPHEN D. LEVENEDepartment of Chemistry, University of California (San

4 Oct 2010: Dünweg, and C. Holm, J. Phys.: Condens. Matter 16,4063 2004. 24 K.

27 Oct 2010: 24 M. S. JOSHI AND A. J. WASSERMANNFor f 2 L1(Rn); (see appendix) dene the Fourier transform f̂ byf̂() = 1(2)n=2 Z eix:f(x)dx

23 Mar 2010: 24. Everything is relative. This slide shows the city’s tall buildings set against a heavily compressed section of the city showing, on the left, Castle Hill, and, on the right,

10 Nov 2010: Dr. Gosse’s present address is Institut Curie, Paris, France. E-mail:charlie.gosse@curie.fr. Address reprint requests to Vincent Croquette, Laboratoire de PhysiqueStatistique, École Normale Supérieure, 24 rue Lhomond, ... and, using Eq. 20,. Bu

30 Oct 2010: the applied force, the loadingrate varies as the molecule is stretched and Equation 17 cannot be used directly(22, 24).

22 Nov 2010: MULTI-TEMPERATURE MODEL FOR POST-ERUPTIVE CORONAL LOOPS. OBSERVED AT THE EUV-RANGE AND MICROWAVES M.A Livshits, Pushkov Institute of Terrestrial Magnetism, Ionosphere and Radio Wave Propagation of Russian Academy of Sciences, Troitsk A.M. Urnov,

4 Oct 2010: Electrophoresis of DNA and other polyelectrolytes:Physical mechanisms. Jean-Louis Viovy. Laboratoire Physico-Chimie Curie (UMR CNRS 168), Institut Curie Section de Recherche,26 Rue d’Ulm, 75230 Paris cedex 05, France. The dramatic recent advances

4 Oct 2010: 3. 2. ηe. εrsε0kTue = 3. 2yek. (24) 6[ yek. 2 ln 2z {1 exp(zyek)}]. ... Henry [24]gave two series expansions for the function f1, one forsmall κa and one for large κa.

2 Feb 2010: g(p) dp = g(ε) dε. (4.1.9). 4 IDEAL GAS 24. Most of the time we will be discussing gases of nonrelativistic particles, for which.

22 Nov 2010: Slide 19. Slide 20. Slide 21. Slide 22. Slide 23. Slide 24.

28 Oct 2010: REVIEW OF SCIENTIFIC INSTRUMENTS VOLUME 75, NUMBER 9 SEPTEMBER 2004. REVIEW ARTICLE. Optical trappingKeir C. Neuman and Steven M. Blocka). Department of Biological Sciences, and Department of Applied Physics, Stanford University,Stanford, California

10 Sep 2010: Much cited result - still 30 pa. L&L 1959. 24. a startStress system in a suspension of force-free particles JFM 1970.

4 May 2010: This is the averaged system. proposed in [24], and it can be solved using standard procedures. ... Indeed, there are profound connections between ourapproach and theheterogeneous multiscale method [2, 13, 24].

22 Dec 2010: Perhaps the first work to point clearly to that fact was thestudy reported in [24], in which a surface temperature frontwas prevented from col-lapsing by applying an artificial diffusivity, holding ... J. Atmos. Sci.64, 4417–4431 (2007). [24] Snyder, C.

19 Feb 2010: 0 for T Tc(8.3.24). Therefore (CV /T)V,N has a term proportional to (2µ/T 2)V,N and is discontin-.

23 Sep 2010: The distributions constitute a filtration, that is. C C. 5C 6C = T J 6 (24). ... ȳ1 = DȳDx̄. The contact transformation preserves the whole filtration (24).Now consider the seventh-order ODE (18).