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18 Oct 2019: Find the condition for population growth/decay. 24. Cop. yri. ght.

14 Nov 2019: foodsources [15–18], behave near boundaries [19–23] and movein complex fluids [24–27]. ... k sin(2k)(13k2 48), (46). mw = 6 cos(2k)(24 48k2 7k4) 4(k6 9k4 36).

6 Feb 2019: 2 |Z3|2), where Zj = X2j1 iX2j.24 of the 48 fermions χabc are dual to tr λZ and obey equations of the form[. ... 2j (4-d). (16). Holographic Fermi surfaces 24 S. Gubser. There are two unrelated reasons for this:.

6 Feb 2019: where k is a free parameter. Cut Mn, =X. 1+2=1Mn1,1Mn2,2. 24/39.

26 Feb 2019: We claim that Θ and Ξ are convex. For Θ. 24.

6 Feb 2019: Geometry and Quantum NoiseJose Barbon. Instituto de Fisica Teorica Madrid, Spain. Eliezer Rabinovici Racah Institute of Physics Hebrew University. Jerusalem, Israel. EUROSTRINGS 2015. 25.03.2015. CMS. Cambridge. a panorama of previous work….

2 Jun 2019: Rev.Fluid Mech., 43 (2011), pp. 1–24. [19] C. C. T. Pringle, Y. ... Rev. E, 78(2008), p. 037301. [24] T. M. Schneider, D. Marinc, and B.

6 Feb 2019: Eurostrings, Cambridge, 24/3/2015. With David Skinner. arxiv:1311.2564, and variouscollaborations with Tim Adamo, Eduardo Casali, Yvonne Geyer,Arthur Lipstein, Ricardo Monteiro & Kai Roehrig, 1312.3828,1404.6219,

27 May 2019: electrohydrodynamics of a cylindrical and helical particle[24,25] (see the Supplemental Material [26] for details). ... Rev. Fluid Mech. 48, 105 (2016).[24] C. Pozrikidis, A Practical Guide to Boundary Element.

6 Nov 2019: This preprint is the final version published in J. Fluid Mech. 881, 182–217 (2019),apart from a few changes dictated by the journal’s house style. 1. Wave–vortex interactions, remote recoil, the1Aharonov–Bohm effect and the2.

6 Feb 2019: theory on the boundary. Embed in string? 24. Further questions. • Far on “moduli space”, got a description with.

27 May 2019: pRR. pTR. 24. 35. lR þlTe lRþlTð ÞtlR þ lT. lT lTe lRþlTð ÞtlR þ lT. ... Tt. :. (24). The MSD follows from a double integration in time of eqn (24),leading to the result.

6 Nov 2019: The following theorem is of crucial importance for MCMC methods. Theorem 1.24. ... until j reaches thedesired sample size J. 24. Example 1.26. We want to sample from the two-dimensional distribution.

16 Jul 2019: 24 2.4. SINGULAR VALUE DECOMPOSITION OF COMPACT OPERATORS. Remark 2.8. Since Eigenvalues of KK with Eigenvectors uj are also Eigenvalues of KK.

16 Jul 2019: 24. 3.2.1 A priori parameter choice rules. 263.2.2 A posteriori parameter choice rules. ... supjN‖Aj‖L(U,V) <. 23. 24 3.2. PARAMETER CHOICE RULES. Theorem 3.1.5. Let U, V be Hilbert spaces, A L(U,V) and {Rα}α>0 a

6 Feb 2019: zf)iCn/Zn (0.24). SEE. = TrX. log X. =. Amin. 4GN. (0.25). ... 1 n log Trn. (0.23). Trn = h. (zi. )(zf)iCn/Zn (0.24).

4 Nov 2019: J. Am. Chem. Soc. 2010; 132:14403. [24] Ghosh A. and Fischer P. ... 1992; 24: 313–58. [55] Purcell E. M. Life at low Reynolds number.

30 Aug 2019: measurements. This gives a non-linear alternative to other methods like generalizedsampling [2, 5, 6, 8, 32, 34, 41] and the Parametrized-Background Data-Weak (PBDW)-method [13, 14, ... This was then further analysed and extended to the PBDW-method by

9 Nov 2019: Received 5 February 1988 and accepted 24 March 1988). Abstract. The parabolic fourth-moment equation is integrated numericallyusing a method based on operator splitting. ... while substitution of (25) into (24) indicates that the height of the peak

6 Feb 2019: Random wall sources in operator-meson correlators. • Correlators fitted between• tmin = 2 4 and tmax = 16 on coarse ensembles• tmin = 4 8 and tmax = 24 on fine ensembles. •