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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:.

28 Aug 2019: with it. In fact there are two dierent 1’s lurking in the expression (2.24). ... 25 –. We can deal with the infinity in (2.24) in a more practical way.

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

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,

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

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….

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

18 Oct 2019: Example sheet 1 Presentation 28 October 2019, 2-3:30pm, MR15.Please submit after the lecture on 24 October 2019.

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 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: 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 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.

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

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: I The number of supersymmetries preserved [Duff] are. 1, 2, 3, 4 , 5, 6, 8, 10, 12, 14, 16, 18, 20, 22, 24, 26, 28, 32. ... I Backgrounds preserving more than 24 supersymmetries arehomogenous [Figueroa-O’Farrill]. Classification D = 4 Heterotic

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.

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).