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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: I Minimal unitary representation of E8(24) over L2(R29) from its geometric. ... realization as a quasiconformal group MG, Pavlyk, 2004. E8(24) = 12 561 E7(25) SO(1, 1) 561 12.

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.

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).

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

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 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. •

19 Feb 2019: 2ψ̈ μ4 sin ψ. 1 μ cos ψ[. 24 32. ψ̇ 2 14. ... ε2 = 1 (1 D). (24)We therefore expand. ψ (σ ) = ε[ψ0 (σ ) εψ1 (σ ) ε2ψ2 (σ ) O. (

6 Feb 2019: Townsend: Axion-dilaton Domain Walls and Fake Supergravity CQG 24 (2007]. 2. • ... dynamics of symmetry breaking. 24. • T-reversal invariance means collective mode spectrum (manifested in our example as QNMs) must be symmetric under.

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: and YAKOV SHLAPENTOKH-ROTHMAN. Eurostrings. DAMTP, Cambridge, March 24, 2015. 1. Outline. ... 24. The V -energy theory. To define a forward map which one can indeed hope to show is invertible, we must.

27 May 2019: 24 s. cba. fed. 0 10 20 40300. 0.2. 0.4. 0.6. ... The shaded area starting at time =24 s indicates the duration of motility-deactivation.

6 Feb 2019: C.R. Mafra (DAMTP) Non-linear SYM 25.03.2015 24 / 26. Simpler representation for the 3-loop k4f 4mn.

6 May 2019: h(xF) = h1, (2.11a). h0(xF) = 3h1L. sgd. BL3. 24, (2.11b). ... ĥ =. 24( L̂ x̂)3( x̂) ĥ. ( L̂ x̂)3. L̂3, (2.21).

6 Feb 2019: 24/26. Summary I. The superspace approach to supergravity forms is based onconsistent, soluble sets of Bianchi identities.

28 Aug 2019: in spacetime such that they satisfy the operator equation. @. @t= i[H, ] (5.24). ... Figure 23: An incoming anti-fermion Figure 24: An outgoing anti-fermion. • Each vertex gets a factor of i. •

6 Feb 2019: Matthias Gaberdiel ETH Zürich. based mainly on. Eurostrings, Cambridge 24 March 2015.