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

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 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).

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.

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

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.

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: 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. •

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

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.

4 Jun 2019: J. Amer. Math. Soc., 24(1):81–124, 2011. [13] K. H. Jin, M. ... In IEEE Symposium on Securityand Privacy, pages 582–597. IEEE, 2016. [24] M.

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: 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

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. •

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

14 Nov 2019: Phys. J. E (2015) 38: 7. portant similarities with self-thermophoresis [24] or theself-propulsion of droplets through Marangoni effects, forwhich the slip velocity is replaced with a surface shearstress discontinuity ... 1 µ cosh τcosh τ µ eρ, (24).

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.

22 Jan 2019: In Ref. [24], electronmicroscopy images of the flagellotropic χ phage, shown in Figs. ... coli [24]. The head measures 65–67.5 nm between the parallel sides ofthe hexagon [24].

14 Nov 2019: Boundary element methods have long been usedto study problems in bacteria locomotion including flagellarpropulsion,23 interaction between two swimming bacteria,24.

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

28 Apr 2019: 5.24). for a flat worldsheet metric. The first term gives the usual 1/k2 propagator in 2d momentum.

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.

30 Oct 2019: 24). This requires B(r) and S(r) to have the same Taylor expansion aroundthe point of interest, r. ... 39). The above integral is the single-layer boundary integral representation for flow around a translatingsphere [24].

6 Feb 2019: 16. DαΓβ{Γα, Γβ}1. 24{Γα, Γβ}{Γα, Γβ}. ) 1. 2(DαΦ̄ i Φ̄Γα)(DαΦ i ΓαΦ) m0Φ̄Φ. ... 24). Shiraz Minwalla. Duality. It is not too difficult to verify that the S matrices above mapto themselves under the duality map, if we also

18 Dec 2019: The predominant approach to this problem has been througha Lagrangian formulation [3, 10], which is the most appropriate for computationalstudies [2, 24, 29, 30]. ... Phys. 203 (2005), no. 2, 539–571. doi:10.1016/j.jcp.2004.08.023. [24] Hou, T. Y.;

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

27 May 2019: Typical curves for the near-field capillaryforce, eqn (24), and the magnetic attraction, eqn (25), areshown in Fig. ... 6c. As expected eqn (25) shows a linear increase. while eqn (24) decreases monotonically allowing for a singlemean separation.

6 Feb 2019: δ(BBs) 2.7% 6.6%. δ 24.5% 40.5%. Trento, Beautiful Mesons and Baryons on the Lattice A. ... 1995 ALEPH Λcl 1.02 0.24 0.67 0.16. 1992 ALEPH Λcl 1.12 0.37 0.74 0.24.

4 Dec 2019: t0〈k||m〉eiωkmt′ dt′ = km. Ek Em(1 eiωkmt. ), (9.24). where km = 〈k||m〉 and ωkm = (Ek Em)/. ... k|†|m〉(ωkm ω). [ei(ωkmω)t 1. ]. (9.32). This is very similar to our result (9.24), with the time–dependence of the perturbation.

2 Jun 2019: Re2L =1708. 24[2(1 2)](13). can be made. The minimum of ReL occurs when = 1/4 and is. ... un1 = un J1F(un,Re) (24). where Jij := Fi/uj is the Jacobian and is an NT NT sized complex matrix.

10 Apr 2019: Moreover, we have for the transform, that it is linear:. W {af(x) bg(x)} = aW {f(x)} bW {g(x)} a,b R, f,g L2([0, 1]d), ... 5.1 Classical compressed sensing. Compressed sensing was introduced by Candès, Romberg & Tao (19) and Donoho (24)and is

27 May 2019: Despite these variations, acoherent flagellar bundle is expected to be maintained generically by long-range hydrodynamicinteractions [24,25]. ... 2.24). For a symmetric configuration such that (N. i=1 ω̃(i)t Ri) ez = 0, only the first term of Mprop.

6 Feb 2019: Unquenched calculation. Northwestern University 24 K. K. Seth. Lattice at Trento April 2–6, 2012. ... RBC-UKQCD (2010) 60 8 MeV 24 5 MeV. HPQCD (2012) 70 9 MeV 35 3 MeV.

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: Pierre Vanhove (IPhT & IHES) D6 R4 Cambridge March 2015 24 / 37.

28 Aug 2019: where µsatisfies. µ. = µ (1.24). For example, a rotation by about the x3-axis, and a boost by v < 1 along the x1-axis. ... transformations. µ= µ! µ. (1.49). where! µis infinitesimal. The condition (1.24) for to be a Lorentz transformation.

2 Jun 2019: ν = 0 at boundary, (24). ν = 0. (25). Now, considering variations in u (with the condition that δu = 0 on the boundary): T0. ... Step.3 Backwards time integrate the dual linearized Navier-Stokes equation (35)with incompressibility (25) and boundary

6 Feb 2019: Wang arXiV:1108.2971]. Alexander Khodjamirian Exclusive semileptonic B and Λb decays at large hadronic recoil 24 / 37.

20 Oct 2019: 339,. 936–940 (2013). 24. Duan, W. et al. Synthetic nano- and micromachines in analytical chemistry: sensing, migration, capture, delivery and separation.

6 Feb 2019: timeL a(fm) ml ms mπ(MeV) # configs. sources. 24 0.11 0.005 0.040 331 1636 124 0.11 0.010 0.040 419 1419 132 0.08 ... EeffBs = 3.1025(12), χ2/dof = 0.41, p = 98% I L = 24.

19 Jul 2019: qg = 2n with n 2 Z (1.24). This is the famous Dirac quantisation condition. ... qg = 2n with n 2 Z. This, of course, is the Dirac quantisation condition (1.24).

6 Feb 2019: 12 -208 208.455 53252. 15 513 512.958 192401. 23. ATISH DABHOLKAR QUANTUM ENTROPY OF BLACK HOLES 24. •

11 Jul 2019: X12. X34. X24. X13 X14. 23. 21. 12. 32. 14 24.

5 Nov 2019: J. 24, 6308–6324 (2018). 24. Moran, J. L. & Posner, J.

6 Dec 2019: ca,β ca′,β. (10.24). If the original state |Ψ〉 was simple, so that (say) the ca,β are non–zero only for a singlevalue of β, for which ca, ... However, if |Ψ〉 is a more general, entangledstate then the sum in (10.24) means that ρA is the

11 Jul 2019: D′ψC′D′E′F′ψE′F′. A′B′ , (2.24). which are in general independent. We verify by explicit calculation that if ψABCD and ψA′B′C′D′ arise from ... Proposition 2.3. Let I, J, I′, J′ be the invariants (2.24) of the Weyl