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

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).

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: 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. •

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.

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: 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.

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: 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].

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.

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: 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

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.

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

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: 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.

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].

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.

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.

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

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

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: 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.

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: 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.

6 May 2019: 44. 40C. 08:0. 1:4. 07. DD. D 2. 01. 834. 24. ... 01. 834. 24. 4. 530 J. S. Nijjer, D. R. Hewitt and J.

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

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.

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

22 Jul 2019: ic.oup.com/gji/article-abstract/218/1/247/5382046 by U. niversity of Cam. bridge user on 24 June 2019. ... bridge user on 24 June 2019. Evolution of thin-skinned fold-thrust belts 257.

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

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.

6 Feb 2019: O1(x1)O2(x2)O3(x3)O4(x4)〉. =k. λ k12λk. 34@. @k=p. λ p13λp. 24. @. @p.

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: Chetyrkin et al. 2009. mb(mb) [GeV]. 4.64.44.24. I ETMC mb error bugdet. •

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

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

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