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Introduction to Optimal Transport Matthew Thorpe F2.08, Centre for ...
www.damtp.cam.ac.uk/research/cia/files/teaching/Optimal_Transport_Notes.pdf26 Feb 2019: We claim that Θ and Ξ are convex. For Θ. 24. -
2. Free Fields “The career of a young theoretical ...
www.damtp.cam.ac.uk/user/tong/qft/two.pdf28 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. -
DOI 10.1140/epje/i2018-11728-2 Regular Article Eur. Phys. J. E (2018) …
www.damtp.cam.ac.uk/user/lauga/papers/153.pdf14 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). -
Slide 1
www.damtp.cam.ac.uk/research/hep/files/conferences/EurostringTalks/Aharony.pdf6 Feb 2019: theory on the boundary. Embed in string? 24. Further questions. • Far on “moduli space”, got a description with. -
This preprint is the final version published in J. ...
www.damtp.cam.ac.uk/user/mem/papers/AB/wave-vortex19-jfm-rev2-web-191004-in-press.pdf6 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. -
Active Particles Powered by Quincke Rotation in a Bulk Fluid
www.damtp.cam.ac.uk/user/lauga/papers/162.pdf27 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. -
Bayesian Inverse ProblemsLecture notes, Lent term 2019 University of…
www.damtp.cam.ac.uk/research/cia/files/teaching/Inverse_Problems_Lent_2018/19y_01m_16d_LectureNotes.pdf6 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. -
Inverse Problems Matthias J. Ehrhardt and Lukas F. Lang ...
www.damtp.cam.ac.uk/research/cia/files/teaching/Inverse_Problems_Lent_2018/lecture_notes_20180313.pdf16 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. -
Can the supersymmetric backgrounds be classified?
www.damtp.cam.ac.uk/research/hep/files/conferences/branes/pkt_talks/papadopoulos.pdf6 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 -
Inverse Problems in Imaging Yury Korolev Last updated on: ...
www.damtp.cam.ac.uk/research/cia/files/teaching/Inverse_Problems_Michaelmas_2018/lecture_notes_current.pdf16 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 -
A stochastic model for bacteria-driven micro-swimmers
www.damtp.cam.ac.uk/user/lauga/papers/158.pdf27 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. -
Anomalies and Gaps in HEE Alejandra Castro EuroStrings 2015 ...
www.damtp.cam.ac.uk/research/hep/files/conferences/EurostringTalks/Castro.pdf6 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). -
JOURNAL OF MODERN OPTICS, 1988, VOL . 35, NO. ...
www.damtp.cam.ac.uk/user/ms100/PAPERS/JModOpt88.pdf9 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 -
Extracting B physics from lattice simulations via lattice…
www.damtp.cam.ac.uk/research/hep/files/conferences/trentobeauty/CJMonahan.pdf6 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. • -
Nonlinear and nonlocal elasticity in coarse-grained…
www.damtp.cam.ac.uk/user/gold/pdfs/epithelia.pdf19 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. ( -
Multiparticle superfields and superstring amplitudes
www.damtp.cam.ac.uk/research/hep/files/conferences/EurostringTalks/Mafra.pdf6 Feb 2019: C.R. Mafra (DAMTP) Non-linear SYM 25.03.2015 24 / 26. Simpler representation for the 3-loop k4f 4mn. -
Z:\03-Pagination\UK\Bocquet\ApplicationFiles\book.dvi
www.damtp.cam.ac.uk/user/lauga/papers/78.pdf4 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. -
Forms and algebras in supergravity
www.damtp.cam.ac.uk/research/hep/files/conferences/branes/pkt_talks/howe.pdf6 Feb 2019: 24/26. Summary I. The superspace approach to supergravity forms is based onconsistent, soluble sets of Bianchi identities. -
Self-organization of swimmers drives long-range fluid transport in…
www.damtp.cam.ac.uk/user/lauga/papers/159.pdf27 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. -
dynamics of symmetry breaking with Joe Bhaseen, Ben Simons, ...
www.damtp.cam.ac.uk/research/hep/files/conferences/branes/pkt_talks/sonner.pdf6 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. -
DAMTP/?? October 21, 2019 Lectures on Conformal Field Theories ...
www.damtp.cam.ac.uk/user/ho/CFTNotes.pdf21 Oct 2019: Such invariants need four points as in (2.24). 20. 3.1 Scalar and Vector Fields on the Null Cone. ... so that SAB, S̄AB have the same Lie algebra as LAB in (3.24). -
DAMTP?2015.dvi
www.damtp.cam.ac.uk/research/hep/files/conferences/EurostringTalks/Dafermos.pdf6 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. -
J. Fluid Mech. (2018), vol. 841, pp. 989–1011. c� ...
www.damtp.cam.ac.uk/user/jneufeld/pubfiles/Box-2018a.pdf6 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). -
5. Quantizing the Dirac Field We would now like ...
www.damtp.cam.ac.uk/user/tong/qft/five.pdf28 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. • -
Cambridge15
www.damtp.cam.ac.uk/research/hep/files/conferences/EurostringTalks/Gaberdiel.pdf6 Feb 2019: Matthias Gaberdiel ETH Zürich. based mainly on. Eurostrings, Cambridge 24 March 2015. -
Hydrodynamics of bacteriophage migration along bacterial flagella
www.damtp.cam.ac.uk/user/lauga/papers/156.pdf22 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]. -
Scattering in Susy large N Chern Simons Theory
www.damtp.cam.ac.uk/research/hep/files/conferences/EurostringTalks/Minwalla.pdf6 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 -
5 Non-Linear Sigma Models in d = 1 + ...
www.damtp.cam.ac.uk/user/dbs26/SUSY/chap5.pdf28 Apr 2019: 5.24). for a flat worldsheet metric. The first term gives the usual 1/k2 propagator in 2d momentum. -
Trento, Beautiful Mesons and Baryons on the Lattice A. ...
www.damtp.cam.ac.uk/research/hep/files/conferences/trentobeauty/Lenz_Trento.pdf6 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. -
DOI 10.1140/epje/i2015-15007-6 Regular Article Eur. Phys. J. E (2015) …
www.damtp.cam.ac.uk/user/lauga/papers/104.pdf14 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). -
What do AI algorithms actually learn? – On false ...
www.damtp.cam.ac.uk/research/afha/anders/False_Structures_DL.pdf4 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. -
Exact Coherent States: Theory &Methods Rich Kerswell Lectures 1…
www.damtp.cam.ac.uk/user/rrk26/Udine_LT12_RRK.pdf2 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. -
A Compact Eulerian Representation of Axisymmetric Inviscid Vortex…
www.damtp.cam.ac.uk/user/gold/pdfs/eulerian.pdf18 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.; -
NON-UNIFORM RECOVERY GUARANTEES FOR BINARY MEASUREMENTS…
www.damtp.cam.ac.uk/research/afha/anders/main_Thesing.pdf30 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 -
Method of regularized stokeslets: Flow analysis and improvement of…
www.damtp.cam.ac.uk/user/lauga/papers/166.pdf30 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]. -
Trento12.dvi
www.damtp.cam.ac.uk/research/hep/files/conferences/trentobeauty/seth_Trento12.pdf6 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. -
Exact Coherent States: VariationalMethods Rich Kerswell Lectures 5…
www.damtp.cam.ac.uk/user/rrk26/Udine_LT56_RRK.pdf2 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 -
B-meson physics with dynamical domain-wall light quarks and…
www.damtp.cam.ac.uk/research/hep/files/conferences/trentobeauty/witzel_oliver.pdf6 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. -
The near and far of a pair of magnetic capillary disks
www.damtp.cam.ac.uk/user/lauga/papers/157.pdf27 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. -
Exclusive semileptonic B and b decays at large hadronic recoil
www.damtp.cam.ac.uk/research/hep/files/conferences/trentobeauty/Khodjamirian.pdf6 Feb 2019: Wang arXiV:1108.2971]. Alexander Khodjamirian Exclusive semileptonic B and Λb decays at large hadronic recoil 24 / 37. -
J. Fluid Mech. (2018), vol. 837, pp. 520–545. c� ...
www.damtp.cam.ac.uk/user/jneufeld/pubfiles/Nijjer-2018a.pdf6 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. -
Computing the motor torque of Escherichia coli
www.damtp.cam.ac.uk/user/lauga/papers/149.pdf14 Nov 2019: Boundary element methods have long been usedto study problems in bacteria locomotion including flagellarpropulsion,23 interaction between two swimming bacteria,24. -
EuroStrings2015.key
www.damtp.cam.ac.uk/research/hep/files/conferences/EurostringTalks/Dabholkar.pdf6 Feb 2019: 12 -208 208.455 53252. 15 513 512.958 192401. 23. ATISH DABHOLKAR QUANTUM ENTROPY OF BLACK HOLES 24. • -
The N-flagella problem: elastohydrodynamic motility transition of…
www.damtp.cam.ac.uk/user/lauga/papers/161.pdf27 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. -
D6 R4
www.damtp.cam.ac.uk/research/hep/files/conferences/EurostringTalks/Vanhove.pdf6 Feb 2019: Pierre Vanhove (IPhT & IHES) D6 R4 Cambridge March 2015 24 / 37. -
9 Perturbation Theory II: Time Dependent Case In this ...
www.damtp.cam.ac.uk/user/dbs26/PQM/chap9.pdf4 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. -
Bootstrapping the (2,0) theories in six dimensions
www.damtp.cam.ac.uk/research/hep/files/conferences/EurostringTalks/VanRees.pdf6 Feb 2019: O1(x1)O2(x2)O3(x3)O4(x4)〉. =k. λ k12λk. 34@. @k=p. λ p13λp. 24. @. @p. -
Geophys. J. Int. (2019) 218, 247–267 doi: 10.1093/gji/ggz139Advance…
www.damtp.cam.ac.uk/user/jneufeld/pubfiles/Ball-2019.pdf22 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. -
Universal optimal geometry of minimal phoretic pumps
www.damtp.cam.ac.uk/user/lauga/papers/165.pdf20 Oct 2019: 339,. 936–940 (2013). 24. Duan, W. et al. Synthetic nano- and micromachines in analytical chemistry: sensing, migration, capture, delivery and separation. -
B-meson and Bottomonium spectroscopy from radiatively improved NRQCD
www.damtp.cam.ac.uk/research/hep/files/conferences/trentobeauty/Dowdall-trento2012-v2.pdf6 Feb 2019: 6.2. 6.21. 6.22. 6.23. 6.24. 6.25. 6.26. 6.27. 6.28. 6.29. 6.3.
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