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On structure and optimisation in computationalharmonic analysis - The …
www.damtp.cam.ac.uk/research/afha/people/anders/Springer_Harm_Analysis2019.pdf6 May 2019: 20] A. Cohen, W. Dahmen, and R. DeVore. Compressed sensing and best k-termapproximation. ... Mathematical problems for the next century. Mathematical Intelli-gencer, 20:7–15, 1998. [51] S. -
Solving Wiener–Hopf Type Problems NumericallyA Spectral Method…
www.damtp.cam.ac.uk/user/mjc249/talks/WH_talk_mjc.pdf15 Aug 2019: 1 x2 Un(x). Rapid Convergence! 0 20 40 60 80 100 12010-15. ... Infinite Plate Example. 0 5 10 15 20 25 30 35 40 4510-14. -
Cheng.key
www.damtp.cam.ac.uk/research/hep/files/conferences/EurostringTalks/Cheng.pdf6 Feb 2019: 50 100 150 200 250 300D(n,l). 20. 40. 60. 80. 100. ... 10 20 30 40x. 10. 20. 30. 40. 50. logc(0,N - x). -
15_Cambridge
www.damtp.cam.ac.uk/research/hep/files/conferences/EurostringTalks/Gauntlett.pdf6 Feb 2019: 050. 10. 20. 30. 40. 50. 60. ω/μ. Re(σ). Find Drude peaks at low T. ... 00. 20. 40. 60. 80. 100. ω/k. ReG. 11/k4. T/k=0.14. T/k=0.3. T/k=0.5. -
The Unified TransformA New Tool for Scattering Problems Matthew ...
www.damtp.cam.ac.uk/user/mjc249/talks/Waves_talk2.pdf30 Apr 2019: 1 (2x 1)2 Un(2x 1). Rapid Convergence! 0 20 40 60 80 100 12010-15. ... Radiated Power. 10 20 30 40 50 60 70 80 90 100. -
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: p2/(2πL)2 E 20. 0 1 2 3 4 50. 0.05. 0.1. ... 10.20. 10.40. 0 5 10 15 20. Z Vbb. time slice. -
Active Particles Powered by Quincke Rotation in a Bulk Fluid
www.damtp.cam.ac.uk/user/lauga/papers/162.pdf27 May 2019: The normal compo-nent of the electric field En nE undergoes a jump dueto the mismatch in electrical properties between the twomedia [20], resulting in a surface charge distribution givenby ... 111 (1969).[20] L. D. Landau, L. P. Pitaevskiì, and E. M. -
4. Phonons Until now, we’ve discussed lattices in which ...
www.damtp.cam.ac.uk/user/tong/aqm/aqmfour.pdf19 Jul 2019: as(k) and a†s(k) in (4.20) also become operators. To proceed, we need the momentum. ... classical dynamics,. i(x) =@L. @u̇i= u̇i. Written in terms of the solution (4.20), we have. -
B-physics calculations from Lattice QCD by ETM Collaboration
www.damtp.cam.ac.uk/research/hep/files/conferences/trentobeauty/Dimopoulos.pdf6 Feb 2019: point. β = 4.20. β = 4.05. β = 3.90. β = 3.80. ... 0.35. 0.30. 0.25. 0.20. CL - phys. point. β = 4.20. -
Cop yri ght c ©20 19U niv ersi tyof ...
www.damtp.cam.ac.uk/research/dd/files/teaching/MB17Gog.pdf18 Oct 2019: 1. 2. 3. 4. a = 5 b=60. 0 20 40 60 80 1000. ... 0 10 20 30 40 50. αβ =. 0 10 20 30 40 50.
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