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Interactions of vortices with rarefaction solitary waves in a ...
www.damtp.cam.ac.uk/user/ngb23/publications/interact2.pdf25 Jun 2004: p / 4) is shown in Fig. 3. Initially the center of the rarefactionpulse is 20[Fig. ... rarefactionpulses and the straight-line vortex att = 35 that are initially a dis-tance of 20 healing lengths apart. -
Capture of an impurity by a vortex line in ...
www.damtp.cam.ac.uk/user/ngb23/publications/capture.pdf25 Jun 2004: Gross, NuovoCimento 20, 454 1961! 4 C.A. Jones and P.H. Roberts, J. ... Acad. Sci., Ser. III 325, 195. 1997!20 W.H. Raymond and H.L. -
Evolution of rarefaction pulses into vortex rings Natalia G. ...
www.damtp.cam.ac.uk/user/ngb23/publications/evolution.pdf25 Jun 2004: is l 5 20. The solutions starting with the thirdpanel possess vorticity and evolve into equally spaced vortex rings. ... In these computationswe use e 5 0.3 and l 5 60,30,20,15. -
INSTITUTE OF PHYSICS PUBLISHING JOURNAL OF PHYSICS A: MATHEMATICAL ...
www.damtp.cam.ac.uk/user/ngb23/publications/pair.pdf19 Jan 2004: 20 10 0 10 2020. 10. 0. 10. 20. 20 10 0 10 2020. ... 10. 20. 20. 010. 20. 10 20. 0. 0.25. 0.5. 0.75. -
INSTITUTE OF PHYSICS PUBLISHING JOURNAL OF PHYSICS A: MATHEMATICAL ...
www.damtp.cam.ac.uk/user/ngb23/publications/motionIX.pdf8 Oct 2004: 20). Here γ 0.577216 is Euler’s constant. When we approximate (19) for kh 1, we obtain(18). ... Phys. A: Math. Gen. 4 55[19] Saffman P G 1992 Vortex Dynamics (Cambridge: Cambridge University Press)[20] Schwarz K W 1988 Phys. -
IserlesNorsett1.dvi
www.damtp.cam.ac.uk/user/na/NA_papers/NA2004_03.pdf26 Jan 2004: 0. 0.002. 0.004. 0.006. 0.008. 20 40 60 80 100. omega. ... omega. 2e–06. 3e–06. 4e–06. 5e–06. 20 40 60 80 100. omega. -
vtalk.dvi
www.damtp.cam.ac.uk/user/tong/talks/vsvs.pdf29 Nov 2004: The mass of the kink is given by. Mkink = r(χ+ χ) = r(mj mi) (20). ... The 4d theory contains dyons. The 2d theory also contains dyonic kink objects, asfirst noted 10 years ago by Abraham and Townsend [20]. -
Scenario of strongly nonequilibrated Bose-Einstein condensation…
www.damtp.cam.ac.uk/user/ngb23/publications/svist1.pdf25 Jun 2004: Gross,Nuovo Cimento 20, 454 1961!; L.P. Pitaevskii, Sov. Phys.JETP 13, 451 1961! ... 20# C.W. Gardiner et al., Phys. Rev. Lett. 81, 5266 1998!; M.J.Davis, C.W. -
EXPONENTIAL BROWNIAN MOTION AND DIVIDED DIFFERENCES B. J. C. ...
www.damtp.cam.ac.uk/user/na/NA_papers/NA2004_06.pdf14 Jul 2004: obtain. (4.20) r(z) = u[z0] u[z0,. , zn](z z0) (z zn).We obtain (4.17) by equating the coefficients of zn in (4.20) and the product of -
Reconstruction Algorithms for PositronEmission Tomography and Single…
www.damtp.cam.ac.uk/user/na/NA_papers/NA2004_07.pdf11 Oct 2004: 20] B.F. Hutton, Cardiac Single–Photon Emission Tomography: Is Attenuation Correc-tion Enough? ... Prob. 20, 175 (2004). [31] T. Hebert, R. Leahy, M. Singh, Fast MLE for SPECT using an Intermediate PolarRepresentation and a Stopping Criterion, IEEE
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