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25 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.

26 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.

19 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.

8 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.

29 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].

25 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.

14 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

11 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

25 Mar 2004: . . . 0 0 0 20 0 2 00 2 0 02 0 0 0.

14 Nov 2004: . . . . (4.20). The technique of the previous paragraph is employed only if at least one ofthe signs sk, k = 1, 2,. , ... We. 20. write t instead of MOVE, in order to retain the notation of Section 4.