Collective Modes in Vortex Ring Beams

  • G. Gamota


The existence of quantized vortex rings was conjectured by Feynman1 in his discussion of superfluid helium, but it was not until several years later that Rayfield and Reif2 first identified a charged vortex ring in He II. Since then many experiments dealing with the individual properties of vortex rings were performed and a report on these can be found in a recent review article.3 In this work we are interested in investigating phenomena arising from the mutual interactions among charged vortices. We seek plasmalike effects that can be found in a gas made up of individual charged vortex rings. The conjecture of such a phenomenon was first made by Careri.* The initial work on the gaslike properties of charged vortices, referred to as dc experiments, was reported earlier.5 There it was shown that a single pulse of charged vortices does not smear out as would a pulse of, say, electrons in a vacuum, but in fact compresses longitudinally until it reaches a steady-state distribution. The final width of this “bell”-shaped distribution was found to be rather insensitive to the initial width of the pulse as well as the energy. Hasegawa and Varma6 explained this behavior by a simple one-dimensional theory which assumed that the vortices acted as particles in a gas. The theory includes the Coulomb interaction among the vortices as well as pressure due to fluctuations. They assume that the vortices are, in fact, not monoenergetic but that there exists a distribution whose average value is equal to the accelerating energy given to the beam.† The subsequent work, referred to as the ac experiments and reported here, involves the study of collective modes of oscillation of these vortex beams which also arise from the above interactions. Again Hasegawa and Varma6 take a one-dimensional picture but use the Vlasov equation, instead of the fluid equation used earlier, to write a phase-space distribution function f (x, p, t). This is solved and a wave dispersion relation is found which shows that an instability in the wave would occur if k was below a critical wave number k c . Due to this instability the wave is expected to grow as a function of the propagation distance.


Vortex Ring Collective Mode Vlasov Equation Superfluid Helium Vortex Beam 
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  1. 1.
    R.P. Feynman, in Progress in Low Temperature Physics,C.J. Gorter, ed., North-Holland, Amsterdam (1955), vol. I,Chapter II.Google Scholar
  2. 2.
    G.W. Rayfield and F. Reif, Phys. Rev. Lett. 11, 305 (1963);ADSCrossRefGoogle Scholar
  3. G.W. Rayfield and F. Reif, Phys. Rev. 136, A1194 (1964).ADSCrossRefGoogle Scholar
  4. 3.
    G. Gamota, J. Phys. (Paris), Colloq. C3, 39 (1970).Google Scholar
  5. 4.
    G. Careri, in Liquid Helium, Proc. Intern. School of Physics “Enrico Fermi”, Academic Press, New York (1963), Vol. XXI.Google Scholar
  6. 5.
    G. Gamota, A. Hasegawa, and C.M. Varma, Phys. Rev. Lett. 26, 960 (1971).ADSCrossRefGoogle Scholar
  7. 6.
    A. Hasegawa and C.M. Varma, Phys. Rev. Leu. 28, 1689 (1972).ADSCrossRefGoogle Scholar
  8. 7.
    G. Gamota, Phys. Rev. Lett. 28, 1691 (1972).ADSCrossRefGoogle Scholar
  9. 8.
    A.B. Basset, A Treatise on the Motion of Vortex Rings, MacMillan, London (1883).Google Scholar

Copyright information

© Springer Science+Business Media New York 1974

Authors and Affiliations

  • G. Gamota
    • 1
  1. 1.Bell LaboratoriesMurray HillUSA

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