Evolution of Alfvénic wave envelopes in spin-1/2 quantum Hall-magnetohydrodynamic plasmas
Phys. Plasmas 16, 102309 (2009); doi:10.1063/1.3250987
Published 28 October 2009
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The one-dimensional oblique propagation of large amplitude magnetohydrodynamic (MHD) waves in a high-
quantum Hall-MHD plasma is studied with electron spin-1/2 effects. The plasma
becomes high by the condition for the nonrelativistic fluid model to be valid and the condition for the collective effects to be important in quantum plasmas. Such a high-
value is a prerequisite for large perturbations of the perpendicular magnetic field comparable with the longitudinal magnetic field. It is shown that the nonlinear evolution of such waves is described by a derivative nonlinear Schrödinger (DNLS) equation. It is found that the DNLS equation does not depend on the higher order quantum coupling associated with the Bohm potential, rather the pressure such as spin force plays the crucial role. Such an evolution equation is shown to admit spin-modified localized envelope solitons whose width L is reduced by
2/v
and the amplitude increases with increasing
2/v
values, where
is the temperature normalized Zeeman energy and v
is the electron thermal energy normalized by the Alfvén wave energy. Moreover, the MHD waves are found to be modulationally unstable for a wave number exceeding its critical value, which typically depends on
2/v
. The growth rate of the modulational instability is also investigated. Furthermore, the effect of dissipation due to plasma resistivity is shown to exhibit envelope shocklike structures instead of envelope solitons. The present nonlinear excitations can account for large scale structures in dense astrophysical plasma environments.
©2009 American Institute of Physics
quantum Hall-MHD plasma is studied with electron spin-1/2 effects. The plasma
becomes high by the condition for the nonrelativistic fluid model to be valid and the condition for the collective effects to be important in quantum plasmas. Such a high-
value is a prerequisite for large perturbations of the perpendicular magnetic field comparable with the longitudinal magnetic field. It is shown that the nonlinear evolution of such waves is described by a derivative nonlinear Schrödinger (DNLS) equation. It is found that the DNLS equation does not depend on the higher order quantum coupling associated with the Bohm potential, rather the pressure such as spin force plays the crucial role. Such an evolution equation is shown to admit spin-modified localized envelope solitons whose width L is reduced by
2/v
2/v
is the temperature normalized Zeeman energy and v
2/v| History: | Received 24 August 2009; accepted 29 September 2009; published 28 October 2009 |
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1070-664X (print)
1089-7674 (online)
REFERENCES (39)
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- A. Rogister, Phys. Fluids 14, 2733 (1971).
- E. Mjølhus,
J. Plasma Phys. 16, 321 (1976) . - K. Mio, T. Ogino, K. Minami, and S. Takeda,
J. Phys. Soc. Jpn. 41, 265 (1976) . - S. R. Spangler and J. P. Sheerin,
J. Plasma Phys. 27, 193 (1982) . - J. I. Sakai and B. U. Ö. Sonnerup,
J. Geophys. Res. 88, 9069, doi:10.1029/JA088iA11p09069 (1983) . - Nonlinear Waves and Chaos in Space Plasmas, edited by T. Hada and H. Matsumoto (Terra, Tokyo, 1997), pp. 121–169.
- S. R. Spangler, in Nonlinear Waves and Chaos in Space Plasmas, edited by T. Hada and H. Matsumoto (Terra, Tokyo, 1997), pp. 171–223.
- B. Buti, V. L. Galinski, V. I. Shevchenko, G. S. Lakhina, T. Tsurutani, B. E. Goldstein, P. Diamond, and M. V. Medvedev,
Astrophys. J. 523, 849 (1999) . - P. K. Shukla and L. Stenflo, Phys. Plasmas 12, 084502 (2005).
- M. S. Ruderman,
J. Plasma Phys. 67, 271 (2002) . - M. S. Ruderman, Phys. Plasmas 9, 2940 (2002).
- P. K. Shukla and F. Verheest,
Astron. Astrophys. 401, 849 (2003) . - E. Mjølhus,
Phys. Scr. 40, 227 (1989) . - A. A. Mamun,
Phys. Scr. 60, 365 (1999) . - B. P. Pandey, S. V. Vladimirov, and A. Samarian, Phys. Plasmas 15, 053705 (2008).
- M. Marklund, G. Brodin, L. Stenflo, and C. S. Liu,
Europhys. Lett. 84, 17006 (2008) . - G. Manfredi and P. A. Heryieux, Appl. Phys. Lett. 91, 061108 (2007).
- W. Li, P. J. Tanner, and T. F. Gallagher, Phys. Rev. Lett. 94, 173001 (2005).
- A. K. Harding and D. Lai,
Rep. Prog. Phys. 69, 2631 (2006) . - F. Haas, Phys. Plasmas 12, 062117 (2005).
- A. P. Misra and P. K. Shukla, Phys. Rev. E 79, 056401 (2009).
- A. P. Misra, C. Bhowmik, and P. K. Shukla, Phys. Plasmas 16, 072116 (2009).
- A. P. Misra, Phys. Plasmas 16, 033702 (2009).
- G. Manfredi and F. Haas, Phys. Rev. B 64, 075316 (2001).
- F. Haas, L. G. Garcia, J. Goedert, and G. Manfredi, Phys. Plasmas 10, 3858 (2003).
- P. K. Shukla,
Nat. Phys. 5, 92 (2009) . - A. P. Misra, Phys. Plasmas 14, 064501 (2007).
- P. K. Shukla and B. Eliasson, Phys. Rev. Lett. 96, 245001 (2006)
- P. K. Shukla,
Phys. Lett. A 352, 242 (2006) . - A. P. Misra and N. K. Ghosh,
Phys. Lett. A 372, 6412 (2008) . - A. P. Misra and P. K. Shukla, Phys. Plasmas 15, 052105 (2008).
- M. Marklund and G. Brodin, Phys. Rev. Lett. 98, 025001 (2007).
- M. Marklund, B. Eliasson, and P. K. Shukla, Phys. Rev. E 76, 067401 (2007).
- G. Brodin, M. Marklund, and G. Manfredi, Phys. Rev. Lett. 100, 175001 (2008).
- G. Brodin and M. Marklund,
New J. Phys. 9, 277 (2007) . - G. Brodin, M. Marklund, B. Eliasson, and P. K. Shukla, Phys. Rev. Lett. 98, 125001 (2007).
- M. Marklund and P. K. Shukla, Rev. Mod. Phys. 78, 591 (2006).
- G. Manfredi, Fields Inst. Commun. 46, 263 (2005).
- T. Hada, C. F. Kennel, B. Buti, and E. Mjølhus, Phys. Fluids B 2, 2581 (1990).







