TY - JOUR
T1 - Reflection of solitons at critical density of negative ions
T2 - Contribution of thermal and gyratory motions of ions
AU - Malik, Hitendra Kumar
AU - Singh, Kunwar Pal
AU - Kawata, Shigeo
AU - Stroth, Ulrich
AU - Singh, Dhananjay Kumar
AU - Jain, Vinod Kumar
AU - Nishida, Yasushi
AU - Nejoh, Yasu Nori
N1 - Funding Information:
Manuscript received December 20, 2007; revised February 22, 2008. The work of H. K. Malik was supported in part by the All India Council of Technical Education (AICTE), Government of India, by Deutscher Akademischer Austausch Dienst (DAAD), Government of Germany, and by the Government of Japan. H. K. Malik and U. Stroth are with the Institute for Plasmaforschung, Stuttgart University, 70569 Stuttgart, Germany. K. P. Singh is with the Simutech, Gainesville, FL 32608 USA. S. Kawata is with the Department of Advanced Interdisciplinary Sciences, Utsunomiya University, Utsunomiya 321-8585, Japan. D. K. Singh is with SSLNT College Dhanbad, Dhanbad 826001, India. V. K. Jain is with the School of Environmental Sciences, Jawaharlal Nehru University, New Delhi 110 067, India. Y. Nishida is with the Lunghwa University of Science and Technology, Gueishan, Taoyuan 33306, Taiwan, R.O.C. Y. N. Nejoh is with the Graduate School of Engineering, Hachinohe Institute of Technology, Hachinohe 031-8501, Japan. Digital Object Identifier 10.1109/TPS.2008.923745
PY - 2008/6
Y1 - 2008/6
N2 - On the basis of appropriate modified Korteweg-deVries (mKdV) equation derived for three cases of nn0 < ne0, nn0 = ne0, and nn0 > together with nn0 (ne0 as the density of negative ions (electrons), we observe that compressive and rarefactive mKdV solitons propagate in an inhomogeneous magnetized plasma having negative ions at their critical density. Two types of modes (fast and slow) separately evolve as the compressive and rarefactive solitons. However, only the solitons corresponding to the fast mode get reflected, if the obliqueness of the magnetic field lies under certain critical angle Ψ CR which gets larger under higher thermal motions of the ions and shows stronger dependence on it when less number of negative ions are present in the plasma. There is a possibility of the change of polarities after the reflection of the solitons. The solitons suffer stronger reflection under the effect of larger ion thermal motions and smaller obliqueness of the magnetic field. The compressive solitons are found to downshift, whereas the rarefactive solitons are upshifted after the reflection, and these shifts get higher for the increasing concentration of the negative ions and lower obliqueness of the magnetic field. The compressive (rarefactive) solitons shift less (more) in the plasmas with ions of higher thermal energy; however, the upshift shows opposite behavior for the case of nn0 > ne0.
AB - On the basis of appropriate modified Korteweg-deVries (mKdV) equation derived for three cases of nn0 < ne0, nn0 = ne0, and nn0 > together with nn0 (ne0 as the density of negative ions (electrons), we observe that compressive and rarefactive mKdV solitons propagate in an inhomogeneous magnetized plasma having negative ions at their critical density. Two types of modes (fast and slow) separately evolve as the compressive and rarefactive solitons. However, only the solitons corresponding to the fast mode get reflected, if the obliqueness of the magnetic field lies under certain critical angle Ψ CR which gets larger under higher thermal motions of the ions and shows stronger dependence on it when less number of negative ions are present in the plasma. There is a possibility of the change of polarities after the reflection of the solitons. The solitons suffer stronger reflection under the effect of larger ion thermal motions and smaller obliqueness of the magnetic field. The compressive solitons are found to downshift, whereas the rarefactive solitons are upshifted after the reflection, and these shifts get higher for the increasing concentration of the negative ions and lower obliqueness of the magnetic field. The compressive (rarefactive) solitons shift less (more) in the plasmas with ions of higher thermal energy; however, the upshift shows opposite behavior for the case of nn0 > ne0.
KW - Compressive and rarefactive solitons
KW - Critical density
KW - Negative ions
KW - Soliton reflection
KW - Thermal and gyratory motions of ions
UR - http://www.scopus.com/inward/record.url?scp=45949089244&partnerID=8YFLogxK
U2 - 10.1109/TPS.2008.923745
DO - 10.1109/TPS.2008.923745
M3 - Article
AN - SCOPUS:45949089244
SN - 0093-3813
VL - 36
SP - 738
EP - 747
JO - IEEE Transactions on Plasma Science
JF - IEEE Transactions on Plasma Science
IS - 3 PART 2
ER -