High-frequency field intensity along focal point of a long metallic parabolic reflector coated by a magnetized plasma layer using oblique incidence

Abdul Ghaffar; Majeed A. S. Alkanhal

doi:doi:10.3788/COL201513.090801

Chinese Optics Letters, 2015, 13 (9): 090801, Published Online: Sep. 14, 2018

High-frequency field intensity along focal point of a long metallic parabolic reflector coated by a magnetized plasma layer using oblique incidence Download： 665次

Abdul Ghaffar ^1,2,*Majeed A. S. Alkanhal ¹

Author Affiliations

¹ Department of Electrical Engineering, King Saud University, Riyadh 11421, Saudi Arabia

² Department of Physics, University of Agriculture, Faisalabad 38040, Pakistan

Figures & Tables

Fig. 1. Metallic parabolic reflector coated with a layer of magnetized plasma.

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Fig. 2. Comparison of normalized results obtained by Maslov’s method and HKI.

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Fig. 3. Reflected wave field intensities distribution for different values of kd versus kz.

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Fig. 4. Transmitted wave field intensities versus kz for different values of kd: (a) TE and (b) TM polarized.

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Fig. 5. Transmitted wave field intensities versus kz for different values of ωp: (a) TE and (b) TM polarized.

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Fig. 6. Transmitted wave field intensities versus kz different values of θ0: (a) TE and (b) TM polarized.

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Fig. 7. Transmitted wave field intensities versus kz for different values of ωc for TE polarized.

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Abdul Ghaffar, Majeed A. S. Alkanhal. High-frequency field intensity along focal point of a long metallic parabolic reflector coated by a magnetized plasma layer using oblique incidence[J]. Chinese Optics Letters, 2015, 13(9): 090801.

High-frequency field intensity along focal point of a long metallic parabolic reflector coated by a magnetized plasma layer using oblique incidence Download： 665次

Fig. 1. Metallic parabolic reflector coated with a layer of magnetized plasma.

Fig. 2. Comparison of normalized results obtained by Maslov’s method and HKI.

Fig. 3. Reflected wave field intensities distribution for different values of kd versus kz.

Fig. 4. Transmitted wave field intensities versus kz for different values of kd: (a) TE and (b) TM polarized.

Fig. 5. Transmitted wave field intensities versus kz for different values of ωp: (a) TE and (b) TM polarized.

Fig. 6. Transmitted wave field intensities versus kz different values of θ0: (a) TE and (b) TM polarized.

Fig. 7. Transmitted wave field intensities versus kz for different values of ωc for TE polarized.

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High-frequency field intensity along focal point of a long metallic parabolic reflector coated by a magnetized plasma layer using oblique incidence Download： 665次

Fig. 1. Metallic parabolic reflector coated with a layer of magnetized plasma.

Fig. 2. Comparison of normalized results obtained by Maslov’s method and HKI.

Fig. 3. Reflected wave field intensities distribution for different values of kd versus kz.

Fig. 4. Transmitted wave field intensities versus kz for different values of kd: (a) TE and (b) TM polarized.

Fig. 5. Transmitted wave field intensities versus kz for different values of ωp: (a) TE and (b) TM polarized.

Fig. 6. Transmitted wave field intensities versus kz different values of θ0: (a) TE and (b) TM polarized.

Fig. 7. Transmitted wave field intensities versus kz for different values of ωc for TE polarized.

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