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Fig 1.

A cylindrical waveguide comprising of central chamber containing beam-plasma environment.

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Fig 1 Expand

Fig 2.

Real parts of the electric field and magnetic fields at the interface z = − L and

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Fig 2 Expand

Fig 3.

Imaginary parts of the electric field and magnetic fields at the interface z = − L and

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Fig 3 Expand

Fig 4.

Real parts of the electric field and magnetic fields at the interface z = − L and

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Fig 4 Expand

Fig 5.

Imaginary parts of the electric field and magnetic fields at the interface z = − L and

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Fig 5 Expand

Fig 6.

Real parts of the electric field and magnetic fields at the interface z = L and

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Fig 6 Expand

Fig 7.

Imaginary parts of the electric field and magnetic fields at the interface z = L and

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Fig 7 Expand

Fig 8.

Real parts of the electric field and magnetic fields at the interface z = L and

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Fig 8 Expand

Fig 9.

Imaginary parts of the electric field and magnetic fields at the interface z = L and

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Fig 9 Expand

Fig 10.

Power flux versus (A) beam radius plasma radius a , and ( C ) chamber length L .

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Fig 10 Expand

Fig 11.

Power flux versus (A) angular frequency ω , ( B ) plasma frequency and ( C ) beam frequency

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Fig 11 Expand

Fig 12.

Comparison of reflected energy versus the angular frequency in (A) vacuum, and (B) plasma settings.

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Fig 12 Expand

Fig 13.

Comparison of transmitted energy versus the angular frequency in (A) vacuum, and (B) plasma settings.

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Fig 13 Expand

Table 1.

Conservation of power versus number of terms N .

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Table 1 Expand

Fig 14.

Reflected powers versus number of terms N in (A) vacuum, and (B) cold plasma, in different-sized waveguides.

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Fig 14 Expand

Fig 15.

Transmitted powers versus number of terms N in (A) vacuum, and (B) cold plasma, in different-sized waveguides.

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Fig 15 Expand

Table 2.

Cut-on modes versus plasma radius a.

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Table 2 Expand