Double-gap klystron photonic crystal resonator with additional planar resonant elements

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Abstract

The results of investigation of the main electrodynamic parameters of a double-gap photonic crystal resonator will come to use in the development of resonator systems for klystron-type devices operating as amplifiers and generators in radar, telecommunications, and communication facilities.

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About the authors

A. Gnusarev

Саратовский государственный технический университет им. Ю. А. Гагарина

Author for correspondence.
Email: 19953@bk.ru

аспирант кафедры «Электронные приборы и устройства»

Russian Federation

A. Miroshnichenko

Саратовский государственный технический университет им. Ю. А. Гагарина

Email: alexm2005@list.ru

д. т. н., доцент, заведующий кафедрой «Электронные приборы и устройства»

Russian Federation

V. Tsarev

Саратовский государственный технический университет им. Ю. А. Гагарина

Email: tsarev_va@mail.ru

д. т. н., профессор кафедры «Электронные приборы и устройства»

Russian Federation

N. Akafyeva

Саратовский государственный технический университет им. Ю. А. Гагарина

Email: akafieva_na@mail.ru

к. т. н., доцент кафедры «Электронные приборы и устройства»

Russian Federation

References

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  2. Bearzatto C., Bres M., Faillon G. Advantages of Multiple Beam Klystrons // Vakuum elektronik und Displays: Vortrage der ITG Fachtagagung. Garmisch-Partenkirchen, 4–5 May 1992. Garmisch-Partenkirchen: ITG, 1992. РР. 4–32.
  3. Korolyov A.N., Gelvich E. A., Zhary Y. V., Zakurdayev A. D., Poognin V. I. Multiple-beam klystron amplifiers: Performance parameters and development trends // IEEE Transactions on Plasma Science. 2004. Vol. 32. no. 3. РР. 1109–1118. doi: 10.1109/TPS.2004.828807.
  4. Nusinovich G. S., Levush B., Abe D. K. A review of the development of multiple-beam klystrons and TWTs. Washington: Naval Research Laboratory, 2003. 42 p.
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Supplementary files

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1. JATS XML
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2. Fig. 1. DFRC construction: a-resonator construction; B-RPR construction

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3. Fig. 2. The studied resonator models: a – a two-gap resonator without a photonic crystal lattice; b – DFCR with a standard photonic crystal lattice; c - DFCR with an increased diameter of the rods of the first layer of the photonic crystal lattice

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4. Fig. 3. Frequency distribution of the resonator in the range from 10 to 40 GHz for three design options

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5. Fig. 4. Dependences of the frequency, Q-factor (a) and characteristic resistance (b) of the resonator on changes in the diameter of the rods of the first layer of the photonic crystal lattice: 1 – π-mode; 2 – 2π-mode. Solid line – frequency; dotted line – quality factor

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6. Fig. 5. Dependence of frequency, intrinsic Q-factor (a) and characteristic resistance (b) on parameter A: 1 – π-mode; 2 – 2π-mode. Solid line – frequency; dotted line – intrinsic quality

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7. Fig. 6. Dependence of the frequency, intrinsic Q–factor (a) and characteristic resistance (b) of the resonator on the parameter G: 1 - π-mode; 2 – 2π-mode. Solid line – frequency; dotted line – intrinsic quality

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8. Fig. 7. Dependence of frequency, intrinsic Q-factor (a), characteristic resistance (b) on the parameter F of the PRP: 1 – π-mode; 2 – 2π-mode. The solid line is the frequency, the dotted line is the intrinsic quality

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9. Fig. 8. The dependence of frequency and intrinsic Q-factor (a), characteristic resistance (b) on the parameter W PRP: 1 – π-mode; 2 – 2π-mode. Solid line – frequency; dotted line – intrinsic quality

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10. Fig. 1. Table.

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11. Fig. 2. Table.

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Copyright (c) 2023 Gnusarev A., Miroshnichenko A., Tsarev V., Akafyeva N.