[go: up one dir, main page]

CN106128914A - A kind of novel gyrotron traveling wave tube input coupler - Google Patents

A kind of novel gyrotron traveling wave tube input coupler Download PDF

Info

Publication number
CN106128914A
CN106128914A CN201610397238.1A CN201610397238A CN106128914A CN 106128914 A CN106128914 A CN 106128914A CN 201610397238 A CN201610397238 A CN 201610397238A CN 106128914 A CN106128914 A CN 106128914A
Authority
CN
China
Prior art keywords
waveguide
rectangular
input
wave tube
input coupler
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Granted
Application number
CN201610397238.1A
Other languages
Chinese (zh)
Other versions
CN106128914B (en
Inventor
王建勋
任绪迅
夏建波
罗勇
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
University of Electronic Science and Technology of China
Original Assignee
University of Electronic Science and Technology of China
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by University of Electronic Science and Technology of China filed Critical University of Electronic Science and Technology of China
Priority to CN201610397238.1A priority Critical patent/CN106128914B/en
Publication of CN106128914A publication Critical patent/CN106128914A/en
Application granted granted Critical
Publication of CN106128914B publication Critical patent/CN106128914B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J23/00Details of transit-time tubes of the types covered by group H01J25/00
    • H01J23/36Coupling devices having distributed capacitance and inductance, structurally associated with the tube, for introducing or removing wave energy
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J25/00Transit-time tubes, e.g. klystrons, travelling-wave tubes, magnetrons
    • H01J25/34Travelling-wave tubes; Tubes in which a travelling wave is simulated at spaced gaps

Landscapes

  • Microwave Amplifiers (AREA)
  • Gyroscopes (AREA)

Abstract

A kind of novel gyrotron traveling wave tube input coupler of this disclosure of the invention, belongs to microwave, millimetric wave device technical field.Including coaxial configuration, it is respectively arranged at ending circular waveguide and exporting circular waveguide and be arranged at the rectangular input waveguides of coaxial configuration side of coaxial configuration two ends, wherein being provided with several coupling gaps on coaxial configuration inner wire, rectangular input waveguides E face is provided with short circuit branch rectangular waveguide.The present invention, on the basis of tradition gyrotron traveling wave tube, arranges a short circuit branch waveguide in rectangular input waveguides E face.By position and the structural parameters of appropriate design short circuit branch waveguide, it is possible to the effective reflection offsetting input coupler, increase the efficiency of transmission of front end, thus effectively extension inputs bandwidth.

Description

一种新型回旋行波管输入耦合器A New Input Coupler for Convolutional TWT

技术领域technical field

本发明属于微波、毫米波器件技术领域,具体涉及一种新型回旋行波管输入耦合器及其设计方法。The invention belongs to the technical field of microwave and millimeter wave devices, and in particular relates to a novel gyrotron traveling wave tube input coupler and a design method thereof.

背景技术Background technique

在回旋行波管中,输入的电磁波与作螺旋运动的电子发生相互作用,这时由于相对论负质量效应的影响,电子注在横向形成角向群聚,并且继续向前螺旋运动到达高频互作用区落入减速场。在高频减速场中,电子注部分能量转换给高频场,实现高频场的放大,从而在输出端得到高功率微波、毫米波。In the cyclotron traveling wave tube, the input electromagnetic wave interacts with the electrons in spiral motion. At this time, due to the influence of relativistic negative mass effect, the electron beams form angular clusters in the lateral direction, and continue to spiral forward to reach the high-frequency interaction. The area of effect falls into the deceleration field. In the high-frequency deceleration field, part of the energy of the electron injection is converted to the high-frequency field to realize the amplification of the high-frequency field, so that high-power microwaves and millimeter waves are obtained at the output end.

回旋行波管输入耦合器是一种耦合输入装置,它的作用是将前级放大器输出的微波信号,通过模式变换结构转化为回旋行波管中的工作模式,从而把微波信号输入回旋行波管。当输入耦合器的性能较差时,由于回旋行波管高增益特性,不仅回波会对前级放大器造成一定的损坏,而且输入模式的纯度低对回旋管的输出功率、效率和增益产生较为显著的影响,严重情况会使回旋行波管无法工作。因此对输入耦合器的优化十分必要。传统的回旋行波管输入耦合器如图5所示,由截止圆波导、输出圆波导、同轴结构和矩形输入波导组成,其中同轴结构内导体上设置有若干个耦合缝隙。输入信号TE10模从矩形输入波导输入到同轴结构,TE10模式在同轴腔内转化为TEmn1模式,TEmn1模式通过同轴腔内导体的耦合缝隙输入到输出圆波导中,同时模式由TEmn1模式转换成输出圆波导中的TE01模式,从而为回旋行波管提供工作所需的圆波导TE01模式。但是这种结构通常在频带的高端反射大,传输率低,进而导致带宽较窄。不能满足宽频带的要求。The gyrotraveling wave tube input coupler is a coupling input device. Its function is to convert the microwave signal output by the pre-amplifier into the working mode in the gyrotraveling wave tube through the mode conversion structure, so as to input the microwave signal into the gyrotraveling wave Tube. When the performance of the input coupler is poor, due to the high-gain characteristics of the gyrotron, not only the echo will cause certain damage to the pre-amplifier, but also the low purity of the input mode will have a relatively large impact on the output power, efficiency and gain of the gyrotron. Significant effects, severe cases will make the gyro TWT unable to work. Therefore, it is necessary to optimize the input coupler. The traditional gyrotron TWT input coupler is shown in Figure 5. It consists of a cut-off circular waveguide, an output circular waveguide, a coaxial structure, and a rectangular input waveguide. Several coupling slots are set on the inner conductor of the coaxial structure. The TE10 mode of the input signal is input from the rectangular input waveguide to the coaxial structure, the TE10 mode is converted into the TEmn1 mode in the coaxial cavity, and the TEmn1 mode is input into the output circular waveguide through the coupling gap of the conductor in the coaxial cavity, and the mode is converted by the TEmn1 mode The TE01 mode in the output circular waveguide is formed, so as to provide the circular waveguide TE01 mode required for the work of the convoluted traveling wave tube. However, this structure usually has large reflection and low transmission rate at the high end of the frequency band, resulting in narrow bandwidth. Can not meet the requirements of broadband.

发明内容Contents of the invention

为了消除传统回旋行波管输入耦合器输入矩形波导与同轴腔之间的反射,扩展输入耦合器的带宽,增加微波传输效率。本发明提出了一种新型回旋行波管输入耦合器,在传统的回旋行波管的基础上,在矩形输入波导E面设置一个短路分支波导。通过合理设计短路分支波导的位置和结构参数,可以有效的抵消输入耦合器的反射,增加高频端的传输效率,从而有效扩展输入带宽。In order to eliminate the reflection between the input rectangular waveguide and the coaxial cavity of the traditional gyrotron TWT input coupler, expand the bandwidth of the input coupler and increase the microwave transmission efficiency. The invention proposes a new type of convoluted traveling wave tube input coupler. On the basis of the traditional convoluted traveling wave tube, a short-circuit branch waveguide is arranged on the E surface of the rectangular input waveguide. By rationally designing the position and structural parameters of the short-circuit branch waveguide, the reflection of the input coupler can be effectively offset, the transmission efficiency at the high-frequency end can be increased, and the input bandwidth can be effectively expanded.

本发明具体技术方案如下:Concrete technical scheme of the present invention is as follows:

一种新型回旋行波管输入耦合器,其结构如图1,2所示。包括同轴结构、分别设置于同轴结构两端的截止圆波导与输出圆波导、以及设置于同轴结构侧面的矩形输入波导,其中同轴结构内导体上设置有若干个耦合缝隙,其特征在于:矩形输入波导E面设置有短路分支矩形波导。A new type of gyrotron TWT input coupler, the structure of which is shown in Figures 1 and 2. It includes a coaxial structure, a cut-off circular waveguide and an output circular waveguide respectively arranged at both ends of the coaxial structure, and a rectangular input waveguide arranged on the side of the coaxial structure, wherein the inner conductor of the coaxial structure is provided with several coupling slots, which are characterized in that : The E-side of the rectangular input waveguide is provided with a short-circuit branch rectangular waveguide.

矩形波导TE10模作为输入信号由矩形输入波导进入到同轴结构的内外导体之间,信号模式由矩形波导TE10模转变成同轴腔内的TE411模。同轴TE411模经过同轴结构内导体的耦合缝隙输入到输出圆波导中,同时将模式变换为圆波导TE01模,输出圆波导为回旋行波管提供所需要的TE01模输入信号。The TE10 mode of the rectangular waveguide is used as the input signal to enter between the inner and outer conductors of the coaxial structure from the rectangular input waveguide, and the signal mode is transformed from the TE10 mode of the rectangular waveguide to the TE411 mode in the coaxial cavity. The coaxial TE411 mode is input into the output circular waveguide through the coupling gap of the inner conductor of the coaxial structure, and the mode is transformed into the circular waveguide TE01 mode at the same time, and the output circular waveguide provides the required TE01 mode input signal for the convoluted traveling wave tube.

背景技术中的矩形波导输入信号在输入到同轴腔时,由于结构形式的变化不可避免地产生反射,使得输入耦合效率降低,这对回旋管的输出功率、效率和增益产生较为显著的影响。同时还可能缩减带宽,降低带内增益平坦度,严重情况会使回旋行波管无法工作。本发明通过在矩形波导的宽边设置短路分支波导,利用等幅反相叠加原理,使同轴的反射波与矩形短路分支的反射波相互抵消,从而减少来自同轴结构的反射波,达到提升模式纯度,扩展工作带宽的有益效果。When the input signal of the rectangular waveguide in the background art is input into the coaxial cavity, reflection is inevitably generated due to the change of the structure form, which reduces the input coupling efficiency, which has a significant impact on the output power, efficiency and gain of the gyrotron. At the same time, the bandwidth may be reduced and the flatness of the gain in the band may be reduced. In severe cases, the TWT may not work. The present invention arranges the short-circuit branch waveguide on the wide side of the rectangular waveguide, and uses the principle of equal-amplitude anti-phase superposition to make the coaxial reflected wave and the reflected wave of the rectangular short-circuit branch cancel each other, thereby reducing the reflected wave from the coaxial structure and achieving the improvement Mode purity, beneficial effect of extending operating bandwidth.

与传统的回旋行波管输入耦合器相比,本发明引入短路分支波导来吸收输入信号的反射波;通过调整短路分支波导的窄边长度,纵向长度和距离同轴腔的距离,来满足反射波的与短路分支波导的波的相位反向和相等幅值的条件,从而将反射波吸收,进而实现工作频带的展宽。Compared with the traditional gyratory traveling wave tube input coupler, the present invention introduces a short-circuit branch waveguide to absorb the reflected wave of the input signal; by adjusting the length of the narrow side of the short-circuit branch waveguide, the longitudinal length and the distance from the coaxial cavity, the reflection waveguide is satisfied. The condition of phase reversal and equal amplitude of the wave and the wave of the short-circuit branch waveguide, so as to absorb the reflected wave, and then realize the broadening of the working frequency band.

附图说明Description of drawings

图1是本发明提供的回旋行波管输入耦合器的剖面图的正视图。Fig. 1 is a front view of a section view of an input coupler for a gyrotron traveling wave tube provided by the present invention.

图2是本发明提供的回旋行波管输入耦合器的剖面图的俯视图。Fig. 2 is a top view of a cross-sectional view of the input coupler of the gyrotron traveling wave tube provided by the present invention.

图3是本发明提供的回旋行波管输入耦合器的原理示意图。Fig. 3 is a schematic diagram of the principle of the input coupler of the gyrotron traveling wave tube provided by the present invention.

图4是本发明实施例提供的新型回旋行波管输入耦合器与传统回旋行波管输入耦合器的测试得出的S11参数对照图。Fig. 4 is a comparison diagram of S11 parameters obtained from tests of the new gyro TWT input coupler provided by the embodiment of the present invention and the conventional gyro TWT input coupler.

图5是回旋行波管传统输入耦合器结构三维模型示意图。Fig. 5 is a schematic diagram of a three-dimensional model of a traditional input coupler structure of a gyrotron TWT.

具体实施方式detailed description

下面结合设计实例及附图对本发明作进一步的详细阐述。Below in conjunction with design example and accompanying drawing, the present invention will be described in further detail.

本实施例提供了一个工作在Ku波段、TE01模的回旋行波管输入耦合器,其技术指标要求如下:This embodiment provides a convoluted traveling wave tube input coupler working in the Ku band and TE01 mode, and its technical specification requirements are as follows:

主波导工作模式:圆波导TE01模。Main waveguide working mode: circular waveguide TE01 mode.

输入信号模式:矩形波导TE10模。Input signal mode: rectangular waveguide TE10 mode.

工作频段:Ku波段,即12.4GHz-18GHz。Working frequency band: Ku band, namely 12.4GHz-18GHz.

标准矩形波导型号:BJ180,宽边尺寸12.954毫米,窄边尺寸:6.477毫米。Standard rectangular waveguide model: BJ180, wide side size 12.954 mm, narrow side size: 6.477 mm.

本实施例提供的回旋行波管输入耦合器结构如图1、图2所示,主要结构及具体尺寸如下所示:1为同轴腔结构,其内导体内半径为12.3mm,厚度0.5mm,外导体内半径为16mm,内外导体之间空隙的长度为14mm;2为截止圆波导,半径为10mm,长度为10mm;3为输出圆波导,内半径为12.3mm,长度为21.88mm;4为输入矩形波导,采用标准矩形波导型号BJ180,宽边12.954mm,窄边6.477mm,长度20.33mm;5为短路分支波导,宽边12.954mm,窄边4mm,长度16mm;6为内导体耦合缝隙,宽度0.8mm,长度8mm,距离同轴内导体上、下边沿长度均为3mm,共计4个耦合缝隙,第一个耦合缝与矩形输入波导中心夹角为45度,相邻耦合缝夹角为90度。The structure of the input coupler of the gyrotron traveling wave tube provided in this embodiment is shown in Figure 1 and Figure 2. The main structure and specific dimensions are as follows: 1 is a coaxial cavity structure, the inner radius of the inner conductor is 12.3mm, and the thickness is 0.5mm , the inner radius of the outer conductor is 16mm, and the length of the gap between the inner and outer conductors is 14mm; 2 is the cut-off circular waveguide, the radius is 10mm, and the length is 10mm; 3 is the output circular waveguide, the inner radius is 12.3mm, and the length is 21.88mm; 4 For the input rectangular waveguide, the standard rectangular waveguide model BJ180 is used, the wide side is 12.954mm, the narrow side is 6.477mm, and the length is 20.33mm; 5 is the short-circuit branch waveguide, the wide side is 12.954mm, the narrow side is 4mm, and the length is 16mm; 6 is the inner conductor coupling gap , width 0.8mm, length 8mm, distance from the upper and lower edges of the coaxial inner conductor is 3mm, a total of 4 coupling slots, the angle between the first coupling slot and the center of the rectangular input waveguide is 45 degrees, the angle between adjacent coupling slots is 90 degrees.

设从A点出射经过同轴内导体反射后回到A点波的相位为Suppose the phase of the wave coming out from point A and returning to point A after being reflected by the coaxial inner conductor is but

同轴结构处产生的反射场E1可表示为The reflection field E1 generated at the coaxial structure can be expressed as

波进入短路分支波导回到A点时的相位设为 The phase when the wave enters the short-circuit branch waveguide and returns to point A is set to

短路分支波导中的反射场E2可表示为The reflection field E2 in the short-circuit branch waveguide can be expressed as

要使传输增强,反射降低,需To enhance the transmission and reduce the reflection, it is necessary to

E1+E2=0 ⑸E1+E2=0 ⑸

若要反射波与分支波导出射波相抵消,则相位条件为If the reflected wave cancels the outgoing wave of the branch waveguide, the phase condition is

幅值条件为The amplitude condition is

Er1=Er2 ⑺Er1=Er2⑺

其中,为A点出射经过同轴内导体反射后回到A点电磁波的相位,kz1为矩形输入波导的传播常数,L1为从A点到同轴结构电磁波传播的距离,θ为波在同轴结构反射时产生的相移的角度,kz2为短路分支波导的传播常数,L2为短路分支波导的长度,ω为电磁波的角频率。Er1为同轴结构处产生的反射场的幅值,Er2为短路分支波导中的反射场的幅值。为电磁波进入短路分支波导回到A点时的相位。in, is the phase of the electromagnetic wave emitted from point A and returned to point A after being reflected by the coaxial inner conductor, k z1 is the propagation constant of the rectangular input waveguide, L 1 is the distance from point A to the coaxial structure electromagnetic wave propagation, θ is the wave in the coaxial The angle of the phase shift generated when the structure reflects, k z2 is the propagation constant of the short - circuit branch waveguide, L2 is the length of the short-circuit branch waveguide, and ω is the angular frequency of the electromagnetic wave. Er1 is the magnitude of the reflection field generated at the coaxial structure, and Er2 is the magnitude of the reflection field in the short-circuit branch waveguide. is the phase when the electromagnetic wave enters the short-circuit branch waveguide and returns to point A.

Er1决定于已定的同轴结构,不可更改。而Er2决定于短路波导的窄边宽度b的取值。设计通过优化窄边宽度b的取值可满足等幅反相要求。Er1 is determined by the established coaxial structure and cannot be changed. Er2 is determined by the value of the narrow side width b of the short-circuit waveguide. The design can meet the requirements of constant amplitude inversion by optimizing the value of narrow side width b.

本实例提供的新型回旋行波管输入耦合器和一般型回旋行波管输入耦合器的反射系数测试结果如图4所示;由图可以知道该新型回旋行波管输入耦合器工作在15GHz—17.4GHz内的反射系数大于-8dB,其中2dB带宽为1.96GHz,传统结构2dB带宽为1.3GHz,相对于传统结构带宽增量约为50%;3dB带宽为2.12GHz,传统结构3dB带宽为1.66GHz,相对于传统结构带宽增量约为27.7%。The reflection coefficient test results of the new type of gyro-traveling-wave tube input coupler and the general-type gyro-traveling-wave tube input coupler provided in this example are shown in Fig. The reflection coefficient within 17.4GHz is greater than -8dB, of which the 2dB bandwidth is 1.96GHz, and the 2dB bandwidth of the traditional structure is 1.3GHz, which is about 50% of the bandwidth increase of the traditional structure; the 3dB bandwidth is 2.12GHz, and the 3dB bandwidth of the traditional structure is 1.66GHz , relative to the bandwidth increment of the traditional structure is about 27.7%.

Claims (1)

1. The utility model provides a novel travelling wave tube input coupler circles round waveguide and output round waveguide including coaxial structure, set up respectively in the ending at coaxial structure both ends and set up in the rectangle input waveguide of coaxial structure side, wherein is provided with a plurality of coupling gap, its characterized in that on the coaxial structure inner conductor: the E surface of the rectangular input waveguide is provided with a short-circuit branched rectangular waveguide.
CN201610397238.1A 2016-06-07 2016-06-07 A kind of novel gyrotron traveling wave tube input coupler Active CN106128914B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201610397238.1A CN106128914B (en) 2016-06-07 2016-06-07 A kind of novel gyrotron traveling wave tube input coupler

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201610397238.1A CN106128914B (en) 2016-06-07 2016-06-07 A kind of novel gyrotron traveling wave tube input coupler

Publications (2)

Publication Number Publication Date
CN106128914A true CN106128914A (en) 2016-11-16
CN106128914B CN106128914B (en) 2018-08-21

Family

ID=57270163

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201610397238.1A Active CN106128914B (en) 2016-06-07 2016-06-07 A kind of novel gyrotron traveling wave tube input coupler

Country Status (1)

Country Link
CN (1) CN106128914B (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN111293015A (en) * 2020-02-20 2020-06-16 电子科技大学 Compact type gyrotron traveling wave tube input system
CN114360988A (en) * 2022-01-07 2022-04-15 电子科技大学 A V-shaped rectangular groove staggered double-grid waveguide slow-wave structure traveling wave tube

Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4282458A (en) * 1980-03-11 1981-08-04 The United States Of America As Represented By The Secretary Of The Navy Waveguide mode coupler for use with gyrotron traveling-wave amplifiers
CN104051205A (en) * 2014-06-17 2014-09-17 电子科技大学 Novel gyro traveling-wave tube coupling input structure
CN105552506A (en) * 2014-10-30 2016-05-04 核工业西南物理研究院 Hole-coupling directional coupler for millimeter-wave-band megawatt microwave parameter measurement

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4282458A (en) * 1980-03-11 1981-08-04 The United States Of America As Represented By The Secretary Of The Navy Waveguide mode coupler for use with gyrotron traveling-wave amplifiers
CN104051205A (en) * 2014-06-17 2014-09-17 电子科技大学 Novel gyro traveling-wave tube coupling input structure
CN105552506A (en) * 2014-10-30 2016-05-04 核工业西南物理研究院 Hole-coupling directional coupler for millimeter-wave-band megawatt microwave parameter measurement

Non-Patent Citations (2)

* Cited by examiner, † Cited by third party
Title
刘国: "G波段带状束返波管及Ku波段带状束行波管高频结构研究", 《中国博士学位论文全文数据库 信息科技辑》 *
徐勇等: "Ka波段TE01模回旋行波管宽带输入耦合器的设计", 《真空科学与技术学报》 *

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN111293015A (en) * 2020-02-20 2020-06-16 电子科技大学 Compact type gyrotron traveling wave tube input system
CN111293015B (en) * 2020-02-20 2021-04-30 电子科技大学 A compact gyroscopic traveling wave tube input system
CN114360988A (en) * 2022-01-07 2022-04-15 电子科技大学 A V-shaped rectangular groove staggered double-grid waveguide slow-wave structure traveling wave tube
CN114360988B (en) * 2022-01-07 2023-04-18 电子科技大学 V-shaped rectangular groove staggered double-grid waveguide slow-wave structure traveling-wave tube

Also Published As

Publication number Publication date
CN106128914B (en) 2018-08-21

Similar Documents

Publication Publication Date Title
CN105470075B (en) A kind of energy coupler suitable for cosine grid loading folded waveguide slow-wave structure
CN102064069B (en) Energy coupling device suitable for rectangular-crossed double-gate slow-wave structure
CN113113279B (en) Cosine grid loading sine-like waveguide slow wave structure
CN113113278B (en) Similar-trapezoid staggered double-gate slow wave structure
CN108172962B (en) A Broadband Circular Waveguide Directional Coupler for Microwave Power Measurement
CN110060911B (en) Broadband high-gain slow wave structure
CN105489459A (en) Novel half-cycle staggered double-gate slow-wave structure
CN108550511B (en) A dual-frequency dual-mode gyroscopic traveling wave tube input coupler
CN105226395B (en) Broad-band chip integrated waveguide electromagnetic horn without wide wall
CN105914117B (en) A kind of confocal waveguide broad-band input coupling device
CN104051205B (en) Coupling-input structure of gyro-traveling-wave tube
CN112615123B (en) Angular power division waveguide structure applied to medium-loaded gyrotron traveling wave tube
CN105552483B (en) A kind of TEO0n/TEO1n mode exciters
CN106128914B (en) A kind of novel gyrotron traveling wave tube input coupler
CN108091533B (en) Double-frequency oscillator
CN109994350B (en) An energy coupling device from H-plane insertion rectangular waveguide to staggered double gates
CN109950115A (en) A Novel High-Frequency Structure of Double Confocal Waveguide Gyroscopic Traveling Wave Tube
CN114783847A (en) Novel slow wave structure based on staggered double-gate and zigzag waveguide
CN113161216B (en) A Compact Dual Confocal Waveguide Gyroscopic Traveling Wave Tube Input Coupler
CN103560065A (en) Coupling output segment of gyrotron traveling wave tube amplifier
CN111128646A (en) A Rectangular Frame-Double-Rod Slow-Wave Structure
CN117747382A (en) Expansion interaction klystron based on line standing wave mode work
CN201887011U (en) Energy coupling device suitable for rectangular staggered double grid slow-wave structure
CN114758938B (en) A weakly reflective folded waveguide slow-wave structure
CN104852113B (en) A kind of coaxial waveguide converter based on artificial magnetic conductor

Legal Events

Date Code Title Description
C06 Publication
PB01 Publication
C10 Entry into substantive examination
SE01 Entry into force of request for substantive examination
GR01 Patent grant
GR01 Patent grant