CN101119609B - Combination of slit and large slit microwave plasma reaction chamber - Google Patents
Combination of slit and large slit microwave plasma reaction chamber Download PDFInfo
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Abstract
Description
技术领域technical field
本发明属于微波等离子体激发技术领域,特别涉及用于产生大面积微波等离子体的反应腔结构设计。 The invention belongs to the technical field of microwave plasma excitation, and in particular relates to the structural design of a reaction chamber for generating large-area microwave plasma. the
背景技术Background technique
等离子体在新材料、微电子等工业和生物研究等领域有很强的实用价值,特别是利用微波激发等离子体的方式,相对其它的等离子体激发方式而言,等离子体的存在空间较大,带电粒子密度较高,有很大的应用拓展空间。特别是大面积(大体积)微波等离子体,在相关工业上的使用价值更高。 Plasma has strong practical value in the fields of new materials, microelectronics and other industries and biological research, especially the way of using microwaves to excite plasma. Compared with other plasma excitation methods, the existence of plasma is larger. The density of charged particles is high, so there is a lot of room for application expansion. In particular, large-area (large-volume) microwave plasma has higher application value in related industries. the
微波等离子体反应腔一般采用单一或混合的微波模式使等离子体团产生于结构不同的腔体的内部,由于结构不同,产生的等离子体的面积也不相同。而现有的用于产生大面积微波等离子体的反应腔,其主要利用了狭缝天线对微波的衍射作用,称之为狭缝式反应腔。此类微波等离子体反应腔的结构及激发原理如图1、2所示,该反应腔包括:在圆柱形反应腔体2、22(目前成熟腔体基本为圆柱形)的外围环绕有环形波导1、21,在环形波导和反应腔的结合共有部位3、28(环形波导内壁,同时为反应腔外壁),根据微波波导波长的大小在环形波导驻波波节处分布与之相对应的狭缝4、24(图中示出八个狭缝),每个狭缝位置均对应驻波26的波节,27为环形波导中心线;环形波导外壁29上开有圆孔5、25。通过狭缝将环形波导内的微波能量输入进反应腔形成表面波,激发等离子体。这种反应腔产生的等离子体面积尽管较大,但由于狭缝天线衍射产生的电场主要集中在狭缝附近,在腔体中心部位电场一般较小,而微波等离子体激发一般依靠电场作用,因此,在较高气压下(>104pa)腔体形成的等离子体多集中于狭缝附近,很难在腔体中心部位形成,造成腔内等离子体分布不均匀。这种分布的不均匀,必然会限制微波等离子体的使用价值,因此,研究如何扩大微波电场的分布使等离子体分布均匀,是十分必要的。 Microwave plasma reaction chambers generally use single or mixed microwave modes to generate plasmons inside chambers with different structures. Due to the different structures, the areas of the generated plasma are also different. However, the existing reaction chamber for generating large-area microwave plasma mainly utilizes the diffraction effect of the slit antenna on the microwave, and is called a slit-type reaction chamber. The structure and excitation principle of this type of microwave plasma reaction chamber are shown in Figures 1 and 2. The reaction chamber includes: a circular waveguide surrounded by cylindrical reaction chambers 2 and 22 (currently mature chambers are basically cylindrical) 1, 21, in the combined joints of the ring waveguide and the reaction cavity 3, 28 (the inner wall of the ring waveguide and the outer wall of the reaction cavity), according to the wavelength of the microwave waveguide, the corresponding narrow bands are distributed at the standing wave nodes of the ring waveguide Slots 4, 24 (eight slits are shown in the figure), each slit position corresponds to the node of the standing wave 26, and 27 is the centerline of the ring waveguide; circular holes 5, 25 are opened on the outer wall 29 of the ring waveguide. The microwave energy in the ring waveguide is input into the reaction cavity through the slit to form a surface wave and excite the plasma. Although the plasma area generated by this reaction chamber is large, the electric field generated by the diffraction of the slit antenna is mainly concentrated near the slit, and the electric field in the center of the chamber is generally small, and microwave plasma excitation generally relies on the action of the electric field, so , under relatively high pressure (>10 4 Pa) the plasma formed in the cavity is mostly concentrated near the slit, and it is difficult to form in the center of the cavity, resulting in uneven distribution of plasma in the cavity. This uneven distribution will inevitably limit the use value of microwave plasma. Therefore, it is very necessary to study how to expand the distribution of microwave electric field to make the plasma distribution uniform.
发明内容Contents of the invention
本发明的目的是为了克服现有狭缝式反应腔中,电场分布不均匀造成的不足。提出一种狭缝与大缝结合式微波等离子体反应腔,它在原狭缝式微波等离子体反应腔的基础上进行了改进,在环形波导上额外设计了大缝的结构,使之与狭缝的结构相配合,有效的改善了电场分布,产生的等离子体更加均匀,在腔体中心部位也能存在。 The object of the present invention is to overcome the deficiency caused by uneven electric field distribution in the existing slit-type reaction chamber. A microwave plasma reaction chamber combining slit and large slit is proposed, which is improved on the basis of the original slit microwave plasma reaction chamber, and a large slit structure is additionally designed on the ring waveguide, so that it is compatible with the slit With the combination of the structure, the electric field distribution is effectively improved, the generated plasma is more uniform, and it can also exist in the center of the cavity. the
本发明的技术方案如下:包括上下均由可拆卸法兰密闭的竖直放置空心圆柱形反应腔体,在腔体中部,环绕有一横截面为矩形的环形波导,环形波导内壁与腔体外壁重合;环形波导内壁上开凿有与环形波导内驻波波节数目对应的狭缝,狭缝的位置恰好在驻波波节处;环形波导外壁开有用于与方圆模式转换波导(或者耦合天线)相连的一个通孔(微波通过模式转换波导从通孔向环形波导内传输);其特征在于,在环形波导内壁上,还开有大缝,用于在反应腔形成中部最大、向外围逐渐降低的对称强电场,与狭缝形成的电场互补,使反应腔内电场分布均匀。 The technical scheme of the present invention is as follows: It includes a vertically placed hollow cylindrical reaction chamber sealed by detachable flanges up and down, in the middle of the chamber, surrounded by a ring waveguide with a rectangular cross section, the inner wall of the ring waveguide coincides with the outer wall of the chamber ; There are slits corresponding to the number of standing wave nodes in the ring waveguide on the inner wall of the ring waveguide, and the position of the slit is just at the standing wave node; the outer wall of the ring waveguide is used to connect with the square-circle mode conversion waveguide (or coupling antenna) A through hole (the microwave is transmitted from the through hole to the ring waveguide through the mode conversion waveguide); it is characterized in that, on the inner wall of the ring waveguide, there is also a large slit, which is used to form the largest in the middle of the reaction chamber and gradually decrease to the periphery. The symmetrical strong electric field is complementary to the electric field formed by the slit, so that the electric field in the reaction chamber is evenly distributed. the
大缝可以开在微波刚进入环形波导时的首端,也可以开在与之对应的末端,也可两端均开凿。该大缝的中心最好处于通孔中心与腔体中心的连线及其延长线上 The large slit can be opened at the head end when the microwave just enters the ring waveguide, or at the corresponding end, or at both ends. The center of the large slit is preferably on the line connecting the center of the through hole and the center of the cavity and its extension line
腔体的中心、环形波导的中心与狭缝及大缝的中心处于同一水平面。 The center of the cavity, the center of the ring waveguide and the center of the slit and the large slit are on the same horizontal plane. the
上述整个腔体选择对微波吸收较少的金属材料制作。 The above-mentioned entire cavity is made of a metal material that absorbs less microwaves. the
本发明的原理为:微波传输的过程为:功率源输出的微波能,先通过标准矩形波导传输,经过环流器、销钉调节器、定向耦合器、短路活塞等标准器件后,通过方圆转换波导传入环形波导,再通过狭缝和大缝进入反应腔体形成电场。通过环形波导内壁的狭缝传输入反应腔中,使反应腔中部的某一平面在狭缝附近形成高电场,由于狭缝为沿反应腔外壁平均分布,则形成的高电场区域易呈环状,且也分布于反应腔中该平面的外围,中心部位电场很低。微波通过大缝也传输入反应腔中,在反应腔该平面上形成中部最大、向外围逐渐降低的对称强电场,与狭缝形成的电场互补。这种电场与狭缝作用下的电场共同作用,使腔内该平面的整体电场值较高,分布变得均匀,有助于等离子体的均匀激发和分布。而大缝形成的这一电场可通过大缝的尺寸与反应腔的尺寸、微波频率等参数进行配合获得优化。 The principle of the present invention is: the process of microwave transmission is: the microwave energy output by the power source is first transmitted through a standard rectangular waveguide, and after passing through standard devices such as a circulator, a pin regulator, a directional coupler, and a short-circuit piston, it is transmitted through a square-circle conversion waveguide. into the ring waveguide, and then enter the reaction chamber through the slit and large slit to form an electric field. It is transmitted into the reaction chamber through the slit on the inner wall of the ring waveguide, so that a certain plane in the middle of the reaction chamber forms a high electric field near the slit. Since the slit is evenly distributed along the outer wall of the reaction chamber, the formed high electric field area tends to be ring-shaped. , and are also distributed in the periphery of the plane in the reaction chamber, and the electric field in the center is very low. Microwaves are also transmitted into the reaction chamber through the large slit, and a symmetrical strong electric field is formed on the plane of the reaction chamber, which is the largest in the middle and gradually decreases toward the periphery, which is complementary to the electric field formed by the slit. This electric field works together with the electric field under the action of the slit, so that the overall electric field value of the plane in the cavity is higher and the distribution becomes uniform, which is conducive to the uniform excitation and distribution of plasma. The electric field formed by the large slit can be optimized by matching the size of the large slit with the size of the reaction chamber, microwave frequency and other parameters. the
腔体中狭缝、大缝、环形波导等的具体尺寸,根据设计中环形波导内的驻波数、微波传输的频率不同而不同。环形波导中心线的周长一般为波导内驻波波长的整数倍。环形波导的横截面尺寸与传输该频率微波所用的标准矩形波导相近。狭缝与大缝的高度一般为环形波导高度的一半,大缝的宽度与环形波导横截面的宽度接近。具体尺寸可通过电磁学理论估算并借助专业软件仿真优化。 The specific dimensions of slits, large slits, and ring waveguides in the cavity vary according to the number of standing waves in the ring waveguide and the frequency of microwave transmission in the design. The circumference of the center line of the ring waveguide is generally an integer multiple of the wavelength of the standing wave in the waveguide. The cross-sectional dimensions of the ring waveguide are similar to the standard rectangular waveguide used to transmit microwaves of this frequency. The height of the slit and the large slit is generally half of the height of the ring waveguide, and the width of the large slit is close to the width of the cross section of the ring waveguide. The specific size can be estimated by electromagnetic theory and optimized with the help of professional software simulation. the
本发明的创新之处在于提出狭缝与大缝相配合的结构,这种结构,必然可使反应腔内电场分布的均匀性提高,弥补仅含有狭缝结构的反应腔体的不足。在实际应用中,只要环形波导内壁上开凿的大缝的中心位置在通孔中心与腔体中心(腔体水平放置时,该中心为与通孔中心同水平面的腔体轴心)的连线及其延长线上,或者大缝中心位置与该连线及其延长线的水平或垂直距离在半个驻波波长内,大缝形状一般为矩形,也可为圆形、椭圆等对称结构,都能使整体电场分布得到明显改善。 The innovation of the present invention is to propose a structure in which slits and large slits cooperate. This structure will inevitably improve the uniformity of electric field distribution in the reaction chamber and make up for the shortcomings of the reaction chamber with only slit structures. In practical applications, as long as the center of the large slit dug on the inner wall of the ring waveguide is on the line connecting the center of the through hole and the center of the cavity (when the cavity is placed horizontally, the center is the axis of the cavity at the same level as the center of the through hole) and its extension line, or the horizontal or vertical distance between the central position of the large slit and the connection line and its extension line is within half a standing wave wavelength. The shape of the large slit is generally rectangular, and it can also be a symmetrical structure such as a circle or an ellipse. The overall electric field distribution can be significantly improved. the
本发明的腔体的尺寸设计、狭缝的个数选择、微波传输器件的选取等属成熟技术,并非本专利需要保护内容。 The size design of the cavity, the selection of the number of slits, and the selection of microwave transmission devices in the present invention belong to mature technologies, and are not the contents to be protected by this patent. the
本发明的有益效果: Beneficial effects of the present invention:
本发明以已有的狭缝微波等离子体反应腔为基础,在环形波导的内壁上,又额外设置一种大缝的结构,通过狭缝和大缝的共同作用,使反应腔内电场分布均匀,等离子体团分布范围扩大,有助于工业应用。 The present invention is based on the existing slit microwave plasma reaction chamber, and additionally sets a large slit structure on the inner wall of the ring waveguide, through the joint action of the slit and the large slit, the electric field distribution in the reaction chamber is uniform , the plasmoid distribution range is expanded, which is helpful for industrial applications. the
附图说明Description of drawings
图1是普通8狭缝式反应腔的外观示意图。 Figure 1 is a schematic diagram of the appearance of a common 8-slit reaction chamber. the
图2是普通8狭缝式反应腔中心平面的剖面图。 Fig. 2 is a sectional view of the center plane of an ordinary 8-slit reaction chamber. the
图3是本发明的实施例中反应腔中心平面的剖面图。 Fig. 3 is a sectional view of the central plane of the reaction chamber in the embodiment of the present invention. the
图4是本实施例的反应腔内电场作用原理图。 Fig. 4 is a schematic diagram of the action of the electric field in the reaction chamber of this embodiment. the
图5是实施例通过电脑计算得出的反应腔内电场效果图及普通8狭缝式反应腔内电场效果图;其中(a)为普通8狭缝式反应腔内电场效果图,(b)为本实施例的反应腔内电场效果图。 Fig. 5 is the effect diagram of the electric field in the reaction chamber calculated by the embodiment and the effect diagram of the electric field in the common 8 slit type reaction chamber; wherein (a) is the effect diagram of the electric field in the common 8 slit type reaction chamber, (b) It is the effect diagram of the electric field in the reaction chamber of this embodiment. the
具体实施方式Detailed ways
下面结合附图和实施例对本发明作进一步说明。 The present invention will be further described below in conjunction with drawings and embodiments. the
本发明提出的狭缝与大缝结合式微波等离子体反应腔的一个实施例结构如图3所示。在本实施例中以2.45GHz微波频率输入,反应腔体32为竖直放置的空心圆柱形,上下均由可拆卸法兰密闭(图中未示出)。在腔体中部,环绕有一横截面为矩形的环形波导31,环形波导内壁38与反应腔体外壁重合;环形波导内壁上开凿有与环形波导内四个驻波的波节数目对应的八个狭缝34,狭缝的位置恰好在驻波波节处;环形波导31外壁开有一通孔35,该通孔与方圆模式转换波导(或者耦合天线)相连,微波通过模式转换波导从通孔向环形波导内传输;在环形波导31的末端还开有大缝33。圆柱形反应腔体32及环形波导31由黄铜制造。 The structure of an embodiment of the combined slit and large slit microwave plasma reaction chamber proposed by the present invention is shown in FIG. 3 . In this embodiment, the microwave frequency is input at 2.45 GHz, and the
本实施例的环形波导的横截面为矩形,且其与微波传输的标准矩形波导(WR430)横截面尺寸相似。在环形波导内,微波以TE10模式传播,经计算,驻波波长约为15.5cm,对应环形波导中心线周长在62cm左右,因此环形波导的平均直径约为20cm。反应腔直径约在13~14cm之间,狭缝高100mm宽15mm,大缝高100mm宽50mm。 The cross-section of the ring waveguide in this embodiment is rectangular, and its cross-sectional dimension is similar to that of the standard rectangular waveguide (WR430) for microwave transmission. In the ring waveguide, the microwave propagates in TE 10 mode. After calculation, the standing wave wavelength is about 15.5cm, corresponding to the centerline circumference of the ring waveguide is about 62cm, so the average diameter of the ring waveguide is about 20cm. The diameter of the reaction chamber is about 13-14cm, the slit is 100mm high and 15mm wide, and the large slit is 100mm high and 50mm wide.
本实施例的反应腔内电场作用原理如图4所示,图中,环形波导41内的微波将通过狭缝44以TE41模式46进入反应腔42中。而由于反应腔直径的限制,通过大缝43进入反应腔42中的微波模式主要为TE11、TM01等低次轴对称模47,高次模大部分被截止,不能进入腔体,因此,在腔体内将形成TE11、TM01以及TE41模式为主的混合模,而TE41模在狭缝44附近形成较强电场,并向腔中心处递减,TE11、TM01模式在腔体中心处形成较强电场,并向外递减,几种电场的叠加,恰好使整体电场更加均匀。 The working principle of the electric field in the reaction chamber of this embodiment is shown in FIG. 4 , in which the microwave in the
图5为电脑计算反应腔内电场效果图,其中:(a)为普通八狭缝式反应腔的效果图,(b) 为本实施例的反应腔效果图。对比普通八狭缝式反应腔和本实施例的两缝结合的反应腔,可明显看出发明的结构对腔内电场的改善作用。大缝和狭缝结合腔体中,相关尺寸经过仿真优化后,大缝与其两侧的狭缝部分重合,在图中表现为一个大缝和六个狭缝。从图中看出,在仅有八个狭缝的普通大面积微波等离子体腔体中,电场的高值区域(图中用灰色的深浅表示电场值的高低)集中在狭缝附近以及环形波导内,不利于腔体中心部位等离子体的获得,而本发明的大缝和狭缝结合的腔体结构,得到的电场高值区域在整个腔体内,且腔体内电场分布均匀,2/3以上的面积区域电场差别在30%内,有助于获得相对均匀的等离子体。同时,环形波导内电场较低,能量向腔内的转换效率较高。 Fig. 5 is the effect diagram of the electric field in the reaction chamber calculated by computer, wherein: (a) is the effect diagram of the common eight-slit type reaction chamber, and (b) is the effect diagram of the reaction chamber of the present embodiment. Comparing the ordinary eight-slit reaction chamber with the reaction chamber with two slits combined in this embodiment, it can be clearly seen that the inventive structure improves the electric field in the chamber. In the combination cavity of large slits and slits, after the relevant dimensions are optimized by simulation, the large slits partially overlap with the slits on both sides, which is shown as one large slit and six slits in the figure. It can be seen from the figure that in an ordinary large-area microwave plasma cavity with only eight slits, the high-value region of the electric field (the shade of gray in the figure indicates the level of the electric field value) is concentrated near the slit and in the ring waveguide , which is not conducive to the acquisition of plasma in the center of the cavity, and the cavity structure combined with large slits and slits of the present invention, the high-value region of the electric field obtained is in the entire cavity, and the electric field in the cavity is evenly distributed, and more than 2/3 of the The electric field difference between the area and area is within 30%, which helps to obtain a relatively uniform plasma. At the same time, the electric field in the ring waveguide is low, and the energy conversion efficiency into the cavity is high. the
该实施例指出了两种缝配合的腔体结构对电场的改善作用,这种结构有利于均匀等离子体的获得。利用这种组合的原理,可设计不同狭缝个数与大缝组合的腔体结构。由于缝隙个数、腔体尺寸均可变化,产生的电场模式与实例并不一定相同,但只要反应腔中的综合电场是依靠狭缝与大缝产生的电场的叠加效应使其均匀性得到改善,应属于本发明涵盖的结构范围。 This embodiment points out that two kinds of seam-fit cavity structures can improve the electric field, and this structure is beneficial to obtain uniform plasma. Utilizing the principle of this combination, cavity structures with combinations of different numbers of slits and large slits can be designed. Since the number of slits and the size of the cavity can be changed, the generated electric field pattern is not necessarily the same as the example, but as long as the comprehensive electric field in the reaction chamber relies on the superposition effect of the electric field generated by the slits and large slits, its uniformity can be improved , should belong to the structure scope covered by the present invention. the
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CN102080619B (en) * | 2010-12-03 | 2012-05-23 | 清华大学 | Engine ignition device on basis of microwave plasma |
US9330889B2 (en) * | 2013-07-11 | 2016-05-03 | Agilent Technologies Inc. | Plasma generation device with microstrip resonator |
CN106061090B (en) * | 2016-05-31 | 2019-03-12 | 吉林大学 | A Secondary Coupling Microwave Plasma Reforming Device |
CN108811290A (en) * | 2017-04-28 | 2018-11-13 | 北京北方华创微电子装备有限公司 | Plasma generating device and semiconductor equipment |
CN109219226B (en) * | 2017-07-06 | 2023-01-24 | 北京北方华创微电子装备有限公司 | Plasma generating device |
CN108770174B (en) * | 2018-05-25 | 2019-07-19 | 中国科学院微电子研究所 | Microwave plasma generating device with double-coupling resonator with microporous micro-nano structure |
CN108770175B (en) * | 2018-05-25 | 2019-07-16 | 中国科学院微电子研究所 | Micro-porous micro-nano-structured double-coupled resonator for microwave plasma generators |
CN109195299B (en) * | 2018-10-31 | 2020-09-11 | 上海工程技术大学 | A cylindrical surface wave plasma generator |
CN112888134B (en) * | 2021-01-19 | 2024-03-08 | 成都奋羽电子科技有限公司 | Microwave plasma generating device |
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