CN117691437A - Electron beam-plasma system terahertz radiation source based on adjustable grating - Google Patents
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Abstract
Description
技术领域Technical field
本发明属于太赫兹辐射源技术领域,更为具体地讲,涉及一种基于可调光栅的电子束-等离子体系统太赫兹辐射源。The invention belongs to the technical field of terahertz radiation sources, and more specifically, relates to an electron beam-plasma system terahertz radiation source based on an adjustable grating.
背景技术Background technique
电子束-等离子体系统是一种新型高功率电磁辐射源,在太赫兹领域有着巨大的应用潜力。其工作原理分为两步:1、利用高能电子束穿过高密度等离子体通过双流不稳定性驱动频率位于等离子体频率(基频)及其倍频的等离子体波(即电子静电波);2、系统通过激发多种电磁不稳定性机制将等离子体波的能量交给电磁波从而实现电磁辐射。在上述原理的第二步中,存在着一个制约此类辐射源效率的重要问题,即等离子体波基频的能量转换效率低。The electron beam-plasma system is a new type of high-power electromagnetic radiation source with huge application potential in the terahertz field. Its working principle is divided into two steps: 1. Use high-energy electron beams to pass through high-density plasma and drive plasma waves (i.e., electron electrostatic waves) with frequencies located at the plasma frequency (fundamental frequency) and its multiples through dual-flow instability; 2. The system transfers the energy of plasma waves to electromagnetic waves by stimulating various electromagnetic instability mechanisms to achieve electromagnetic radiation. In the second step of the above principle, there is an important problem that restricts the efficiency of this type of radiation source, that is, the energy conversion efficiency of the plasma wave fundamental frequency is low.
目前,将基频等离子体波转换为太赫兹辐射的潜在机制有以下三种:1、磁化等离子体中的切伦科夫辐射;2、离子热运动对等离子体波的散射;3、等离子体波对离子波(或离子密度调制)的相干散射。上述三种方式都存在辐射转换效率低的缺点,通常能量转换效率不到千分之一。由于电子束在与等离子体相互作用时,电子交出的能量中90%以上都储存于基频等离子体波,而传统的方法难以有效地将基频等离子体波的能量提取出来,限制了此类辐射源的能量转换效率。Currently, there are three potential mechanisms for converting fundamental frequency plasma waves into terahertz radiation: 1. Cherenkov radiation in magnetized plasma; 2. Scattering of plasma waves by ion thermal motion; 3. Plasma Coherent scattering of waves on ion waves (or ion density modulation). The above three methods all have the disadvantage of low radiation conversion efficiency, and usually the energy conversion efficiency is less than one thousandth. Since when the electron beam interacts with the plasma, more than 90% of the energy handed over by the electrons is stored in the fundamental frequency plasma wave. However, it is difficult for traditional methods to effectively extract the energy of the fundamental frequency plasma wave, which limits this Energy conversion efficiency of radiation-like sources.
同时,传统电子束-等离子体系统的辐射频率、方向、和功率难以控制。这是因为这些参数取决于等离子体的电子密度分布,而等离子体在自由空间中存在扩散,因此需要对其控制从而达到合适的分布状态。At the same time, the radiation frequency, direction, and power of traditional electron beam-plasma systems are difficult to control. This is because these parameters depend on the electron density distribution of the plasma, and plasma diffuses in free space, so it needs to be controlled to achieve a suitable distribution state.
发明内容Contents of the invention
本发明的目的在于克服现有技术的不足,提供一种基于可调光栅的电子束-等离子体系统太赫兹辐射源,利用可调光栅作为耦合器实现等离子体波与太赫兹电磁辐射的场匹配,从而有效地提取基频等离子体波的能量;并且利用可调光栅作为控制器,通过改变可调光栅的周期和电压来控制太赫兹辐射源的工作参数。The purpose of the present invention is to overcome the shortcomings of the existing technology, provide an electron beam-plasma system terahertz radiation source based on an adjustable grating, and use the adjustable grating as a coupler to achieve field matching between plasma waves and terahertz electromagnetic radiation. , thereby effectively extracting the energy of the fundamental frequency plasma wave; and using the tunable grating as a controller to control the operating parameters of the terahertz radiation source by changing the period and voltage of the tunable grating.
为了实现上述发明目的,本发明基于可调光栅的电子束-等离子体系统太赫兹辐射源包括真空腔,介质管,进气孔,排气孔,电极,介质管前端金属箔,介质管后端金属箔,光栅,电子束发射源,电子束收集极和输出窗口,其中:In order to achieve the above-mentioned object of the invention, the terahertz radiation source of the electron beam-plasma system based on the adjustable grating of the present invention includes a vacuum chamber, a dielectric tube, an air inlet, an exhaust hole, an electrode, a metal foil at the front end of the dielectric tube, and a rear end of the dielectric tube. Metal foil, grating, electron beam emission source, electron beam collector and output window, where:
进气孔和排气孔设置于真空腔侧壁;The air inlet and exhaust holes are provided on the side wall of the vacuum chamber;
介质管位于真空腔内部,介质管的前端开口和后端开口的侧面分别设置有一个支路出口,分别连接进气孔和排气孔,用于向介质管充入工作气体;介质管的前端开口覆盖有介质管前端金属箔,后端开口覆盖有介质管后端金属箔;The medium tube is located inside the vacuum chamber. A branch outlet is provided on the side of the front opening and the rear opening of the medium tube, respectively connected to the air inlet and the exhaust hole, for filling the working gas into the medium tube; the front end of the medium tube The opening is covered with metal foil at the front end of the medium tube, and the rear end opening is covered with metal foil at the rear end of the medium tube;
可调光栅位于真空腔内部,设置于介质管的外壁,其光栅表面与电子束入射方向平行;The adjustable grating is located inside the vacuum chamber and is installed on the outer wall of the dielectric tube. Its grating surface is parallel to the incident direction of the electron beam;
电子束发射源和电子束收集极位于真空腔内部,分别设置于介质管的前端开口处和后端开口处,电子束发射源从介质管的前端开口处射入电子束,电子束穿过介质管从后端开口处射出,由电子束收集极接收;The electron beam emission source and electron beam collector are located inside the vacuum chamber and are respectively arranged at the front end opening and the rear end opening of the dielectric tube. The electron beam emission source emits the electron beam from the front end opening of the dielectric tube, and the electron beam passes through the medium. The tube emerges from the rear end opening and is received by the electron beam collector;
输出窗口设置于真空腔侧壁上可调光栅对应的位置,用于输出太赫兹电磁波;The output window is set at the position corresponding to the adjustable grating on the side wall of the vacuum chamber, and is used to output terahertz electromagnetic waves;
实现太赫兹波辐射的工作流程如下:The workflow to realize terahertz wave radiation is as follows:
将工作气体从进气孔送入介质管内,同时在电极上施加预设重复频率和电压的电脉冲,将工作气体电离为等离子体;等离子体随气流运动充满介质管,在介质管内部形成等离子体通道,剩余气体通过排气孔排出;The working gas is fed into the dielectric tube from the air inlet, and an electric pulse with a preset repetition frequency and voltage is applied to the electrode at the same time to ionize the working gas into plasma; the plasma moves with the air flow and fills the dielectric tube, forming plasma inside the dielectric tube. body channel, and the remaining gas is discharged through the exhaust hole;
真空腔内的电子束发射源发射电子束,电子束穿过介质管前端金属箔进入等离子体通道,并与等离子体相互作用激发太赫兹波段的等离子体波;随后,电子束穿过介质管后端金属箔离开等离子体通道,最终被电子束收集极吸收;The electron beam emission source in the vacuum chamber emits an electron beam. The electron beam passes through the metal foil at the front end of the dielectric tube and enters the plasma channel. It interacts with the plasma to excite plasma waves in the terahertz band; subsequently, the electron beam passes through the dielectric tube. The terminal metal foil leaves the plasma channel and is eventually absorbed by the electron beam collector;
等离子体波在可调光栅表面形成布洛赫模式,其中波数小于相同频率电磁波的波数的谐波可以转换为辐射场,从可调光栅表面向外界辐射,所形成的太赫兹辐射从输出窗口输出。The plasma wave forms a Bloch mode on the surface of the tunable grating, in which harmonics with a wave number smaller than that of the electromagnetic wave of the same frequency can be converted into a radiation field and radiated from the surface of the tunable grating to the outside world. The formed terahertz radiation is output from the output window. .
本发明基于可调光栅的电子束-等离子体系统太赫兹辐射源,在真空腔内部设置介质管,在介质管内部形成等离子体通道,电子束穿过等离子体通道激发等离子体波,在介质管外壁的可调光栅表面形成布洛赫模式,其中波数小于相同频率电磁波的波数的谐波可以转换为辐射场,从可调光栅表面向外界辐射,从而形成太赫兹辐射输出。The invention is based on an electron beam-plasma system terahertz radiation source with an adjustable grating. A dielectric tube is arranged inside the vacuum chamber, and a plasma channel is formed inside the dielectric tube. The electron beam passes through the plasma channel to excite plasma waves. The tunable grating surface on the outer wall forms a Bloch mode, in which harmonics with wave numbers smaller than those of electromagnetic waves of the same frequency can be converted into radiation fields and radiated from the tunable grating surface to the outside world, thereby forming terahertz radiation output.
本发明具有以下有益效果:The invention has the following beneficial effects:
1)本发明通过可调光栅建立等离子体波与电磁辐射的场匹配,能够有效地实现等离子体基频波能量的辐射,从根本上解决了电子束-等离子体系统的辐射效率低的问题。1) The present invention establishes field matching between plasma waves and electromagnetic radiation through an adjustable grating, which can effectively realize the radiation of plasma fundamental frequency wave energy and fundamentally solve the problem of low radiation efficiency of the electron beam-plasma system.
2)本发明提出了一种更为便捷的控制方法,能够解决传统电子束-等离子体系统辐射参数难以控制的问题,即通过改变可调光栅的电压,可以实现对太赫兹辐射频率、功率和效率的调节;通过改变可调光栅的周期,可以实现辐射方向、功率和效率的调节。2) The present invention proposes a more convenient control method, which can solve the problem of difficulty in controlling the radiation parameters of the traditional electron beam-plasma system. That is, by changing the voltage of the adjustable grating, the terahertz radiation frequency, power and Adjustment of efficiency; by changing the period of the adjustable grating, the radiation direction, power and efficiency can be adjusted.
附图说明Description of the drawings
图1是本发明基于可调光栅的电子束-等离子体系统太赫兹辐射源的一种具体实施方式结构图;Figure 1 is a structural diagram of a specific embodiment of the terahertz radiation source of the electron beam-plasma system based on the adjustable grating of the present invention;
图2是本实施例中154.2ps时刻模拟区域内部的电场分布图;Figure 2 is the electric field distribution diagram inside the simulation area at 154.2ps in this embodiment;
图3是本实施例中光栅耦合等离子体波发射的太赫兹辐射频谱图;Figure 3 is a terahertz radiation spectrum diagram of grating-coupled plasma wave emission in this embodiment;
图4是本实施例中辐射场的功率与能量转换效率示意图。Figure 4 is a schematic diagram of the power and energy conversion efficiency of the radiation field in this embodiment.
具体实施方式Detailed ways
下面结合附图对本发明的具体实施方式进行描述,以便本领域的技术人员更好地理解本发明。需要特别提醒注意的是,在以下的描述中,当已知功能和设计的详细描述也许会淡化本发明的主要内容时,这些描述在这里将被忽略。Specific embodiments of the present invention will be described below in conjunction with the accompanying drawings, so that those skilled in the art can better understand the present invention. It is important to note that in the following description, when detailed descriptions of known functions and designs may dilute the main content of the present invention, these descriptions will be omitted here.
实施例Example
图1是本发明基于可调光栅的电子束-等离子体系统太赫兹辐射源的一种具体实施方式结构图。如图1所示,本发明基于可调光栅的电子束-等离子体系统太赫兹辐射源包括真空腔1,介质管2,进气孔3,排气孔4,电极5,介质管前端金属箔6,介质管后端金属箔7,光栅8,电子束发射源9,电子束收集极10和输出窗口11,其中:Figure 1 is a structural diagram of a specific embodiment of the terahertz radiation source of the electron beam-plasma system based on the adjustable grating of the present invention. As shown in Figure 1, the terahertz radiation source of the electron beam-plasma system based on the adjustable grating of the present invention includes a vacuum chamber 1, a dielectric tube 2, an air inlet 3, an exhaust hole 4, an electrode 5, and a metal foil at the front end of the dielectric tube. 6. Metal foil 7 at the rear end of the dielectric tube, grating 8, electron beam emission source 9, electron beam collector 10 and output window 11, among which:
进气孔3和排气孔4设置于真空腔1侧壁;The air inlet 3 and the exhaust hole 4 are provided on the side wall of the vacuum chamber 1;
介质管2位于真空腔1内部,介质管2的前端开口和后端开口的侧面分别设置有一个支路出口21、22,分别连接进气孔3和排气孔4,用于向介质管2充入工作气体。介质管2的前端开口覆盖有介质管前端金属箔6,后端开口覆盖有介质管后端金属箔7。介质管前端金属箔6和介质管后端金属箔7用于对介质管2进行封闭,能够将电子束源和工作气体隔离,防止泄露,同时只允许高能电子束穿过。The medium pipe 2 is located inside the vacuum chamber 1. The front and rear openings of the medium pipe 2 are respectively provided with a branch outlet 21 and 22 on the side, which are respectively connected to the air inlet 3 and the exhaust hole 4 for supplying air to the medium pipe 2. Fill with working gas. The front opening of the medium tube 2 is covered with the metal foil 6 at the front end of the medium tube, and the rear end opening is covered with the metal foil 7 at the rear end of the medium tube. The metal foil 6 at the front end of the dielectric tube and the metal foil 7 at the rear end of the dielectric tube are used to seal the dielectric tube 2, which can isolate the electron beam source and the working gas to prevent leakage, while only allowing high-energy electron beams to pass through.
可调光栅8位于真空腔1内部,设置于介质管2的外壁,其光栅表面与电子束入射方向平行。经研究发现,可调光栅8的优选周期长度D∈[0.1L,10L],L表示等离子体波的波长。可调光栅8在介质管2的分布位置和大小都可以根据实际需要设置。The adjustable grating 8 is located inside the vacuum chamber 1 and is arranged on the outer wall of the dielectric tube 2. Its grating surface is parallel to the incident direction of the electron beam. After research, it is found that the optimal period length D∈[0.1L, 10L] of the tunable grating 8, L represents the wavelength of the plasma wave. The distribution position and size of the adjustable grating 8 in the medium tube 2 can be set according to actual needs.
电子束发射源9和电子束收集极10位于真空腔1内部,分别设置于介质管2的前端开口处和后端开口处,电子束发射源9从介质管2的前端开口处射入电子束,电子束穿过介质管2从后端开口处射出,由电子束收集极10接收。The electron beam emission source 9 and the electron beam collector 10 are located inside the vacuum chamber 1 and are respectively arranged at the front end opening and the rear end opening of the dielectric tube 2. The electron beam emission source 9 injects electron beams from the front end opening of the dielectric tube 2. , the electron beam passes through the dielectric tube 2 and is emitted from the rear end opening, and is received by the electron beam collector 10.
输出窗口11设置于真空腔1侧壁上可调光栅8对应的位置,用于输出太赫兹电磁波。The output window 11 is provided at a position corresponding to the adjustable grating 8 on the side wall of the vacuum chamber 1, and is used to output terahertz electromagnetic waves.
本发明实现太赫兹波辐射的工作流程如下:The work flow of this invention to realize terahertz wave radiation is as follows:
将工作气体从进气孔3送入介质管2内,同时在电极5上施加预设重复频率和电压的电脉冲,将工作气体电离为等离子体。经实验研究发现,对于太赫兹波辐射,电脉冲的重复频率位于1~100kHz范围,电压位于1~50kV范围内的效果较为优秀。等离子体随气流运动充满介质管2,在介质管2内部形成等离子体通道,剩余气体通过排气孔4排出。等离子体通道的密度量级为1020~1024m-3。The working gas is sent into the dielectric tube 2 from the air inlet 3, and at the same time, an electric pulse with a preset repetition frequency and voltage is applied to the electrode 5 to ionize the working gas into plasma. Experimental research has found that for terahertz wave radiation, the repetition frequency of the electric pulse is in the range of 1 to 100kHz, and the voltage is in the range of 1 to 50kV, which has better effects. The plasma moves with the air flow and fills the medium tube 2 , forming a plasma channel inside the medium tube 2 , and the remaining gas is discharged through the exhaust hole 4 . The density of the plasma channel is on the order of 10 20 to 10 24 m -3 .
真空腔1内的电子束发射源9发射电子束,电子束穿过介质管前端金属箔6进入等离子体通道,并与等离子体相互作用激发太赫兹波段的等离子体波。随后,电子束穿过介质管后端金属箔7离开等离子体通道,最终被电子束收集极10吸收。The electron beam emission source 9 in the vacuum chamber 1 emits an electron beam, which passes through the metal foil 6 at the front end of the dielectric tube, enters the plasma channel, and interacts with the plasma to excite plasma waves in the terahertz band. Subsequently, the electron beam passes through the metal foil 7 at the rear end of the dielectric tube and leaves the plasma channel, and is finally absorbed by the electron beam collector 10 .
等离子体波在可调光栅8表面形成布洛赫模式,其中波数小于相同频率电磁波的波数的谐波可以转换为辐射场,从可调光栅8表面向外界辐射,所得到的太赫兹辐射从输出窗口11输出。The plasma wave forms a Bloch mode on the surface of the adjustable grating 8, in which the harmonics with a wave number smaller than the wave number of the electromagnetic wave of the same frequency can be converted into a radiation field, which is radiated from the surface of the adjustable grating 8 to the outside world, and the resulting terahertz radiation is output from Window 11 output.
经研究发现,通过调节可调光栅8的周期可以调节太赫兹辐射的方向以及输出功率。通过对可调光栅8上施加电压可以改变光栅下的等离子体电子密度分布,从而实现太赫兹辐射频率的调节,基于电子束-等离子体系统实现可控的太赫兹辐射源。It has been found through research that the direction and output power of terahertz radiation can be adjusted by adjusting the period of the adjustable grating 8 . By applying voltage to the adjustable grating 8, the plasma electron density distribution under the grating can be changed, thereby adjusting the terahertz radiation frequency, and realizing a controllable terahertz radiation source based on the electron beam-plasma system.
为了说明本发明的技术效果,采用具体实例对本发明进行实验仿真。本实施例中采用PIC粒子模拟对可调光栅加载的电子束-等离子体系统太赫兹辐射源进行仿真演示。模拟中考虑通过调节可调光栅8的电压,使可调光栅8下方的电子等离子体密度维持在1×1022m-3,等离子体通道内径为0.3mm,长度为1.2cm,管壁厚0.05mm。经过计算可以得到等离子体波的基频为0.9THz。电子束直径为0.1mm,电子束密度为1.0×1018m-3,加速电压为511kV。可调光栅8位于介质管2的上管壁,周期与等离子体波长相等。In order to illustrate the technical effects of the present invention, specific examples are used to conduct experimental simulations of the present invention. In this embodiment, PIC particle simulation is used to simulate and demonstrate the terahertz radiation source of the electron beam-plasma system loaded with an adjustable grating. In the simulation, it is considered to adjust the voltage of the adjustable grating 8 to maintain the electron plasma density under the adjustable grating 8 at 1×10 22 m -3 . The inner diameter of the plasma channel is 0.3mm, the length is 1.2cm, and the tube wall thickness is 0.05 mm. After calculation, it can be found that the fundamental frequency of the plasma wave is 0.9THz. The electron beam diameter is 0.1mm, the electron beam density is 1.0×10 18 m -3 , and the acceleration voltage is 511kV. The adjustable grating 8 is located on the upper tube wall of the medium tube 2, and its period is equal to the plasma wavelength.
图2是本实施例中154.2ps时刻模拟区域内部的电场分布图。图2显示了电子束穿过等离子体通道、驱动等离子体波,并在可调光栅作用下发射太赫兹辐射的图像。图2中水平方向周期排列的小方块为可调光栅;可调光栅8的下方是沿水平方向传播的等离子体波,而在可调光栅8的上方产生了沿竖直方向传播的太赫兹辐射。由于介质管2的下方未设置可调光栅,可以发现,无光栅时的电磁辐射强度远不及有光栅的情况。Figure 2 is the electric field distribution diagram inside the simulation area at 154.2ps in this embodiment. Figure 2 shows an image of an electron beam passing through a plasma channel, driving the plasma wave, and emitting terahertz radiation under the action of a tunable grating. The small squares arranged periodically in the horizontal direction in Figure 2 are tunable gratings; below the tunable grating 8 is the plasma wave propagating in the horizontal direction, and above the tunable grating 8 is the terahertz radiation propagating in the vertical direction. . Since there is no adjustable grating underneath the dielectric tube 2, it can be found that the electromagnetic radiation intensity without the grating is far less than that with the grating.
图3是本实施例中光栅耦合等离子体波发射的太赫兹辐射频谱图。图3所展示的监测位置位于图2中的星形点处。由图3可以看出,在附加光栅后,基频0.9THz的等离子体波的强度远高于高次谐波。Figure 3 is a terahertz radiation spectrum diagram of grating-coupled plasma wave emission in this embodiment. The monitoring position shown in Figure 3 is located at the star point in Figure 2. It can be seen from Figure 3 that after adding a grating, the intensity of the plasma wave with a fundamental frequency of 0.9THz is much higher than the higher harmonics.
图4是本实施例中辐射场的功率与能量转换效率示意图。由图4可知,得到基频波辐射功率可达到千瓦级别,能量转换效率可达到百分之一量级,超过传统小型化方案的水平。图4也体现了可调光栅电压对辐射功率与效率的调节作用,图中横坐标为不同光栅电压引起的等离子体电子密度变化幅值(对初始密度归一化)。可以发现,不同的光栅电压可以对电子密度产生变化。而在不同的电子密度变化量下,太赫兹辐射的功率与能量转换效率产生了显著变化。这一结果表明,利用光栅对电子束-等离子体系统的辐射参数进行控制是可行的。Figure 4 is a schematic diagram of the power and energy conversion efficiency of the radiation field in this embodiment. As can be seen from Figure 4, the obtained fundamental frequency wave radiation power can reach the kilowatt level, and the energy conversion efficiency can reach the order of one percent, exceeding the level of traditional miniaturization solutions. Figure 4 also reflects the adjustment effect of adjustable grating voltage on radiation power and efficiency. The abscissa in the figure is the amplitude of changes in plasma electron density caused by different grating voltages (normalized to the initial density). It can be found that different grating voltages can produce changes in electron density. Under different changes in electron density, the power and energy conversion efficiency of terahertz radiation change significantly. This result shows that it is feasible to use gratings to control the radiation parameters of the electron beam-plasma system.
尽管上面对本发明说明性的具体实施方式进行了描述,以便于本技术领域的技术人员理解本发明,但应该清楚,本发明不限于具体实施方式的范围,对本技术领域的普通技术人员来讲,只要各种变化在所附的权利要求限定和确定的本发明的精神和范围内,这些变化是显而易见的,一切利用本发明构思的发明创造均在保护之列。Although the illustrative specific embodiments of the present invention are described above to facilitate those skilled in the art to understand the present invention, it should be clear that the present invention is not limited to the scope of the specific embodiments. For those of ordinary skill in the art, As long as the various changes are within the spirit and scope of the present invention as defined and determined by the appended claims, these changes are obvious, and all inventions and creations utilizing the concept of the present invention are protected.
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