CN112558137B - A beam transverse and longitudinal detector device based on ceramic vacuum tube - Google Patents
A beam transverse and longitudinal detector device based on ceramic vacuum tube Download PDFInfo
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Abstract
Description
技术领域technical field
本发明涉及一种基于陶瓷真空管道束流横纵向探测器装置,属于重离子束(包括质子束)环形加速器束流冷却或束流反馈领域。The invention relates to a beam transverse and longitudinal detector device based on a ceramic vacuum pipe, belonging to the field of beam cooling or beam feedback of a heavy ion beam (including a proton beam) annular accelerator.
背景技术Background technique
束流随机冷却技术是利用一个宽带微波反馈系统对束流进行冷却,位于束流上游的束流探测器探测到与粒子偏差成正比的射频信号,这一输出信号经过滤波、延迟、移相和放大系统后被加到下游的冲击器上,粒子在冲击器上得到正比于偏差的校正,从而达到冷却的目的。当然这要求校正信号与粒子同步到达冲击器。随机冷却系统主要由束流横纵探测器、低噪声放大器、微波电桥、滤波器、移相器、可变衰减器、相位均衡器、可调延迟线、功率放大器和冲击器等组成。其中,束流横纵向探测器是随机冷却硬件系统的最核心器件之一,位于随机冷却系统的最前端,其优劣直接影响随机冷却系统的工作效率。The beam stochastic cooling technology uses a broadband microwave feedback system to cool the beam. The beam detector located upstream of the beam detects a radio frequency signal proportional to the particle deviation. The output signal is filtered, delayed, phase-shifted and After the amplification system is added to the downstream impactor, the particles are corrected proportional to the deviation on the impactor, so as to achieve the purpose of cooling. Of course this requires that the correction signal arrives at the impactor in synchrony with the particles. The random cooling system is mainly composed of beam transverse and longitudinal detectors, low noise amplifiers, microwave bridges, filters, phase shifters, variable attenuators, phase equalizers, adjustable delay lines, power amplifiers and impactors. Among them, the beam transverse and longitudinal detector is one of the core components of the stochastic cooling hardware system, which is located at the front end of the stochastic cooling system. Its pros and cons directly affect the working efficiency of the stochastic cooling system.
随机冷却系统的束流横纵向探测器结构可以分为行波结构和驻波(谐振)结构。这种束流探测器结构最重要的指标之一就是分路阻抗,其代表了结构的效率。其中,行波结构的分路阻抗与该结构沿束流方向总长度的平方成正比,如周期性开槽同轴结构,此类结构最大的特性要求极板的相速度与束流的Beta值相匹配;驻波结构的分路阻抗与该结构沿束流方向总长度成正比,典型的驻波(谐振)结构包括类似于Pillbox谐振腔体。目前在运行的大部分随机冷却系统的束流探测器具有结构复杂,分路阻抗不高等缺点,例如欧洲核子研究中心(CERN)反质子减速器(AD)随机冷却系统的束流探测器采用级联超级电极(super-electrode)四分之一波长微带线结构,两米长结构总的纵向分路阻抗仅为1600Ω,即800Ω/m。The beam transverse and longitudinal detector structures of stochastic cooling systems can be divided into traveling wave structures and standing wave (resonant) structures. One of the most important specifications of this beam detector structure is the shunt impedance, which represents the efficiency of the structure. Among them, the shunt impedance of the traveling wave structure is proportional to the square of the total length of the structure along the beam direction, such as a periodically slotted coaxial structure. The maximum characteristic of such a structure requires the phase velocity of the polar plate and the Beta value of the beam. The shunt impedance of the standing wave structure is proportional to the total length of the structure along the beam direction, and a typical standing wave (resonant) structure includes a resonant cavity similar to a Pillbox. Most of the beam detectors of the stochastic cooling system currently in operation have the disadvantages of complex structure and low shunt impedance. For example, the beam detector of the stochastic cooling system of the CERN With the super-electrode quarter-wavelength microstrip line structure, the total longitudinal shunt impedance of the two-meter-long structure is only 1600Ω, that is, 800Ω/m.
发明内容SUMMARY OF THE INVENTION
针对上述问题,本发明的目的是提供一种基于陶瓷真空管道束流横纵向探测器装置,该探测器具有高分路阻抗、并适合于350°高温超高真空烘烤,同时具有安装、运行维护简单可靠等优点,可以解决现有技术中存在的不足。In view of the above-mentioned problems, the purpose of the present invention is to provide a beam transverse and longitudinal detector device based on a ceramic vacuum pipe, the detector has high shunt impedance, is suitable for 350° high temperature and ultra-high vacuum baking, and has installation, operation The advantages of simple and reliable maintenance, etc., can solve the deficiencies in the prior art.
为实现上述目的,本发明采取以下技术方案:一种基于陶瓷真空管道束流横纵向探测器装置,其包括:陶瓷真空管道、周期性环型开槽单元、宽带合路器单元以及用于支撑上述各部件的探测器支架;所述陶瓷真空管道两端分别与环形加速器相连,用于为束流提供通道;所述周期性环形开槽单元套设在所述陶瓷真空管道外表面,其内设置有用于对所述陶瓷真空管道内穿过的束流进行感应的若干电极;所述宽带合路器单元设置在所述周期性环形开槽单元外部,并与所述周期性环形开槽单元内部设置的各所述电极相连,用于对所述电极的感应信号进行相加合成得到校正信号并输出到后续粒子校正系统。In order to achieve the above-mentioned purpose, the present invention adopts the following technical scheme: a beam horizontal and vertical detector device based on a ceramic vacuum pipe, which includes: a ceramic vacuum pipe, a periodic annular slotting unit, a wide-band combiner unit, and a support unit for supporting The detector bracket of the above components; the two ends of the ceramic vacuum pipe are respectively connected to the annular accelerator to provide a channel for the beam; the periodic annular slotted unit is sleeved on the outer surface of the ceramic vacuum pipe, and the inner There are several electrodes for inducing the beam current passing through the ceramic vacuum tube; the broadband combiner unit is arranged outside the periodic annular slotted unit, and is arranged inside the periodic annular slotted unit Each of the electrodes is connected to each other, and is used for adding and synthesizing the induction signals of the electrodes to obtain a correction signal, which is output to the subsequent particle correction system.
进一步,所述陶瓷真空管道包括氧化铝陶瓷管道,所述氧化铝陶瓷管道内表面设置有TiN镀膜层,且所述氧化铝陶瓷管道两端分别经两可伐与第一端面法兰和第二端面法兰焊接,所述第一端面法兰和第二端面法兰与环形加速器中其他元件相连。Further, the ceramic vacuum pipe includes an alumina ceramic pipe, the inner surface of the alumina ceramic pipe is provided with a TiN coating layer, and the two ends of the alumina ceramic pipe are respectively connected to the first end face flange and the second end face flange through two kovars. The end face flanges are welded, and the first end face flange and the second end face flange are connected with other elements in the annular accelerator.
进一步,所述氧化铝陶瓷管道采用96%-99%的AI2O3陶瓷制作,其相对介电常数为9.6-9.8,损耗正切为0.01-0.03%。Further, the alumina ceramic pipes are made of 96%-99% AI 2 O 3 ceramics, the relative permittivity is 9.6-9.8, and the loss tangent is 0.01-0.03%.
进一步,所述氧化铝陶瓷管道的壁厚为5-10mm,所述氧化铝陶瓷管道的管径比束流动力学要求最小的束流管道尺寸大1-3mm;所述TiN镀膜层的厚度为1-10nm。Further, the wall thickness of the alumina ceramic pipe is 5-10mm, and the pipe diameter of the alumina ceramic pipe is 1-3mm larger than the size of the beam pipe that requires the smallest beam dynamics; the thickness of the TiN coating layer is 1-3 mm. -10nm.
进一步,所述周期性环型开槽单元包括两个相同的半环型开槽单元,两个所述半环形开槽单元的外边缘共同形成正八边形结构,两个所述半环形开槽单元的内边缘共同形成圆形结构,且两个所述半环形开槽单元相邻的两个侧面上设置有螺孔,用于通过螺栓固定形成一个围设在所述氧化铝陶瓷管道外表面的圆环;两所述半环形开槽单元的内侧均开设有开槽结构,两所述开槽结构上均匀设置有第一~第八共8个电极,且第一电极位于其中一所述开槽结构的上端部,其他电极依次逆时针分布在正八边形其他边的中部,并通过设置在所述半环形开槽单元外侧壁上的端头针引出后,与所述宽带合路器单元相连。Further, the periodic annular slotted unit includes two identical half annular slotted units, the outer edges of the two semi annular slotted units together form a regular octagonal structure, and the two half annular slotted units together form a regular octagonal structure. The inner edges of the units together form a circular structure, and two adjacent sides of the two semi-annular slotted units are provided with screw holes for fixing by bolts to form a surrounding on the outer surface of the alumina ceramic pipe The inner side of the two semi-annular slotted units is provided with a slotted structure, and the two slotted structures are evenly provided with a total of 8 electrodes from the first to the eighth, and the first electrode is located in one of the At the upper end of the slotted structure, other electrodes are distributed in the middle of the other sides of the regular octagon in turn counterclockwise, and are drawn out through the end needles arranged on the outer sidewall of the semi-annular slotted unit, and then connected with the wide-band combiner. units are connected.
进一步,所述开槽结构的槽高的高度为所述半环形开槽单元外侧高度的一半。Further, the height of the groove height of the grooved structure is half of the height of the outer side of the semi-annular grooved unit.
进一步,各所述电极与所述半环形开槽单元形成微带线的特性阻抗为50Ω。Further, the characteristic impedance of the microstrip line formed by each of the electrodes and the half-ring slotted unit is 50Ω.
进一步,各所述电极采用铜镀金材料制作。Further, each of the electrodes is made of copper gold-plated material.
进一步,所述宽带合路器单元采用16路宽带合路器,所述16路宽带合路器包括16路宽带合路器和合路器底板;各所述合路器底板分别固定设置在所述周期性环形开槽单元的八边形的每条边上,且各所述合路器底板末端分别与所述周期性环形开槽单元的各电极相连,各所述合路器底板的首端分别与各所述宽带合路器的一端相连,各所述宽带合路器另一端与所述探测器支架相连。Further, the broadband combiner unit adopts a 16-channel broadband combiner, and the 16-channel broadband combiner includes a 16-channel broadband combiner and a combiner base plate; each of the combiner base plates is respectively fixed on the on each side of the octagon of the periodic annular slotted unit, and the ends of each of the combiner base plates are respectively connected with each electrode of the periodic annular slotted unit, and the head end of each of the combiner base plates They are respectively connected with one end of each of the wideband combiners, and the other end of each of the wideband combiners is connected with the detector support.
进一步,所述16路宽带合路器单元采用两级级联的威尔金森功分/合路器实现。Further, the 16-channel broadband combiner unit is implemented by two-stage cascaded Wilkinson power dividers/combiners.
进一步,所述16路宽带合路器单元通过对每个所述半环型开槽单元上电极的感应信号进行和差运算处理得到垂直、水平和纵向的校正信号,其计算公式如下:Further, the 16-channel broadband combiner unit obtains vertical, horizontal and vertical correction signals by performing sum-difference operation processing on the induction signals of the upper electrodes of each of the half-ring slotted units, and the calculation formula is as follows:
纵向信号=第一电极+第二电极+…+第八电极Longitudinal signal=first electrode+second electrode+...+eighth electrode
垂直信号=(第一电极+第二电极)-(第四电极+第五电极)Vertical signal=(first electrode+second electrode)-(fourth electrode+fifth electrode)
水平信号=(第二电极+第三电极)-(第六电极+第七电极)Horizontal signal=(second electrode+third electrode)-(sixth electrode+seventh electrode)
进一步,所述探测器支架包括两探测器支架半圆结构、四个垂直竿和探测器支架斜体部分;两所述探测器支架半圆结构内壁设置有与所述16路宽带合路器单元中的各宽带合路器相匹配的凹槽,用于与各所述宽带合路器相连;其中一所述探测器支架半圆结构下部分别与两所述垂直竿相连,另一所述探测器支架半圆结构下部分别与另两所述垂直竿相连;所述探测器支架斜体部分包括探测夹支架斜体以及设置在探测器支架斜体上表面的两个固定结构,其中一所述固定结构用于与两所述垂直竿下端固定连接,另一所述固定结构用于与另两所述垂直竿下端固定连接。Further, the detector bracket includes two detector bracket semicircular structures, four vertical rods and an italic part of the detector bracket; the inner walls of the two detector bracket semicircular structures are provided with each of the 16-channel broadband combiner units. The matching groove of the broadband combiner is used to connect with each of the broadband combiners; one of the lower parts of the semicircular structure of the detector support is connected with the two vertical rods respectively, and the other semicircular structure of the detector support The lower part is respectively connected with the other two vertical rods; the italic part of the detector bracket includes a detection clip bracket italic body and two fixing structures arranged on the upper surface of the detector bracket italic body, wherein one of the fixing structures is used for connecting with the two said fixing structures. The lower ends of the vertical rods are fixedly connected, and the other fixed structure is used for fixed connection with the lower ends of the other two vertical rods.
进一步,所述探测夹支架斜体的倾斜角度范围为30°-60°。Further, the inclination angle range of the italic body of the detection clip bracket is 30°-60°.
本发明由于采取以上技术方案,其具有以下优点:1、本发明在束流横纵向探测装置中引入了陶瓷真空管道,可以有效提高束流探测器的分路阻抗。2、本发明通过引入陶瓷真空管道,使得束流探测器结构位于真空管道外,适合于350°高温超高真空烘烤,同时具有安装、运行维护简单可靠等优点,可以广泛应用于重离子束(包括质子束)环形加速器束流随机冷却领域中。3、本发明在陶瓷真空管道外设置有周期性环型开槽单元,通过对其开槽结构的槽宽以及陶瓷真空管道的壁厚进行调整,有效提高了探测器的分路阻抗。本发明可以广泛应用于重离子束环形加速器束流冷却或束流反馈领域。Due to the adoption of the above technical solutions, the present invention has the following advantages: 1. The present invention introduces a ceramic vacuum pipe into the beam transverse and longitudinal detection device, which can effectively improve the shunt impedance of the beam detector. 2. The present invention makes the structure of the beam detector located outside the vacuum pipe by introducing a ceramic vacuum pipe, which is suitable for 350° high temperature and ultra-high vacuum baking, and has the advantages of simple and reliable installation, operation and maintenance, and can be widely used in heavy ion beam ( Including proton beams) in the field of stochastic cooling of toroidal accelerator beams. 3. In the present invention, a periodic annular slotting unit is arranged outside the ceramic vacuum pipe, and the shunt impedance of the detector is effectively improved by adjusting the slot width of the slotted structure and the wall thickness of the ceramic vacuum pipe. The invention can be widely used in the fields of beam cooling or beam feedback in a heavy ion beam annular accelerator.
附图说明Description of drawings
图1是本发明中基于陶瓷真空管道束流横纵向探测器装置整体闭合示意图;1 is a schematic diagram of the overall closure of the horizontal and vertical detector device based on a ceramic vacuum pipe beam in the present invention;
图2是本发明中基于陶瓷真空管道束流横纵向探测器装置整体张开示意图;2 is a schematic diagram of the overall opening of the horizontal and vertical detector device based on the ceramic vacuum pipe beam in the present invention;
图3是本发明中陶瓷真空管道示意图;Fig. 3 is the schematic diagram of ceramic vacuum pipeline in the present invention;
图4是本发明中由2个半环型开槽单元组合成1个周期性环型开槽单元示意图;Fig. 4 is a schematic diagram of a periodic annular slotting unit composed of two half-ring slotting units in the present invention;
图5是本发明中半环型开槽单元示意图;5 is a schematic diagram of a half-ring type slotted unit in the present invention;
图6是本发明中1个周期性环型开槽单元(单元纵向长为13.5mm,陶瓷管道内径为118mm)的纵向分路阻抗仿真结果图;Fig. 6 is a longitudinal shunt impedance simulation result diagram of a periodic annular slotted unit in the present invention (unit longitudinal length is 13.5mm, inner diameter of ceramic pipe is 118mm);
图7是本发明中74个周期性环型开槽单元(纵向总长为1m,陶瓷管道内径为118mm)总的纵向分路阻抗仿真结果图;Fig. 7 is the simulation result diagram of the total longitudinal shunt impedance of 74 periodic annular slotted units (the total longitudinal length is 1m, and the inner diameter of the ceramic pipe is 118mm) in the present invention;
具体实施方式Detailed ways
以下结合附图来对本发明进行详细的描绘。然而应当理解,附图的提供仅为了更好地理解本发明,它们不应该理解成对本发明的限制。The present invention will be described in detail below with reference to the accompanying drawings. It should be understood, however, that the accompanying drawings are provided only for a better understanding of the present invention, and they should not be construed to limit the present invention.
如图1、图2、图3、图4和图5所示,本发明提供的一种基于陶瓷真空管道束流横纵向探测器装置,包括陶瓷真空管道1、周期性环型开槽单元2、16路宽带合路器单元3以及用于支撑上述各部件的探测器支架4。其中,陶瓷真空管道1两端分别与环形加速器中其他元件相连,用于供束流通过的同时,提高探测器的分路阻抗;周期性环形开槽单元2套设在陶瓷真空管道1外表面,其内设置有用于对陶瓷真空管道1内穿过的束流信息进行感应的若干电极;16路宽带合路器单元3设置在周期性环形开槽单元2外部,并与周期性环形开槽单元2内部设置的各电极相连,用于对各电极的感应信号进行相加合成得到校正信号并输出,该校正信号经过滤波、延迟、移相和放大系统后被加到下游的冲击器上,粒子在冲击器上得到正比于偏差的校正,从而达到冷却的目的。As shown in FIG. 1 , FIG. 2 , FIG. 3 , FIG. 4 and FIG. 5 , the present invention provides a beam transverse and longitudinal detector device based on a ceramic vacuum pipe, including a
进一步,如图3所示,陶瓷真空管道1包括氧化铝陶瓷管道106,氧化铝陶瓷管道106内表面设置有TiN镀膜层104,氧化铝陶瓷管道106两端分别经可伐103和可伐105与第一端面法兰101和第二端面法兰102焊接,第一端面法兰101和第二端面法兰102用于与环型加速器中其他元件比如波纹管或不锈钢真空管道连接。Further, as shown in FIG. 3 , the
进一步,氧化铝陶瓷管道106采用96%-99%的AI2O3陶瓷制作,其相对介电常数为9.6-9.8,损耗正切为0.01-0.03%。Further, the alumina
进一步,氧化铝陶瓷管道106的壁厚为5-10mm,氧化铝陶瓷管道106的管径比束流动力学要求最小的束流管道尺寸大1-3mm,以防止束流打到陶瓷内管壁上;TiN镀膜层104的厚度约为1-10nm,其主要目的为了释放束流感应的静电荷。Further, the wall thickness of the
进一步,如图4、图5所示,周期性环型开槽单元2包括两个相同的半环型开槽单元,两个半环形开槽单元的外边缘共同形成正八边形结构,两个半环形开槽单元的内边缘共同形成圆形结构,且两个半环形开槽单元相邻的两个外侧面上设置有螺孔212,用于通过螺栓固定形成一个围设在氧化铝陶瓷管道106外表面的圆环。其中,两半环形开槽单元的内侧均开设有开槽结构211,两开槽结构211上均匀设置有8个电极201~208,使得每一个电极均位于正八边形结构每条边的中央处,并通过设置在半环形开槽单元外侧壁上的端头针209引出后,与16路宽带合路器单元3相连。Further, as shown in FIG. 4 and FIG. 5 , the periodic
如图6和图7所示,经仿真分析,开槽结构211的横向槽宽决定分路阻抗峰值对应的谐振频率大小,当开槽结构211的横向槽宽增大时,分路阻抗峰值对应的谐振频率减小,当开槽结构211的横向槽宽为33mm,氧化铝陶瓷管道的壁厚为8mm时,分路阻抗峰值对应的谐振频率约为0.95GHz,且beta=0.83时,纵向分路阻抗为4000Ω/m,是欧洲核子研究中心(CERN)反质子减速器(AD)随机冷却系统的束流探测器分路阻抗的五倍。As shown in FIG. 6 and FIG. 7 , after simulation analysis, the lateral slot width of the slotted
进一步,开槽结构211的槽高210的高度为半环形开槽单元外侧高度的一半。Further, the height of the
进一步,电极201~208与半环形开槽单元形成微带线的特性阻抗为50Ω。Further, the characteristic impedance of the microstrip line formed by the
进一步,电极201~208采用铜镀金材料制作,以减小插入损耗。Further, the electrodes 201-208 are made of copper gold-plated material to reduce insertion loss.
进一步,如图2所示,16路宽带合路器单元3包括16路宽带合路器301和合路器底板302。其中,各合路器底板302分别固定设置在周期性环形开槽单元2外边缘正八边形的每条边上,且各合路器底板302末端分别与周期性环形开槽单元2的各电极相连,各合路器底板302的首端分别与各宽带合路器301的一端相连,各宽带合路器301另一端与探测器支架4相连。Further, as shown in FIG. 2 , the 16-channel
进一步,电极201~208与16路宽带合路器单元3中的各合路器底板302的连接采用压接方式。Further, the connection between the
进一步,如图2所示,探测器支架4包括两个探测器支架半圆结构401~402、垂直竿405~408和探测器支架斜体部分。其中,探测器支架半圆结构401和402内壁设置有与16路宽带合路器单元3中的各宽带合路器301相匹配的凹槽,用于与各宽带合路器301相连;探测器支架半圆结构401下部分别与垂直竿405和406相连,探测器支架半圆结构402下部分别与垂直竿407和408相连;探测器支架斜体部分包括探测夹支架斜体以及设置在探测器支架斜体上表面的两个固定结构403和404;其中,固定结构403用于与垂直竿405和垂直竿406下端固定连接;固定结构404用于与垂直竿407和408下端固定连接。Further, as shown in FIG. 2 , the
进一步,探测器支架斜体的倾斜角度范围为30°-60°,本发明优选为45°。Further, the inclination angle of the italic body of the detector bracket is in the range of 30°-60°, and is preferably 45° in the present invention.
进一步,16路宽带合路器单元3采用两级级联的威尔金森功分/合路器实现。Further, the 16-channel
进一步,16路宽带合路器单元3用于实现对电极感应信号相加合成功能。通过对每个半环型开槽单元上电极的感应信号进行和差运算处理可以得到垂直、水平和纵向的校正信号,计算公式如下:Further, the 16-channel
1)纵向信号=电极201+电极202+电极203+电极204+电极205+电极206+电极207+电极2081) Vertical signal =
2)垂直信号=(电极201+电极208)-(电极204+电极205)2) Vertical signal=(
3)水平信号=(电极202+电极203)-(电极206+电极207)3) Horizontal signal=(
本发明提出的基于陶瓷真空管道束流横纵向探测器装置的具体使用过程如下:The specific use process of the ceramic vacuum pipeline beam transverse and longitudinal detector device proposed by the present invention is as follows:
首先将陶瓷真空管道1安装于环型加速器随机冷却探测器所处束线管道位置,然后将探测器支架4包括探测器支架半圆结构401~402、垂直竿405~408和探测器支架斜体部分403~404安装到位,具体安装顺序为先安装探测器支架斜体部分403~404,再安装垂直竿405~408,然后安装探测器支架半圆结构401~402,最后将安装好的周期性环型开槽单元2和16路宽带合路器单元3固定在探测器支架半圆结构401~402上,使其最终合拢形成探测器整体圆环型结构。Firstly, the
当束流管道内有束流通过时,周期性环形开槽单元2采集管道内的束流信息,利用16路宽带合路器单元3对电极感应信号相加合成,并通过对每个半环型开槽单元上电极的感应信号进行和差运算处理可以得到垂直、水平和纵向的校正信号,输出校正信号经过滤波、延迟、移相和放大系统后被加到下游的冲击器上,粒子在冲击器上得到正比于偏差的校正,从而达到冷却的目的。When the beam passes through the beam pipe, the periodic
上述各实施例仅用于说明本发明,其中各部件的结构、连接方式和制作工艺等都是可以有所变化的,凡是在本发明技术方案的基础上进行的等同变换和改进,均不应排除在本发明的保护范围之外。The above-mentioned embodiments are only used to illustrate the present invention, and the structure, connection method and manufacturing process of each component can be changed to some extent. Any equivalent transformation and improvement based on the technical solution of the present invention should not be used. Excluded from the scope of protection of the present invention.
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| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2008170445A (en) * | 2008-01-25 | 2008-07-24 | Hamamatsu Photonics Kk | X-ray image pick-up device |
| CN103983874A (en) * | 2014-05-16 | 2014-08-13 | 中国科学院新疆理化技术研究所 | Electron accelerator and method for achieving electron beam low-fluence environment |
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| Publication number | Priority date | Publication date | Assignee | Title |
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| GB1391619A (en) * | 1972-07-25 | 1975-04-23 | V Ni I Pi Ochistke Tekhnolo Gi | Apparatus for evaporative cooling |
| JPS6052389B2 (en) * | 1979-08-16 | 1985-11-19 | 日本電気株式会社 | Atomic beam detector |
| JPH10260260A (en) * | 1997-03-17 | 1998-09-29 | Kagaku Gijutsu Shinko Jigyodan | Method and apparatus for measuring X-ray detection efficiency of CCD with resolution finer than pixel |
| GB9717877D0 (en) * | 1997-08-26 | 1997-10-29 | Ellis Richard J | Order charge separation and order -charge type separation |
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| CN204314472U (en) * | 2014-09-13 | 2015-05-06 | 中国科学院近代物理研究所 | High energy high-current accelerator Faraday cylinder |
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| CN111208550B (en) * | 2020-01-08 | 2021-08-17 | 中国科学院近代物理研究所 | A Transverse and Longitudinal Beam Schottky Signal Detector |
-
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| Publication number | Priority date | Publication date | Assignee | Title |
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