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排序方式: 共有43条查询结果,搜索用时 15 毫秒
1.
BEPCII直线注入器的尾场效应   总被引:2,自引:0,他引:2  
BEPCII直线注入器中的强流、短束团的尾场效应将损害束流的性能.用分析解和数值模拟计算的方法,系统地研究了尾场对纵向和径向束流动力学的影响,包括单束团的短程尾场和多束团的长程尾场对束流能量、能散、发射度、轨道和初级电子束在正电子产生靶上束斑尺寸的影响等.研究了有效抑制这些尾场效应的措施  相似文献   
2.
提出的数值模拟过程是关于直线加速器加速结构耦合器的设计的。Mafia程序和Hfss程序分别被用来模拟一截S—Band的三腔等梯度加速结构,其两端分别为输入耦合器和输出耦合器。通过Mafia程序和Hfss程序模拟了该结构的传输特性,发现两者的模拟结果能很好吻合。  相似文献   
3.
直线加速器驻波腔中的瞬态束流负载效应   总被引:1,自引:0,他引:1  
在高能加速器中, 随着单个束团和束团串中电荷量的提高, 当粒子束穿过加速腔的时候, 感应出的瞬态束流负载电压也越来越高. 但是, 在通常分析束流负载的时候, 往往对稳态束流负载研究的比较多, 而对瞬态束流负载的研究要相对少一些. 本文首先对束流负载的瞬态特性和束团穿过加速腔时高频源所看到谐振腔谐振频率的变化方式进行了分析, 然后又对两种情况下谐振腔的最优失谐条件进行了讨论, 并给出了相应的解析公式. 在第1种情况下, 当粒子束穿过加速腔的时候, 谐振腔的自然谐振频率能够及时地得到调节, 从而使高频源的电流与谐振腔的腔压同相, 以提高高频源的效率; 在第2种情况下, 当粒子束穿过加速腔的时候, 谐振腔的自然谐振频率保持不变, 不能被调节. 最后, 还对BEPCⅡ现有预注入器的预聚束腔、BEPCⅡ未来预注入器的两个次谐波聚束腔中的瞬态束流负载效应进行了分析.  相似文献   
4.
For the injector Scheme-Ⅰ test stand of the China-ADS (Accelerator Driven subcritical System), a beam with the maximum power of 100 kW will be produced and transported to the beam dump. To solve the very high thermal load problem at the dump, two measures are taken to deal with the huge power density at the target. One is to enlarge the contact area between the beam and the target, and this is to be accomplished by expanding the beam profile at the target and using slanted target plates. The other is to produce a more homogenous beam profile at the target to minimize the maximum power density. Here the beam dump line is designed to meet the requirement of beam expansion and homogenization at 3 different energies (3.2 MeV, 5 MeV and 10 MeV), and the step-like field magnets are employed for the beam spot homogenization. Taking into account the fact that the space charge effects are very strong at such low beam energies, the simulations have included space charge effects and errors which show that the beam line can meet the requirements very well. In the meantime, the alternative beam design using standard multipole magnets is also presented.  相似文献   
5.
设计了工作于S波段的波导耦合型预聚束器和束流相位探测腔。为了增加功率容量,预聚束器采用波导耦合机制代替了传统的同轴耦合环耦合,而偏心圆结构的设计能够补偿因耦合窗口的引入导致的径向电场不对称,进一步改善了强流束流品质。预聚束器设计指标与测试结果:耦合系数1.73,空载品质因数2195,腔体谐振频率的可调范围为2 854.55~2 856.9 MHz。为实现测量束流相对射频脉冲的时间,进行强流输入功率补偿,选择了能够在线进行束流相位实时测量的束流相位探测腔,采用旋转对称结构,并通过两个同轴耦合环提取束流通过时激发的感应信号,作为直线相控系统的参考信号。束流相位探测腔设计与测试结果:空载品质因数2392,3dB带宽为2.05MHz,腔体谐振频率的可调范围为2 805.45~2 809.45MHz。所有器件的仿真设计与测试结果基本一致。  相似文献   
6.
李小平  裴国玺  裴士伦 《中国物理 C》2012,36(10):1009-1012
Polarized positrons can be generated through the electron-positron pair creation from circularly polarized gamma-rays hitting a conversion target. Laser-Compton scattering is an efficient method to generate circularly polarized gamma-rays. Simulation studies on these two processes have been done with the Monte Carlo codes, CAIN and GEANT4. Using CAIN to simulate the Laser-Compton scattering process, the energy spectrum of the generated polarized photons could be obtained. GEANT4 was used to study the yield, energy spectrum and the mean polarization of the positrons emanating from the conversion target. To increase the yield of the generated positrons, an optimization study on the thickness of conversion target was also performed.  相似文献   
7.
For the injector Scheme- test stand of the China-ADS(Accelerator Driven subcritical System), a beam with the maximum power of 100 k W will be produced and transported to the beam dump. To solve the very high thermal load problem at the dump, two measures are taken to deal with the huge power density at the target.One is to enlarge the contact area between the beam and the target, and this is to be accomplished by expanding the beam profile at the target and using slanted target plates. The other is to produce a more homogenous beam profile at the target to minimize the maximum power density. Here the beam dump line is designed to meet the requirement of beam expansion and homogenization at 3 different energies(3.2 Me V, 5 Me V and 10 Me V), and the step-like field magnets are employed for the beam spot homogenization. Taking into account the fact that the space charge effects are very strong at such low beam energies, the simulations have included space charge effects and errors which show that the beam line can meet the requirements very well. In the meantime, the alternative beam design using standard multipole magnets is also presented.  相似文献   
8.
提出的数值模拟过程是关于直线加速器加速结构耦合器的设计的。Mafia程序和Hfss程序分别被用来模拟一截S—Band的三腔等梯度加速结构,其两端分别为输入耦合器和输出耦合器。通过Mafia程序和Hfss程序模拟了该结构的传输特性,发现两者的模拟结果能很好吻合。  相似文献   
9.
With the development of free electron laser (FEL) and the international linear collider (ILC), the electron bunch length is getting smaller and smaller. The traveling-wave transverse RF deflecting structure is an important part of the RF deflecting method for bunch length measurement and phase space diagnostics. The operation mode in RF deflector is the ``TM11-like' mode. Since the TM11-like mode in this structure has a pair of degenerate dipole modes, two additional holes are provided on either side of each iris to stabilize the mode. The simulation and optimization have been done. A prototype has been fabricated and tested. The cold test results have been compared with the simulations of the first three modes.  相似文献   
10.
The upgrade project of the Beijing Electron Positron Collider (BEPCII) and its injector linac is working well. The linac upgrade aims at a higher injection rate of 5OmA/min into the storage ring, which requires an injected beam with low emittance, low energy spread and high beam orbit and energy stabilities. This goal is finally reached recently by upgrading the linac components and by dealing with rich and practical beam physics, which are described in this study.  相似文献   
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