Accurate Burst Trigger Mode for Dragon-Ⅰ Electron Beam Measurement System

JIANG Xiao-Guo; LI Cheng-Gang; WANG Yuan; DAI Wen-Hua; XIA Lian-Sheng; CHEN Nan; YANG Guo-Jun

Chinese Physics C> 2006, Vol. 30> Issue(8) : 784-787

Accurate Burst Trigger Mode for Dragon-Ⅰ Electron Beam Measurement System

Institute of Fluid Physics, China Academy of Engineering Physics, Mianyang 621900, China

Abstract
HTML
Reference
Related

PDF

Abstract：
The electron beam measurement system for Dragon-I must work synchronously with the beam production and transportation accurately in order to obtain correct data．The synchronization with about 1ns is important．The output waveform of Blumlein lines in pulsed-power system is of amplitude of about 250kV and 20ns active edge time(following edge)．The electron beam will hit the conversion target in about 145ns later steadily and the jitter time is about 1—2ns．The synchronization precision with the same level of the jitter time will be reached if the sharp following edge of waveform is selected to be the time base．The synchronization trigger signal for measurement system can be obtained by the way of differentiating the following edge and the accuracy of about ns can also be reached with suitable circuit parameters．The optical fiber is also adopted to remove the interference on the measurement system from the high voltage system．This kind of burst trigger mode overcomes many disadvantages such as low accuracy, long delay time, large jitter in normal trigger mode and can provide the trigger time accurately．It can meet the need to measure the electron beam parameters at any required time．

References

[1]

. DING Bo-Nan, DENG Jian-Jun, WANG Hua-Cen etal．HEP NP, 2005, 29(6): 604-610(in Chinese)(丁伯南，邓建军，王华岑等.高能物理与核物理，2005, 29(6):604-610)2. JIANG Xiao-Guo, GUO Bao-Ping, DENG Jian-Jun et al.Opto-Electronic Engineering, 2006(accepted)(in Chinese)(江孝国，郭宝平，邓建军等.光电工程，2006(已录用))3. JIANG Xiao-Guo, LI Cheng-Gang,WANG Yuan et al. Det-onation and Shock Waves, 2005, 1: 19-22(in Chinese)(江孝国，李成刚，王远等.爆轰波与冲击波,2005,1:19-22)4. XUE Fei-Biao, YANG Jian-Lun, LI Zheng-Hong. HighPower Laser and Particle Beams, 2005, 17(1): 149-152(in Chinese)(薛飞彪，杨建伦，李正宏.强激光与粒子束，2005, 17(1):149-152)5. GAO Ping, LIU De-Ben, DAI Gang et al. Eighth Sym-posium on High Power Particle Beam and High Volt-age．Sanya, 2001. 272-274(in Chinese)(高平，刘德本，代刚等.第八届高功率粒子束暨高压学术交流会.三业，2001. 272-274)

[1]	GUO Yun-Jun , HE Kang-Lin . Muon Identification Using the Efficiencies Ratio Method at BESⅡ. Chinese Physics C, 2007, 31(11): 1050-1055.
[2]	HUANG Wen-Xue , WANG Yue , ZHU Zhi-Chao , TIAN Yu-Lin , XU Hu-Shan , SUN Zhi-Yu , XIAO Guo-Qing , ZHAN Wen-Long . Experimental Study of the High-Voltage Breakdown and Simulations for the RFQ Cooler and Buncher RFQ1L. Chinese Physics C, 2006, 30(S2): 261-264.
[3]	LI Ming-Liang , ZHU Sheng-Jiang , CHE Xing-Lai , YU Ying-Nan . Research on Two-Quasiparticle Bands in ⁹⁸Sr. Chinese Physics C, 2004, 28(S1): 75-77.
[4]	HU Xi-Duo , SHAO Ming-Zhu , LUO Shi-Yu , LIU Yong-Sheng , ZHU De-Hai . Average Field Idea and Single Particle Model for 2 Dimension Crystallization Beams(Ⅱ). Chinese Physics C, 2004, 28(2): 196-199.
[5]	PENG Quan-Ling , SUN Jian , ZHAO Guang-Yuan , SHI Cai-Tu . Principle and Software Design of Helmhotz Coil Measurement System. Chinese Physics C, 2001, 25(9): 920-925.
[6]	Guo Hua . In-medium QMC Model Parameters and Quark Condensation in Nuclear Matter. Chinese Physics C, 1999, 23(5): 459-468.
[7]	Yang Jianjun , Ma Boqiang , Li Guanglie . Non-perturbative Quark Propagator and the Study of the Non-trivial Q² Dependence in the Nucleon Structure Functions. Chinese Physics C, 1997, 21(2): 146-156.
[8]	Xu Jianming . Matching Problem of Lattice with Transverse Coupling. Chinese Physics C, 1995, 19(1): 73-81.
[9]	BES Collaboration . Experimental Study of Resonance f₂(1270) in the J/ψ Hadronic Decay. Chinese Physics C, 1993, 17(2): 97-106.
[10]	WANG Man , LI Jin , CUI Xiang-Zong , XIA Xiao-Mi , LAI Yuan-Fen , YAO Xiao-Guang . PROTOTYPE OF END CAP SHOWER COUNTERAND ITS BEAM TEST. Chinese Physics C, 1987, 11(3): 321-326.
[11]	Sa Ben-hao , Zhang Xi-zhen , Li Zhu-xia , Shi Yi-jin . A PRIMARY RESEARCH OF THE PHONON RENORMALIZATION OF NUCLEAR FIELD THEORY. Chinese Physics C, 1980, 4(3): 398-400.

Access

Get Citation

JIANG Xiao-Guo, LI Cheng-Gang, WANG Yuan, DAI Wen-Hua, XIA Lian-Sheng, CHEN Nan and YANG Guo-Jun. Accurate Burst Trigger Mode for Dragon-Ⅰ Electron Beam Measurement System[J]. Chinese Physics C, 2006, 30(8): 784-787.

RIS(for EndNote,Reference Manager,ProCite)

BibTex

Txt

Milestone

Received: 2005-11-02
Revised: 2006-01-16

Article Metric

Article Views(4919)
PDF Downloads(729)
Cited by(0)

Policy on re-use

To reuse of subscription content published by CPC, the users need to request permission from CPC, unless the content was published under an Open Access license which automatically permits that type of reuse.

通讯作者: 陈斌, bchen63@163.com

1.
沈阳化工大学材料科学与工程学院沈阳 110142

Accurate Burst Trigger Mode for Dragon-Ⅰ Electron Beam Measurement System

Corresponding author: JIANG Xiao-Guo,

Institute of Fluid Physics, China Academy of Engineering Physics, Mianyang 621900, China

Received Date: 2005-11-02
Accepted Date: 2006-01-16
Available Online: 2006-08-05

Abstract: The electron beam measurement system for Dragon-I must work synchronously with the beam production and transportation accurately in order to obtain correct data．The synchronization with about 1ns is important．The output waveform of Blumlein lines in pulsed-power system is of amplitude of about 250kV and 20ns active edge time(following edge)．The electron beam will hit the conversion target in about 145ns later steadily and the jitter time is about 1—2ns．The synchronization precision with the same level of the jitter time will be reached if the sharp following edge of waveform is selected to be the time base．The synchronization trigger signal for measurement system can be obtained by the way of differentiating the following edge and the accuracy of about ns can also be reached with suitable circuit parameters．The optical fiber is also adopted to remove the interference on the measurement system from the high voltage system．This kind of burst trigger mode overcomes many disadvantages such as low accuracy, long delay time, large jitter in normal trigger mode and can provide the trigger time accurately．It can meet the need to measure the electron beam parameters at any required time．