IBIC2015 - List of Authors (Hu, J.)

Paper	Title	Page
MOPB026	Phase and Energy Measurement System for C-ADS Injector I	95
	J.H. Yue, Q.Y. Deng, J. Hu, S.J. Wei, Q. Ye IHEP, Beijing, People's Republic of China
	For proton linac, phase and energy measurement is very important. Beam phase always can be measured by quadrature sampling, energy can be measured by the method of time of flight (TOF), in this way we need to know the beam phase of two points whose distance is given. C-ADS injector I is a 10MeV proton linac with 10mA continuous current. It consists of an ECR (Electron Cyclotron Resonance) ion source, a LEBT (Low Energy Beam Transport), a 3MeV RFQ (Radio-frequency Quadruple) and a superconductivity linac accelerator with 3~10MeV. In the initial phase, the beam energy is about 3MeV. In this paper, phase and beam energy system of C-ADS Injector I have been introduced and some preliminary results have been shown.
Export •	reference for this paper to ※ BibTeX, ※ LaTeX, ※ Text, ※ RIS/RefMan, ※ EndNote (xml)

Paper

Title

Page

Phase and Energy Measurement System for C-ADS Injector I

95

J.H. Yue, Q.Y. Deng, J. Hu, S.J. Wei, Q. Ye
IHEP, Beijing, People's Republic of China

For proton linac, phase and energy measurement is very important. Beam phase always can be measured by quadrature sampling, energy can be measured by the method of time of flight (TOF), in this way we need to know the beam phase of two points whose distance is given. C-ADS injector I is a 10MeV proton linac with 10mA continuous current. It consists of an ECR (Electron Cyclotron Resonance) ion source, a LEBT (Low Energy Beam Transport), a 3MeV RFQ (Radio-frequency Quadruple) and a superconductivity linac accelerator with 3~10MeV. In the initial phase, the beam energy is about 3MeV. In this paper, phase and beam energy system of C-ADS Injector I have been introduced and some preliminary results have been shown.

Export •

reference for this paper to ※ BibTeX, ※ LaTeX, ※ Text, ※ RIS/RefMan, ※ EndNote (xml)