CYCLOTRONS 2010 - List of Authors (Zheng, J.H.)

Paper	Title	Page
MOPCP106	Beam-Phase Measurement System for HIRFL	263
	J.H. Zheng, W. Liu, W. Ma, R.S. Mao, Y. Wang, J.X. Wu, Y. Yin IMP, Lanzhou, People's Republic of China
	The beam phase measurement system in HIRFL is introduced. The system had been improved using RF-signal mixing and filtering techniques and noise cancellation method. Therefore,the influence of strongly RF field disturbing signal was eliminated and the signal to noise rate was increased, and a stable and sensitive phase measurement system was developed. The phase history of the ion beam was detected by using 15 set of capacitive pick-up probes installed in the SSC cyclotron. The phase information of the measurement was necessary for tuning purposes to obtain an optimized isochronous magnetic field, where the beam intensity was increased and the beam quality was optimized . The measuremnet results before and after isochronous magnetic field for ion and ion in SSC was given . The phase measurement system was reliable by optimizing isochronous magnetic field test,and the precision reached ±0.5°,the sensitivity of the beam signal measurement was about 10nA as well.

MOPCP100	Axial Injection Beam Line of a Compact Cyclotron	254
	J.Q. Zhang, Y. Cao, L.Z. Ma, A. Shi, M.T. Song, L.P. Sun, X.T. Yang, Q.G. Yao, Z.M. You, X.Q. Zhang, X.Z. Zhang, H.W. Zhao, J.H. Zheng IMP, Lanzhou, People's Republic of China
	Axial injection beam line of the therapy cyclotron is presented. It is intended for transportation of the C⁵⁺ ion beam obtained in the permanent magnet ion source. The beam line is only 3.486 m from the ion source to the entrance of spiral inflector, it consists of two sets glasser lens, one set double 90° bend magnet, one quadrupole lens and two solenoid lens. A big vacuum chamber is installed in the vertical part of the beam line, the sinusoidal buncher, the Faraday cap, the slit collimator and chopper are located in the vacuum chamber. The sinusoidal buncher is used for increasing of the seizing efficiency. The Faraday cap is used for the beam diagnostics. The bend magnet with the slit collimator is used for choice of C⁵⁺ ion beam. The chopper is used for choice of the beam utilizing time.

Paper

Title

Page

Beam-Phase Measurement System for HIRFL

263

J.H. Zheng, W. Liu, W. Ma, R.S. Mao, Y. Wang, J.X. Wu, Y. Yin
IMP, Lanzhou, People's Republic of China

The beam phase measurement system in HIRFL is introduced. The system had been improved using RF-signal mixing and filtering techniques and noise cancellation method. Therefore,the influence of strongly RF field disturbing signal was eliminated and the signal to noise rate was increased, and a stable and sensitive phase measurement system was developed. The phase history of the ion beam was detected by using 15 set of capacitive pick-up probes installed in the SSC cyclotron. The phase information of the measurement was necessary for tuning purposes to obtain an optimized isochronous magnetic field, where the beam intensity was increased and the beam quality was optimized . The measuremnet results before and after isochronous magnetic field for ion and ion in SSC was given . The phase measurement system was reliable by optimizing isochronous magnetic field test,and the precision reached ±0.5°,the sensitivity of the beam signal measurement was about 10nA as well.

MOPCP100

Axial Injection Beam Line of a Compact Cyclotron

254

J.Q. Zhang, Y. Cao, L.Z. Ma, A. Shi, M.T. Song, L.P. Sun, X.T. Yang, Q.G. Yao, Z.M. You, X.Q. Zhang, X.Z. Zhang, H.W. Zhao, J.H. Zheng
IMP, Lanzhou, People's Republic of China

Axial injection beam line of the therapy cyclotron is presented. It is intended for transportation of the C⁵⁺ ion beam obtained in the permanent magnet ion source. The beam line is only 3.486 m from the ion source to the entrance of spiral inflector, it consists of two sets glasser lens, one set double 90° bend magnet, one quadrupole lens and two solenoid lens. A big vacuum chamber is installed in the vertical part of the beam line, the sinusoidal buncher, the Faraday cap, the slit collimator and chopper are located in the vacuum chamber. The sinusoidal buncher is used for increasing of the seizing efficiency. The Faraday cap is used for the beam diagnostics. The bend magnet with the slit collimator is used for choice of C⁵⁺ ion beam. The chopper is used for choice of the beam utilizing time.