POSITION SENSING BY CHARGE DIVISION METHOD IN SELF-QUENCHING STREAMER TUBE

MA Jin-Yuan; LI Pei-Qin; LU Wei-Da; LU Chang-Guo; ZHOU Yue-Hua; ZHANG Yu; GU Wei-Xin; CUI Xiang-Zong

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《中国物理C》（英文）编辑部

2024年10月30日

Chinese Physics C> 1984, Vol. 8> Issue(3) : 261-266

POSITION SENSING BY CHARGE DIVISION METHOD IN SELF-QUENCHING STREAMER TUBE

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Abstract：
The experimental results of charge division method with the self-quenching streamer pulses are reported. It is shown that the position resolution at the middle point of 2.5 m long tube can reach 3.3 mm even the signals are sent to ADC module by 60 m long cable. It is much better than using the proportional pulses, and the non-linearity is less than 0.14% of 2.5 m full scale. Some other aspects, such as ADC gate width and selecting of the decoupling capacitor etc. are also discussed, they would provide some practical basis for the design of the sample and hold system in the gas sampling shower counter of the Beijing e⁺e^－ collider spectrometer.

References

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V. Radeka and P. Reh,ak, BNL 25070, Oct. 1378[2] J. L. Albexi and V. Radeka, IEEE NS-23(1976), 25.[3] D. Bernstein and D. Hutcli.nson, IEEE NS-29, No, 1(1982), 294.[4] PEP-4 TPC Collaboration, IEEE NS-30, No. 1(1983)，117.[5] 陆昌国, 高能物理与核物理, 1(1983), 643,[6] V. Radeka, IEEE NS-21, No. 1(1974), 51.[7] M. Atac and F. Bedeschi, IEEE NS-29 (1982), 396.

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MA Jin-Yuan, LI Pei-Qin, LU Wei-Da, LU Chang-Guo, ZHOU Yue-Hua, ZHANG Yu, GU Wei-Xin and CUI Xiang-Zong. POSITION SENSING BY CHARGE DIVISION METHOD IN SELF-QUENCHING STREAMER TUBE[J]. Chinese Physics C, 1984, 8(3): 261-266.

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Received: 1900-01-01
Revised: 1900-01-01

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沈阳化工大学材料科学与工程学院沈阳 110142

POSITION SENSING BY CHARGE DIVISION METHOD IN SELF-QUENCHING STREAMER TUBE

Corresponding author: MA Jin-Yuan,

Received Date: 1900-01-01
Accepted Date: 1900-01-01
Available Online: 1984-06-05

Abstract: The experimental results of charge division method with the self-quenching streamer pulses are reported. It is shown that the position resolution at the middle point of 2.5 m long tube can reach 3.3 mm even the signals are sent to ADC module by 60 m long cable. It is much better than using the proportional pulses, and the non-linearity is less than 0.14% of 2.5 m full scale. Some other aspects, such as ADC gate width and selecting of the decoupling capacitor etc. are also discussed, they would provide some practical basis for the design of the sample and hold system in the gas sampling shower counter of the Beijing e⁺e^－ collider spectrometer.