Extending the dynamic range of electronics in a Time Projection Chamber

被引:8
作者
Estee, J. [1 ,2 ]
Lynch, W. G. [1 ,2 ]
Barney, J. [1 ,2 ]
Cerizza, G. [1 ]
Jhang, G. [1 ]
Lee, J. W. [3 ]
Wang, R. [1 ]
Isobe, T. [4 ]
Kaneko, M. [5 ]
Kurata-Nishimura, M. [4 ]
Murakami, T. [5 ]
Shane, R. [1 ]
Tangwancharoen, S. [1 ,2 ]
Tsang, C. Y. [1 ]
Tsang, M. B. [1 ]
Hong, B. [3 ]
Lasko, P. [6 ]
Lukasik, J. [6 ]
McIntosh, A. B. [7 ]
Pawlowski, P. [6 ]
Pelczar, K. [8 ]
Sakurai, H. [4 ]
Santamaria, C. [1 ]
Suzuki, D. [4 ]
Yennello, S. J. [7 ,9 ]
Zhang, Y. [10 ]
机构
[1] Natl Superconducting Cyclotron Lab, E Lansing, MI 48824 USA
[2] Michigan State Univ, Dept Phys & Astron, E Lansing, MI 48824 USA
[3] Korea Univ, Dept Phys, Seoul 02841, South Korea
[4] RIKEN, Nishina Ctr, Hirosawa 2-1, Wako, Saitama 3510198, Japan
[5] Kyoto Univ, Dept Phys, Kyoto 6068502, Japan
[6] Inst Nucl Phys PAN, Ul Radzikowskiego 152, PL-31342 Krakow, Poland
[7] Texas A&M Univ, Cyclotron Inst, College Stn, TX 77843 USA
[8] INFN, Gran Sasso Natl Lab, Via G Acitelli 22, I-67100 Laquila, AQ, Italy
[9] Texas A&M Univ, Dept Chem, College Stn, TX 77843 USA
[10] Tsinghua Univ, Dept Phys, Beijing 100084, Peoples R China
基金
新加坡国家研究基金会; 美国国家科学基金会;
关键词
TPC; Heavy ion collisions; Dynamic range; GENERIC ELECTRONICS; DETECTOR; SYSTEM; TPCS;
D O I
10.1016/j.nima.2019.162509
中图分类号
TH7 [仪器、仪表];
学科分类号
0804 ; 080401 ; 081102 ;
摘要
When Time Projection Chambers (TPCs) are used in low to intermediate heavy ion collisions, the mass and momentum range of the emitted particles cover a wide range in energy losses. Many TPC readout electronics currently only have a single gain output with a fixed dynamic range. In a recent set of experiments using the SAMURAI Pion-Reconstruction and Ion-Tracker (S pi RIT) TPC, it was important to simultaneously measure relativistic pions and heavy ion tracks from the same collisions. As the ionization from a track's energy loss is collected and multiplied by the anode wires, a distribution of image charges is induced on the TPC read-out pads. If the avalanche on a wire is large enough, the charge collected by pads directly underneath will saturate the readout electronics; pads farther away in the distribution will not be saturated. Using these unsaturated pads and the known pad distribution function, we can estimate the charge on saturated pads, increasing the dynamic range by a factor of 5.
引用
收藏
页数:8
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