期刊文献+

Fast simulation of the forward tracking detector of HPLUS 被引量:1

Fast simulation of the forward tracking detector of HPLUS
原文传递
导出
摘要 The necessity of installing a forward tracking detector stack is discussed for the Hadron Physics LanzhoU Spectrometer(HPLUS). A local tracker is developed to solve the multi-track finding problem. The track candidates are searched iteratively via Hough Transform. The fake tracks are removed by a least square fitting process. With this tracker we have studied the feasibility of pp→pp +Ф(→K^+K^-), a typical physical channel proposed on HPLUS. The single track momentum resolution due to the uncertainty of the positioning in FTD is 1.3%. The multiple scattering effect contributes about 20% to the momentum resolution in the FTD coverage. The width and the signal-to-background ratio of the reconstructed Ф are 1.51 MeV and 4.36, respectively, taking into account the direct Kaon channel pp→pp + K^+K^- as background. The geometry coverage of FTD for Ф events is about 85.4%. Based on the current fast simulation and estimation, the geometrical configuration of FTD meets the physical requirement of HPLUS under the current luminosity and multiplicity conditions. The tracker is applicable in the full simulation coming next and is extendable to other tracking component of HPLUS. The necessity of installing a forward tracking detector stack is discussed for the Hadron Physics LanzhoU Spectrometer(HPLUS). A local tracker is developed to solve the multi-track finding problem. The track candidates are searched iteratively via Hough Transform. The fake tracks are removed by a least square fitting process. With this tracker we have studied the feasibility of pp→pp +Ф(→K^+K^-), a typical physical channel proposed on HPLUS. The single track momentum resolution due to the uncertainty of the positioning in FTD is 1.3%. The multiple scattering effect contributes about 20% to the momentum resolution in the FTD coverage. The width and the signal-to-background ratio of the reconstructed Ф are 1.51 MeV and 4.36, respectively, taking into account the direct Kaon channel pp→pp + K^+K^- as background. The geometry coverage of FTD for Ф events is about 85.4%. Based on the current fast simulation and estimation, the geometrical configuration of FTD meets the physical requirement of HPLUS under the current luminosity and multiplicity conditions. The tracker is applicable in the full simulation coming next and is extendable to other tracking component of HPLUS.
出处 《Chinese Physics C》 SCIE CAS CSCD 北大核心 2008年第10期831-836,共6页 中国物理C(英文版)
基金 HIRFL-CSR Project (Lanzhou, China) One Hundred Talents Program of Chinese Academy of Sciences, Knowledge Innovation Project of Chinese Academy of Sciences (KJCX2-SW-N02, KJCX2-SW-N07) Major State Basic Research Development Program (TG2000077401) National Natural Foundation of Science (10675148,10635080)
关键词 SIMULATION track finding event reconstruction Hough Transform simulation, track finding, event reconstruction, Hough Transform
  • 相关文献

参考文献11

  • 1姜焕清.CSR能区重离子反应中的介子产生[J].原子核物理评论,2002,19(3):301-305. 被引量:5
  • 2DING Yong,XU Rong-Guang,MA Bo-Qiang. Physics Letters B . 2005
  • 3DING Yong,XU Rong-Guang,MA Bo- Qiang. Physical Review D Particles Fields Gravitation and Cosmology . 2005
  • 4ZOU B S,Riska D O. Physical Review Letters . 2005
  • 5LIU B C,ZOU B S. Physical Review Letters . 2006
  • 6ZHU Shi-Lin. Int J Mod Phys. A . 2004
  • 7CEN Yu-Qi,LI Xue-Qian. Physical Review Letters . 2004
  • 8DING Yong,MA Bo-Qiang. Physics Letters B . 2004
  • 9ZOU Bin-Song. Nucl. Phys. Rev . 2003
  • 10LI Xi-Guo. Nucl. Phys. Rev . 2005

二级参考文献12

  • 1[1]Stock R, Particle Productions in High Energy Nucleus-nucleus Collisions [J]. Phys Rep, 1986, 135: 259.
  • 2[2]Aichelin J. "Quantum" Molecular Dynamics: A dynamical microscopic n-body approach to investigate fragment formation and the nuclear equation of state in heavy ion collisions [J]. Phys Rep, 1991, 202: 233.
  • 3[3]Wagner A, Muentz C, Oeschler H, et al. Evidence for Different Freeze-out Radii of High- and Low-energy Pions Emitted in Au+Au Collisions at 1 A GeV [J]. Phys Rev Lett, 2001, 86: 39.
  • 4[4]Wagner A, Muentz C, Oeschler H, et al. Emission Partern of High-energy Pions: A new probe for the early phase of heavy ion collisions[J]. Phys Rev Lett, 2000, 85: 18.
  • 5[5]Averbeck R, Holzmann R, Metag V, et al. Neutral Pions and Eta Mesons as Probes of the Hadronic Fireball in Nucleus-nucleus Collisions Around 1 A GeV, nucl-ex/0012007.
  • 6[6]Buescher M, Loffe B L, Koptev V, et al. Phenomenological Analysis of K+ Meson Production in Proton-nucleus Collisions [J]. Phys Rev, 2002, C65: 014603.
  • 7[7]Efremov S V, Parvev E Ya. Subthreshold K+ Meson Production in Proton-nucleus Reactions [J]. Eur Phys J, 1998, A1: 99.
  • 8[8]Li G Q, Lee C-H, Brown G E. Kaons in Dense Matter, Kaon Production in Heavy-ion Collisions, and Kaon Condensation in Neutron Stars [J]. Nucl Phys, 1997, A625: 372.
  • 9[9]Li G Q, Ko C M. Subthreshold Kaon Production and the Nuclear Eqution of State [J]. Phys Lett, 1995, B349: 405.
  • 10[10]Sturm C, Boettchler I, Debowski M, et al. Evidence for a Soft Nuclear Equation-of-state from Kaon Production in Heavy Ion Collisions[J]. Phys Rev Lett, 2001, 86: 39.

共引文献4

同被引文献6

引证文献1

二级引证文献1

相关作者

内容加载中请稍等...

相关机构

内容加载中请稍等...

相关主题

内容加载中请稍等...

浏览历史

内容加载中请稍等...
;
使用帮助 返回顶部