A Heavy Flavor Tracker for STAR

Chasman, C. ; Beavis, D. ; Debbe, R. ; Lee, J.H. ; Levine, M.J. ; Videbaek, F. ; Xu, Z. ; Kleinfelder, S. ; Li, S. ; Cendejas, R. ; Huang, H. ; Sakai, S. ; Whitten, C. ; Joseph, J. ; Keane, D. ; Margetis, S. ; Rykov, V. ; Zhang, W.M. ; Bystersky, M. ; Kapitan, J. ; Kushpil, V. ; Sumbera, M. ; Baudot, J. ; Hu-Guo, C. ; Shabetai, A. ; Szelezniak, M. ; Winter, M. ; Kelsey, J. ; Milner, R. ; Plesko, M. ; Redwine, R. ; Simon, F. ; Surrow, B. ; Van Nieuwenhuizen, G. ; Anderssen, E. ; Dong, X. ; Greiner, L. ; Matis, H.S. ; Morgan, S. ; Ritter, H.G. ; Rose, A. ; Sichtermann, E. ; Singh, R.P. ; Stezelberger, T. ; Sun, X. ; Thomas, J.H. ; Tram, V. ; Vu, C. ; Wieman, H.H. ; Xu, N. ; Hirsch, A. ; Srivastava, B. ; Wang, F. ; Xie, W. ; Bichsel, H.

Lawrence Berkeley National Laboratory

关键词: Decay;    Rhic, Heavy Flavor, Vertex Detector, Active Pixel Sensor;    Radiation Length;    46;    Quarks;   

DOI  :  10.2172/939892
RP-ID  :  LBNL-PUB-5509-2008
RP-ID  :  DE-AC02-05CH11231
RP-ID  :  939892

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来源: UNT Digital Library

【 摘 要 】

The STAR Collaboration proposes to construct a state-of-the-art microvertex detector,the Heavy Flavor Tracker (HFT), utilizing active pixel sensors and silicon strip technology. The HFT will significantly extend the physics reach of the STAR experiment for precision measurement of the yields and spectra of particles containing heavy quarks. This will be accomplished through topological identification of D mesons by reconstruction of their displaced decay vertices with a precision of approximately 50 mu m in p+p, d+A, and A+A collisions. The HFT consists of 4 layers of silicon detectors grouped into two sub-systems with different technologies, guaranteeing increasing resolution when tracking from the TPC and the Silicon Strip Detector (SSD) towards the vertex of the collision. The Intermediate Silicon Tracker (IST), consisting of two layers of single-sided strips, is located inside the SSD. Two layers of Silicon Pixel Detector (PIXEL) are inside the IST. The PIXEL detectors have the resolution necessary for a precision measurement of the displaced vertex. The PIXEL detector will use CMOS Active Pixel Sensors (APS), an innovative technology never used before in a collider experiment. The APSsensors are only 50 mu m thick and at a distance of only 2.5 cm from the interaction point. This opens up a new realm of possibilities for physics measurements. In particular, a thin detector (0.28percent radiation length per layer) in STAR makes it possible to do the direct topological reconstruction of open charm hadrons down to very low pT by the identification of the charged daughters of the hadronic decay.