The NA62 Gigatracker pixel detector system

被引：5

作者：

Mazza, G. ^{[1
]}

Ceccucci, A. ^{[2
]}

Cortina, E. ^{[3
]}

Ramusino, A. Cotta ^{[3
]}

Dellacasa, G. ^{[1
]}

Fiorini, M. ^{[2
]}

Garbolino, S. ^{[1
]}

Jarron, P. ^{[2
]}

Kaplon, J. ^{[2
]}

Kluge, A. ^{[2
]}

Marchetto, F. ^{[1
]}

Martin, E. ^{[4
]}

Martoiu, S. ^{[1
]}

Noy, M. ^{[2
]}

Petrucci, F. ^{[3
]}

Riedler, P. ^{[2
]}

Rivetti, A. ^{[1
]}

Tiuraniemi, S. ^{[2
]}

机构：

[1] Ist Nazl Fis Nucl, Sez Torino, I-10125 Turin, Italy

[2] CERN, CH-1211 Geneva 23, Switzerland

[3] Ist Nazl Fis Nucl, Sez Ferrara, I-44100 Ferrara, Italy

[4] UCL, Louvain, Belgium

来源：

NUCLEAR INSTRUMENTS & METHODS IN PHYSICS RESEARCH SECTION A-ACCELERATORS SPECTROMETERS DETECTORS AND ASSOCIATED EQUIPMENT | 2010年 / 617卷 / 1-3期

关键词：

Hybrid pixel detector; Silicon pixel ASIC; TDC;

D O I：

10.1016/j.nima.2009.10.013

中图分类号：

TH7 [仪器、仪表];

学科分类号：

0804 ; 080401 ; 081102 ;

摘要：

The silicon tracker for the NA62 experiment has to provide both a time resolution of 150 ps rms and a space resolution of about 100 mu m rms. These challenging specifications require the development of a new readout electronics in order to address the problem of measuring the tracks arrival time with such a high channel density. Moreover, the high particle density (up to 1.5 MHz/mm(2) in the center and 0.8-1 GHz in total) requires a high speed measurement and data transmission in order to keep the dead time below 1%. (C) 2009 Elsevier B.V. All rights reserved.

引用

页码：558 / 559

页数：2

共 3 条

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NUCLEAR INSTRUMENTS & METHODS IN PHYSICS RESEARCH SECTION A-ACCELERATORS SPECTROMETERS DETECTORS AND ASSOCIATED EQUIPMENT, 2007, 572 (01) :290-291

[2]

KLUGE A, 2009, P SPIE C, V7249

[3]

MUNDAY D, 2004, CERNSPSC2004029 CERN

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