001545495 001__ 1545495
001545495 003__ SzGeCERN
001545495 005__ 20211231040336.0
001545495 0247_ $$2DOI$$a10.1016/j.nima.2013.06.101
001545495 0248_ $$aoai:cds.cern.ch:1545495$$pcerncds:FULLTEXT$$pcerncds:CERN:FULLTEXT$$pcerncds:CERN
001545495 035__ $$9arXiv$$aoai:arXiv.org:1305.0531
001545495 035__ $$9Inspire$$a1231739
001545495 037__ $$9arXiv$$aarXiv:1305.0531$$cphysics.ins-det
001545495 041__ $$aeng
001545495 084__ $$2PACS$$a29.40.Gx
001545495 084__ $$2PACS$$a29.40.Wk
001545495 100__ $$aBaudot, Jérôme$$uStrasbourg, IPHC
001545495 245__ $$aOptimisation of CMOS pixel sensors for high performance vertexing and tracking
001545495 269__ $$c03 May 2013
001545495 260__ $$c2013
001545495 300__ $$a4 p
001545495 500__ $$9arXiv$$aPresented at the Vienna Conference on Instrumentation 2013 4 pages, 5 figures
001545495 520__ $$aCMOS Pixel Sensors tend to become relevant for a growing spectrum of charged particle detection instruments. This comes mainly from their high granularity and low material budget. However, several potential applications require a higher read-out speed and radiation tolerance than those achieved with available devices based on a 0.35 micrometers feature size technology. This paper shows preliminary test results of new prototype sensors manufactured in a 0.18 micrometers process based on a high resistivity epitaxial layer of sizeable thickness. Grounded on these observed performances, we discuss a development strategy over the coming years to reach a full scale sensor matching the specifications of the upgraded version of the Inner Tracking System (ITS) of the ALICE experiment at CERN, for which a sensitive area of up to about 10 square meters may be equipped with pixel sensors.
001545495 520__ $$9arXiv$$aCMOS Pixel Sensors tend to become relevant for a growing spectrum of charged particle detection instruments. This comes mainly from their high granularity and low material budget. However, several potential applications require a higher read-out speed and radiation tolerance than those achieved with available devices based on a 0.35 micrometers feature size technology. This paper shows preliminary test results of new prototype sensors manufactured in a 0.18 micrometers process based on a high resistivity epitaxial layer of sizeable thickness. Grounded on these observed performances, we discuss a development strategy over the coming years to reach a full scale sensor matching the specifications of the upgraded version of the Inner Tracking System (ITS) of the ALICE experiment at CERN, for which a sensitive area of up to about 10 square meters may be equipped with pixel sensors.
001545495 540__ $$aarXiv nonexclusive-distrib. 1.0$$barXiv$$uhttp://arxiv.org/licenses/nonexclusive-distrib/1.0/
001545495 595__ $$aLANL EDS
001545495 65017 $$2arXiv$$aDetectors and Experimental Techniques
001545495 65027 $$2arXiv$$aParticle Physics - Experiment
001545495 690C_ $$aARTICLE
001545495 690C_ $$aCERN
001545495 695__ $$9LANL EDS$$aphysics.ins-det
001545495 695__ $$9LANL EDS$$ahep-ex
001545495 700__ $$aBesson, Auguste$$uStrasbourg, IPHC
001545495 700__ $$aClaus, Gilles$$uStrasbourg, IPHC
001545495 700__ $$aDulinski, Wojciech$$uStrasbourg, IPHC
001545495 700__ $$aDorokhov, Andrei$$uStrasbourg, IPHC
001545495 700__ $$aGoffe, Mathieu$$uStrasbourg, IPHC
001545495 700__ $$aHu-Guo, Christine$$uStrasbourg, IPHC
001545495 700__ $$aMolnar, Levente$$iINSPIRE-00254710$$uStrasbourg, IPHC
001545495 700__ $$aSanchez-Castro, Xitzel$$iINSPIRE-00290349$$uStrasbourg, IPHC
001545495 700__ $$aSenyukov, Serhiy$$iINSPIRE-00270653$$uStrasbourg, IPHC
001545495 700__ $$aWinter, Marc$$uStrasbourg, IPHC
001545495 773__ $$c480-483$$pNucl. Instrum. Methods Phys. Res., A$$v732$$y2013
001545495 8564_ $$uhttp://arxiv.org/pdf/1305.0531.pdf$$yPreprint
001545495 8564_ $$81260603$$s85842$$uhttp://cds.cern.ch/record/1545495/files/arXiv:1305.0531.pdf
001545495 8564_ $$81260604$$s29876$$uhttp://cds.cern.ch/record/1545495/files/m32ter_P25_real3colorsPlot_compareIrrad_BW.png$$y00005 Expected performances of a square pixel ($20\times20$~$\mu$m$^{2}$) integrating a preamplification, with emulated binary output from test beam results. The detection efficiency (black bullets), the fake rate (blue squares) and the spatial resolution (red triangles) evolutions with the discriminator threshold (in units of noise) are displayed for three different radiation loads and at the highest coolant temperature of 30$^{\circ}$C.
001545495 8564_ $$81260605$$s30517$$uhttp://cds.cern.ch/record/1545495/files/L4_1_SNR_BW.png$$y00003 MIMOSA32 $20\times40$~$\mu$m$^{2}$ elongated pixel beam test results (60-120~GeV $\pi$): SNR distribution for four temperature-radiation load conditions.
001545495 8564_ $$81260606$$s21470$$uhttp://cds.cern.ch/record/1545495/files/Eff_vs_Irrad_Temp_P25_P6_P31_L41_BW.png$$y00004 MIMOSA32 test beam results: evolution of the detection efficiency with the temperature and radiation load conditions, for three pixel variants.
001545495 8564_ $$81260607$$s24009$$uhttp://cds.cern.ch/record/1545495/files/p6_Xrays_no+3MRad.png$$y00002 Charges collected from $^{55}Fe$ X-rays illumination of a MIMOSA32 pixel including PMOS transistors. Left: seed pixel alone. Right: $2\times2$ cluster. Solid empty histogram: before irradiation, Dotted filled histogram: after a 3~MRad TID.
001545495 8564_ $$81260608$$s16263$$uhttp://cds.cern.ch/record/1545495/files/m28_3colorsPlot_compareIrrad_BW.png$$y00000 Measurement of MIMOSA28 charged particle detection efficiency (bullets) and fake hit rate (crosses) as a function of the threshold values (in mV) of the discriminators implemented in the sensor before (solid lines) and after irradiation (dashed lines).
001545495 8564_ $$82344222$$s9563$$uhttp://cds.cern.ch/record/1545495/files/fig00001.png$$y00001 noimgComparison of the requirements of various vertex detectors, in terms of read-out speed ($\sigma_{t}$) and radiation tolerance related to the total ionising dose (TID) and non-ionising particle fluence.
001545495 916__ $$sn$$w201317
001545495 960__ $$a13
001545495 962__ $$b1509547$$k480-483$$nvienna20130211
001545495 980__ $$aARTICLE
001545495 980__ $$aConferencePaper