Ústav technické a experimentální fyziky Institute of Experimental and Applied Physics

Processing and characterization of edgeless radiation detectors for large area detection

NázevTitle
Processing and characterization of edgeless radiation detectors for large area detectionProcessing and characterization of edgeless radiation detectors for large area detection
Druh výsledkuResult type
Článek v časopiseJournal article
AutořiAuthors
J. Kalliopuska, X. Wu, J. Jakůbek, S. Eranen, T. Virolainen
DOIDOI
10.1016/j.nima.2013.06.097
Časopis / citaceJournal / citation
Nuclear Instruments and Methods in Physics Research, Section A, Accelerators, Spectrometers, Detectors and Associated Equipment. 2013, 731(731), 205-209. ISSN 0168-9002.
RokYear
2013
JazykLanguage
eng
WoSWoS
000327487500040
ScopusScopus
2-s2.0-84888389275
RIVRIV
RIV/68407700:21670/13:00215991!RIV14-GA0-21670___
ProjektProject
Energetické a napjatostní aspekty kvazikřehkého lomu – důsledky pro určování lomově-mechanických parametrů silikátových kompozitůEnergetic and stress state aspects of quasi-brittle fracture – consequences for determination of fracture-mechanical parameters of silicate composites; Pracoviště pro nedestruktivní testování, diagnostiku a 3D zobrazování pomocí neutronové radiografie a tomografie (2011-2015, TA0/TA)Facility for nondestructive testing, diagnostics and 3D imaging based on neutron radiography and tomography.

AbstraktAbstract

The edgeless or active edge silicon pixel detectors have been gaining a lot of interest due to improved silicon processing capabilities. At VTT, we have recently triggered a multi-project wafer process of edgeless silicon detectors. Totally 80 pieces of 150 mm wafers were processed to provide a given number of detector variations. Fabricated detector thicknesses were 100, 200, 300 and 500 µm. The polarities of the fabricated detectors on the given thicknesses were n-in-n, p-in-n, n-in-p and p-in-p. On the n-in-n and n-in-p wafers the pixel isolation was made either with a common p-stop grid or with a shallow p-spray doping. The wafer materials were high resistivity Float Zone and Magnetic Czochralski silicon with crystal orientation of <100>. In this paper, the electric properties on various types of detectors are presented. The results from spectroscopic measurement show a good energy resolution of the edge pixels, indicating an excellent charge collection near the edge pixels of the edgeless detector.

The edgeless or active edge silicon pixel detectors have been gaining a lot of interest due to improved silicon processing capabilities. At VTT, we have recently triggered a multi-project wafer process of edgeless silicon detectors. Totally 80 pieces of 150 mm wafers were processed to provide a given number of detector variations. Fabricated detector thicknesses were 100, 200, 300 and 500 µm. The polarities of the fabricated detectors on the given thicknesses were n-in-n, p-in-n, n-in-p and p-in-p. On the n-in-n and n-in-p wafers the pixel isolation was made either with a common p-stop grid or with a shallow p-spray doping. The wafer materials were high resistivity Float Zone and Magnetic Czochralski silicon with crystal orientation of <100>. In this paper, the electric properties on various types of detectors are presented. The results from spectroscopic measurement show a good energy resolution of the edge pixels, indicating an excellent charge collection near the edge pixels of the edgeless detector.