Comparative measurements of highly irradiated n-in-p and p-in-n 3D silicon strip detectors

Silicon detectors in 3D technology are a candidate for applications in environments requiring an extreme radiation hardness, as in the innermost layers of the detectors at the proposed High-Luminosity LHC. In 3D detectors, the electrodes are made of columns etched into the silicon perpendicular to the surface. This leads to higher electric fields, a smaller depletion voltage and a reduced trapping probability of the charge carriers compared to standard planar detectors. In this article, the signal and the noise of irradiated n-in-p and p-in-n 3D silicon strip detectors are compared. The devices under test have been irradiated up to a fluence of 2×1016 1 MeV neutron equivalent particles per square centimetre (neq/cm2), which corresponds to the fluence expected for the inner pixel detector layers at the High-Luminosity LHC. A relative charge collection efficiency of approximately 70% was obtained even after the highest irradiation fluence with both detector types. The influence of different temperatures on the signal and the noise is investigated and results of annealing measurements are reported.

[1]  A. A. Affolder,et al.  Collected charge of planar silicon detectors after pion and proton irradiations up to 2.2 ×1016 neq cm−2 , 2010 .

[2]  Marko Zavrtanik,et al.  Effective trapping time of electrons and holes in different silicon materials irradiated with neutrons, protons and pions , 2002 .

[3]  R. Bates,et al.  Simulations of radiation-damaged 3D detectors for the Super-LHC , 2008 .

[4]  R. Bates,et al.  Beam Test Measurements With 3D-DDTC Silicon Strip Detectors on n-Type Substrate , 2010, IEEE Transactions on Nuclear Science.

[5]  Marko Zavrtanik,et al.  Determination of effective trapping times for electrons and holes in irradiated silicon , 2002 .

[6]  V. Cindro,et al.  Investigation of Irradiated Silicon Detectors by Edge-TCT , 2010, IEEE Transactions on Nuclear Science.

[7]  Celeste Fleta,et al.  First double-sided 3-D detectors fabricated at CNM-IMB , 2008 .

[8]  K. Fujita,et al.  Micro-discharge at strip edge of silicon microstrip sensors , 1996 .

[9]  D. Cauz,et al.  ATLAS pixel detector electronics and sensors , 2008 .

[10]  W. N. Grant Electron and hole ionization rates in epitaxial silicon at high electric fields , 1973 .

[11]  M. Beuzekom,et al.  Precision scans of the Pixel cell response of double sided 3D Pixel detectors to pion and X-ray beams , 2011 .

[12]  V. Cindro,et al.  Annealing effects in n+–p strip detectors irradiated with high neutron fluences☆ , 2011 .

[13]  C. Piemonte,et al.  Test Beam Results of 3D Silicon Pixel Sensors for the ATLAS upgrade , 2011, 1101.4203.

[14]  V. Eremin,et al.  Concept of Double Peak electric field distribution in the development of radiation hard silicon detectors , 2007 .

[15]  R. Bates,et al.  Charge Collection Studies and Electrical Measurements of Heavily Irradiated 3D Double-Sided Sensors and Comparison to Planar Strip Detectors , 2011, IEEE Transactions on Nuclear Science.

[16]  R. Klanner,et al.  Properties of a radiation-induced charge multiplication region in epitaxial silicon diodes ☆ , 2010, 1007.4735.

[17]  R. Bates,et al.  Beam Test Measurements With Planar and 3D Silicon Strip Detectors Irradiated to sLHC Fluences , 2011, IEEE Transactions on Nuclear Science.

[18]  M. Cavalli-Sforza,et al.  3D-FBK pixel sensors: Recent beam tests results with irradiated devices , 2011 .

[19]  C. Piemonte,et al.  Double-Sided, Double-Type-Column 3-D Detectors: Design, Fabrication, and Technology Evaluation , 2008, IEEE Transactions on Nuclear Science.

[20]  U. Parzefall,et al.  Functional characterization of 3D-DDTC detectors fabricated at FBK-irst , 2008, 2008 IEEE Nuclear Science Symposium Conference Record.

[21]  V. Eremin,et al.  The origin of double peak electric field distribution in heavily irradiated silicon detectors , 2002 .

[22]  V. Cindro,et al.  Observation of full charge collection efficiency in heavily irradiated n+p strip detectors irradiated up to 3×1015 neq/cm2 , 2010 .

[23]  P. Allport,et al.  Evidence of enhanced signal response at high bias voltages in planar silicon detectors irradiated up to 2.2×1016 neq cm−2 , 2011 .

[24]  S. Stapnes,et al.  Physics potential and experimental challenges of the LHC luminosity upgrade , 2002, hep-ph/0204087.

[25]  K. Rajkanan,et al.  Absorption coefficient of silicon for solar cell calculations , 1979 .

[26]  R. Mcintyre Multiplication noise in uniform avalanche diodes , 1966 .

[27]  C. Kenney,et al.  3D — A proposed new architecture for solid-state radiation detectors , 1997 .

[28]  Ricardo Marco-Hernandez,et al.  A portable readout system for microstrip silicon sensors (ALIBAVA) , 2009, 2008 IEEE Nuclear Science Symposium Conference Record.

[29]  P. Ciampolini,et al.  Radiation hard silicon detectors—developments by the RD48 (ROSE) collaboration , 2001 .

[30]  Michael Schmelling,et al.  The Beetle Reference Manual , 2001 .