Homogeneity and thermal donors in p-type MCz-Si detector materials

Slides:



Advertisements
Similar presentations
CHAPTER 4 CONDUCTION IN SEMICONDUCTORS
Advertisements

Epitaxial Silicon Detectors for Particle Tracking Overview on Radiation Tolerance at Extreme Hadron Fluence G. Lindström (a), E. Fretwurst (a), F. Hönniger.
ELECTRICAL CONDUCTIVITY
Complex characterization of defect centres in neutron irradiated MCz silicon by PITS, photoluminescence and EPR methods Institute of Electronic Materials.
Semiconductor Device Physics
TCT study of silicon epitaxial and MCZ detectors V. Eremin 1, M. Boscardin 2, M. Bruzzi 3, D. Creanza 4, A. Macchiolo 5, D. Menichelli 3, C. Piemonte 2,
Eija Tuominen Siena TEST BEAM RESULTS OF A LARGE AREA STRIP DETECTOR MADE ON HIGH RESISTIVITY CZOCHRALSKI SILICON Helsinki Institute of Physics,
Eija Tuominen DEVELOPMENT OF RADIATION HARD DETECTORS Helsinki Institute of Physics (HIP) In close cooperation with: Microelectronics Centre,
REACTIONS OF INTERSTITIAL CARBON WITH BACKGROUND IMPURITIES IN N- AND P-TYPE SILICON STRUCTURES L.F. Makarenko*, L.I. Murin**, M. Moll***, F.P. Korshunov**,
Trapping in silicon detectors G. Kramberger Jožef Stefan Institute, Ljubljana Slovenia G. Kramberger, Trapping in silicon detectors, Aug , 2006,
Energy Band View of Semiconductors Conductors, semiconductors, insulators: Why is it that when individual atoms get close together to form a solid – such.
Department of Physics VERTEX 2002 – Hawaii, 3-7 Nov Outline: Introduction ISE simulation of non-irradiated and irradiated devices Non-homogeneous.
Characterization of 150  m thick epitaxial silicon pad detectors from different producers after 24 GeV/c proton irradiation Herbert Hoedlmoser (1), Michael.
1Ruđer Bošković Institute, Zagreb, Croatia
Charge collection studies on heavily diodes from RD50 multiplication run G. Kramberger, V. Cindro, I. Mandić, M. Mikuž Ϯ, M. Milovanović, M. Zavrtanik.
Haga clic para modificar el estilo de texto del patrón Progress on p-type isolation technology M. Lozano, F. Campabadal, C. Fleta, S. Martí *, M. Miñano.
KIT – University of the State of Baden-Wuerttemberg and National Research Center of the Helmholtz Association Institut für Experimentelle Kernphysik
KINETICS OF INTERSTITIAL CARBON ANNEALING AND MONITORING OF OXYGEN DISTRIBUTION IN SILICON PARTICLE DETECTORS L.F. Makarenko*, M. Moll**, F.P. Korshunov***,
RD50 Katharina Kaska1 Trento Workshop : Materials and basic measurement problems Katharina Kaska.
M. Bruzzi et al. Thermal donors in MCz Si, Trento Meeting Rd50 February 28, 2005 Mara Bruzzi, D. Menichelli, M. Scaringella INFN Florence, University of.
Implantation of N-O in Diamond
1 Free Electron Model for Metals Metals are very good at conducting both heat and electricity. A lattice of in a “sea of electrons” shared between all.
Gunnar Lindstroem – University of Hamburg1 G. Lindstroem a, E. Fretwurst a, F. Hönniger a, A. Junkes a, K. Koch a and I. Pintilie a,b a Institute for Exp.
12004 MAPLD/138Bytkin Reduction of the Thermo stable Radiation Defects Probability Formation in Si and SiGe as a Physical Basis of the Bipolar npn Transistors.
SILICON DETECTORS PART I Characteristics on semiconductors.
M. Bruzzi, the issue of p-type disuniformity, 7° RD50 Workshop, CERN, November 14-16, 2005 The issue of doping disuniformity in p-type MCz Si sensors M.
D. Menichelli, RD50, Hamburg, august TSC, DLTS and transient analysis in MCz silicon Detectors at different process temperature, irradiation.
BASIC ELECTRONICS Module 1 Introduction to Semiconductors
1 Space charge sign inversion and electric field reconstruction in 24 GeV proton irradiated MCZ Si p + -n(TD)-n + detectors processed via thermal donor.
Silicon detector processing and technology: Part II
8 July 1999A. Peisert, N. Zamiatin1 Silicon Detectors Status Anna Peisert, Cern Nikolai Zamiatin, JINR Plan Design R&D results Specifications Status of.
SALIENT FEATURES OF SHALLOW DONOR INTERACTIONS IN PROTON-IRRADIATED SILICON V.V. Emtsev and G.A. Oganesyan Ioffe Physicotechnical Institute Russian Academy.
CERN, November 2005 Claudio Piemonte RD50 workshop Claudio Piemonte a, Maurizio Boscardin a, Alberto Pozza a, Sabina Ronchin a, Nicola Zorzi a, Gian-Franco.
J.Vaitkus. RD50 Workshop, Liverool, May, 2011 Deep level system Gaussian approximation according the extrinsic photoconductivity in irradiated Si.
INTERSTITIAL DEFECT REACTIONS IN P-TYPE SILICON IRRADIATED AT DIFFERENT TEMPERATURES L.F. Makarenko*, S.B. Lastovski**, L.I. Murin**, M. Moll*** * Belarusian.
Charge Collection and Trapping in Epitaxial Silicon Detectors after Neutron-Irradiation Thomas Pöhlsen, Julian Becker, Eckhart Fretwurst, Robert Klanner,
Junction Formation The position of the junction for a limited source diffused impurity in a constant background is given by The position of the junction.
G. Steinbrück, University of Hamburg, SLHC Workshop, Perugia, 3-4 April Epitaxial Silicon Detectors for Particle Tracking Overview on Radiation Tolerance.
RD50 Michael Moll – PH-TA1-SDMeeting February 25, Three R&D strategies:  Material engineering - Defect engineering of silicon (oxygenation, dimers,
Simulations of Hadron Irradiation Effects for Si Sensors Using Effective Bulk Damage Model A. Bhardwaj 1, H. Neugebauer 2, R. Dalal 1, M. Moll 2, Geetika.
Jaakko Härkönen, 6th "Hiroshima" Symposium, Carmel, California, September Magnetic Czochralski silicon as detector material J. Härkönen, E. Tuovinen,
J.Vaitkus et al. PC spectra. CERN RD50 Workshop, Ljubljana, "Analysis of deep level system transformation by photoionization spectroscopy"
Studies on n and p-type MCz and FZ structures of the SMART Collaboration irradiated at fluences from 1.0 E+14 to 5.6E+15 p cm -2 RD50 Trento Workshop ITC-IRST.
Deep Level Transient Spectroscopy study of 3D silicon Mahfuza Ahmed.
G. PellegriniInstituto de Microelectrónica de Barcelona Status of LGAD RD50 projects at CNM28th RD50 Workshop (Torino) 1 Status of LGAD RD50 projects at.
Boron and Phosphorus Implantation Induced Electrically Active Defects in p-type Silicon Jayantha Senawiratne 1,a, Jeffery S. Cites 1, James G. Couillard.
COURSE NAME: SEMICONDUCTORS Course Code: PHYS 473.
Ioana Pintilie, 11 th RD50 Workshop, November 2007, Geneve
First Investigation of Lithium Drifted Si Detectors
Characterization and modelling of signal dynamics in 3D-DDTC detectors
First production of Ultra-Fast Silicon Detectors at FBK
“Semiconductor Physics”
Irradiation and annealing study of 3D p-type strip detectors
Study of radiation damage induced by 26MeV protons and reactor neutrons on heavily irradiated MCz, FZ and Epi silicon detectors N. Manna Dipartimento.
HG-Cal Simulation using Silvaco TCAD tool at Delhi University Chakresh Jain, Geetika Jain, Ranjeet Dalal, Ashutosh Bhardwaj, Kirti Ranjan CMS simulation.
Study of radiation damage induced by 24/c GeV and 26MeV protons on heavily irradiated MCz and FZ silicon detectors N. Manna Dipartimento Interateneo di.
Modeling Vacancy-Interstitial Clusters and Their Effect on Carrier Transport in Silicon E. Žąsinas, J. Vaitkus, E. Gaubas, Vilnius University Institute.
Sensor Wafer: Final Layout
Strong infrared electroluminescence from black silicon
Results from the first diode irradiation and status of bonding tests
16th RD 50 Workshop - Barcelona, 31 May - 2 June 2010
V2O and V3O DEFECTS IN SILICON: FTIR STUDIES
Example Design a B diffusion for a CMOS tub such that s=900/sq, xj=3m, and CB=11015/cc First, we calculate the average conductivity We cannot calculate.
Einstein Relation—the relation between  and D
Simulation of signal in irradiated silicon detectors
Basic Semiconductor Physics
Vladimir Cindro, RD50 Workshop, Prague, June 26-28, 2006
EE105 Fall 2007Lecture 1, Slide 1 Lecture 1 OUTLINE Basic Semiconductor Physics – Semiconductors – Intrinsic (undoped) silicon – Doping – Carrier concentrations.
Lecture 1 OUTLINE Basic Semiconductor Physics Reading: Chapter 2.1
Energy Band View of Semiconductors
Presentation transcript:

Homogeneity and thermal donors in p-type MCz-Si detector materials P. Luukka, J. Härkönen, E. Tuovinen, H.K. Nordlund and E. Tuominen Helsinki Institute of Physics Gustaf Hällströmin katu 2 00014 University of Helsinki Finland Panja Luukka, 9th RD50 Workshop, CERN, 16-18 October 2006

Panja Luukka, 9th RD50 Workshop, CERN, 16-18 October 2006 Outline Processing issues. Thermal Donors (TD) in Cz-Si Homogeneity of samples Conclusions Panja Luukka, 9th RD50 Workshop, CERN, 16-18 October 2006

Panja Luukka, 9th RD50 Workshop, CERN, 16-18 October 2006 Samples Samples were processed on p-type MCz-Si wafers. The starting material was 4” diameter double-side-polished 300±2 μm thick <100> Cz-Si wafers. The nominal resistivity, measured by the four point probe method, of the boron-doped wafers was 1800 Ωcm. Two types of pad detectors were processed at the Microelectronics Center of Helsinki University of Technology: p+/p/n+ -diode structures and n+/p/p+ structures processed with a different mask set. The active pad implanted area was 5 × 5 mm2. It was surrounded by one wide (100 μm) and 16 (16 μm wide) small guard-rings . The distance between the active area implant and the first guard ring was 10 μm. A 1 mm diameter round opening in the front metallization was left for TCT measurements Panja Luukka, 9th RD50 Workshop, CERN, 16-18 October 2006

Interstitial oxygen concentration in MCz-Si material Oxygen concentration was measured by the Fourier Transformation Infrared (FTIR) spectroscopy at the Institute of Electronic Materials Technology (ITME), Warszawa, Poland from a thick reference wafer. Center 4,95*1017 cm-3 Right 4,89*1017 cm-3 Left 4,93*1017 cm-3 Right 4,93*1017 cm-3 Panja Luukka, 9th RD50 Workshop, CERN, 16-18 October 2006

Processing of Cz-Si Detectors Basically no difference from standard Fz-Si detector process, except… High O content leads to Thermal Donor (TD) formation at temperatures 400°C – 600°C. TD formation can be enhanced if H is present. Typical process steps at 400°C – 600°C - Aluminum sintering (e.g. 30 min @ 450°C) - Passivation insulators over metals (LTO,TEOS etc ~600°C + H2 from Si3H4 process gas) Panja Luukka, 9th RD50 Workshop, CERN, 16-18 October 2006

Thermal Donors in Cz-Si TDs are oxygen complexes that form shallow states in Si band gap within 0.01 eV-0.2 eV energy range below the conduction band. High O content leads to Thermal Donor (TD) formation at temperatures 400°C – 600°C, which can yield to a TD concentration comparable with the initial doping concentration in the high resistivity silicon. TD formation can be enhanced if H is present. Effective resistivity can be adjusted in p-type MCz-Si 500 cm <  < 10 kcm With this method it is possible to engineer the Vfd of p-type MCz-Si n+/p-/p+ detectors Panja Luukka, 9th RD50 Workshop, CERN, 16-18 October 2006

Thermal donor formation Formation of TDs has often been explained to be due to so-called anomalously fast diffusing species (FDS). Oxygen dimers (O2) and trimers (O3) among other oxygen complexes have been proposed to be such FDS’s. Additionally, a fourth-power dependence of thermal donor generation rate on the oxygen concentration has widely been quoted. The fourth-power reaction order assumption for the generation rate has generally been accepted to be evidence that the core of the TD defect consist of four oxygen atoms. Panja Luukka, 9th RD50 Workshop, CERN, 16-18 October 2006

Thermal donor formation There are, however, experimental observations based on the infrared absorption method that claim strong deviations from the fourth-power dependence, which originally was established to be TD generation at 450ºC. With lower temperatures, at e.g. 430ºC, the exponential dependence in the formation has been reported to be close to 1.83. Additionally, Y. J. Lee et al have shown by total energy calculations that the TD formation is not due to the FDS’s but oxygen chains that move and capture relatively unmoving oxygen atoms. They report a reaction order close to 2. J. von Boehm, http://www.csc.fi/lehdet/tietoyhteys/TY3_2004.pdf Panja Luukka, 9th RD50 Workshop, CERN, 16-18 October 2006

Thermal donor generation (experimental results) The TD formation is almost linear It is therefore obvious that the empirical models claiming fourth power dependence on the oxygen concentration, cannot explain our experimental results. One data point is average of 10 diodes over the wafer diameter Error bars represent standard deviation Panja Luukka, 9th RD50 Workshop, CERN, 16-18 October 2006

Panja Luukka, 9th RD50 Workshop, CERN, 16-18 October 2006 Fitting of the model Exponential fit of the proposed model to the experimental data. The data points correspond to the average of the measurements of Neff. We have made an effort to improve the existing models by following the time and temperature depended equation with two fitting parameters. Fitting gives following result: exponent to which the oxygen concentration is raised Panja Luukka, 9th RD50 Workshop, CERN, 16-18 October 2006

Panja Luukka, 9th RD50 Workshop, CERN, 16-18 October 2006 Homogeneity The values of Vfd and Ileak are expressed as averagestandard deviation. The yield percentage refers to the number of bad samples out of 57 excluded from data. Each wafer consisted of 80 diodes from which 57 were measured. The sample was considered to be bad if breakdown occured before the full depletion. P-stop 1×1015 cm-2 P-spray Vfd[V] Ileak[nA] Yield [%] P042 X - 1105.5 3.22.1 93 P068 1×1012 cm-2 1155.7 2.62.0 91 P069 3×1012 cm-2 1154.4 2.21.8 84 P082 5×1012 cm-2 1124.6 3.32.4 86 P083 1064.4 2.62.4 58 Panja Luukka, 9th RD50 Workshop, CERN, 16-18 October 2006

Panja Luukka, 9th RD50 Workshop, CERN, 16-18 October 2006 Conclusions There is a good agreement between the calculations and the experimental data, based on measurement of Vfd, if the TD generation is assumed to obey NTD  Oi1.89 dependence on the oxygen concentration. There is technological importance in TD’s. The shallow donors have twofold influence on the macroscopic properties of the detectors: First, shallow oxygen thermal donors can be utilized during the fabrication process in order to manipulate the effective doping concentration (Neff) of the silicon bulk. Second, the shallow donors interact with the radiation defects and influence the radiation hardness of the detectors. With TD generation method it is possible, with low cost and with a process of low thermal budget, to fabricate detectors with high oxygen concentration that can be depleted at voltages less than 100 V. Panja Luukka, 9th RD50 Workshop, CERN, 16-18 October 2006