Medipix sensors included in MP wafers 2 To achieve good spatial resolution through efficient charge collection: Produced by Micron Semiconductor on n-in-p.

Slides:



Advertisements
Similar presentations
Silicon Technical Specifications Review General Properties Geometrical Specifications Technology Specifications –Mask –Test Structures –Mechanical –Electrical.
Advertisements

Silicon Preshower for the CMS: BARC Participation
Belle-II Meeting Nov Nov Thomas Bergauer (HEPHY Vienna) Status of DSSD Sensors.
1 Generic Silicon Detector R&D Thomas Bergauer Institute for High Energy Physics (HEPHY) Austrian Academy of Sciences, Vienna for the SiLC Collaboration.
Alternative technologies for Low Resistance Strip Sensors (LowR) at CNM CNM (Barcelona), SCIPP (Santa Cruz), IFIC (Valencia) M. Ullán, V. Benítez, J. Montserrat,
Pixel Sensors for ATLAS Sally Seidel University of New Mexico Pixel ‘98 8 May 1998.
November 3-8, 2002D. Bortoletto - Vertex Silicon Sensors for CMS Daniela Bortoletto Purdue University Grad students: Kim Giolo, Amit Roy, Seunghee.
Sensors for CDF RunIIb silicon upgrade LayerR min (cm)1 MeV eq-n cm * * * * * *10.
20th RD50 Workshop (Bari)1 G. PellegriniInstituto de Microelectrónica de Barcelona G. Pellegrini, C. Fleta, M. Lozano, D. Quirion, Ivan Vila, F. Muñoz.
Embedded Pitch Adapters a high-yield interconnection solution for strip sensors M. Ullán, C. Fleta, X. Fernández-Tejero, V. Benítez CNM (Barcelona)
St Malo, 13 th April 2002Václav Vrba, Institute of Physics, AS CR 1 Václav Vrba Institute of Physics, AS CR, Prague Silicon pad sensors for W-Si ECal.
Semiconductor detectors
Charge collection studies on heavily diodes from RD50 multiplication run G. Kramberger, V. Cindro, I. Mandić, M. Mikuž Ϯ, M. Milovanović, M. Zavrtanik.
11 th RD50 Workshop, CERN Nov Results with thin and standard p-type detectors after heavy neutron irradiation G. Casse.
Semi-conductor Detectors HEP and Accelerators Geoffrey Taylor ARC Centre for Particle Physics at the Terascale (CoEPP) The University of Melbourne.
ALBA Synchrotron – 17 June 2010 Centro Nacional de MicroelectrónicaInstituto de Microelectrónica de Barcelona First Measurements on 3D Strips Detectors.
Silicon Microstrip detector Single sided and double sided K.Kameswara rao, Tariq Aziz, Chendvankar, M.R.Patil Tata institute of fundamental research, Mumbai,
Wire Bonding and Analogue Readout ● Cold bump bonding is not easy ● Pixel chip is not reusable ● FE-I3 is not available at the moment ● FE-I4 is coming.
Development of n-in-p planar pixel sensors with active edge for the ATLAS High-Luminosity Upgrade L. Bosisio* Università degli Studi di Trieste & INFN.
Status of the Low-Resistance (LowR) Strip Sensors Project CNM (Barcelona), SCIPP (Santa Cruz), IFIC (Valencia) Contact person: Miguel Ullán.
1 G. Pellegrini The 9th LC-Spain meeting 8th "Trento" Workshop on Advanced Silicon Radiation Detectors 3D Double-Sided sensors for the CMS phase-2 vertex.
QA Workshop at CERN 3-4 November Hamamatsu silicon detectors for high energy physics experiments Kazuhisa Yamamura*, Shintaro Kamada.
SILICON DETECTORS PART I Characteristics on semiconductors.
M. Lozano, C. Fleta*, G. Pellegrini, M. Ullán, F. Campabadal, J. M. Rafí CNM-IMB (CSIC), Barcelona, Spain (*) Currently at University of Glasgow, UK S.
Summary of CMS 3D pixel sensors R&D Enver Alagoz 1 On behalf of CMS 3D collaboration 1 Physics Department, Purdue University, West Lafayette, IN
Evaluation of the Low Resistance Strip Sensors (Low-R) Fabricated at CNM CNM (Barcelona), SCIPP (Santa Cruz), IFIC (Valencia) Contact person: Miguel Ullán.
Foundry Characteristics
1 ATLAS Pixel Sensors Sally Seidel University of New Mexico U.S. ATLAS Pixel Review LBNL, 2 November 2000.
Planar Pixels Sensors Activities in France. Phase-2 and core R&D activities in France -Development of sensor simulations models -Sensor technology Edgeless/active.
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.
US ATLAS Upgrade Strip Meeting, Hartmut F.-W. Sadrozinski, SCIPP 1 Upgrade Silicon Strip Detectors (SSD) Hartmut F.-W. Sadrozinski SCIPP, UC Santa Cruz.
News on microstrip detector R&D —Quality assurance tests— Anton Lymanets, Johann Heuser 12 th CBM collaboration meeting Dubna, October
Thin Silicon R&D for LC applications D. Bortoletto Purdue University Status report Hybrid Pixel Detectors for LC.
1 ATLAS Pixel Sensors Sally Seidel University of New Mexico U.S. ATLAS Pixel Review LBNL, 9 November 2001.
Low Resistance Strip Sensors – RD50 Common Project – RD50/ CNM (Barcelona), SCIPP (Santa Cruz), IFIC (Valencia) Contact person: Miguel Ullán.
Update on Simulation and Sensor procurement for CLICPix prototypes Mathieu Benoit.
CERN-ECFA-NuPECC Workshop on the LHeC LHeC Tracker Design viewed from ATLAS I. Tsurin Chavannes-de-Bogis, Switzerland General requirements Sensor technology.
Technology Overview or Challenges of Future High Energy Particle Detection Tomasz Hemperek
A. Macchiolo, 13 th RD50 Workshop, CERN 11 th November Anna Macchiolo - MPP Munich N-in-n and n-in-p Pixel Sensor Production at CiS  Investigation.
1 J.M. Heuser − STS Development Microstrip detector GSI-CIS Johann M. Heuser, GSI Li Long, CIS CBM Collaboration Meeting, GSI, Update on.
Solid State Detectors for Upgraded PHENIX Detector at RHIC.
TCT measurements with SCP slim edge strip detectors Igor Mandić 1, Vladimir Cindro 1, Andrej Gorišek 1, Gregor Kramberger 1, Marko Milovanović 1, Marko.
Maria Rita Coluccia Simon Kwan Fermi National Accelerator Laboratory
Lehman Review April 2000 D. Bortoletto 1 Forward Pixel Sensors Daniela Bortoletto Purdue University US CMS DOE/NSF Review April 12,2000 Progress.
The Sixth International "Hiroshima" Symposium Giulio Pellegrini Technology of p-type microstrip detectors with radiation hard p-spray, p-stop and moderate.
CNM double-sided 3D strip detectors before and after neutron irradiation Celeste Fleta, Richard Bates, Chris Parkes, David Pennicard, Lars Eklund (University.
Development of Novel Si Stripixel Detectors for For Nuclear and High Energy Physics Experiments* Z. Li and the Si Detector Development and Processing group:
LHeC “shaking hands” meeting Comments on the Tracker Design I. Tsurin Page 1Liverpool December 16th, 2011 Detector granularity Sensor technology Frontend.
Giulio Pellegrini 27th RD50 Workshop (CERN) 2-4 December 2015 Centro Nacional de MicroelectrónicaInstituto de Microelectrónica de Barcelona 1 Status of.
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.
P. Fernández-Martínez – Optimized LGAD PeripheryRESMDD14, Firenze 8-10 October Centro Nacional de MicroelectrónicaInstituto de Microelectrónica de.
Latest news on 3D detectors IRST CNM IceMos. CNM 2 wafers fabricated Double side processing with holes not all the way through, (aka Irst) n-type bulk.
Trench detectors for enhanced charge multiplication G. Casse, D. Forshaw, M. Lozano, G. Pellegrini G. Casse, 7th Trento Meeting - 29/02 Ljubljana1.
TCAD Simulation for SOI Pixel Detectors October 31, 2006 Hirokazu Hayashi, Hirotaka Komatsubara (Oki Elec. Ind. Co.), Masashi Hazumi (KEK) for the SOIPIX.
Giulio Pellegrini Actividades 3D G. Pellegrini, C. Fleta, D. Quirion, JP Balbuena, D. Bassignana.
Comparison of the AC and DC coupled pixels sensors read out with FE-I4 electronics Gianluigi Casse*, Marko Milovanovic, Paul Dervan, Ilya Tsurin 22/06/20161.
Low Mass, Radiation Hard Vertex Detectors R. Lipton, Fermilab Future experiments will require pixelated vertex detectors with radiation hardness superior.
Andrei Nomerotski 1 Andrei Nomerotski, University of Oxford for LCFI collaboration LCWS2008, 17 November 2008 Column Parallel CCD and Raw Charge Storage.
Investigation of the effects of thickness, pitch and manufacturer on charge multiplication properties of highly irradiated n-in-p FZ silicon strips A.
Page 1 Liverpool January 11th, 2012 LHCb Upgrade Meeting Planar Silicon Detectors I. Tsurin Generic sensor R&D ATLAS-oriented commitments LHCb-oriented.
Testing PXD6 - testing plans
New Mask and vendor for 3D detectors
Available detectors in Liverpool
Irradiation and annealing study of 3D p-type strip detectors
Highlights of Atlas Upgrade Week, March 2011
SuperB SVT Silicon Sensor Requirements
Sensor Wafer: Final Layout
Design and fabrication of Endcap prototype sensors (petalet)
Yasuhiro Sugimoto KEK 17 R&D status of FPCCD VTX Yasuhiro Sugimoto KEK 17
Presentation transcript:

Medipix sensors included in MP wafers 2 To achieve good spatial resolution through efficient charge collection: Produced by Micron Semiconductor on n-in-p wafers (150 and 300  m thick) - HV performance (main focus in this work) - Optimal implant geometry

Pixel Detector Programme in Liverpool 6” wafers fabricated by Micron 3 Strip detectors: Polysilicon bias resistors Punch-through biasing Bias rail option Pixel detectors: FE-I3, FE-I4, PSI-46, MPIX-II, APC, APR (interleaved pixels) Pad detectors: RD-50, PSI, MPI guard structures, Cut edge scenarios (8, 4, 2, 1 rings) Test structures: Process control, device modelling in the double metal “n-in-p” FZ process

Pixel Detectors with Wire-bonded Readout 4 Column-parallel / Row-parallel readout Pulse shape analysis Cross-calibration of ToT Fast “Cold” bonding to the readout for annealing studies Re-use of bonding pads No need to irradiate the readout -> good data quality Inter-”strip” resistance and capacitance measurements Measurement of the punch- through voltage of the biasing circuit Shuffled R/O channels to minimise the cross talk between connection lines Working horse: pixel sensors with interleaved readout implants connected to wire bond pads

5 Readout Implants, part I (resistances) Sheet resistance ~400 Ohm/square (implant dose ~10 14 cm -2 ) Inter-”strip” resistance ~1 TOhm/cm for 50 um pitch (see spare slides) PCB for measurements of the punch through voltage, potentials on guard rings and characteristic inter-“strip” resistance and capacitance Sensor’s substrate is attached to the heat sink for cooling by the air flow

Inter-”strip” capacitance ~0.5 pF/cm for 50 um pitch (see spare slides) Readout Implants, part II (capacitances) 6 Capacitance to bulk ~1 pF/sq. mm at full depletion voltage (reduces when the bias network is powered, this effect depends on the sensor size; it is not quantified here) Full depletion voltage ~80 V (unirradiated, bulk resistivity ~15 kOhm.cm) IC(V) curves for the FE-I3 single chip sensors

Punch-through voltage ~1 V/um -> the hybrid designer should pay attention to: - potential of the bias ring connected to ASIC (pixel shortening, chip breakdown) - potential of the 1st GR connected to ASIC (chip breakdown) 7 Readout Implants, part III (punch-through biasing) Atlas pixel sensor Punch-through gap = 3.5um

Guard Structures “RD-50”“PSI”“MPI” “Floating metal” 8 “RD-50” + more geometries (new wafer) I(V) curves for 4x4 mm 2 pads

9 Measurements of the Guard Ring Potentials GR has a substrate potential unless bulk depletion reaches it 1 2 Measurement scheme 1: Device modelling: guard structure is NOT a voltage divider ! GR9 GR1 GR GR9 GR1 GR GR1 GR2 GR6 GR4 GR3

Interference with the Guard Structure :-( :-) Straight implant and metal lines Thin and wide sections for pads Straight implants, broken metal Thinned implants, metal bypass 10 Probe padsAlignment marks I(V) curves for 4x4 mm 2 pads I(V) curves for FE-I4 SC sensors

Cut Edge Studies 11 RD-50 guard structures RD-50 8xPSI 8xMPI 8x Breakdown condition: bulk depletion in the lateral direction reaches the cut edge

12 Charge Collection Measurements after High Radiation Doses A. Affolder, et. al., NIMA (2010) doi /j.nima K. Hara, et. al., NIMA (2010) doi /j.nima Measurements for the Micron n-in-p strip detectors using a data acquisition system based on the SCTA-128VG readout chip (40 MHz readout speed) Detector thickness = 300+/-20 um

Spare Slide 5: new 6-inch Micron Pixel Wafer 5x FE-I4 tiles (2guard ring options, 250 um and 450 um ) 14x FE-I4 SC (4 guard ring options, 450 um and 250 um) 12x FE-I3 SC (4 guard ring options, 40, 80, 200, 600 um) 2x Medipix-II tiles, 2x Medipix SC 4 diodes (process control, new GR) Test structures (transistor models, R, C, punch-through) Delivery: (first batch) There is a room for 14x FE-I4 tiles (good homogeneity across the wafer) n-in-p, single metal FZ process, 300um There are plans to deliver n-in-n, and thinned wafers and 1 wafer with no capacitor oxide

Proposal: making a Medipix only mask, to accommodate tiles, single sensors, variation of the GR structure to study effectiveness of asymmetric reduction of edge..... Look for partners (I know interest from Prague) for sharing the mask cost. I propose production with Micron on 6” wafers (this can be added to the running program with CNM, with whom we can share ideas and test of new geometries.....).