Si mini-pad production for MPC-Ex (A pre-shower upgrade for PHENIX) Y. Kwon (Yonsei Univ.)

Slides:



Advertisements
Similar presentations
of Single-Type-Column 3D silicon detectors
Advertisements

CBM Calorimeter System CBM collaboration meeting, October 2008 I.Korolko(ITEP, Moscow)
Trapping in silicon detectors G. Kramberger Jožef Stefan Institute, Ljubljana Slovenia G. Kramberger, Trapping in silicon detectors, Aug , 2006,
Silicon Preshower for the CMS: BARC Participation
CALICE SiW Electromagnetic Calorimeter Testbeam performance and results Roman Pöschl LAL Orsay IEEE – NSS&MCI '08 Dresden/Germany - October The.
Rochester Institute of Technology - MicroE © REP/LFF 8/17/2015 Metal Gate PMOS Process EMCR201 PMOS page-1  10 Micrometer Design Rules  4 Design Layers.
RF background, analysis of MTA data & implications for MICE Rikard Sandström, Geneva University MICE Collaboration Meeting – Analysis session, October.
Charge collection studies on heavily diodes from RD50 multiplication run G. Kramberger, V. Cindro, I. Mandić, M. Mikuž Ϯ, M. Milovanović, M. Zavrtanik.
Fabrication of Active Matrix (STEM) Detectors
LCWS2002G/H Joint Session Fabrication of a Silicon Pixel/Pad for dE/dx Measurement H. Park (Kyungpook National U.) I.H. Park (Ewha Womans U.)
Semiconductor detectors An introduction to semiconductor detector physics as applied to particle physics.
Dahee Kim (Ewha womans university) for MPC-EX collaboration TEST OF MINI-PAD SILICON SENSOR FOR PHENIX MPC-EX.
IC Process Integration
Medipix sensors included in MP wafers 2 To achieve good spatial resolution through efficient charge collection: Produced by Micron Semiconductor on n-in-p.
Possibility for Double DVCS measurement in Hall A Alexandre Camsonne SBS Meeting June 4 th 2013.
Prospect for Si sensors in Korea Y. Kwon (Yonsei Univ.)
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.
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
INTEGRATED CIRCUITS Dr. Esam Yosry Lec. #3. Diffusion  Introduction  Diffusion Process  Diffusion Mechanisms  Why Diffusion?  Diffusion Technology.
Status report on the Asian Solid State Tracking R&D March 31, 2003 M. Iwasaki University of Tokyo.
Silicon detector processing and technology: Part II
Forward photon measurement and generic detector R&D Y. Kwon Yonsei Univ.
8 July 1999A. Peisert, N. Zamiatin1 Silicon Detectors Status Anna Peisert, Cern Nikolai Zamiatin, JINR Plan Design R&D results Specifications Status of.
V.Dzhordzhadze1 Nosecone Calorimeter Simulation Vasily Dzhordzhadze University of Tennessee Muon Physics and Forward Upgrades Workshop Santa Fe, June 22,
10/21/06 PragueE.Kistenev, NCC meeting NCC status report Physics case Design status Mechanics ROU’s & Front End Pad-structured Stripixel Sensors Pad-structured.
CERN, November 2005 Claudio Piemonte RD50 workshop Claudio Piemonte a, Maurizio Boscardin a, Alberto Pozza a, Sabina Ronchin a, Nicola Zorzi a, Gian-Franco.
Nov Beam Catcher in KOPIO (H. Mikata Kaon mini worksyop1 Beam Catcher in the KOPIO experiment Hideki Morii (Kyoto Univ.) for the KOPIO.
Measurement of J/  -> e + e - and  C -> J/  +   in dAu collisions at PHENIX/RHIC A. Lebedev, ISU 1 Fall 2003 DNP Meeting Alexandre Lebedev, Iowa State.
RD50 funding request Fabrication and testing of new AC coupled 3D stripixel detectors G. Pellegrini - CNM Barcelona Z. Li – BNL C. Garcia – IFIC R. Bates.
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.
11/18/2016 Test beam studies of the W-Si tracking calorimeter for the PHENIX forward upgrade Y. Kwon, Yonsei Univ., PHENIX.
MPC-EX hardware design and capability The MPC-EX detector system is an extension of the existing Muon Piston Calorimeters (MPCs) of the PHENIX experiment.
Lehman Review April 2000 D. Bortoletto 1 Forward Pixel Sensors Daniela Bortoletto Purdue University US CMS DOE/NSF Review April 12,2000 Progress.
Jaakko Härkönen, 6th "Hiroshima" Symposium, Carmel, California, September Magnetic Czochralski silicon as detector material J. Härkönen, E. Tuovinen,
Forward hard  measurement by a W/Si calorimeter Y. Kwon, J. H. Kang, M. G. Song (Yonsei Univ.) 1.
ICT 1 SINTEF Edge-On Sensor with Active Edge Fabricated by 3D-Technology T. E. Hansen 1), N. Ahmed 1), A. Ferber 2) 1) SINTEF MiNaLab 2) SINTEF Optical.
Giulio Pellegrini 27th RD50 Workshop (CERN) 2-4 December 2015 Centro Nacional de MicroelectrónicaInstituto de Microelectrónica de Barcelona 1 Status of.
Claudio Piemonte Firenze, oct RESMDD 04 Simulation, design, and manufacturing tests of single-type column 3D silicon detectors Claudio Piemonte.
Prospects for Si sensors in Korea Y. Kwon (Yonsei Univ.)
Preshower PRR July NCSR DEMOKRITOS Production Center : Institute of Microelectronics (IMEL) Regional Center : Institute of Nuclear Physics (INP)
A Forward Calorimeter (FoCal) as upgrade for the ALICE experiment at CERN S. Muhuri a, M. Reicher b and T. Tsuji c a Variable Energy Cyclotron Centre,
Low Cost Silicon Sensor Y. Kwon in exploration with J. Lajoie, E. Kistenev, A. Sukhanov, and Z. Li as part of MPC-EX R&D.
K2K and JHF-nu muon monitor Jun Kameda (KEK) 1. K2K muon monitor 2. JHF-ν muon monitor 3. Summary International workshop on Neutrino Beam Instrumentation,
Development of Silicon Microstrip Sensors in 150 mm p-type Wafers
New Mask and vendor for 3D detectors
First Investigation of Lithium Drifted Si Detectors
Characterization and modelling of signal dynamics in 3D-DDTC detectors
Simplified process flow for bonding interface characterization
Preliminary results from 3D CMS Pixel Detectors
First production of Ultra-Fast Silicon Detectors at FBK
EMT362: Microelectronic Fabrication
Irradiation and annealing study of 3D p-type strip detectors
MPC-Ex Project in Korea
K2K and JHF-nu muon monitor
Detection of muons at 150 GeV/c with a CMS Preshower Prototype
Results from the first diode irradiation and status of bonding tests
Fab. Example: Piezoelectric Force Sensor (1)
Thin Planar Sensors for Future High-Luminosity-LHC Upgrades
ILC Detector Activities in Korea
A Silicon-Tungsten ECal for the SiD Concept
A FOrward CALorimeter for the PHENIX experiment
First physics from the ALICE electromagnetic calorimeters
Simulation study for Forward Calorimeter in LHC-ALICE experiment
Ion-Side Small Angle Detection Forward, Far-Forward, & Ultra-Forward
Production and test of Si sensors for W-Si sandwich calorimeter
Pixel sensor for ALICE ITS upgrade & CIS
Pixel sensor for ALICE ITS upgrade & CIS
Fabrication of 3D detectors with columnar electrodes of the same doping type Sabina Ronchina, Maurizio Boscardina, Claudio Piemontea, Alberto Pozzaa, Nicola.
Presentation transcript:

Si mini-pad production for MPC-Ex (A pre-shower upgrade for PHENIX) Y. Kwon (Yonsei Univ.)

FOCAL 2011-June W/Si sandwich calorimeter --- Old history

Calorimeter geometry & test setup Preamp hybrid 7 vertical channels grouped (cost issue) 8 pad sensors in one carrier board Beam

Energy distribution fits with Gaussian function (with highly suppressed low energy tail) Beam energy resolution  Detector energy resolution 75(GeV) electron at normal incidence

Summary Deposited energy distribution ~ Gaussian Lateral shower containment in 5 x 5 pads Good linearity Energy resolution for electron Longitudinal/Lateral shower development : Good agreement with simulation Position resolution from pad : 2.1 mm The detector performs as designed. But not funded!

6 inch fabrication line 6/32 8 inch fabrication line R&D environment 300 cm 2 ~ $ 500 What survived!

MPC-EX A new start, W/Si preshower upgrade

Minipad Sensor for PHENIX MPC-Ex MPC-Ex (Muon Piston Calorimeter Extension) is a pre-shower detector for the electromagnetic calorimeter called MPC(Muon Piston Calorimeter) of the experiment PHENIX. Minipad will be used as the active sensors in MPC-Ex to detect charged particles appearing in pre-shower, initial part of an electromagnetic shower. MPC-Ex will reconstruct π 0 particles within its acceptance up to the momentum of 50 (GeV/c).

What is Si sensor? (Sensor on Si wafer)

What is Si sensor? (Diced sensor)

FZ N - Wafer 1.Starting Material (FZ N - Wafer, > 5 kΩ.cm) 2.Thermal Oxidation: 900 nm 3.Front-Side PR Coating 4.Photo Mask(1); N-Channel Stop (Option) 5.Back-Side Oxide Wet-Etch N-Ch. Stop (Option) Oxide PIN Process - Process flow

FZ N - Wafer 6.POCl 3 Doping: 900 ℃, Rs Target < 20 Ω.cm 7.Oxide Wet Etch: 100 nm 8.Thermal Oxidation: 900 ℃, 100 nm (N+ Side Target=300 nm) 9.High Temperature Drive-in (Option) N-Ch. Stop (Option) N+ Oxide Process flow

FZ N - Wafer 10.Photo Mask(2); P+ Active 11.Oxide Dry & Wet Etch/PR Strip 12.Buffer Oxidation: 850 ℃, 20 nm 13.Active Ion Implantation: B11, 80 keV, 1×10 15 cm Annealing: 900 ℃, 170 min N-Ch. Stop (Option) N+ Guardring Active Area Oxide P+ Process flow

FZ N - Wafer 15.Metal Deposition: TiW/Ai-1%Si/TiW=70/800/100 nm 16.Photo Mask(2); Metal 17.Metal Etch/PR Strip N-Ch. Stop (Option) N+ Guardring Active Area Oxide P+ Metal Process flow

FZ N - Wafer 18.PE-CVD Oxide Deposition: 1,000 nm 19.Photo Mask(3); Pad 20.Oxide & TiW Dry Etch/PR Strip N-Ch. Stop (Option) N+ Guardring Active Area Oxide P+ Metal PE-Oxide Pad Area Process flow

FZ N - Wafer 21.Front-Side PR Coating 22.Back-Side Oxide Wet Etch/PR Strip 23.Back-Side Metal Deposition: Al-1%Si=1,000 nm 24.Alloy: N 2 /H ℃, 30 min N-Ch. Stop (Option) N+ Guardring Active Area Oxide P+ Metal PE-Oxide Pad Area Metal Process flow

FZ N - Wafer 25.Wafer Dicing N-Ch. Stop (Option) N+ Guardring Active Area Oxide P+ Metal PE-Oxide Pad Area Metal Process flow

Actual process sheet

Actual masks (passivation)

Issue with metal etching Etched metal region : Clean (test pattern area to check metal pattern) Metal spot (We checked the spot is real and of varying size ~ a few Micron typical) 5  75  35 

Fabrication & Delivery

Sensor Classification GRADESTANDARDNOTE A~1  A leakage for 60V. B1~10  A. COver 10  ABroken or Short Reverse bias I-V 표 2.1 I-V 측정으로 60V bias 에서 leakage current 에 따른 센서 등급표

A Grade Sensor 그림 2.9 I-V curve : Guard ring( 좌 ), Main pattern( 우 ) Main pattern 에서 leakage current 기준으로 A Grade

Sensor Documentation 표 2.3 A 부터 F 까지 set sensor 의 등급비율표. 각각 24 장 Final sensor yield ~ 75%

Dahee in sensor test at Unitech Where’s Seyong?

R & D Yes, there was R&D with BNL instrumentation.

2 Concept of Novel GRS A segmented, low-dose (a few times of /cm 2 ) n + -implant on near GRS can remove the detector oxide-property dependence with lower E-field Segmented, low-dose n + -implant Lower E-fields

Two publications from R&D and more efforts in progress

To be published around Dec. 15

Sensors will work OK for the expected neutron fluence.

Clue for next generation R&D (Guardringless Si sensor?)

Comparison between 2D (planar) and 3D detectors p+p+ n+n+ n+n+ p+p+ p+p+ p+p+ p+p+ p+p+ n+n+ p+p+ n+n+ d Thickness C Electrode spacing C 2D (planar) detector Conventional 3D-column electrode detector (S. Parker, et al) Electrodes are planar (2D) ion implants (<1 µm deep) Electrodes are vertically (3D) etched and doped columns (100’s µm deep) C =d full depletion voltage V fd depends on detector thickness d C is decoupled from d full depletion voltage V fd is independent of detector thickness d V fd can be too large for large d (>1mm) or after heavy radiation V fd can be small if C is made small (<100  m)

YONSEI BIO-IT Micro Fab.

Summary As of Nov. 2 nd, 2014, We delivered 481 good Si Mini-Pad sensors to our colleagues, and the delivered sensors are being integrated into the MPC-EX detector. Simple math to show the scale of exercise : Stability of all sensors was tested for 2 hours at the bias of 60(V), twice full depletion voltage. 2 hours/sensor * 481 sensors = 40 days

Prospect? Analysis : Dr. S. H. Lim is working on shower reconstruction. Various wild trials are under progress. Stay tuned! Extension of R&D : Increased R&D network and facility. Yes, of course, we can make Si sensors effectively.

Exclusive diffractive process at RHIC & Roman Pot

Roman Pot?

Focus so far at RHIC = EIC

 -A &  -p physics

STAR UPC program (  -A dominated?)

HERA MEASUREMENT A report from H. Kowalski, L. Motyka, and G. Watt Phys. Rev. D74,

Dipole model V  real photon : Deeply virtual Compton scattering