COMPONENT TEST H4IRRAD 15 TH NOVEMBER 2011 G. Spiezia, P. Peronnard, G. Foucard, S. Danzeca, P. Gander, E. Fadakis (EN/STI/ECE)

Slides:



Advertisements
Similar presentations
Stefan Roesler SC-RP/CERN on behalf of the CERN-SLAC RP Collaboration
Advertisements

Transistors (MOSFETs)
The Latchup Monitor System, ESA Meeting, December 9 th 2014 R. Secondo, A Masi, R. Losito, P. Peronnard, R. D’Aguanno, R. Ferraro The Latchup Monitor System,
MDT-ASD PRR C. Posch30-Aug-01 1 Radiation Hardness Assurance   Total Ionizing Dose (TID) Change of device (transistor) properties, permanent   Single.
CELeSTA CERN LATCHUP STUDENT SATELLITE TEST BOARD DEVELOPMENT AND CHARM PRELIMINARY RESULTS Raffaello Secondo ESA/ESTEC CERN Visit - DECEMBER 9 th 2014.
5 th LHC Radiation Day Radiation response of RADMON sensors T. Wijnands (TS/LEA), C. Pignard (TS/LEA) Acknowledgements : UCL Louvain-La-Neuve, PSI Villingen,
Optical Fibre Dosimetry First Thoughts. Goal Target Measuring dose in a distributed way using optical fibres (“active”) Constraints: – Mixed-Radiation.
Abstract: Based on the principle of the RADMON on line radiation monitoring system for the LHC, a new type of low cost, battery powered radiation monitors.
J. MEKKI (1/14) 05/12/12 – RadWG meeting Summary of the radiation levels of the equipments at CNRAD RF MosFETs Cryogenics TE/EPC LED warning system BPM.
A radiation-tolerant LDO voltage regulator for HEP applications F.Faccio, P.Moreira, A.Marchioro, S.Velitchko CERN.
2012 H4IRRAD test campaigns Summary of results S. Uznanski CERN, Geneva, Switzerland Radiation Working Group meeting Oct 16, 2012.
12004 MAPLD: 141Buchner Single Event Effects Testing of the Atmel IEEE1355 Protocol Chip Stephen Buchner 1, Mark Walter 2, Moses McCall 3 and Christian.
Performance of SPIROC chips in SKIROC mode
News from ESA-CNES Final Presentation Days 2013 A Masi, News from ESA-CNES Final Presentation Days 2013 News from ESA-CNES Final Presentation Days 2013.
Status of the PiN diodes irradiation tests B. Abi( OSU), R. Boyd (OU), P. Skubic (OU), F. Rizatdinova (OSU), K.K. Gan (Ohio State U.)
Radiation test - PSI Date Equipment Owner Test groupDUT May 20th EN/STI OSL, TLD BE/BI Detector June 1stTE/EPCEN/STI Mosfet Voltage regulators Voltage.
RADWG 6 TH TH OCTOBER 2012 G. Spiezia (EN/STI/ECE)
Chamber parameters that we can modify and that affect the rising time Number of ionisation clusters produced in the drift gap: Poisson Distribution Probability.
Total Dose Effects on Devices and Circuits - Principles and Limits of Ground Evaluation-
Online Radiation Dose Measurement System for ATLAS experiment I. Mandić a, representing ATLAS collaboration a Jožef Stefan Institute, Jamova 39, Ljubljana,
Online Radiation Dose Measurement System for ATLAS experiment I. Mandić a, V. Cindro a, I. Dolenc a, A. Gorišek a, G. Kramberger a, M. Mikuž a,b, J. Hartert.
TRAD, Tests & Radiations 13/09/2011 LHC POWER CONVERTER Radiation analysis.
Radiation Test Facilities G. Spiezia. Engineering Department ENEN Radiation tests facilities  Radiation test in the accelerator sector  External facilities.
Development of DC-DC converter ASICs S.Michelis 1,3, B.Allongue 1, G.Blanchot 1, F.Faccio 1, C.Fuentes 1,2, S.Orlandi 1, S.Saggini 4 1 CERN – PH-ESE 2.
FIPDiag PSI Radiation test Presentation Radwg meeting August 2011 Julien Palluel BE/CO/FE 1 1.Devices Under test 2.Description of the test setup 3.Beam.
Radiation Tolerant Electronics New Policy? Ph. Farthouat, CERN.
P. Denes Page 1 FPPA-Rad1 UHF1x and FPPA Radiation Hardness Radiation studies performed at OPTIS (PSI) with 72 MeV p and at 88” (LBL) with 55 MeV.
Apr, 2014 TE-EPC-CCE Radiation Tests
(1/8) J. Mekki RadWG meeting – 03/02/2015 CHARM facility update 03/02/2015.
Radiation Tolerant Electronics Expected changes Ph. Farthouat, CERN.
Valerio Re, Massimo Manghisoni Università di Bergamo and INFN, Pavia, Italy Jim Hoff, Abderrezak Mekkaoui, Raymond Yarema Fermi National Accelerator Laboratory.
CS TC 22 CT Basics CT Principle Preprocessing. 2 CT Basics CT principle preprocessing CS TC 22 Blockdiagram image processor.
Institute for Nuclear Research and Nuclear Energy Dimitrov L.P., Iaydjiev P.S., Mitev G.M., Vankov I.V.
RADWG 4 TH TH JULY 2012 G. Spiezia (EN/STI/ECE)
14/Sept./2004 LECC2004 Irradiation test of ASIC and FPGA for ATLAS TGC Level-1Trigger System 1 TID (  -ray) and SEE (proton) tests and results for ROHM.
CERN IT Department CH-1211 Genève 23 Switzerland t HP ProCurve 2910 Ethernet switch in CNRAD April-June 2012 RadWG Meeting Gyorgy.
TRIUMF and ISIS Test Facilities Radiation 2 Electronics (R2E) LHC Activities TRIUMF and ISIS test facilities Rubén García Alía, Salvatore Danzeca, Adam.
LHC Beam Loss Monitors, B.Dehning 1/15 LHC Beam loss Monitors Loss monitor specifications Radiation tolerant Electronics Ionisation chamber development.
J. MEKKI (1/8) 06/03/12 – RadWG meeting CNRAD plan Beam schedule – 1 st Slot Overall beam schedule for 2012 Equipments to be installed o Higher flux locations.
M.Moll, M.Silari, H.Vincke – 3.April Feedback  In total 134 forms filled:
Numerical signal processing for LVDT reading based on rad tol components Salvatore Danzeca Ph.D. STUDENT (CERN EN/STI/ECE ) Students’ coffee meeting 1/3/2012.
M.Moll, M.Silari, H.Vincke – 3.April Mixed field irradiation -- Who answered ?  In total 36 forms filled / 34 persons answered: 38% 62% CERN:
Radiation 4-5 December 2005 AB/BDI/BL.
Mixed field irradiation -- Who answered ?  In total 36 forms filled / 34 persons answered: 38% 62% CERN: mainly LHC related topics CERF: beside LHC topics.
AWAKE: D2E for Alexey beam properties Silvia Cipiccia, Eduard Feldbaumer, Helmut Vincke DGS/RP.
COTS Regulator Studies Derek Donley*, Mitch Newcomer, Mike Reilly *Hospital of the University of Pennsylvania, Radiation Oncology.
1 Single event upset test of the voltage limiter for the ATLAS Semiconductor tracker TSL Experiment Number: F151 distance between power supplies and modules.
TWEPP Paris, 09 Radiation Tests on the complete system of the instrumentation electronics for the LHC Cryogenics at the CNGS test facility Evangelia Gousiou.
(1/16) 08/05/12 – RadWG meeting G. Spiezia, P. Peronnard, E. Lefteris, P. Oser, J. Mekki PSI tests - Comparator Results Devices under test and beam conditions.
HECII-Workshop Munich, 12./13. February 2009 Measurement Strategy Workshop on Technology Selection for the SLHC Hadronic Endcap Calorimeter, Munich 2009.
Irradiation results of technologies for a custom DC-DC converter F.Faccio, G.Blanchot, S.Michelis, C.Fuentes, B.Allongue, S.Orlandi CERN – PH-ESE.
RadMon thermal neutron cross-section calibration D.Kramer for the RadMon team L.Viererbl, V.Klupak NRI Rez 1.
The New Radiation test facility at CERN: CHARM December 8 th 2014 CERN R2E project ESA/CERN meeting - December 8 th 2014 The new radiation tests facility.
New Irradiation Test Facility : CHARM June 10 th 2014 CERN R2E project CHARM Introduction June 10 th 2014 New CERN Irradiation facility : CHARM !!! Many.
Macom RF switches radiation-test results
Comparison Study of Bulk and SOI CMOS Technologies based Rad-hard ADCs in Space Feitao Qi , Tao Liu , Hainan Liu , Chuanbin Zeng , Bo Li , Fazhan Zhao.
CALIFES 2015 run preliminary results
DerivFIP – Radiation test
R2E-MD preliminary report – 3rd/4th July th July LSWG meeting
Irradiation test of Commercial (BASLER) digital cameras
CERN/SSC Technology Transfer Day
Radiation hardness tests of GaAs and Si sensors at JINR S. M
Irradiation test results for SAMPA MPW1 and plans for MPW2 irradiation tests Sohail Musa Mahmood
PSI test REPORT MARCH 2011 G. Spiezia, P. Peronnard (EN/STI/ECE)
Compact readout unit for the EP-RADMON radiation monitoring sensors
PhD student: Matteo Brucoli - EN/STI/ECE
Report on radiation test done in Casaccia on January 11, 2006
Collimator Control (SEUs & R2E Outlook)
High Rate Photon Irradiation Test with an 8-Plane TRT Sector Prototype
Radiation Working Group RADWG
Presentation transcript:

COMPONENT TEST H4IRRAD 15 TH NOVEMBER 2011 G. Spiezia, P. Peronnard, G. Foucard, S. Danzeca, P. Gander, E. Fadakis (EN/STI/ECE)

Outline  Component description  Goal of the test  Setup  Radiation conditions and dosimetry  Results  Conclusions

Components under test DUT Type- Tec Voltag e Parameters Nb parts Temperature ºC AD822Jfet-Amp+/-5 V Current bias/Offset Latch-up 2Room AD8220DiffAmp+/-5 V Offset Latch-up 2Room LTC2052 OpAmp- CMOS +/-5 V Offset Latch-up 2Room XC95108CPLD+5 VLatch-up370 XC95108CPLD+5 VLatch-up3Room MAX11046ADC +5 V Latch-up375 PCM1702kDAC+/-5 VLatch-up375

Motivation  Compare test at H4IRRAD and PSI for a better understanding of the ELDRS effect and destructive events  Some devices taken from the TRAD report  AD822  Known to be sensitive to ELDRS  To be tested at PSI at higher dose rate  AD8220  Tested at PSI and failed at 40 Gy  Comparison with H4IRRAD  LTC2052  LET threshold for latch-up at <10 MeV.cm2/mg.,  th =10 -6 cm 2  sat =10 -4  Test at H4IRRAD and PSI to verify if latch-up are induced

Motivation  CPLD XC95108  Tested at PSI HI and showed latch-up  Comparison with H4IRRAD. Test at room temperature and heated  Implementation of a shift registers  MAX bit ADC  Tested at PSI. No Latch-up  Comparison with H4IRRAD. Test at room temperature and heated  PCM1702K- 20 bit DAC  Possible use of the component  Test at H4IRRAD to verify destructive events. Test at room temperature and heated  Test at PSI to verify the TID and the cross section for Soft and destructive SEE

SETUP  Monitoring of the parameter drift  Amplifier parameters, ADC reference, and current consumption measured with a multimeter. Slow acquisition  Latch-up test  Separate anti latch-up circuit for each positive and negative Voltage supply  Unique anti latch-up circuit for the 3 ADC MAX11046 and the amplifiers  16 channels acquired at 1 MS/s for the latch-up detection

H4IRRAD – Beam conditions  H4IRRAD Internal location  Mixed field and high energy hadrons ±5 cm ±10 M. Calviani

H4IRRAD – Beam conditions  H4IRRAD Internal location target Top of internal rack with component test

H4IRRAD – Beam conditions  H4IRRAD Internal location  1.2e9 pot per cycle  Cycle ~ 45 s  Bunch length 5 s  TID/Pot ~ 3e-12 [Gy/pot]  TID per cycle ~ 3.6 mGy  TID during extraction (5s)=2.6Gy/h  Average Dose rate (3.6 mGy over 45 sec) = 0.3 Gy/h  Recommended dose rate to evaluate ELDR

H4IRRAD – Dosimetry  FLUKA calculation (TID in air)  High gradient on the target line  TID 35 Gy, HEH 4-5x10 10 cm -2

H4IRRAD – Dosimetry for TID  FLUKA calculation (TID in air)  High gradient on the target line  Score position to be reviewed  Radfets on the RADMON (2 oxide Thickness) FLUKA [Gy Air ]±50%400nm [Gy -Si]100nm [Gy -Si]TID ±50% 19/06-27/ /06-25/ ±50 19/06-21/ ±40 SLOT 3 19/10-7/ (TO be Verified)3535±17

H4IRRAD – Dosimetry for TID  FLUKA calculation (TID in air)  High gradient on the target line  Score position to be reviewed  Radfets on the RADMON (2 oxide Thickness)  HEH fluence is ~5x10 10 cm -2 POT= 1.12e+013 Radmon 1Radmon 2Radmon 3Radmon 4Radmon 5 Fluka Fluence HEH [cm -2 ] 5,62E+091,20E+102,62E+106,12E+108,35E+09 Fluence with SEU/TID ±11% 3,50E+091,07E+102,59E+104,78E+105,66E+09 Fluence with SEU/POT ±16% 0,00E+00 3,20E+105,07E+100,00E+00 % Difference Fluka vs SEU/TID % Difference Fluka vs SEU/POT

Results DUT Type Technology PSI, p+, >250Gy/h * H4IRRAD 0.3 Gy/h * H4IRRAD HEH [cm - 2 ]** Temperature AD822Jfet-AmpNo tested35-ok0 latchRoom AD8220DiffAmp 40 Gy - broken 35-ok0 latchRoom LTC2052OpAmp-CMOS Not tested yet 35-ok0 latchRoom XC95108CPLD35 – ok0 latchRoom XC95108CPLD35 - ok2 latch70 C MAX11046ADC- BiCMOS 200 Gy- Broken 35 – ok0 latch80 C PCM1702kDAC0 latch70 C *Max TID without failure or TID at which measurements are out of spec **Fluence/ nb latch

Results  Notes  Signals are noisy due to long cables  Decimation is applied for analysis Amplitude [V] OctoberNovember Noise Expected level

Results – AD822  H4IRRAD  3 Gy/h(per extraction)  0.3Gy/h (average)  35 Gy  Within specification but TID is low  PSI test to be done  NSREC2009: I bias degradation at about Gy at 0.01 rad/s  0.3 Gy/h ~35 Gy (100nm radfet measurement) I bias current

Results – AD8220  PSI  250 Gy/h  230 MeV p+  30 Gy –failure  I bias very high as soon as the beam is on-1nA  H4IRRAD  3 Gy/h(per extraction)  0.3Gy/h (average)  Within specification Differential amplifier; output signal OctoberNovember

Results – CPLD  H4IRRAD  5x10 10 cm 2  2 Latch-up events on the heated CPLD

Results – CPLD  H4IRRAD  5x10 10 cm 2  2 Latch-up events on the heated CPLD Power ON Power OFF Current increase to 500 mA First event

Results – CPLD  H4IRRAD  5x10 10 cm 2  2 Latch-up events on the heated CPLD Power ON Power OFF Current increase to 500 mA

Results – CPLD  H4IRRAD  5x10 10 cm 2  2 Latch-up events on the heated CPLD Latch

Conclusions  AD822  almost at the limit of specifications;  Seem to agree with literature  PSI test to be done  CPLD  Other components within specifications  2 Latch-up on the CPLD  No Latch-up on MAX11046 and PCM  Note  Signals are noisy  Detailed tests on mixed signal devices require a protected zone where a mother board can be placed  Comparison H4IRRAD (low dose rate and mixed field) – PSI (p+ 230 MeV, high flux, high dose rate)  Total TID 35 Gy; HEH fluence 5x10 10 cm -2  Less Fluence than expected  Difficult to compare

Back-up 

How to explain  H4IRRAD spectrum  Spectrum in the target line is dominated by high energy hadrons (Needed to verify destructive events)  Dose enhancement effect seems to appear mainly in case of Co60 irradiation  Microelectronics may degrade less in a Hadron environment with respect to pure gamma irradiation  Open point: depending on the technology, the Hadron energy (literature focused on proton), and the percentage composition of our spectrum

Results-slot 1 &2 DUT Type- Technology PSI, p+, >250Gy/h * H4IRRAD 0.3 Gy/h * Comment MAX410OpAmp-Bip100 Gy-ok85-ok OPA2227OpAmp200 Gy -ok85-ok TL072OpAmp200 Gy-ok- TL431Voltage Ref200 Gy-ok85 – ok TL432Voltage Ref 200 Gy-ok 85 - ok LM4041Voltage Ref200 Gy-Ok85 – ok INA141DiffAmp 130Gy-Out of spec 85 - ok Limit of spec MAX6341 Voltage Ref (ADC) 25 Gy-Out of spec 25 Gy-Out of spec. 3 mV drift over 100 Gy * Max TID without failure or TID at which measurements are out of spec