- Herve Grabas - Ecole Superieure d’Electicite 1 Internship presentation - University of Chicago – 3 sept. 2009.

Slides:



Advertisements
Similar presentations
1 Continuous Scintillator Slab with Microchannel Plate PMT for PET Heejong Kim 1, Chien-Min Kao 1, Chin-Tu Chen 1, Jean-Francois Genat 2, Fukun Tang 2,
Advertisements

Recent news about SiPM based applications R&D in DESY Nicola D’Ascenzo University of Hamburg - DESY.
COSMIC RAY MUON DETECTION USING SCINTILLATION COUNTER AND WAVELENGTH SHIFTING FIBERS ARUNODAYA BHATTACHARYA VSRP-2009,TIFR,MUMBAI 6/7/09.
A scalable DAQ system using the DRS4 sampling chip H.Friederich 1, G.Davatz 1, U.Hartmann 2, A.Howard 1, H.Meyer 1, D.Murer 1, S.Ritt 2, N.Schlumpf 2 1.
TileCal Electronics A Status Report J. Pilcher 17-Sept-1998.
SANE S pin A symmetries of the N ucleon E xperiment SEEN THROUGH THE EYES OF JOHN GERMAN MASTERS STUDENT FROM NORTH CAROLINA A&T STATE UNIVERSITY. JUNE.
Microchannel Plates signals, Picosecond timing, Design’s minimum performance.
4-channel ASIC Tests Michael Baumer, Jean-Francois Genat, Sam Meehan, Eric Oberla August 26 th 2009.
Directional Detectors and Digital Calorimeters Ed Norbeck and Yasar Onel University of Iowa For the 25 th Winter Workshop on Nuclear Dynamics Big Sky,
Solid State Detectors- 5 T. Bowcock 2 Schedule 1Position Sensors 2Principles of Operation of Solid State Detectors 3Techniques for High Performance Operation.
Large Area, High Speed Photo-detectors Readout Jean-Francois Genat + On behalf and with the help of Herve Grabas +, Samuel Meehan +, Eric Oberla +, Fukun.
Development of Picosecond-Resolution Large-Area Time-of-Flight Systems C. Ertley 2, J. Anderson 1, K.Byrum 1, G.Drake 1, H.Frisch 2, J. Genat 2, H. Sanders.
Photomultiplier Tube. What is it? Extremely sensitive detector of light in the ultraviolet, visible and near infrared Multiplies the signal produced by.
The Time-of-Flight system of the PAMELA experiment: in-flight performances. Rita Carbone INFN and University of Napoli RICAP ’07, Rome,
10 Picosecond Timing Workshop 28 April PLANACON MCP-PMT for use in Ultra-High Speed Applications.
1 Light Collection  Once light is produced in a scintillator it must collected, transported, and coupled to some device that can convert it into an electrical.
Development of a 20 GS/s Sampling Chip in 130nm CMOS Technology Jean-Francois Genat On behalf of Mircea Bogdan 1, Henry J. Frisch 1, Herve Grabas 3, Mary.
Photon detection Visible or near-visible wavelengths
Why silicon detectors? Main characteristics of silicon detectors: Small band gap (E g = 1.12 V)  good resolution in the deposited energy  3.6 eV of deposited.
Report on SiPM Tests SiPM as a alternative photo detector to replace PMT. Qauntify basic characteristics Measure Energy, Timing resolution Develop simulation.
Derandomiser block E.Atkin, A.Kluev MEPhI,A.Voronin SINP MSU.
MR (7/7/05) T2K electronics Beam structure ~ 8 (9?) bunches / spill bunch width ~ 60 nsec bunch separation ~ 600 nsec spill duration ~ 5  sec Time between.
The George Washington University School of Engineering and Applied Science Department of Electrical and Computer Engineering ECE122 – Lab 7 MOSFET Parameters.
FLC Group Test-beam Studies of the Laser-Wire Detector 13 September 2006 Maximilian Micheler Supervisor: Freddy Poirier.
10/26/20151 Observational Astrophysics I Astronomical detectors Kitchin pp
PSD Chip Calculations. Energy Conversions Erad Energy of incident radiation (MeV) evis Energy of visible photon radiation (eV) εcon Conversion efficiency.
L.ROYER – TWEPP Oxford – Sept The chip Signal processing for High Granularity Calorimeter (Si-W ILC) L.Royer, J.Bonnard, S.Manen, X.Soumpholphakdy.
NESTOR SIMULATION TOOLS AND METHODS Antonis Leisos Hellenic Open University Vlvnt Workhop.
1 G.Pessina, RICH Elec Upg, 11 April 2010 Analog Channels per chip4 to 8 Digital channel per chip4 to 8 Wire-bond pitch (input channels) Input capacitance.
16-Nov-2002Konstantin Beloous1 Digital Hadron Calorimeter Energy Resolution.
July 4, 2008 SuperBelle Meeting, KEKPeter Križan, Ljubljana Peter Križan University of Ljubljana and J. Stefan Institute Burle MCP PMTs as photon detector.
A 20 GS/s sampling ASIC in 130nm CMOS technology.
Techniques for Nuclear and Particle Physics Experiments By W.R. Leo Chapter Eight:
Update on Physical Parameters that influence Timing Jean-Francois Genat LPNHE Paris LAPPD Electronics & Integration Review July 9th 2012, Chicago.
Lecture 3-Building a Detector (cont’d) George K. Parks Space Sciences Laboratory UC Berkeley, Berkeley, CA.
Sampling chip psTDC_02 Jean-Francois Genat – Herve Grabas Mary Heinz – Eric Oberla 1/27/ psTDC_02 presentation.
Jean-François Genat Fast Timing Workshop June 8-10th 2015 FZU Prague Timing Methods with Fast Integrated Technologies 1.
MCP Testing Using Square Conductive Pads as Readout Anode Sagar Setru 1/19/2014.
ASIC Development for Vertex Detector ’07 6/14 Y. Takubo (Tohoku university)
Testbeam analysis Lesya Shchutska. 2 beam telescope ECAL trigger  Prototype: short bars (3×7.35×114 mm 3 ), W absorber, 21 layer, 18 X 0  Readout: Signal.
TORCH IOP meeting Manchester March 31, 2015 TORCH Maarten van Dijk On behalf of the TORCH collaboration (CERN, University of Oxford,
PArISROC Photomultiplier Array Integrated in Sige Read Out Chip Selma Conforti Frédéric Dulucq Christophe de La Taille Gisèle Martin-Chassard Wei
EKT 314/4 WEEK 10 : CHAPTER 4 DATA ACQUISITION AND CONVERSION ELECTRONIC INSTRUMENTATION.
Analog Circuits Hiroyuki Murakami. CONTENTS Structure of analog circuits Development of wide linear range CSA system Problem of analog circuits How to.
 13 Readout Electronics A First Look 28-Jan-2004.
1Jean-Francois Genat on behalf of the LAPPD collaboration (
Transient Waveform Recording Utilizing TARGET7 ASIC
A 2 Gsps Waveform Digitizer ASIC in CMOS 180 nm Technology
Analog FE circuitry simulation
MoNA detector physics How to detect neutrons. Thomas Baumann NSCL.
96-channel, 10-bit, 20 MSPS ADC board with Gb Ethernet optical output
Increasing the Spatial Resolution of the Tile Calorimeter
A First Look J. Pilcher 12-Mar-2004
A Low Power Readout ASIC for Time Projection Chambers in 65nm CMOS
Storage cell – Psec timing project
Progress on the development of a low-cost fast-timing microchannel plate photodetector Junqi Xie1, Karen Byrum1, Marcel Demarteau1, Joseph Gregar1, Edward.
Jean-Francois Genat, Sam Meehan, Eric Oberla August 26th 2009
The New Readout Electronics for the SLAC Focusing DIRC Prototype (SLAC experiment T-492 ) L. L. Ruckman, G. S. Varner Instrumentation Development Laboratory.
Jean-Francois Genat, Herve Grabas, Eric Oberla August 2d 2010
MCP Electronics Time resolution, costs
Chis status report.
Latest Results from T979: PSec Time-of-flight
Jean-Francois Genat – Herve Grabas Mary Heinz – Eric Oberla
ASPID (Application of Silicon Photomultipliers to Imaging Detectors)
Presented by T. Suomijärvi
TOF read-out for high resolution timing
Improved study of the cells
PHYS 3446 – Lecture #17 Wednesday ,April 4, 2012 Dr. Brandt
Why silicon detectors? Main characteristics of silicon detectors:
Presentation transcript:

- Herve Grabas - Ecole Superieure d’Electicite 1 Internship presentation - University of Chicago – 3 sept. 2009

Contents Project description Detectors in High Energy Physics Signal processing for Pico-second time resolution Detector to Chip integration Chip structure and characteristics Operation of the chip Storage cells Design 2 Internship presentation - University of Chicago – 3 sept

Acknowledgements 3 Internship presentation - University of Chicago – 3 sept

Contents 4 Internship presentation - University of Chicago – 3 sept

Project description At the present time: PMT High gain High bandwidth Low noise In the future: MCP-PMT’s All of the above Smaller path-lengths Possible tailoring Readout electronics: integrated analog memory and ADC 5 Internship presentation - University of Chicago – 3 sept

Contents 6 Internship presentation - University of Chicago – 3 sept

Detectors HEP detectors structure 7 Internship presentation - University of Chicago – 3 sept

Particle measurements Mass m Velocity  Momentum p 8 Internship presentation - University of Chicago – 3 sept p =  m  The goal of a HEP detector is to measure one of these three characteristics

Calorimeter The goal of a calorimeter is to measure the particle's energy loss in a dense medium 9 Internship presentation - University of Chicago – 3 sept  Calorimeters gives the particle’s energy but requires a lot of radial space

Cerenkov angle measurement Cerenkov formula: cos  n  10 Internship presentation - University of Chicago – 3 sept  Cerenkov light detectors give the velocity of the particle and also require a lot of radial space

Time-of-flight measurement Reconstruction of the particle trajectory Determination of the time of flight of the particle 11 Internship presentation - University of Chicago – 3 sept  Time-of-flight detectors can be very thin

Photomultiplier tubes Photo-electric effect Secondary emission effect 12 Internship presentation - University of Chicago – 3 sept  Big electron path-length ~10cm

MCP detector principle 13 Internship presentation - University of Chicago – 3 sept Input window Photo-cathode Micro-channel plate Anode plate <1cm

Photo-electric effect 14 Internship presentation - University of Chicago – 3 sept Photocathode Secondary electrons Advanced structures

Micro-channel plates 15 Internship presentation - University of Chicago – 3 sept microns glass MCP - Incom

Amplification principle Secondary emission Very small path-length High gain: 10 5 High space resolution: pore size Best to date: 2  m 16 Internship presentation - University of Chicago – 3 sept

Anode plate 17 Internship presentation - University of Chicago – 3 sept Delay line readout: position resolution <100  m AND time to pico-second range

18 Internship presentation - University of Chicago – 3 sept

Contents 19 Internship presentation - University of Chicago – 3 sept

Single threshold 20 Internship presentation - University of Chicago – 3 sept

Multiple threshold 21 Internship presentation - University of Chicago – 3 sept

Constant fraction discriminator 22 Internship presentation - University of Chicago – 3 sept

Waveform sampling and digital signal processing 23 Internship presentation - University of Chicago – 3 sept

Simulation Results 24 Internship presentation - University of Chicago – 3 sept

Contents 25 Internship presentation - University of Chicago – 3 sept

Anode plate 26 Internship presentation - University of Chicago – 3 sept

27 Internship presentation - University of Chicago – 3 sept

Contents 28 Internship presentation - University of Chicago – 3 sept

29 Internship presentation - University of Chicago – 3 sept Chip general sketch

30 Internship presentation - University of Chicago – 3 sept Timing generator

31 Internship presentation - University of Chicago – 3 sept Sampling cells

32 Internship presentation - University of Chicago – 3 sept ADC’s

33 Internship presentation - University of Chicago – 3 sept Token controlled readout register

34 Internship presentation - University of Chicago – 3 sept Spec:

Contents 35 Internship presentation - University of Chicago – 3 sept

Operating of the chip Writing Cell writing Trigger event Reading 36 Internship presentation - University of Chicago – 3 sept

Contents 37 Internship presentation - University of Chicago – 3 sept

38 Internship presentation - University of Chicago – 3 sept Storage cell principle V in wr C in V out rd V in wr C in V out rd V in wr C in V out rd Write stateIntermediate stateRead state

Storage cell issues Input bandwidth Leakages Charge injection 39 Internship presentation - University of Chicago – 3 sept

40 Internship presentation - University of Chicago – 3 sept Write state bandwidth V in wr C in V in C in R on

41 Internship presentation - University of Chicago – 3 sept Leakages in the cell V stored C in R off Switch leakages Capacitor leakages

42 Internship presentation - University of Chicago – 3 sept Charge injection V in wr C in V in +  Q/C in

43 Internship presentation - University of Chicago – 3 sept Input switch

44 Internship presentation - University of Chicago – 3 sept Input resistance With Matlab Comparison of Matlab and Spice

45 Internship presentation - University of Chicago – 3 sept Small signal model Cutting frequency:

46 Internship presentation - University of Chicago – 3 sept Simulations:

47 Internship presentation - University of Chicago – 3 sept Non-linear storage cell

Large signal analysis The output is not linear Subthreshold voltage are not stored 48 Internship presentation - University of Chicago – 3 sept

49 Internship presentation - University of Chicago – 3 sept Saturation V in (sat) value function of R L

50 Internship presentation - University of Chicago – 3 sept Output with and without saturation

51 Internship presentation - University of Chicago – 3 sept Linearity fit

52 Internship presentation - University of Chicago – 3 sept Small signal analysis

53 Internship presentation - University of Chicago – 3 sept Bandwidth

54 Internship presentation - University of Chicago – 3 sept Cell issues

55 Internship presentation - University of Chicago – 3 sept Read and write sequencing WriteIntermediate stateRead

56 Internship presentation - University of Chicago – 3 sept Read and write state

Cell issues Leakages: due to the switch Charge injection 57 Internship presentation - University of Chicago – 3 sept

58 Internship presentation - University of Chicago – 3 sept Linear storage cell

59 Internship presentation - University of Chicago – 3 sept Cell with real current source

60 Internship presentation - University of Chicago – 3 sept DC characteristic Input (blue) Output(black)

61 Internship presentation - University of Chicago – 3 sept Linear fit

62 Internship presentation - University of Chicago – 3 sept Small signal analysis

63 Internship presentation - University of Chicago – 3 sept Input and output bandwidth

64 Internship presentation - University of Chicago – 3 sept Transient signals

Contents 65 Internship presentation - University of Chicago – 3 sept

66 Internship presentation - University of Chicago – 3 sept Cell design

67 Internship presentation - University of Chicago – 3 sept Layout IBM 130nm CMRF-8-SF

68 Internship presentation - University of Chicago – 3 sept Storage cell assembly IBM 130nm CMRF-8-SF

69 Internship presentation - University of Chicago – 3 sept Channel layout IBM 130nm CMRF-8-SF

70 Internship presentation - University of Chicago – 3 sept Chip layout IBM 130nm CMRF-8-SF

71 Internship presentation - University of Chicago – 3 sept Conclusion