Gated mode operation with Hybrid 5

Size: px
Start display at page:

Download "Gated mode operation with Hybrid 5"

Transcription

1 Gated mode operation with Hybrid 5 J. Dingfelder, L. Germic, T. Hemperek, Jan Cedric Hönig, H. Krüger, F. Lütticke, C. Marinas, B. Paschen, N. Wermes

2 Gated Mode operation Continuous injection of particles (50 Hz) Newly injected particles tend to oscillate more. Injected bunches 100 ns apart! Revolution time 10 µs. Revolution time of 10 µs, while detector read out time is 20 µs Noise created by bunches flying through the detector Gated Mode: Mechanism to make the detector 'blind' to passing bunches! It has been proven that the DEPFET matrix can be operated in 'blind' (gated) mode! Bonn

3 How does gated mode work There are two types of gated mode: With and without read out. Here: Gated mode with read out! Bonn

4 DHP programing Possible to program sequence into DHE memory! DHE adaptercard allows to read out this sequence. Laser DHE adapter makes timing the laser possible DHE Adaptercard DHE Configures, controls and times Sends Data Bonn

5 Adapter for DHE Adapter card warrants the ability to display internal veto and trigger signals! A trigger signal can be sent to the pulse generator connected to the laser. Possibility to program a sequence to control precisely how long is triggered, when gated mode is active and when to shoot the laser. hoenig@physik.uni-bonn.de Bonn

6 DHE memory sequence At the start of the sequence the DHE receives the signal to expect data. At the same time DHP trigger is switched on. At some point gated mode is enabled by the veto signal. Laser is shot twice once during gated mode and once during normal readout. Bonn

7 DHE sequence DHE can be programed to follow a sequence, as soon as the gated mode is activated. In Frame 1 the laser is fired. In Frame 2 positions where the laser has been shot are checked for non cleared charge. In Frame 3 the laser is fired again during gated mode. In Frame 4 it is measured how much charge was injected, despite gated mode shielding. hoenig@physik.uni-bonn.de Bonn

8 Way measurements are evaluated (1) Frame 1 Frame 2 Frame 3 Frame 4 Row number and time move upwards! ADC row column hoenig@physik.uni-bonn.de Bonn

9 Way measurements are evaluated (2) Frame 1 Frame 2 Frame 3 Frame 4 Row number and time move upwards! ADC row column hoenig@physik.uni-bonn.de Bonn

10 Way measurements are evaluated (3) Frame 1 Frame 2 Frame 3 Frame 4 Row number and time move upwards! Cut through the matrix along the hit column! ADC row column hoenig@physik.uni-bonn.de Bonn

11 Way measurements are evaluated (4) Row number and time move to the right! ADC Code Frame 1 Frame 2 No gated mode + Laser is shot No gated mode + Laser is not shot Cut through the matrix along the hit column! Frame 3 Frame 4 Gated mode + Laser is shot No gated mode + Laser is not shot ADC Code row hoenig@physik.uni-bonn.de Bonn row

12 Laser delay measurement Shift laser pulse through veto sequence Start with laser pulses before the beginning of the gated mode sequence. Then delay the laser until it hits in the gated mode sequence. Bonn

13 Laser delay measurement preconditions Row number and time move to the right! Frame 1 Frame 2 No gated mode + Laser is shot Upper part not important for this measurement! No gated mode + Laser is not shot ADC Code Cut through the matrix along the hit column! ADC Code Frame 3 Frame 4 Gated mode + Laser is shot Shift laser through the gated mode sequence! No gated mode + Laser is not shot row hoenig@physik.uni-bonn.de Bonn row

14 What do we expect? 1.) One shoots shortly before the gated mode sequence. The injected charge is measured twice. Once during gated mode and then again after gated mode. 2.) One shoots during gated mode. The injected charge is hindered from reaching the internal gate. Thus no signal is measured. 3.) One shoots after the gated mode sequence. The signal appears in the next frame. The following measurements contain an offset of 3x8 = 24 GCK, obtained in separate measurements about laser delay! hoenig@physik.uni-bonn.de Bonn

15 What do we see? Plot only shows frame 4 for different laser delays! ADC ADC rows rows rows rows rows rows hoenig@physik.uni-bonn.de Bonn

16 Pixel inside gated area Before start of GM sequence Measured pixel is being read out ADC ADC rows rows rows rows rows rows End of gated mode sequence Bonn

17 Scan different area Shift measurement point from gated area to pixel outside the gated area. But shoot while pixels are gated! Bonn

18 Pixel outside of the gated region Plot shows signal after gated mode for different laser delays! ADC ADC rows rows rows rows rows rows Bonn

19 Clear high gate off measurement (perquisite) Complete set of standard voltages: Source: 7000 mv Scan of clear low and clear high: Potential wall height important! Gate off: Gate on: Clear gate: Clear on: Clear off: 3000 mv mv mv mv 6000 mv Gate Off: mv step size: 500 mv High voltage: Drift: mv mv Clear high: mv step size: 1000 mv Bonn

20 Gate off [mv] Signal [ADC Units] Clear high gate off (outside pixel) charge preservation Added common mode correction Clear high [mv] Bonn

21 What challenges are there with gated mode? Row number and time move upwards! Frame 1 Frame 2 Frame 3 Frame 4 Increased pedestals No common mode correction active! ADC row column hoenig@physik.uni-bonn.de Bonn

22 Clear high clear low measurement (perquisite) Complete set of standard voltages: Scan of clear low and clear high: Clear low: mv step size: 250 mv Clear high: mv step size: 250 mv Source: Gate off: Gate on: Clear gate: Clear on: Clear off: High voltage: Drift: 7000 mv 3000 mv mv mv mv 6000 mv mv mv Bonn

23 Clear high clear low measurement Following plots are for a pixel inside of the GM region! hoenig@physik.uni-bonn.de Bonn

24 Clear high clear low measurement no gated mode Clear high [mv] Bonn

25 Clear high clear low measurement gated mode Non working area Clear high [mv] Bonn

26 Why do low clear low voltages not work? High pedestals Clear high: mv Clear low: 2000 mv Pixel columns Bonn

27 Clear low measurement high clear low do not work ADC code Frame 1 No gated mode + Laser is shot Clear high: mv Clear low: 8000 mv Frame 2 No gated mode + Laser is not shot ADC code Frame 3 Gated mode + Laser is shot Frame 4 No gated mode + Laser is not shot Row # Row # hoenig@physik.uni-bonn.de Bonn

28 Clear high clear low measurement gated mode Non working area Clear high [mv] Bonn

29 Clear high measurement (working point) ADC code Frame 1 No gated mode + Laser is shot Clear high: mv Clear low: 6000 mv Frame 2 No gated mode + Laser is not shot ADC code Frame 3 Gated mode + Laser is shot Frame 4 No gated mode + Laser is not shot Row # Row # hoenig@physik.uni-bonn.de Bonn

30 Clear high measurement (overview) Clear high: mv Clear high: mv Signal is not properly cleared after injection. Gated mode does not work correctly. Clear high: mv Signal is properly cleared after injection! But going out of gated mode creates large pedestal oscillations! Clear low: 6000 mv Bonn

31 Clear high measurement (extreme case) gated mode ADC code Frame 1 No gated mode + Laser is shot Clear high: mv Clear low: 6000 mv Frame 2 No gated mode + Laser is not shot Signal is properly cleared after injection! But going out of gated mode creates large pedestal oscillations! ADC code Frame 3 Gated mode + Laser is shot Frame 4 No gated mode + Laser is not shot Row # Row # hoenig@physik.uni-bonn.de Bonn

32 Clear high clear low scan different area Shift measurement point from gated area to pixel outside the gated area. But shoot while pixels are gated! Bonn

33 Clear low [mv] Signal [ADC Units] Clear high clear low (outside pixel) shielding Added common mode correction Non working area Clear high [mv] Bonn

34 Clear high clear low charge preservation How much of the injected charge remains inside the internal gate during gated mode? Bonn

35 Clear low [mv] Signal [ADC Units] Clear high clear low (outside pixel) charge preservation Added common mode correction Input signal How much of the injected charge remains inside the internal gate during gated mode? Clear high [mv] Non working area Bonn

36 What challenges are there with gated mode? Row number and time move upwards! Frame 1 Frame 2 Frame 3 Frame 4 Increased pedestals No common mode correction active! ADC row column hoenig@physik.uni-bonn.de Bonn

37 What challenges are there with gated mode? Row number and time move upwards! Frame 1 Frame 2 Frame 3 Frame 4 Increased pedestals No common mode correction active! ADC row With adapted voltages column hoenig@physik.uni-bonn.de Bonn

38 DHE sequence DHE can be programed to follow a sequence, as soon as the gated mode is activated. In Frame 1 the laser is fired. In Frame 2 positions where the laser has been shot are checked for non cleared charge. In Frame 3 the laser is fired again during gated mode. In Frame 4 it is measured how much charge was injected, despite gated mode shielding. hoenig@physik.uni-bonn.de Bonn

39 Y coordinate [moco] Position dependent scans How strongly does gated mode s performance depend on the location where charge is injected? Pixel outside of gated region! ADC code X coordinate [moco] hoenig@physik.uni-bonn.de Bonn

40 Y coordinate [moco] Cluster signal (shielding) laser shot for 4 GCK Reference: How much charge was injected, on average? Pixel outside of gated region! Measurement: How much charge was measured despite shielding? ADC code X coordinate [moco] hoenig@physik.uni-bonn.de Bonn

41 Y coordinate [moco] Cluster signal (shielding) laser shot for 2 GCK Reference: How much charge was injected, on average? Pixel inside of gated region! Measurement: How much charge was measured despite shielding? ADC code X coordinate [moco] hoenig@physik.uni-bonn.de Bonn

42 Y coordinate [moco] Cluster signal (preservation) laser shot for 4 GCK Reference: How much charge was injected, on average? Pixel outside of gated region! Measurement: How much charge was preserved during gated mode? ADC code X coordinate [moco] hoenig@physik.uni-bonn.de Bonn

43 Y coordinate [moco] Cluster signal (preservation) laser shot for 2 GCK Reference: How much charge was injected, on average? Pixel inside of gated region! Measurement: How much charge was preserved during gated mode? ADC code X coordinate [moco] hoenig@physik.uni-bonn.de Bonn

44 Outlook and conclusion Measurements: How DEPFET behaves while going in and out of gated mode: Pedestal increase due to quick switching of clear signal when going out of gated mode How gate off voltage influences shielding efficiency. Minimal gate off voltage required How clear low and clear high influence gated mode performance: Gated mode sets an upper limit for clear high Position dependent performance measurements: Differences between pixels, but location where charge is injected inside a pixel not important Still needed are position dependent optimization of clear low, clear high and gate off voltage! hoenig@physik.uni-bonn.de Bonn

45 Conclusions Gated mode with readout proven to work (charge removal/charge preservation) Set of suggested optimized voltages: ClearHigh = V ClearLow = 6 V GateOff = 3 V Timing: Going in and out of gated mode ~200 ns (+ gated time itself) on H5 system and small matrix. Still further optimization is needed. Some issues to understand: Extrapolation to large matrices (~800 ns?) Further understanding up/down matrix effects while going into gated mode operation hoenig@physik.uni-bonn.de Bonn

46 Thank you Bonn

47 Backup

48 Y coordinate [moco] Cluster signal (shielding) laser shot for 4 GCK GM efficiency Pixel outside of gated region! Measurement: How much charge was measured despite shielding? ADC code X coordinate [moco] hoenig@physik.uni-bonn.de Bonn

49 Y coordinate [moco] Cluster signal (shielding) laser shot for 2 GCK GM efficiency Pixel inside of gated region! Measurement: How much charge was measured despite shielding? ADC code X coordinate [moco] hoenig@physik.uni-bonn.de Bonn

50 Y coordinate [moco] Cluster signal (preservation) laser shot for 2 GCK Reference: How much charge was injected, on average? Pixel inside of gated region! Measurement: How much charge was preserved during gated mode? ADC code X coordinate [moco] hoenig@physik.uni-bonn.de Bonn

51 Clear low [mv] Signal [ADC Units] Clear high clear low (outside pixel) gated mode Added common mode correction Non working area Clear high [mv] Bonn

52 DHP programing Trigger Trigger pulse given at position 5 DHE Configures, controls and times Sends Data hoenig@physik.uni-bonn.de Bonn

53 Seed signal laser shot for 1 gate Frame 1 No gated mode + Laser is shot ADC code X coordinate [moco] hoenig@physik.uni-bonn.de Bonn

54 Seed signal after gated mode laser shot for 1 gate Frame 4 No gated mode + Laser is not shot ADC code X coordinate [moco] hoenig@physik.uni-bonn.de Bonn

55 Seed signal after gated mode laser shot for 2 gate Frame 4 No gated mode + Laser is not shot Same picture if laser signal is doubled! ADC code X coordinate [moco] hoenig@physik.uni-bonn.de Bonn

56 What to optimize Multiple paths which need to be checked for correct functionality. So far worked on optimizing DCD performance. DHE Configures, controls and times Sends Data Bonn

57 DCD optimization DCD is part of the electronics directly connected to the matrix. It is responsible for digitizing the signal current generated in the matrix. Half speed Low gain Optimize DCD for: - range of curve - linearity - missing codes/bit errors - noise hoenig@physik.uni-bonn.de Bonn

58 DCD measurement Optimization done with 2D scans over multiple channels. Quality of each curve is determined with the earlier mentioned criteria for all measured channels (256 DCD channels). Bonn

59 DCD measurement and evaluation Quality of each configuration is determined by counting number of tests not passed. Best working point lowest value Bonn

60 What is the DCD DCD Plenty of voltages to change. Important ones are: RefIn, AmpLow, VPSource, VPSource2, VFBPBias Bonn

DEPFET Active Pixel Sensors for the ILC

DEPFET Active Pixel Sensors for the ILC DEPFET Active Pixel Sensors for the ILC Laci Andricek for the DEPFET Collaboration (www.depfet.org) The DEPFET ILC VTX Project steering chips Switcher thinning technology Simulation sensor development

More information

CAEN Tools for Discovery

CAEN Tools for Discovery Viareggio March 28, 2011 Introduction: what is the SiPM? The Silicon PhotoMultiplier (SiPM) consists of a high density (up to ~10 3 /mm 2 ) matrix of diodes connected in parallel on a common Si substrate.

More information

Beam test of the QMB6 calibration board and HBU0 prototype

Beam test of the QMB6 calibration board and HBU0 prototype Beam test of the QMB6 calibration board and HBU0 prototype J. Cvach 1, J. Kvasnička 1,2, I. Polák 1, J. Zálešák 1 May 23, 2011 Abstract We report about the performance of the HBU0 board and the optical

More information

PHOTOTUBE SCANNING SETUP AT THE UNIVERSITY OF MARYLAND. Doug Roberts U of Maryland, College Park

PHOTOTUBE SCANNING SETUP AT THE UNIVERSITY OF MARYLAND. Doug Roberts U of Maryland, College Park PHOTOTUBE SCANNING SETUP AT THE UNIVERSITY OF MARYLAND Doug Roberts U of Maryland, College Park Overview We have developed a system for measuring and scanning phototubes for the FDIRC Based primarily on

More information

Laser Beam Analyser Laser Diagnos c System. If you can measure it, you can control it!

Laser Beam Analyser Laser Diagnos c System. If you can measure it, you can control it! Laser Beam Analyser Laser Diagnos c System If you can measure it, you can control it! Introduc on to Laser Beam Analysis In industrial -, medical - and laboratory applications using CO 2 and YAG lasers,

More information

Atlas Pixel Replacement/Upgrade. Measurements on 3D sensors

Atlas Pixel Replacement/Upgrade. Measurements on 3D sensors Atlas Pixel Replacement/Upgrade and Measurements on 3D sensors Forskerskole 2007 by E. Bolle erlend.bolle@fys.uio.no Outline Sensors for Atlas pixel b-layer replacement/upgrade UiO activities CERN 3D test

More information

Digital Delay / Pulse Generator DG535 Digital delay and pulse generator (4-channel)

Digital Delay / Pulse Generator DG535 Digital delay and pulse generator (4-channel) Digital Delay / Pulse Generator Digital delay and pulse generator (4-channel) Digital Delay/Pulse Generator Four independent delay channels Two fully defined pulse channels 5 ps delay resolution 50 ps

More information

The TDCPix ASIC: Tracking for the NA62 GigaTracker. G. Aglieri Rinella, S. Bonacini, J. Kaplon, A. Kluge, M. Morel, L. Perktold, K.

The TDCPix ASIC: Tracking for the NA62 GigaTracker. G. Aglieri Rinella, S. Bonacini, J. Kaplon, A. Kluge, M. Morel, L. Perktold, K. : Tracking for the NA62 GigaTracker CERN E-mail: matthew.noy@cern.ch G. Aglieri Rinella, S. Bonacini, J. Kaplon, A. Kluge, M. Morel, L. Perktold, K. Poltorak CERN The TDCPix is a hybrid pixel detector

More information

Scintillation Tile Hodoscope for the PANDA Barrel Time-Of-Flight Detector

Scintillation Tile Hodoscope for the PANDA Barrel Time-Of-Flight Detector Scintillation Tile Hodoscope for the PANDA Barrel Time-Of-Flight Detector William Nalti, Ken Suzuki, Stefan-Meyer-Institut, ÖAW on behalf of the PANDA/Barrel-TOF(SciTil) group 12.06.2018, ICASiPM2018 1

More information

Performance of a double-metal n-on-n and a Czochralski silicon strip detector read out at LHC speeds

Performance of a double-metal n-on-n and a Czochralski silicon strip detector read out at LHC speeds Performance of a double-metal n-on-n and a Czochralski silicon strip detector read out at LHC speeds Juan Palacios, On behalf of the LHCb VELO group J.P. Palacios, Liverpool Outline LHCb and VELO performance

More information

KLM: TARGETX. User-Interface for Testing TARGETX Brief Testing Overview Bronson Edralin 04/06/15

KLM: TARGETX. User-Interface for Testing TARGETX Brief Testing Overview Bronson Edralin 04/06/15 KLM: TARGETX User-Interface for Testing TARGETX Brief Testing Overview Bronson Edralin 1 TARGETX Test Team TARGETX Waveform Sampling/Digitizing ASIC Designer Dr. Gary S. Varner Features 1 GSa/s 16 Channels

More information

Front End Electronics

Front End Electronics CLAS12 Ring Imaging Cherenkov (RICH) Detector Mid-term Review Front End Electronics INFN - Ferrara Matteo Turisini 2015 October 13 th Overview Readout requirements Hardware design Electronics boards Integration

More information

Threshold Tuning of the ATLAS Pixel Detector

Threshold Tuning of the ATLAS Pixel Detector Haverford College Haverford Scholarship Faculty Publications Physics Threshold Tuning of the ATLAS Pixel Detector P. Behara G. Gaycken C. Horn A. Khanov D. Lopez Mateos See next page for additional authors

More information

4 MHz Lock-In Amplifier

4 MHz Lock-In Amplifier 4 MHz Lock-In Amplifier SR865A 4 MHz dual phase lock-in amplifier SR865A 4 MHz Lock-In Amplifier 1 mhz to 4 MHz frequency range Low-noise current and voltage inputs Touchscreen data display - large numeric

More information

Features of the 745T-20C: Applications of the 745T-20C: Model 745T-20C 20 Channel Digital Delay Generator

Features of the 745T-20C: Applications of the 745T-20C: Model 745T-20C 20 Channel Digital Delay Generator 20 Channel Digital Delay Generator Features of the 745T-20C: 20 Independent delay channels - 100 ps resolution - 25 ps rms jitter - 10 second range Output pulse up to 6 V/50 Ω Independent trigger for every

More information

Prototype of a Gigabit Data Transmitter in 65-nm CMOS for DEPFET Pixel Detectors at Belle-II

Prototype of a Gigabit Data Transmitter in 65-nm CMOS for DEPFET Pixel Detectors at Belle-II Prototype of a Gigabit Data Transmitter in 65-nm CMOS for DEPFET Pixel Detectors at Belle-II Tetsuichi Kishishita H. Krüger, T. Hemperek, M. Lemarenko, M. Koch, M. Gronewald, N. Wermes University of Bonn

More information

A fast and precise COME & KISS* QDC and TDC for diamond detectors and further applications

A fast and precise COME & KISS* QDC and TDC for diamond detectors and further applications A fast and precise COME & KISS* QDC and TDC for diamond detectors and further applications 3 rd ADAMAS Collaboration Meeting (2014) Trento, Italy *use commercial elements and keep it small & simple + +

More information

GFT Channel Digital Delay Generator

GFT Channel Digital Delay Generator Features 20 independent delay Channels 100 ps resolution 25 ps rms jitter 10 second range Output pulse up to 6 V/50 Ω Independent trigger for every channel Fours Triggers Three are repetitive from three

More information

CBF500 High resolution Streak camera

CBF500 High resolution Streak camera High resolution Streak camera Features 400 900 nm spectral sensitivity 5 ps impulse response 10 ps trigger jitter Trigger external or command 5 to 50 ns analysis duration 1024 x 1024, 12-bit readout camera

More information

The FLASH objective: SASE between 60 and 13 nm

The FLASH objective: SASE between 60 and 13 nm Injector beam control studies winter 2006/07 talk from E. Vogel on work performed by W. Cichalewski, C. Gerth, W. Jalmuzna,W. Koprek, F. Löhl, D. Noelle, P. Pucyk, H. Schlarb, T. Traber, E. Vogel, FLASH

More information

RF2TTC and QPLL behavior during interruption or switch of the RF-BC source

RF2TTC and QPLL behavior during interruption or switch of the RF-BC source RF2TTC and QPLL behavior during interruption or switch of the RF-BC source Study to adapt the BC source choice in RF2TTC during interruption of the RF timing signals Contents I. INTRODUCTION 2 II. QPLL

More information

HP 71910A and 71910P Wide Bandwidth Receiver Technical Specifications

HP 71910A and 71910P Wide Bandwidth Receiver Technical Specifications HP 71910A and 71910P Wide Bandwidth Receiver Technical Specifications 100 Hz to 26.5 GHz The HP 71910A/P is a receiver for monitoring signals from 100 Hz to 26.5 GHz. It provides a cost effective combination

More information

Commissioning and Initial Performance of the Belle II itop PID Subdetector

Commissioning and Initial Performance of the Belle II itop PID Subdetector Commissioning and Initial Performance of the Belle II itop PID Subdetector Gary Varner University of Hawaii TIPP 2017 Beijing Upgrading PID Performance - PID (π/κ) detectors - Inside current calorimeter

More information

HAPD and Electronics Updates

HAPD and Electronics Updates S. Nishida KEK 3rd Open Meeting for Belle II Collaboration 1 Contents Frontend Electronics Neutron Irradiation News from Hamamtsu 2 144ch HAPD HAPD (Hybrid Avalanche Photo Detector) photon bi alkali photocathode

More information

ISOMET. Compensation look-up-table (LUT) and How to Generate. Isomet: Contents:

ISOMET. Compensation look-up-table (LUT) and How to Generate. Isomet: Contents: Compensation look-up-table (LUT) and How to Generate Contents: Description Background theory Basic LUT pg 2 Creating a LUT pg 3 Using the LUT pg 7 Comment pg 9 The compensation look-up-table (LUT) contains

More information

Commissioning and Performance of the ATLAS Transition Radiation Tracker with High Energy Collisions at LHC

Commissioning and Performance of the ATLAS Transition Radiation Tracker with High Energy Collisions at LHC Commissioning and Performance of the ATLAS Transition Radiation Tracker with High Energy Collisions at LHC 1 A L E J A N D R O A L O N S O L U N D U N I V E R S I T Y O N B E H A L F O F T H E A T L A

More information

A pixel chip for tracking in ALICE and particle identification in LHCb

A pixel chip for tracking in ALICE and particle identification in LHCb A pixel chip for tracking in ALICE and particle identification in LHCb K.Wyllie 1), M.Burns 1), M.Campbell 1), E.Cantatore 1), V.Cencelli 2) R.Dinapoli 3), F.Formenti 1), T.Grassi 1), E.Heijne 1), P.Jarron

More information

Front End Electronics

Front End Electronics CLAS12 Ring Imaging Cherenkov (RICH) Detector Mid-term Review Front End Electronics INFN - Ferrara Matteo Turisini 2015 October 13 th Overview Readout requirements Hardware design Electronics boards Integration

More information

GFT Channel Slave Generator

GFT Channel Slave Generator GFT1018 8 Channel Slave Generator Features 8 independent delay channels 1 ps time resolution < 100 ps rms jitter for optical triggered delays 1 second range Electrical or optical output Three trigger modes

More information

Test beam data analysis for the CMS CASTOR calorimeter at the LHC

Test beam data analysis for the CMS CASTOR calorimeter at the LHC 1/ 24 DESY Summerstudent programme 2008 - Course review Test beam data analysis for the CMS CASTOR calorimeter at the LHC Agni Bethani a, Andrea Knue b a Technical University of Athens b Georg-August University

More information

ILC Detector Work. Dan Peterson

ILC Detector Work. Dan Peterson ILC Detector Work Dan Peterson ** Cornell/Purdue TPC development program Large Detector Concept TPC Detector Response Simulation and Track Reconstruction World Wide Study Detector R&D Panel This project

More information

Update on DAQ for 12 GeV Hall C

Update on DAQ for 12 GeV Hall C Update on DAQ for 12 GeV Hall C Brad Sawatzky Hall C Winter User Group Meeting Jan 20, 2017 SHMS/HMS Trigger/Electronics H. Fenker 2 SHMS / HMS Triggers SCIN = 3/4 hodoscope planes CER = Cerenkov(s) STOF

More information

Hello and welcome to this presentation of the STM32L4 Analog-to-Digital Converter block. It will cover the main features of this block, which is used

Hello and welcome to this presentation of the STM32L4 Analog-to-Digital Converter block. It will cover the main features of this block, which is used Hello and welcome to this presentation of the STM32L4 Analog-to-Digital Converter block. It will cover the main features of this block, which is used to convert the external analog voltage-like sensor

More information

Development of BPM Electronics at the JLAB FEL

Development of BPM Electronics at the JLAB FEL Development of BPM Electronics at the JLAB FEL D. Sexton, P. Evtushenko, K. Jordan, J. Yan, S. Dutton, W. Moore, R. Evans, J. Coleman Thomas Jefferson National Accelerator Facility, Free Electron Laser

More information

An extreme high resolution Timing Counter for the MEG Upgrade

An extreme high resolution Timing Counter for the MEG Upgrade An extreme high resolution Timing Counter for the MEG Upgrade M. De Gerone INFN Genova on behalf of the MEG collaboration 13th Topical Seminar on Innovative Particle and Radiation Detectors Siena, Oct.

More information

Study of the performances of the ALICE muon spectrometer

Study of the performances of the ALICE muon spectrometer Study of the performances of the ALICE muon spectrometer Blanc Aurélien, December 2008 PhD description Study of the performances of the ALICE muon spectrometer instrumentation/detection. Master Physique

More information

Readout techniques for drift and low frequency noise rejection in infrared arrays

Readout techniques for drift and low frequency noise rejection in infrared arrays Readout techniques for drift and low frequency noise rejection in infrared arrays European Southern Observatory Finger, G., Dorn, R.J, Hoffman, A.W., Mehrgan, H., Meyer, M., Moorwood, A.F.M., Stegmeier,

More information

Photo Multipliers Tubes characterization for WA105 experiment. Chiara Lastoria TAE Benasque 07/09/2016

Photo Multipliers Tubes characterization for WA105 experiment. Chiara Lastoria TAE Benasque 07/09/2016 Photo Multipliers Tubes characterization for WA105 experiment Chiara Lastoria TAE Benasque 07/09/2016 Outline WA105 experiment Dual Phase technology and TPC photon detection Photo Multipliers Tubes working

More information

Sources of Error in Time Interval Measurements

Sources of Error in Time Interval Measurements Sources of Error in Time Interval Measurements Application Note Some timer/counters available today offer resolution of below one nanosecond in their time interval measurements. Of course, high resolution

More information

EDDY CURRENT IMAGE PROCESSING FOR CRACK SIZE CHARACTERIZATION

EDDY CURRENT IMAGE PROCESSING FOR CRACK SIZE CHARACTERIZATION EDDY CURRENT MAGE PROCESSNG FOR CRACK SZE CHARACTERZATON R.O. McCary General Electric Co., Corporate Research and Development P. 0. Box 8 Schenectady, N. Y. 12309 NTRODUCTON Estimation of crack length

More information

DAQ Systems in Hall A

DAQ Systems in Hall A CODA Users Workshop Data Acquisition at Jefferson Lab Newport News June 7, 2004 DAQ Systems in Hall A Overview of Hall A Standard Equipment: HRS, Beamline,... Parity Experiments Third Arms: BigBite, RCS

More information

DXP-xMAP General List-Mode Specification

DXP-xMAP General List-Mode Specification DXP-xMAP General List-Mode Specification The xmap processor can support a wide range of timing or mapping operations, including mapping with full MCA spectra, multiple SCA regions, and finally a variety

More information

Status of readout electronic design in MOST1

Status of readout electronic design in MOST1 Status of readout electronic design in MOST1 Na WANG, Ke WANG, Zhenan LIU, Jia TAO On behalf of the Trigger Group (IHEP) Mini-workshop for CEPC MOST silicon project,23 November,2017,Beijing Outline Introduction

More information

Characterizing Transverse Beam Dynamics at the APS Storage Ring Using a Dual-Sweep Streak Camera

Characterizing Transverse Beam Dynamics at the APS Storage Ring Using a Dual-Sweep Streak Camera Characterizing Transverse Beam Dynamics at the APS Storage Ring Using a Dual-Sweep Streak Camera Bingxin Yang, Alex H. Lumpkin, Katherine Harkay, Louis Emery, Michael Borland, and Frank Lenkszus Advanced

More information

Development of an Abort Gap Monitor for High-Energy Proton Rings *

Development of an Abort Gap Monitor for High-Energy Proton Rings * Development of an Abort Gap Monitor for High-Energy Proton Rings * J.-F. Beche, J. Byrd, S. De Santis, P. Denes, M. Placidi, W. Turner, M. Zolotorev Lawrence Berkeley National Laboratory, Berkeley, USA

More information

The Cornell/Purdue TPC

The Cornell/Purdue TPC The Cornell/Purdue TPC Cornell University Purdue University D. P. Peterson G. Bolla L. Fields I. P. J. Shipsey R. S. Galik P. Onyisi Information available at the web site: http://w4.lns.cornell.edu/~dpp/tpc_test_lab_info.html

More information

FPGA Based Data Read-Out System of the Belle 2 Pixel Detector

FPGA Based Data Read-Out System of the Belle 2 Pixel Detector FPGA Based Read-Out System of the Belle 2 Pixel Detector Dmytro Levit, Igor Konorov, Daniel Greenwald, Stephan Paul Technische Universität München arxiv:1406.3864v1 [physics.ins-det] 15 Jun 2014 Abstract

More information

Quartzlock Model A7-MX Close-in Phase Noise Measurement & Ultra Low Noise Allan Variance, Phase/Frequency Comparison

Quartzlock Model A7-MX Close-in Phase Noise Measurement & Ultra Low Noise Allan Variance, Phase/Frequency Comparison Quartzlock Model A7-MX Close-in Phase Noise Measurement & Ultra Low Noise Allan Variance, Phase/Frequency Comparison Measurement of RF & Microwave Sources Cosmo Little and Clive Green Quartzlock (UK) Ltd,

More information

CSC Data Rates, Formats and Calibration Methods

CSC Data Rates, Formats and Calibration Methods CSC Data Rates, Formats and Calibration Methods D. Acosta University of Florida With most information collected from the The Ohio State University PRS March Milestones 1. Determination of calibration methods

More information

THE ATLAS Inner Detector [2] is designed for precision

THE ATLAS Inner Detector [2] is designed for precision The ATLAS Pixel Detector Fabian Hügging on behalf of the ATLAS Pixel Collaboration [1] arxiv:physics/412138v1 [physics.ins-det] 21 Dec 4 Abstract The ATLAS Pixel Detector is the innermost layer of the

More information

Testing and Characterization of the MPA Pixel Readout ASIC for the Upgrade of the CMS Outer Tracker at the High Luminosity LHC

Testing and Characterization of the MPA Pixel Readout ASIC for the Upgrade of the CMS Outer Tracker at the High Luminosity LHC Testing and Characterization of the MPA Pixel Readout ASIC for the Upgrade of the CMS Outer Tracker at the High Luminosity LHC Dena Giovinazzo University of California, Santa Cruz Supervisors: Davide Ceresa

More information

First LHC Beams in ATLAS. Peter Krieger University of Toronto On behalf of the ATLAS Collaboration

First LHC Beams in ATLAS. Peter Krieger University of Toronto On behalf of the ATLAS Collaboration First LHC Beams in ATLAS Peter Krieger University of Toronto On behalf of the ATLAS Collaboration Cutaway View LHC/ATLAS (Graphic) P. Krieger, University of Toronto Aspen Winter Conference, Feb. 2009 2

More information

11.1 As mentioned in Experiment 10, sequential logic circuits are a type of logic circuit where the output

11.1 As mentioned in Experiment 10, sequential logic circuits are a type of logic circuit where the output EE 2449 Experiment JL and NWP //8 CALIFORNIA STATE UNIVERSITY LOS ANGELES Department of Electrical and Computer Engineering EE-2449 Digital Logic Lab EXPERIMENT SEQUENTIAL CIRCUITS Text: Mano and Ciletti,

More information

Drift Tubes as Muon Detectors for ILC

Drift Tubes as Muon Detectors for ILC Drift Tubes as Muon Detectors for ILC Dmitri Denisov Fermilab Major specifications for muon detectors D0 muon system tracking detectors Advantages and disadvantages of drift chambers as muon detectors

More information

The hybrid photon detectors for the LHCb-RICH counters

The hybrid photon detectors for the LHCb-RICH counters 7 th International Conference on Advanced Technology and Particle Physics The hybrid photon detectors for the LHCb-RICH counters Maria Girone, CERN and Imperial College on behalf of the LHCb-RICH group

More information

V9A01 Solution Specification V0.1

V9A01 Solution Specification V0.1 V9A01 Solution Specification V0.1 CONTENTS V9A01 Solution Specification Section 1 Document Descriptions... 4 1.1 Version Descriptions... 4 1.2 Nomenclature of this Document... 4 Section 2 Solution Overview...

More information

EASY-MCS. Multichannel Scaler. Profiling Counting Rates up to 150 MHz with 15 ppm Time Resolution.

EASY-MCS. Multichannel Scaler. Profiling Counting Rates up to 150 MHz with 15 ppm Time Resolution. Multichannel Scaler Profiling Counting Rates up to 150 MHz with 15 ppm Time Resolution. The ideal solution for: Time-resolved single-photon counting Phosphorescence lifetime spectrometry Atmospheric and

More information

Parity Quality Beam (PQB) Study

Parity Quality Beam (PQB) Study Parity Quality Beam (PQB) Study Injector Group November 10, 2008 Thanks to: Roger Flood, Pete Francis, Paul King, Bob Michaels, Julie Roche Notes: 1. For each BPM, the wires are: +X+, +X-, +Y+, +Y-. 2.

More information

Beam Test Results and ORCA validation for CMS EMU CSC front-end electronics N. Terentiev

Beam Test Results and ORCA validation for CMS EMU CSC front-end electronics N. Terentiev Beam Test Results and ORCA validation for CMS EMU CSC front-end electronics US N. Terentiev Carnegie Mellon University CMS EMU Meeting, CERN June 18, 2005 Outline Motivation. CSC cathode strip pulse shape

More information

Minimize your cost for Phased Array & TOFD

Minimize your cost for Phased Array & TOFD Minimize your cost for Phased Array & TOFD Latest ultrasonic flaw detector from SIUI, incorporates the latest advancements in Encoder In/Out UT/ TOFD Probe high-performance Phased Array and TOFD detection

More information

Precision testing methods of Event Timer A032-ET

Precision testing methods of Event Timer A032-ET Precision testing methods of Event Timer A032-ET Event Timer A032-ET provides extreme precision. Therefore exact determination of its characteristics in commonly accepted way is impossible or, at least,

More information

High ResolutionCross Strip Anodes for Photon Counting detectors

High ResolutionCross Strip Anodes for Photon Counting detectors High ResolutionCross Strip Anodes for Photon Counting detectors Oswald H.W. Siegmund, Anton S. Tremsin, Robert Abiad, J. Hull and John V. Vallerga Space Sciences Laboratory University of California Berkeley,

More information

A FOUR GAIN READOUT INTEGRATED CIRCUIT : FRIC 96_1

A FOUR GAIN READOUT INTEGRATED CIRCUIT : FRIC 96_1 A FOUR GAIN READOUT INTEGRATED CIRCUIT : FRIC 96_1 J. M. Bussat 1, G. Bohner 1, O. Rossetto 2, D. Dzahini 2, J. Lecoq 1, J. Pouxe 2, J. Colas 1, (1) L. A. P. P. Annecy-le-vieux, France (2) I. S. N. Grenoble,

More information

Citation X-Ray Spectrometry (2011), 40(6): 4. Nakaye, Y. and Kawai, J. (2011), ED

Citation X-Ray Spectrometry (2011), 40(6): 4.   Nakaye, Y. and Kawai, J. (2011), ED TitleEDXRF with an audio digitizer Author(s) Nakaye, Yasukazu; Kawai, Jun Citation X-Ray Spectrometry (2011), 40(6): 4 Issue Date 2011-10-10 URL http://hdl.handle.net/2433/197744 This is the peer reviewed

More information

Achieving More Efficient Data Review with OpenLAB CDS

Achieving More Efficient Data Review with OpenLAB CDS Achieving More Efficient Data Review with OpenLAB CDS Technical Note Introduction Separations have enjoyed major advances that have significantly reduced chromatographic run times. Ultra high performance

More information

Paul Rubinov Fermilab Front End Electronics. May 2006 Perugia, Italy

Paul Rubinov Fermilab Front End Electronics. May 2006 Perugia, Italy Minerva Electronics and the Trip-T Paul Rubinov Fermilab Front End Electronics May 2006 Perugia, Italy 1 Outline Minerva Electronics and the TriP-t Minerva TriP-t The concept for Minerva Overview and status

More information

In-process inspection: Inspector technology and concept

In-process inspection: Inspector technology and concept Inspector In-process inspection: Inspector technology and concept Need to inspect a part during production or the final result? The Inspector system provides a quick and efficient method to interface a

More information

GREAT 32 channel peak sensing ADC module: User Manual

GREAT 32 channel peak sensing ADC module: User Manual GREAT 32 channel peak sensing ADC module: User Manual Specification: 32 independent timestamped peak sensing, ADC channels. Input range 0 to +8V. Sliding scale correction. Peaking time greater than 1uS.

More information

IMAGING GROUP. * With dual port readout at 16MHz/port Detector shown with a C-mount nose and lens, sold separately

IMAGING GROUP. * With dual port readout at 16MHz/port Detector shown with a C-mount nose and lens, sold separately The from Princeton Instruments is the ultimate scientific, intensified CCD camera (ICCD) system, featuring a 1k x 1k interline CCD fiberoptically coupled to Gen III filmless intensifiers. These intensifiers

More information

Lecture 14: Computer Peripherals

Lecture 14: Computer Peripherals Lecture 14: Computer Peripherals The last homework and lab for the course will involve using programmable logic to make interesting things happen on a computer monitor should be even more fun than the

More information

SuperFRS GEM-TPC Development Status Report

SuperFRS GEM-TPC Development Status Report SuperFRS GEM-TPC Development Status Report COLLABORATORS F. García, R. Turpeinen, J. Heino, A. Karadzhinova, E. Tuominen, R. Lauhakangas Helsinki Institute of Physics University of Helsinki - Finland R.

More information

The Alice Silicon Pixel Detector (SPD) Peter Chochula for the Alice Pixel Collaboration

The Alice Silicon Pixel Detector (SPD) Peter Chochula for the Alice Pixel Collaboration The Alice Silicon Pixel Detector (SPD) Peter Chochula for the Alice Pixel Collaboration The Alice Pixel Detector R 1 =3.9 cm R 2 =7.6 cm Main Physics Goal Heavy Flavour Physics D 0 K π+ 15 days Pb-Pb data

More information

HARDROC, Readout chip of the Digital Hadronic Calorimeter of ILC

HARDROC, Readout chip of the Digital Hadronic Calorimeter of ILC HARDROC, Readout chip of the Digital Hadronic Calorimeter of ILC S. Callier a, F. Dulucq a, C. de La Taille a, G. Martin-Chassard a, N. Seguin-Moreau a a OMEGA/LAL/IN2P3, LAL Université Paris-Sud, Orsay,France

More information

CESR BPM System Calibration

CESR BPM System Calibration CESR BPM System Calibration Joseph Burrell Mechanical Engineering, WSU, Detroit, MI, 48202 (Dated: August 11, 2006) The Cornell Electron Storage Ring(CESR) uses beam position monitors (BPM) to determine

More information

arxiv: v3 [astro-ph.im] 2 Nov 2011

arxiv: v3 [astro-ph.im] 2 Nov 2011 Preprint typeset in JINST style - HYPER VERSION Data acquisition electronics and reconstruction software for real time 3D track reconstruction within the MIMAC project arxiv:1110.4348v3 [astro-ph.im] 2

More information

New Results on the Electron Cloud at the Los Alamos PSR

New Results on the Electron Cloud at the Los Alamos PSR New Results on the Electron Cloud at the Los Alamos PSR Robert Macek, LANL, 4/15/02 Co-authors: A. Browman, D. Fitzgerald, R. McCrady, T. Spickermann, & T. S. Wang - LANL For more information see the website

More information

The FEL detector development program at DESY. Heinz Graafsma DESY-Photon Science Detector Group WorkPackage Detectors for XFEL

The FEL detector development program at DESY. Heinz Graafsma DESY-Photon Science Detector Group WorkPackage Detectors for XFEL The FEL detector development program at DESY DESY-Photon Science Detector Group WorkPackage Detectors for XFEL EUROFEL-2009 Hard X-ray SASE Free Electron Lasers LINAC COHERENT LIGHT SOURCE LCLS 2009 2010

More information

Imaging TOP (itop), Cosmic Ray Test Stand & PID Readout Update

Imaging TOP (itop), Cosmic Ray Test Stand & PID Readout Update Imaging TOP (itop), Cosmic Ray Test Stand & PID Readout Update Tom Browder, Herbert Hoedlmoser, Bryce Jacobsen, Jim Kennedy, KurtisNishimura, Marc Rosen, Larry Ruckman, Gary Varner Kurtis Nishimura SuperKEKB

More information

Prospect and Plan for IRS3B Readout

Prospect and Plan for IRS3B Readout Prospect and Plan for IRS3B Readout 1. Progress on Key Performance Parameters 2. Understanding limitations during LEPS operation 3. Carrier02 Rev. C (with O-E-M improvements) 4. Pre-production tasks/schedule

More information

... A COMPUTER SYSTEM FOR MULTIPARAMETER PULSE HEIGHT ANALYSIS AND CONTROL*

... A COMPUTER SYSTEM FOR MULTIPARAMETER PULSE HEIGHT ANALYSIS AND CONTROL* I... A COMPUTER SYSTEM FOR MULTIPARAMETER PULSE HEIGHT ANALYSIS AND CONTROL* R. G. Friday and K. D. Mauro Stanford Linear Accelerator Center Stanford University, Stanford, California 94305 SLAC-PUB-995

More information

ISOMET. Compensation look-up-table (LUT) and Scan Uniformity

ISOMET. Compensation look-up-table (LUT) and Scan Uniformity Compensation look-up-table (LUT) and Scan Uniformity The compensation look-up-table (LUT) contains both phase and amplitude data. This is automatically applied to the Image data to maximize diffraction

More information

Online Monitoring of L1CT in Run IIa. bonus: experience from Run I

Online Monitoring of L1CT in Run IIa. bonus: experience from Run I Online Monitoring of L1CT in Run IIa bonus: experience from Run I Philippe Laurens 20-Feb-2003 L1 Cal Monitoring Monitoring can mean many things Anything related to observation of system s operation Different

More information

Physics Requirements for the CXI Ion Time-of-Flight

Physics Requirements for the CXI Ion Time-of-Flight PHYSICS REQUIREMENT DOCUMENT (PRD) Doc. No. SP-391-000-30 R0 LUSI SUB-SYSTEM CXI Physics Requirements for the CXI Ion Time-of-Flight Sébastien Boutet CXI Scientist, Author Paul Montanez CXI Lead Engineer

More information

PACS. Dark Current of Ge:Ga detectors from FM-ILT. J. Schreiber 1, U. Klaas 1, H. Dannerbauer 1, M. Nielbock 1, J. Bouwman 1.

PACS. Dark Current of Ge:Ga detectors from FM-ILT. J. Schreiber 1, U. Klaas 1, H. Dannerbauer 1, M. Nielbock 1, J. Bouwman 1. PACS Test Analysis Report FM-ILT Page 1 Dark Current of Ge:Ga detectors from FM-ILT J. Schreiber 1, U. Klaas 1, H. Dannerbauer 1, M. Nielbock 1, J. Bouwman 1 1 Max-Planck-Institut für Astronomie, Königstuhl

More information

ILC requirements Review on CMOS Performances: state of the art Progress on fast read-out sensors & ADC Roadmap for the coming years Summary

ILC requirements Review on CMOS Performances: state of the art Progress on fast read-out sensors & ADC Roadmap for the coming years Summary Status on CMOS sensors Auguste Besson on behalf of DAPNIA/Saclay, LPSC/Grenoble, LPC/Clermont-F., DESY, Uni. Hamburg, JINR-Dubna & IPHC/Strasbourg contributions from IPN/Lyon, Uni. Frankfurt, GSI-Darmstadt,

More information

Riccardo Farinelli. Charge Centroid Feasibility

Riccardo Farinelli. Charge Centroid Feasibility Riccardo Farinelli Charge Centroid Feasibility Outline Prototype and TB setup Data set studied Analysis approch Results Charge Centroid Feasibility Ferrara July 07, 2015 R.Farinelli 2 Test chambers Conversion

More information

The Large TPC Prototype: Infrastructure/ Status/ Plans

The Large TPC Prototype: Infrastructure/ Status/ Plans The Large TPC Prototype: Infrastructure/ Status/ Plans Takeshi Matsuda, KEK/ DESY Ties Behnke, DESY For the LC-TPC collaboration Status of the test beam infrastructure Status of the Large Prototype Field

More information

Update on DAQ for 12 GeV Hall C. Brad Sawatzky

Update on DAQ for 12 GeV Hall C. Brad Sawatzky Update on DAQ for 12 GeV Hall C Brad Sawatzky SHMS/HMS Trigger/Electronics H. Fenker 2 SHMS / HMS Triggers SCIN = 3/4 hodoscope planes CER = Cerenkov(s) STOF = S1 + S2 EL-Hi = SCIN + PSh_Hi EL-Lo = 2/3{SCIN,

More information

2016 PDV Conference. Time Alignment of Multiple Real-Time High Bandwidth Scope. Channels

2016 PDV Conference. Time Alignment of Multiple Real-Time High Bandwidth Scope. Channels Time Alignment of Multiple Real-Time High Bandwidth Scope Channels 1 Time Synchronization Between Scope Channels for Data Acquisition Large Acquisition Systems Often Require Synchronization of Multiple

More information

First evaluation of the prototype 19-modules camera for the Large Size Telescope of the CTA

First evaluation of the prototype 19-modules camera for the Large Size Telescope of the CTA First evaluation of the prototype 19-modules camera for the Large Size Telescope of the CTA Tsutomu Nagayoshi for the CTA-Japan Consortium Saitama Univ, Max-Planck-Institute for Physics 1 Cherenkov Telescope

More information

Realization and Test of the Engineering Prototype of the CALICE Tile Hadron Calorimeter

Realization and Test of the Engineering Prototype of the CALICE Tile Hadron Calorimeter Realization and Test of the Engineering Prototype of the CALICE Tile Hadron Calorimeter Mark Terwort on behalf of the CALICE collaboration arxiv:1011.4760v1 [physics.ins-det] 22 Nov 2010 Abstract The CALICE

More information

BABAR IFR TDC Board (ITB): requirements and system description

BABAR IFR TDC Board (ITB): requirements and system description BABAR IFR TDC Board (ITB): requirements and system description Version 1.1 November 1997 G. Crosetti, S. Minutoli, E. Robutti I.N.F.N. Genova 1. Timing measurement with the IFR Accurate track reconstruction

More information

R&D on high performance RPC for the ATLAS Phase-II upgrade

R&D on high performance RPC for the ATLAS Phase-II upgrade R&D on high performance RPC for the ATLAS Phase-II upgrade Yongjie Sun State Key Laboratory of Particle detection and electronics Department of Modern Physics, USTC outline ATLAS Phase-II Muon Spectrometer

More information

Basic rules for the design of RF Controls in High Intensity Proton Linacs. Particularities of proton linacs wrt electron linacs

Basic rules for the design of RF Controls in High Intensity Proton Linacs. Particularities of proton linacs wrt electron linacs Basic rules Basic rules for the design of RF Controls in High Intensity Proton Linacs Particularities of proton linacs wrt electron linacs Non-zero synchronous phase needs reactive beam-loading compensation

More information

TIME RESOLVED XAS DATA COLLECTION WITH AN XIA DXP-4T SPECTROMETER

TIME RESOLVED XAS DATA COLLECTION WITH AN XIA DXP-4T SPECTROMETER TIME RESOLVED XAS DATA COLLECTION WITH AN XIA DXP-4T SPECTROMETER W.K. WARBURTON, B. HUBBARD & C. ZHOU X-ray strumentation Associates 2513 Charleston Road, STE 207, Mountain View, CA 94043 USA C. BOOTH

More information

North Damping Ring RF

North Damping Ring RF North Damping Ring RF North Damping Ring RF Outline Overview High Power RF HVPS Klystron & Klystron EPICS controls Cavities & Cavity Feedback SCP diagnostics & displays FACET-specific LLRF LLRF distribution

More information

Uncooled amorphous silicon ¼ VGA IRFPA with 25 µm pixel-pitch for High End applications

Uncooled amorphous silicon ¼ VGA IRFPA with 25 µm pixel-pitch for High End applications Uncooled amorphous silicon ¼ VGA IRFPA with 25 µm pixel-pitch for High End applications A. Crastes, J.L. Tissot, M. Vilain, O. Legras, S. Tinnes, C. Minassian, P. Robert, B. Fieque ULIS - BP27-38113 Veurey

More information

BER MEASUREMENT IN THE NOISY CHANNEL

BER MEASUREMENT IN THE NOISY CHANNEL BER MEASUREMENT IN THE NOISY CHANNEL PREPARATION... 2 overview... 2 the basic system... 3 a more detailed description... 4 theoretical predictions... 5 EXPERIMENT... 6 the ERROR COUNTING UTILITIES module...

More information

Application Note AN-708 Vibration Measurements with the Vibration Synchronization Module

Application Note AN-708 Vibration Measurements with the Vibration Synchronization Module Application Note AN-708 Vibration Measurements with the Vibration Synchronization Module Introduction The vibration module allows complete analysis of cyclical events using low-speed cameras. This is accomplished

More information

ISC0904: 1k x 1k 18µm N-on-P ROIC. Specification January 13, 2012

ISC0904: 1k x 1k 18µm N-on-P ROIC. Specification January 13, 2012 ISC0904 1k x 1k 18µm N-on-P ROIC Specification January 13, 2012 This presentation contains content that is proprietary to FLIR Systems. Information is subject to change without notice. 1 Version 1.00 January

More information