Beam Line Data Analysis of the PMT and Quartz Coupling Zak Arcara.

Slides:



Advertisements
Similar presentations
Bob MichaelsParity Collab. Mtg. May 17, `07 Integrating Compton DAQ and Analysis Bob Michaels with Reminder about Nov 2006 Results Specification of new.
Advertisements

Dante Nakazawa with Prof. Juan Collar
Beam-based Measurements of HOMs in the HTC Adam Bartnik for ERL Team, Daniel Hall, John Dobbins, Mike Billing, Matthias Liepe, Ivan Bazarov.
Constructing an Analog Digital Converter (ADC) to Measure Neutron Depolarization in Deuterium Aung Kyaw Sint and Dr. Alexander Komives CsI scintillator.
PIXE: Data Analysis What the data can (and cannot) tell us. Larry Lamm PIXE Seminar Winter 2008.
MDC-II LVL-1 Trigger Khaled Teilab for the MDC Trigger Team.
M. Palm, CERN1 Performance test of ACEM-detector (Aluminum Cathode Electron Multiplier) Marcus Palm AB-ATB-EA.
GLAST LAT ProjectIA Workshop 6 – Feb28,2006 Preliminary Studies on the dependence of Arrival Time distributions in the LAT using CAL Low Energy Trigger.
Tagger Electronics Part 1: tagger focal plane microscope Part 2: tagger fixed array Part 3: trigger and digitization Richard Jones, University of Connecticut.
Chapter 7. Light as a wave  carries energy but doesn’t actually move  Think of a cork on water and surfer. The above diagram is a typical way to visualize.
Y. Karadzhov MICE Video Conference Thu April 9 Slide 1 Absolute Time Calibration Method General description of the TOF DAQ setup For the TOF Data Acquisition.
FPIX0 Electronic Test Marina Artuso Paul Gelling Jianchun Wang  The system works fine with charge injection calibration  Gain curve, threshold, and noise.
Veto Wall Test Hyupwoo Lee MINERvA/Jupiter Group Meeting Apr, 16, 2008.
Forward Detectors and Measurement of Proton-Antiproton Collision Rates by Zachary Einzig, Mentor Michele Gallinaro INTRODUCTION THE DETECTORS EXPERIMENTAL.
CHAPTER 9 Oscilloscopes and Graphing Multimeters
LIGO-G Z Coherent Coincident Analysis of LIGO Burst Candidates Laura Cadonati Massachusetts Institute of Technology LIGO Scientific Collaboration.
Page 1 January 2002 doc.: IEEE 802.RR-02/018A-d5 IEEE 802 IEEE 802 proposal relating to DFS and JPT5G proposal.
The next slide shows a simplified diagram of the pulser. A capacitor is charged up to perhaps 10V. Switches T1 and T2 close. Some of the capacitor current.
The Transverse detector is made of an array of 256 scintillating fibers coupled to Avalanche PhotoDiodes (APD). The small size of the fibers (5X5mm) results.
Synthesis advanced techniques. Other modules Synthesis would be fairly dull if we were limited to mixing together and filtering a few standard waveforms.
Vladimir Frolov for Torino group. Experimental activities: The system for testing the MRPC in the Torino INFN laboratory has been fully mounted and checked;
PHY 202 (Blum)1 Analog-to-Digital Converter and Multi-vibrators.
QuarkNet Muon Data Analysis with Shower Array Studies J.L. FISCHER, A. CITATI, M. HOHLMANN Physics and Space Sciences Department, Florida Institute of.
Jornadas LIP 2008 – Pedro Ramalhete. 17 m hadron absorber vertex region 8 MWPCs 4 trigger hodoscopes toroidal magnet dipole magnet hadron absorber targets.
Updates on GEMs characterization with APV electronics K. Gnanvo, N. Liyanage, K. Saenboonruang.
Short Time Fourier Transform-based method for fast transients detection Centre for eResearch, University of Auckland, New Zealand,
Uncertainty in light measurement instrumentation examples1 For light sensors, uncertainty is closely related to light intensity … but not only… Let’s have.
“End station A setup” data analysis Josef Uher. Outline Introduction to setup and analysis Quartz bar start counter MA and MCP PMT in the prototype.
Two-stage amplifier status test buffer – to be replaced with IRSX i signal recent / final (hopefully) design uses load resistor and voltage gain stage.
1 Report on analysis of PoGO Beam Test at Spring-8 Tsunefumi Mizuno July 15, 2003 July 21, 2003 revised August 1, 2003 updated.
1 Development of Multi-Pixel Photon Counters (1) S.Gomi, T.Nakaya, M.Yokoyama, M.Taguchi, (Kyoto University) T.Nakadaira, K.Yoshimura, (KEK) Oct
Neutron detection in LHe ( HMI run 2004) R.Golub, E. Korobkina, J. Zou M. Hayden, G. Archibold J. Boissevain, W.S.Wilburn C. Gould.
Cosmic Ray Workshop May 15, Cosmic Ray Detector Kit.
1 SiPM studies: Highlighting current equipment and immediate plans Lee BLM Quasar working group.
Multipixel Geiger mode photo-sensors (MRS APD’s) Yury Kudenko ISS meeting, KEK, 25 January 2006 INR, Moscow.
THE ENERGY OF LIGHT. HOW LIGHT IS ‘MADE’ Today we are going to take a look at how light is made and how we can determine the energy of light In order.
1 Electronics Status Trigger and DAQ run successfully in RUN2006 for the first time Trigger communication to DRS boards via trigger bus Trigger firmware.
F Don Lincoln, Fermilab f Fermilab/Boeing Test Results for HiSTE-VI Don Lincoln Fermi National Accelerator Laboratory.
The requirements of Ideal pulse-type counter :  1 Every particle entering the detector should produce a pulse at the exit of the counter,
Calorimeter global commissioning: progress and plans Patrick Robbe, LAL Orsay & CERN, 25 jun 2008.
A. Tsirigotis Hellenic Open University N eutrino E xtended S ubmarine T elescope with O ceanographic R esearch Reconstruction, Background Rejection Tools.
DAQ and Trigger for HPS run Sergey Boyarinov JLAB July 11, Requirements and available test results 2. DAQ status 3. Trigger system status and upgrades.
Performance of 1600-pixel MPPC for the GLD Calorimeter Readout Jan. 30(Tue.) Korea-Japan Joint Shinshu Univ. Takashi Maeda ( Univ. of Tsukuba)
LIGO-G Z The Q Pipeline search for gravitational-wave bursts with LIGO Shourov K. Chatterji for the LIGO Scientific Collaboration APS Meeting.
Development of Multi-Pixel Photon Counters (1)
Acd Veto Latching The Acd front end electronics generate a veto primitive when a discriminator goes above threshold. But. The signal is split: One path.
Robert Squibb1, Stephanie Deschanel2,
Status of Electronics Simulation and Energy Resoluton Estimation
Counting Mode DAQ for Compton
Ultrasound Physics Image Formation ‘97.
Manual End to End Measuring Modes of ELQ 30A+
OBJECTIVES Explain the principles involved in regenerative braking.
Fitting.
January 2002 doc.: IEEE 802.RR-02/018A-d2
CLAS12 software workshop
SANE Cherenkov - Bigcal Efficiency Update
SuperB LNF meeting March 21st 2012 Marcello Piccolo
Department of Physics and Astronomy,
Alon Attal Martin von der Mey Jay Hauser Mike Lindgren
R’(45) represents the slope of the curve at t = 45.
R&D of MPPC for T2K experiment
High Rate Photon Irradiation Test with an 8-Plane TRT Sector Prototype
Pulsar Data II Single-Pulse Plots
Multi-vibrators
Performance test of ACEM-detector (Aluminum Cathode Electron Multiplier) Marcus Palm AB-ATB-EA M. Palm, CERN.
B. Genolini for the IPNO detector dept.
Pulsar Data II Single-Pulse Plots
Beam Beam electronics Block diagram disc gated disc gate disc gated
Template application to detect KC-like activity.
Automotive Technology Principles, Diagnosis, and Service
Presentation transcript:

Beam Line Data Analysis of the PMT and Quartz Coupling Zak Arcara

Trigger Source – “The Notch” The initial trigger by this device, the notch, initializes the data capturing for the PMT 2 Notch Triggered The initial trigger by this device, “the notch”, initializes the data capturing for the PMT

PMT HV: 1200V Example of a typical two pulse curve detected by the PMT 3 Notch Triggered Example of a typical 2 pulse curve

Threshold 4 The Threshold is set at -0.4V to disregard background – eyeballed the best threshold The Threshold explains why there is a 2 pulse system In order for another pulse to be detected, the return needs to drop below the threshold value Offline Threshold in the Software that can be changed quickly Notch Triggered

PMT HV: 1200V Peak Number, Threshold of -0.4V 5 Two pulses dominate the frequency of peaks (85.8%) There are zero triggers 7% of the time Acceptance * efficiency = 93% Everything right of red line, or 0 triggers, is counted into (acceptance * efficiency) value

PMT HV: 1300V Peak Number, Threshold of -0.4V 6 4.5% of the time, there are zero triggers that are recorded Acceptance * efficiency = 95.5%

PMT HV: 1400V Peak Number, Threshold of -0.4V 7 Zero triggers occur 12.4% of the time when the Notch triggers Acceptance * Efficiency = 77.6 %

PMT HV: 1500V Peak Number, Threshold of -0.4V 8 There are never any zero triggers for this voltage Acceptance * Efficiency = 100%

Acceptance * Efficiency 9 VoltageAcceptance * Efficiency 1200V93% 1300V95.5% 1400V77.6% 1500V100% Acceptance * Efficiency is anytime there is any data capture; at least one pulse detected

PMT HV: 1200V, -0.4V Threshold 10 Interesting Double Peak Structure The two different groups of double peaks are not fully understood yet The time between peaks is the proton beam structure

PMT HV: 1200V Time Between Peaks 11 This histogram is an exact representation of the 37MHz beam structure The 37 MHz structure gives a 24 ns time between blasts

PMT HV: 1300V, -0.4V Threshold 12 Same double peak structure formed Both double peak structures occurred around the same time as 1200V The second peak decreased in frequency Threshold is the explanation

PMT HV: 1300V Time Between Peaks 13 This histogram is an exact representation of the 37MHz beam structure The 37 MHz structure gives a 24 ns time between blasts

PMT HV: 1400V, -0.4V Threshold 14 The Double Peak structure is vanishing Explained by Threshold value Time between peaks matches with the 37MHz structure

PMT HV: 1400V Time Between Peaks 15 There are under 10 data points that recorded a 3 pulse graph The time difference shows the majority around 24 ns where expected The other points are the difference between the 3 point curves

PMT HV: 1500V, -0.4V Threshold 16 Double Peak structure is even less evident Threshold value altered the amount of the second peak recording frequency

PMT HV: 1500V Time Between Peaks 17 The chart has the majority of the data points around 24 ns There is a cluster around 70 ns, which maybe explained by 3 pulse curve Increased the threshold and it gives graphs almost identical to the 1200V

Booster Structure 18 The proton beam structure looks like the figures above It has a distinct 1600 nsec time period between each proton burst That time in between should be no pulsing above a certain background amount The PMT and Quartz crystal coupling need to be able to detect the short time between each burst Selection Window, defined at center plane of the tracker

Afterpulsing 19 Notch Trigger Afterpulsing is an issue because it allows possibility of “fake” data Afterpulsing was tested with a Peak Counter algorithm – same as used for regular, non-delayed data points The 1 ms time window allows the determination to see if there is after pulsing occurring far down the time line PMT Triggered After Pulse 1.6 us in between pulses

1 ms Delay Data To understand the background, a 1 ms delay was integrated The threshold had to decrease in order to see any activity from the beam line From -0.4V to -0.15V Did the change of voltage by eye, new system is being implemented for later data This gives data above the majority of the background noise 20

1200V, 1 ms Delay, -0.15V Threshold 21 This is 1 ms after the Notch triggered This could be the single proton triggers

1300V, 1 ms Delay, -0.15V Threshold 22 Interesting to see multiple pulses after the delay window No double peak structures were seen at 1200V

1400V, 1 ms Delay, -0.15V Threshold 23 Has almost identical structure to 1300V, but there are more entries for this High Voltage

1500V, 1 ms Delay, -0.15V Threshold 24 A couple triple peaks detected for first time

Signal Graph at -1300V

Summary The PMT can detect the 37MHz structure consistently PMT double peak structure varies in time Afterpulsing doesn’t seem to be a real issue after 1 ms At -0.4V, lower the threshold and frequency increases There are visible electron quantum levels that can be used to set appropriate thresholds PMT looks effective at speeds that are needed for Mu2e 26