PMT Calibration Bryan Musolf. Goals Transform raw data into graphs for 30 PMTs Observe how the gain and # of photoelectrons (PE) change as a LED intensity.

Slides:



Advertisements
Similar presentations
Ask a Question What are we testing? Step 1. Step 2 Research your topic. Look at the past work of others to see if this problem has already been tested.
Advertisements

New test result of MPPC M.Taguchi(kyoto).
The Pierre-Auger PMT Test Stand Chris Jillings Feb 6, 2002.
PMT Calibration / Greenhouses Bryan Musolf. PMT Calibration.
Performance of MPPC using laser system Photon sensor KEK Niigata university, ILC calorimeter group Sayaka IBA, Hiroaki ONO, Paul.
Study of Photon Sensors using the Laser System 05/7/12 Niigata University, Japan Sayaka Iba, Editha P. Jacosalem, Hiroaki Ono, Noriko.
Reflectivity Measurements of Critical Materials for the LUX Dark Matter Experiment Theory My experiment was a cyclic process involving software, engineering,
Op-Amps (2). Non-Inverting Amplifier Design Problem Design a non-inverting op-amp with a gain of 6. What is the approximate power supply if Vin must.
1 Cosmic Ray Test Stand with Scintillating Cells for Digital Hadron Calorimeter 06/23/2003 Kurt Francis - Northern Illinois University.
Mechanical check of PMT Check base: Remove black tape and two small screws that secure the base. Tighten the nuts on the BNC connector for the HT input.
Negative vs. positive feedback What is the difference? Consider what happens when there is a perturbation Positive feedback drives op amp into saturation:
H Yepes, C Bigongiari, J Zuñiga, JdD Zornoza IFIC (CSIC - Universidad de Valencia) NEWS ON ABSORPTION LENGTH MEASUREMENT WITH THE OB SYSTEM ANTARES COLLABORATION.
Preliminary Results of the Test Run at SLAC Petra Hüntemeyer.
Veto Wall Test Hyupwoo Lee MINERvA/Jupiter Group Meeting Apr, 16, 2008.
STATUS OF THE ABSORPTION LENGTH MEASUREMENT ANTARES collaboration meeting Clermont-Ferrand (France), May 17th-20th 1 H Yepes, JdD Zornoza, J Zuñiga, C.
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.
Report on SiPM Tests SiPM as a alternative photo detector to replace PMT. Qauntify basic characteristics Measure Energy, Timing resolution Develop simulation.
Results from the PMT test bench in BCN (10-Oct-03) J.Garra, R.Graciani, E.Graugés, X.Xirgu.
1 System Description (2-4) Gains from single photo-electrons in vacuum at room temperature (5-8) Linearity Test at V in vacuum at room temperature.
Tests with JT0623 & JT0947 at Indiana University Nagoya PMT database test results for JT0623 at 3220V: This tube has somewhat higher than usual gain. 5×10.
S. Hansen, S. Pordes & E. SkupR11065 study 10/1-6/ st Look at FNAL at R11065 at room temperature. Plots of pulses on oscilloscope at different voltages.
Cube Measurements Tent Crew. Scintillation BNL 241 Am Semi- collimated  Spectralon Diffuse UV Reflector SBD  -Trigger Scint. Light Poisson.
14/02/2007 Paolo Walter Cattaneo 1 1.Trigger analysis 2.Muon rate 3.Q distribution 4.Baseline 5.Pulse shape 6.Z measurement 7.Att measurement OUTLINE.
Development of Multi-pixel photon counters(2) M.Taguchi, T.Nakaya, M.Yokoyama, S.Gomi(kyoto) T.Nakadaira, K.Yoshimura(KEK) for KEKDTP photon sensor group.
Oct C. Smith - PCAL/EC Commissioning 1 PCAL/EC Commissioning Document
X-Ray Reflection Data Analysis Update Information can be extracted from XRR data: - Film thickness - Roughness.
FLC Group Test-beam Studies of the Laser-Wire Detector 13 September 2006 Maximilian Micheler Supervisor: Freddy Poirier.
1 N eutrino E xtended S ubmarine T elescope with O ceanographic R esearch Operation and performance of the NESTOR test detector.
10/26/20151 Observational Astrophysics I Astronomical detectors Kitchin pp
SLAC, HiRes T-461: “FLASH” part 1 Justin Findlay.
Scintillation Cube Tests HBD Meeting 3/18/08 A.Caccavano & B.Azmoun, C.Woody.
MPPC update including plastic connector T2K experiment collaboration meeting 2007/4/18 (Wed) S.Gomi T.Nakaya M.Yokoyama ( Kyoto University ) T.Nakadaira.
R&D of MPPC for T2K experiment PD07 : Photosensor Workshop /6/28 (Thu) S.Gomi T.Nakaya M.Yokoyama H.Kawamuko ( Kyoto University ) T.Nakadaira.
Development of Multi-pixel photon counters(2) M.Taguchi, T.Nakaya, M.Yokoyama, S.Gomi(kyoto) T.Nakadaira, K.Yoshimura(KEK)
1 Development of Multi-Pixel Photon Counters (1) S.Gomi, T.Nakaya, M.Yokoyama, M.Taguchi, (Kyoto University) T.Nakadaira, K.Yoshimura, (KEK) Oct
1 MPPC update S.Gomi, T.Nakaya, M.Yokoyama, M.Taguchi, (Kyoto University) T.Nakadaira (KEK) Nov KEK.
Abort Gap Monitoring Randy Thurman-Keup 6 / 8 / 2004 LARP Meeting.
MPPC status M.Taguchi(kyoto) T2K ND /7/7.
ROBOX with Multi Anode PMT’s Status and plans A.Mestvirishvili, I. Schmidt, S. Sen, F. Ozok University of Iowa.
Performance of SiPM Ryuhei Nakamura (Kobe Univ.) GLC calorimeter group (KEK, Kobe, Konan, Niigata, Shinshu, Tsukuba) Contents ・ Introduction ・ Test results.
Status of photon sensor study at Niigata University -- SiPM and MPPC -- Photon sensor mini workshop 05/9/16 University Niigata University.
Calorimeter calibration -Initial calibration -Gain following -Archiving.
1 SiPM studies: Highlighting current equipment and immediate plans Lee BLM Quasar working group.
Production PMT Testing and Work on Site with Prototype Tank University of California, Los Angles Department of Physics and Astronomy
TCPD test measurement 1 TCPD (TGEM CCC Photon Detector) test measurement ELTE, MTA KFKI RMKI, REGARD Group (Budapest, Hungary): Levente Kovács G. Hamar,
HAPPEX DAQ / ADC Tests Luis Mercado UMASS 4/17/09.
(s)T3B Update – Calibration and Temperature Corrections AHCAL meeting– December 13 th 2011 – Hamburg Christian Soldner Max-Planck-Institute for Physics.
Experimental Methods for Determining Photodetector Working Points By: Victor Rykalin Mike Smith Jim Maloney.
PMT test device setup functionality –reproducibility of output signal –dynamic range –limitations –test duration conclusion T. Wälchli, TT-Meeting Brussels,
ZDC Status A.Mestvirishvili Iowa. Quite while we had some problems with ZDC, QIE saturations, Reflections, Noise etc. To improve the situation several.
A. Tsirigotis Hellenic Open University N eutrino E xtended S ubmarine T elescope with O ceanographic R esearch Reconstruction, Background Rejection Tools.
Development of UV-sensitive MPPC for upgrade of liquid xenon detector in MEG experiment Daisuke Kaneko, on behalf of the MEG Collaboration µ γ Liquid xenon.
TRIPLEGEM and VFATs at The Test Beam Area TRIPLEGEM and VFATs at The Test Beam Area N. Turini……reporter Eraldo Oliveri! Eraldo Oliveri main worker! N.
The photomultiplier tubes selection for KM2A electromagnetic particle detectors (EDs) hou chao IHEP The 2nd workshop of air shower detection at high altitudes.
Development of Multi-pixel photon counters(2) M.Taguchi, T.Nakaya, M.Yokoyama, S.Gomi(kyoto) T.Nakadaira, K.Yoshimura(KEK) for KEKDTP photon sensor group.
Positronium intensity measurement preparation SNU Bongho Kim.
M.Taguchi and T.Nobuhara(Kyoto) HPK MPPC(Multi Pixel Photon Counter) status T2K280m meeting.
Outgassing studies DC Spark Corrected calibration Mo and Cu data with same calibration data and same experimental environment Field emission measurements.
OD Tuning: SK-IV Roger Wendell TMC 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.
Why we need an improved LASER calibration system
Transistor Characteristics
Instrumentation for Colliding Beam Physics 2017
Time calibration Dmitry Chirkin, LBNL UC Berkeley, November 2004.
R&D of MPPC for T2K experiment
Single photoelectron method introduce
Neutron Beam Test for Measuring Quenching Factor of CsI(Tl) Crystal
Drift Chamber Monitoring
Image cross-correlation analysis reveals the emergence of a dynamic steady state actin distribution in the minimal cortex. Image cross-correlation analysis.
Presentation transcript:

PMT Calibration Bryan Musolf

Goals Transform raw data into graphs for 30 PMTs Observe how the gain and # of photoelectrons (PE) change as a LED intensity changes Observe how the gain and # of PE change as high voltage changes Find the stable region of each PMT by analyzing the noise Extrapolate PMT data Ensure the linearity of each PMT Further test the PMTs

LED intensity Increasing the LED intensity while keeping the high voltage constant As the PMTs become saturated the PE cannot be measured accurately As the PE cannot be measured the gain is no longer constant

High Voltage Increasing the high voltage while keeping the LED intensity constant Comparing the experimental gain vs. the specification gain from the company Approximately1 PE should be hitting the PMT for these tests. This plot ensured that.

Noise counts / min and Extrapolation We then added the noise counts / min to find the stable region of each PMT We also extrapolated the data to find the high voltage that would give us a gain of 5E7 Our gain of 5E7 is right in the stable region of the PMT

All 30 PMT Spec gain vs. high voltage and gain vs. high voltage for all 30 PMT Our measured gain closely reflects the spec gain given to us by the company Gain plot starts to break down when PMTs start to become saturated

All 30 PMT Noise vs. high voltage and the extrapolation for all 30 PMT We have some very nice PMTs!! The extrapolation data will allow us to set high voltages to get specific gains

All 30 PMT Gain / Spec gain / Noise layered

Further testing We found that some of the PMT bases were broken and needed to be repaired In particular, R1 seemed to be the problem on most

Further Testing After fixing the bases we needed to make sure the PMT bases could withstand the LAr we would be using them in

Further Testing We also needed to make some splitters so we could connect the PMTs to a high voltage source and an oscilloscope to take measurements Needless to say, I got a little bit more efficient!

Further Testing We ran one test in liquid nitrogen Everything held up and we got a nice signal Testing in liquid nitrogen or LAr will be ready soon