A Brand new neutrino detector 「 SciBar 」 (2) Y. Takubo (Osaka) - Readout Electronics - Introduction Readout electronics Cosmic ray trigger modules Conclusion.

Slides:



Advertisements
Similar presentations
Cosmic Ray Test of INO RPC Stack M. Bhuyan 1, V.M. Datar 2, S.D. Kalmani 1, S.M. Lahamge 1, N.K. Mondal 1, P. Nagaraj 1, S. Pal 1, L.V. Reddy, A. Redij.
Advertisements

The Angra Neutrino Detector Detector, VETO and electronics conceptual design Laudo Barbosa (May 18th, 2006) Centro Brasileiro de Pesquisas Físicas (CBPF)
1 Cosmic Ray Test Stand with Scintillating Cells for Digital Hadron Calorimeter 06/23/2003 Kurt Francis - Northern Illinois University.
KEK beam test H. Sakamoto. Purpose To optimize a concentration of the second dopant for scintillating fibers KEK beam test to study light yields for various.
How to Build a Neutrino Oscillations Detector - Why MINOS is like it is! Alfons Weber March 2005.
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.
Prototype Performance in D0 test stand & fiber intrinsic performance with KEK test beam M.Yoshida (Osaka Univ.) Osaka.
The Design of MINER  A Howard Budd University of Rochester August, 2004.
The Belle SVD Trigger  Tom Ziegler  Vertex 2002  Kailua-Kona, Hawaii, 4-8 th nov The Belle SVD Trigger Tom Ziegler on behalf of the Belle SVD.
P. Karchin – PMTs for Scintillator Based Muon Systempage 11/7/2004 January 7, 2004 American Linear Collider Physics Group 2004 Workshop Stanford Linear.
NuMI MINOS The MINOS Far Detector Cosmic Rays and their neutrinos are being collected now. How does this work, and of what use is this data? Alec Habig,
ECAL electronics Guido Haefeli, Lausanne PEBS meeting 10.Jan
RENO Electronics - QBEE - 장 지 승 ( 전남대학교 ) RENO Collaboration Meeting,
A crude (lower limit) estimation of resolution and event rate Development and Construction of an Extensive Air Shower Array in HOU Antonis Leisos, Hellenic.
6mm 【 Development of Readout Electronics for MPPC 】 We report the read out electronics of MPPC( Multi-Pixel Photon Counter ). MPPC is a new photodetector.
Development of Readout ASIC for FPCCD Vertex Detector 01 October 2009 Kennosuke.Itagaki Tohoku University.
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.
GLD Calorimeter Status Oct 学術創成会議 S. Uozumi Shinshu University FJPPL meeting held at the end of September. Preparation underway toward the ECAL.
1 S. E. Tzamarias Hellenic Open University N eutrino E xtended S ubmarine T elescope with O ceanographic R esearch Readout Electronics DAQ & Calibration.
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.
PMF: front end board for the ATLAS Luminometer ALFA TWEPP 2008 – 19 th September 2008 Parallel Session B6 – Programmable logic, boards, crates and systems.
Measurement of 'intrinsic' properties of scintillating fibers H. Sakamoto Osaka University, Japan A.Sato M. Yoshida Y. Kuno Osaka Univ. K. Yoshimura KEK.
Beam test of scintillator strips Miho NISHIYAMA Shinshu University ・ scintillator strip calorimeter ・ Kuraray scintillator strips and KNU extruded ・ the.
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.
VC Feb 2010Slide 1 EMR Construction Status o General Design o Electronics o Cosmics test Jean-Sebastien Graulich, Geneva.
Development of Tracking Detector with GEM Kunihiro Fujita RCNP, Osaka Univ. Yasuhiro Sakemi CYRIC, Tohoku Univ. Masaharu Nomachi Dep. of Phys., Osaka Univ.
Thomas Jefferson National Accelerator Facility Page 1 EC / PCAL ENERGY CALIBRATION Cole Smith UVA PCAL EC Outline Why 2 calorimeters? Requirements Using.
Status of the NO ν A Near Detector Prototype Timothy Kutnink Iowa State University For the NOvA Collaboration.
K2K 実験 SciBar 前置ニュートリノ検出器 久野研 田窪 洋介 読み出しシステムと時間情報の較正.
The ALICE Forward Multiplicity Detector Kristján Gulbrandsen Niels Bohr Institute for the ALICE Collaboration.
Development of Multi-pixel photon counters(2) M.Taguchi, T.Nakaya, M.Yokoyama, S.Gomi(kyoto) T.Nakadaira, K.Yoshimura(KEK)
TOP counter overview and issues K. Inami (Nagoya university) 2008/7/3-4 2 nd open meeting for proto-collaboration - Overview - Design - Performance - Prototype.
Fine Pixel CCD for ILC Vertex Detector ‘08 7/31 Y. Takubo (Tohoku U.) for ILC-FPCCD vertex group ILC vertex detector Fine Pixel CCD (FPCCD) Test-sample.
Hold signal Variable Gain Preamp. Variable Slow Shaper S&H Bipolar Fast Shaper 64Trigger outputs Gain correction (6 bits/channel) discriminator threshold.
Development of TOP counter for Super B factory K. Inami (Nagoya university) 2007/10/ th International Workshop on Ring Imaging Cherenkov Counters.
Hongyu Fu, Trigger group The Monte Carlo for Trigger Design of BES3 Scintillating Fibre BEMC Outline: Introduction to BES3 Scin-fibre BEMC Trigger.
KEK BT Summary &Plan Shinshu University Miho Nishiyama.
Update on final LAV front-end M. Raggi, T. Spadaro, P. Valente & G. Corradi, C. Paglia, D. Tagnani.
A Brand-new Neutrino Detector “SciBar” (1) Status and prospects Masaya Hasegawa (Kyoto Univ.) for the K2K SciBar Group for the K2K SciBar Group Hakuba.
MPPC status M.Taguchi(kyoto) T2K ND /7/7.
Development of Multi-Pixel Photon Counters(MPPC) Makoto Taguchi Kyoto University.
Frank L. H. WolfsDepartment of Physics and Astronomy, University of Rochester Status of the TOF February 22, 2001 Straight-line tracking What have we learned?
Development of Multi-Pixel Photon Counters and readout electronics Makoto Taguchi High Energy Group.
Muon/Special Detector Studies Update St. Malo Muon ID - Single muons, single pion rejection. TESLA TDR (M. Piccolo) 2. Muon ID events:  ID efficiency,
The single shower calibration accuracy is about 6.7 degrees but the accuracy on the mean value (full data set calibration accuracy) scales down inversely.
B.G.Cheon Mini-Trigger/DAQ workshop,OCU ECL Trigger overview ByungGu Cheon (SKKU) Outline  ECL calorimeter  ECL trigger scheme & performance.
FSC Status and Plans Pavel Semenov IHEP, Protvino on behalf of the IHEP PANDA group PANDA Russia workshop, ITEP 27 April 2010.
5-9 June 2006Erika Garutti - CALOR CALICE scintillator HCAL commissioning experience and test beam program Erika Garutti On behalf of the CALICE.
Time and amplitude calibration of the Baikal-GVD neutrino telescope Vladimir Aynutdinov, Bair Shaybonov for Baikal collaboration S Vladimir Aynutdinov,
11 October 2002Paul Dauncey - CDR Introduction1 CDR Introduction and Overview Paul Dauncey Imperial College London.
26/May/2008Calor LHCb Preshower(PS) and Scintillating pad detector (SPD): commissioning, calibration, and monitoring Eduardo Picatoste Universitat.
D. Bertrand, J. De Bruyne, P. De Harenne, L. Etienne, S. Hannaert, G. Van Beek The Arch.
Beta-ray test for strip scintillator readout MPPC GLD Cal group KEK 06/2/28 (Tue) Niigata university Sayaka IBA.
Performance of Scintillator-Strip Electromagnetic Calorimeter for the ILC experiment Satoru Uozumi (Kobe University) for the CALICE collaboration Mar 12.
Siena, May A.Tonazzo –Performance of ATLAS MDT chambers /1 Performance of BIL tracking chambers for the ATLAS muon spectrometer A.Baroncelli,
Front-end Electronic for the CALICE ECAL Physic Prototype Christophe de La Taille Julien Fleury Gisèle Martin-Chassard Front-end Electronic for the CALICE.
Study of the MPPC for the GLD Calorimeter Readout Satoru Uozumi (Shinshu University) for the GLD Calorimeter Group Kobe Introduction Performance.
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.
M.Taguchi and T.Nobuhara(Kyoto) HPK MPPC(Multi Pixel Photon Counter) status T2K280m meeting.
Shashlyk DAQ and FEE Status and Plans Pavel Semenov IHEP, Protvino on behalf of the IHEP PANDA group PANDA DAQ and FEE Workshop, Rauischholzhausen Castle.
A.PasseriHigh granularity Pb-SciFi calorimeter1 Construction and tests of a fine granularity lead-scintillating fibers calorimeter P.Branchini, F.Ceradini,
"North American" Electronics
Jinfan Chang Experimental Physics Center , IHEP Feb 18 , 2011
Scintillation Detectors in High Energy Physics
“Performance test of a lead glass
ILC Detector Activities in Korea
BESIII EMC electronics
Commissioning of the ALICE-PHOS trigger
MPPC for T2K Fine-Grained Detector
R&D of MPPC in kyoto M.taguchi.
Presentation transcript:

A Brand new neutrino detector 「 SciBar 」 (2) Y. Takubo (Osaka) - Readout Electronics - Introduction Readout electronics Cosmic ray trigger modules Conclusion

SciBar detector Extruded scintillator (15t) Multi-anode PMT (64 ch.) Wave-length shifting fiber EM calorimeter 1.7m 3m Stopping  2.5 x 1.3 x 300 cm 3 scintillator strips Extruded scintillator with WLS fiber readout ~15000 channels Light yield 7~20p.e./MIP/cm (2 MeV) Requirement for p/π separation Dynamic range>10.6MIP(286p.e.)

Detector Components DAQ board 64ch MAPMT Front-end board AMT Trigger board Timing distributor

Requirement to readout electronics  Fast trigger (Bunch identification)  Large number of channel (~15,000) compact photo-detector and circuit VA/TA front-end electronics DAQ board (VME) AMT, Timing distributor  Large dynamic range (1 p.e. ~ 300 p.e.) for proton energy reconstruction  High sensitivity (MIP : 7 ~ 20 p.e./1strip) Noise level < l p.e. (0.08 pC)

Readout Electronics multiplexer sample&hold slow shaper preamp. fast shaper discri. CH1 CH2 CH32 32ch VA serial output TA (32ch OR) hold PMT signal ∝ charge 1.2  s VATA Chip Front-end board (Energy information) (Timing information) A front-end board has two VATA chips. VA/TA chip VATA is used for MAPMT for the first time.

DAQ board DAQ board is custom module for SciBar readout. Control of VA readout sequence Setting of VA trigger threshold VA serial output is digitized by FADC (dynamic range ~300 p.e.) 8 front-end board (512 ch) are connected to one DAQ board. 8 front-end boards(8×64ch ) 16ch×2 TA signal All channels (~15,000) are read by only 28 DAQ boards. VME bus Timing distributor

Timing Distributor VME 6U module that distributes timing signals to DAQ boards through the bus. 4ch NIM I/O on main board + 2 daughter boards 16ch NIM I/O Daughter board FPGA 16ch NIM I/O 16×2ch LVDS/ECL Input DAQ board Flexible data processing is realized using FPGA.

AMT Develop as Atlas Muon TDC(AMT) VME 6U module Multi-hit TDC 64 channel in a module 100 usec full scale 0.78 nsec/count 64 TA signals All TA signals (448 ch) are read by 8 AMTs

Basic performance of VATA readout TA threshold curve Gain: 80count / pC ~6count / p.e. < Pedestal( ~1.5count) entries 5% non-linearity < 24pC(300p.e.) Gain distribution (all channels) Gain linearity TA threshold canbe set ~0.4 p.e. without noise hit TA threshold (mV) Trigger efficiency (%) 0 Gain (ADC count / pC) ADC cont Input charge (pC) Noise hit

Timing resolution Timing resolution = 1.84/√2 = 1.30 nsec  = 1.84 nsec Timing resolution is estimated by comparing timing of 2 channels. Cosmic ray event is used to estimate timing resolution. nsec Q(ADC) T(nsec) TQ correction Correction of light propagation time in a fiber = 4.03/√2 = 2.85 nsec  = 4.03 nsec Timing resolution nsec

Track direction ID by TOF Direction ID probability = 89.3%  T (nsec) T1T1 T3T3 z1 z8 Track length = 50.5 cm super-layer penetration

Achieved performance 5 % non-linearity at 300p.e. Noise level < 1 p.e.    = 1.3 nsec p/  separation, momentum reconstruction Uniform hit efficiency Additional information for tracking Neutrino event identification from neutron B.G.

Trigger scheme

Cosmic ray trigger modules beampedestalLEDcosmic Time 2.2 sec Data taking cycle Cosmic ray data is taken for the calibration in the off-spill. Trigger board is developed to take cosmic ray event effectively in the off-spill time

Logic for cosmic ray trigger Master trigger board Trigger Board Identification of hit track Make matching with two trigger signals 7 DAQ Board 112 TA A half of the TA channels (224ch/448ch) are used for cosmic ray trigger. Top & side view Trigger Board

Front panel : input 128 (16×8) ch LVDS/ECL Back plane : output 16ch LVDS/ECL VME 9U module input : 128 ch (16×8) Output : 16 ch FPGA decide to make trigger signal. Output : 1ch Using FPGA, trigger logic can be easily implemented for any combinations of 128 inputs.

Current status of cosmic ray event Azimuth angle (degree) Zenith angle(degree) Horizontal line Current cosmic ray trigger takes all though going muons Z(cm) Horizontal position(cm) ν Vertical position(cm) Z(cm) New trigger design is prepared to get horizontal events and uniform hit distribution. Hit distribution Angle distribution

Trigger Design Preparing hit patterns, track pattern matching them is selected. Track with less than 45 degree of zenith angle is taken. Trigger is generated, based on the hit pattern identification. Horizontally through-going muons are taken for calibration effectively. Distribution of cosmic ray hits is uniform. TA signals are trigger board inputs. Requirement Trigger design

Event display of cosmic ray event Top View Side View μ μ

Event display of stopping  event μμ Side Top e e

Summary SciBar detector uses VATA readout system. It has 5 % non-linearity at 300p.e., and its noise level is less than 1 p.e..That satisfies required performance. Trigger board is used for cosmic ray trigger, and upgrade trigger logic is prepared for effective data taking. All readout system is working well.

Omake

Principle of VATA readout 1.  s Pre-amp Fast-shaper TA Slow-shaper Hold_b outm 32ch VA serial output

Multi-anode PMT Hamamatsu H7546 type 64-channel PMT –2 x 2 mm 2 pixel –Bialkali photo-cathode –Compact –Low power : < 1000V, < 0.5mA –Gain : 6 x 10 5 –Cross talk : ~3% –Gain uniformity : ~20% (RMS) –Linearity : ~200 6 x 10 5 Top view

Scintillator & WLS Fiber Kuraray –Y11(200)MS 1.5mmφ –Multi-clad Attenuation length ~3.6m Absorption peak ~430nm Emission peak ~476nm Charged particle Wave-length Shifting Fiber Scintillator Size : 1.3×2.5×300 cm 3 Peak of emission spectrum : 420 nm TiO 2 reflector (white) : 0.25 mm thick 2.5cm 1.3 cm 300 cm 1.8 mmφ

Achieved Performance & Current Status of Cosmic ray trigger Decision time is 100 nsec. Single rate of one TA is about 100 Hz. Trigger rate is about 100 Hz. Data acquisition rate is about 20 Hz. Achieved performance We now use a trigger logic for the commissioning. We make “or” signals of every other layer, and make coincident with those of the top and side separately. We make “and” signal of the top and side. Current Status

Estimation of direction ID z1 z8 T1T1 T2T2  T =Σ   T i +  T i  i=n/2+1 n T1T1 T2T2 TnTn i=0 n/2 Top&S ide Top or Side view  T > 0 : forward direction  T < 0 : backward direction forward backward Track direction is identified by timing information.  T = Σ (T 2  T 1 ) Top& Side If n > 2,

2 super-layer penetration  T (nsec) Track length = 25.2 cm T1T1 T2T2 z1 z8 Direction ID probability = 72.5% Cosmic ray

3 super-layer penetration Direction ID probability = 89.3%  T (nsec) T1T1 T3T3 z1 z8 Track length = 50.5 cm

Hit distribution of cosmic ray event Z(cm) Horizontal position(cm) Z(cm) Vertical position(cm) νν