Application of VATAGP7 ASICs in the Silicon detectors for the BM@N central tracker (forward part) S. Khabarov, A. Makankin, N. Zamiatin, 11.09.2017,

Slides:



Advertisements
Similar presentations
Sci-Fi tracker for IT replacement 1 Lausanne 9. December 2010.
Advertisements

H1 SILICON DETECTORS PRESENT STATUS By Wolfgang Lange, DESY Zeuthen.
Electronics for large LAr TPC’s F. Pietropaolo (ICARUS Collaboration) CRYODET Workshop LNGS, March 2006.
Marco Bregant Vertex05 - Nikko, November 2005 Dipartimento di Fisica Universit à di Trieste & Istituto Nazionale di Fisica Nucleare (INFN) - Trieste ALICE.
SKIROC New generation readout chip for ECAL M. Bouchel, J. Fleury, C. de La Taille, G. Martin-Chassard, L. Raux, IN2P3/LAL Orsay J. Lecoq, G. Bohner S.
Workshop on Silicon Detector Systems, April at GSI Darmstadt 1 STAR silicon tracking detectors SVT and SSD.
Multichannel readout system of inner tracker for NICA-MPD Rogov Victor AFI, JINR, Dubna Afi.jinr.ru.
GLAST LAT Readout Electronics Marcus ZieglerIEEE SCIPP The Silicon Tracker Readout Electronics of the Gamma-ray Large Area Space Telescope Marcus.
GLAST LAT Readout Electronics Marcus ZieglerIEEE SCIPP The Silicon Tracker Readout Electronics of the Gamma-ray Large Area Space Telescope Marcus.
ATLAS SCT module performance: beam test results José E. García.
Module Production for The ATLAS Silicon Tracker (SCT) The SCT requirements: Hermetic lightweight tracker. 4 space-points detection up to pseudo rapidity.
The LHCb Inner Tracker LHCb: is a single-arm forward spectrometer dedicated to B-physics acceptance: (250)mrad: The Outer Tracker: covers the large.
Performance of the DZero Layer 0 Detector Marvin Johnson For the DZero Silicon Group.
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.
SPHENIX GEM Tracker R&D at BNL Craig Woody BNL sPHENIX Design Study Meeting September 7, 2011.
ALICE Rad.Tolerant Electronics, 30 Aug 2004Børge Svane Nielsen, NBI1 FMD – Forward Multiplicity Detector ALICE Meeting on Rad. Tolerant Electronics CERN,
1 Digital Active Pixel Array (DAPA) for Vertex and Tracking Silicon Systems PROJECT G.Bashindzhagyan 1, N.Korotkova 1, R.Roeder 2, Chr.Schmidt 3, N.Sinev.
Pixel hybrid status & issues Outline Pixel hybrid overview ALICE1 readout chip Readout options at PHENIX Other issues Plans and activities K. Tanida (RIKEN)
Progress on STS CSA chip development E. Atkin Department of Electronics, MEPhI A.Voronin SINP, MSU.
Peter, Wieczorek - EE Low Noise Charge Sensitive Preamplifier Development for the PANDA Calorimeter Design and Measurements of the APFEL - Chip.
HallA/SBS – Front Tracker PARAMETERDESIGN VALUE Microstrip Silicon Detector Number of tiles/plane and size2 Number of planes2 Size of the single
The ALICE Forward Multiplicity Detector Kristján Gulbrandsen Niels Bohr Institute for the ALICE Collaboration.
8 July 1999A. Peisert, N. Zamiatin1 Silicon Detectors Status Anna Peisert, Cern Nikolai Zamiatin, JINR Plan Design R&D results Specifications Status of.
Development of the Readout ASIC for Muon Chambers E. Atkin, I. Bulbalkov, A. Voronin, V. Ivanov, P. Ivanov, E. Malankin, D. Normanov, V. Samsonov, V. Shumikhin,
CBM Silicon Tracking System. Microstrip Detector Module Assembly and Test V.M. Pugatch Kiev Institute for Nuclear Research GSI (CBM experiment), Darmstadt.
Valerio Re, Massimo Manghisoni Università di Bergamo and INFN, Pavia, Italy Jim Hoff, Abderrezak Mekkaoui, Raymond Yarema Fermi National Accelerator Laboratory.
1 Device Simulations & Hardware Developments for CBM STS Sudeep Chatterji CBM Group GSI Helmholtz Centre for Heavy Ion Research CBM Collaboration Meeting,
ICPPA-2015 Moscow Oct ASIC for calorimetric measurements in astrophysical experiment NUCLEON (overview) E. Atkin1, A. Voronin1,2, D. Karmanov2,
Solid State Detectors for Upgraded PHENIX Detector at RHIC.
Readout Architecture for MuCh Introduction of MuCh Layout of Much ( proposed several schemes) Read ASIC’s Key features Basic Readout chain ROC Block Diagram.
Front Tracker: main technical solutions 40x50 cm 2 module Front Tracker Chamber: 40x150 cm 2  Use COMPASS approach: 3xGEM, 2D readout - one significant.
Development of radiation hard Sensors & Cables for the CBM Silicon Tracking System Sudeep Chatterji On behalf of CBM-STS Collaboration GSI Helmholtz Centre.
Albuquerque 1 Wolfgang Lohmann DESY On behalf of the FCAL collaboration Forward Region Instrumentation.
Status of the PSD upgrade - Status of the PSD cooling and temperature stabilization system - MAPD gain monitoring system - PSD readout upgrade F.Guber,
CBM 12 th Meeting, October 14-18, 2008, Dubna Present status of the first version of NIHAM TRD-FEE analogic CHIP Vasile Catanescu and Mihai Petrovici NIHAM.
Development of the X-ray Detectors for XTP Cao Xue-lei Institute of High Energy Physics, CAS IHEP, Beijing.
SP- 41 magnet ZDC RPC (TOF) DC ST Target T0 detector MPD / NICA and / Nuclotron Experiments Picosecond Cherenkov detectors for heavy ion experiments.
ADC values Number of hits Silicon detectors1196  6.2 × 6.2 cm  4.2 × 6.2 cm  2.2 × 6.2 cm 2 52 sectors/modules896 ladders~100 r/o channels1.835.
SAMURAI Si Detector M. Kurokawa a), H. Baba a), T. Gunji b), H. Hamagaki b), S. Hayashi b),T. Motobayashi a), H. Murakami a), A. Taketani a), M. Tanaka.
FEE for Muon System (Range System) Status & Plans G.Alexeev on behalf of Dubna group Turin, 16 June, 2009.
1 Projectile Spectator Detector: Status and Plans A.Ivashkin (INR, Moscow) PSD performance in Be run. Problems and drawbacks. Future steps.
MICRO-STRIP METAL DETECTOR FOR BEAM DIAGNOSTICS PRINCIPLE OF OPERATION Passing through metal strips a beam of charged particles or synchrotron radiation.
V.Aulchenko 1,2, L.Shekhtman 1,2, B.Tolochko 3,2, V.Zhulanov 1,2 Budker Institute of Nuclear Physics, , Novosibirsk, Russia Novosibirsk State University,
Trigger system for setup 2016 V. Rogov, V. Yurevich,D.Bogoslovski, S.Sergeev, O.Batenkov* LHEP JINR *V. G. Khlopin Radium Institute, St. Petersburg.
Study of the MPPC for the GLD Calorimeter Readout Satoru Uozumi (Shinshu University) for the GLD Calorimeter Group Kobe Introduction Performance.
QA Tests Tests for each sensor Tests for each strip Tests for structures Process stability tests Irradiation tests Bonding & Module assembly Si detectors1272.
Performance of the PHENIX NCC Prototype Michael Merkin Skobeltyn Institute of Nuclear Physics Moscow State University.
Vasilisa Lenivenko Vladimir Palichik (LHEP, JINR ) Alushta, June 2016.
The design of fast analog channels for the readout of strip detectors in the inner layers of the SuperB SVT 1 INFN Sezione di Pavia I Pavia, Italy.
PADME Front-End Electronics
Budker INP V.Aulchenko1,2, L.Shekhtman1,2, V.Zhulanov1,2
M. Manghisoni, L. Ratti Università degli Studi di Pavia INFN Pavia
Silicon microstrip detector for imaging of fast processes at high intensity synchrotron radiation beam. Budker INP V.Aulchenko1,2, L.Shekhtman1,2, B.Tolochko3,2,
FCAL R&D towards a prototype of very compact calorimeter
Calorimeter Mu2e Development electronics Front-end Review
Evidence for Strongly Interacting Opaque Plasma
Wide Dynamic range readout preamplifier for Silicon Strip Sensor
INFN Pavia and University of Bergamo
Jean-Francois Genat LPNHE Universite Pierre et Marie Curie CNRS/IN2P3
Silicon Pixel Detector for the PHENIX experiment at the BNL RHIC
Børge Svane Nielsen/JJG
A Low Power Readout ASIC for Time Projection Chambers in 65nm CMOS
Status of n-XYTER read-out chain at GSI
SAMURAI Si detector Requirements overview
ECAL Electronics Status
BESIII EMC electronics
Pradeep Ghosh for the CBM Collaboration Goethe-Universität, Frankfurt
ME instrument and in-orbit performance
Coincidence measurement of heavy ion and protons with SAMURAI
Why silicon detectors? Main characteristics of silicon detectors:
Presentation transcript:

Application of VATAGP7 ASICs in the Silicon detectors for the BM@N central tracker (forward part) S. Khabarov, A. Makankin, N. Zamiatin, 11.09.2017, JINR,Dubna ASIC - Application-Specific Integrated Circuit VATAGP7 manufactured by IDEAS (Integrated Detector Electronics AS), Norway DSSD - Duble Side Si Detector – (two coordinate microstrip silicon detector) BM@N - Baryon Matter at Nuclotron

The scheme of BM@N experiment with the legend of main detecting systems Main goal of BM@N experiment is to study properties of baryon matter which produced in heavy ion collisions with fixed target in the beam energy range from 1 to 4.5 GeV per nucleon. Central tracking system is located inside the analyzing magnet and is intended for reconstruction of tracks in nucleon-nucleon interactions of the beam of accelerated ions on a fixed target. The coordinate planes of the tracker consist of silicon double-sided strip detectors and gas detectors GEM with two coordinate readings (strips), these detectors are able to work with high coordinate resolution in a magnetic field.

The appearance of a rectangular detector module on the both sides p+ side n+ side The module consists of two square shape silicon DS-microstrip detector, two electronics read-out cards (one on each side of the detector) and a mechanical frame for precise module positioning, assembling of detectors and read-out cards.

The coordinate Si-plane consist of 8 detector modules with 10240 strips (measuring channels) is assembled on a mechanical frame and placed in a box which is light and electromagnetic shielding

Ultrasonic bonding of the strip to strip between two DS-Si-sensors on module

The functional scheme of detector module and appearance of two electronic boards DSSD with DC topology don’t contain integral resistors and capacitors (RC), therefore external R, C are required to supply bias voltage to each strip and to electrically decouple the DC current from the electronic inputs. This role is performed by Pitch Adapter (PA) with a topology of two types for p+ and n+ sides of the detector. In addition, PA has topology of contact pads similar to chips located on the side of electronic chips. PA modules are made on sapphire plates with an epitaxial layer of silicon (SOI). Integrated poly silicon bias resistors have a value of 0.7 – 1.0 MΩ, decoupled capacitors have a value of 140 pF. PA is assembled together with read-out ASICs on the read-out card. Positive polarity signals come from detectors to P+ read-out card (black PCB) while negative signals come to N+ read-out card (red PCB).

Cross section of the pitch adapter 640 chanels (PA-640)

View of the rear side PA-640

VATAGP7 PA-640

Visual control in LHEP of the PCBs-640 before encapsulation of VATAG7-chips Red PCB-640n+ (№007), chip#2, the type of defect: the small piece of the Al-wire Ø18 mkm on the surface PCB

The architecture of VA and TA parts

The read-out electronics is designed and based on the non-encapsulated ASICs crystals – VATAGP7.1, manufactured by IDEAS2 (Norway). Each board contains five ASICs, bonding and filled with black compound The main parameters of the analog part of this IC: Number of analog inputs – 128; The polarity of the input signals – +/-; Gain – 16,5 μA/fC; Dynamic range of signals – ±30 fC (~8 m.i.p.); Integration time (slow SA) – 500 ns; Integration time (fast SA) – 50 ns; Intrinsic noise (at Cin = 0 pF) – 70 e; Dependence of noise on input capacitance – 12 e/pF; The main parameters of read-out electronics card: Number of analog inputs – 640; Five analog multiplexer output with read out clock - 1.25 MHz Input charges from -30 fC to +30 fC Slow shaper shaping time - 0.5 µs Fast shaper shaping time -50 ns Differential current out – 20 µA/fC Adjustable threshold, from 0.12 fC min, (at 0 load) Power supply -2.0 V and +1.5 V Total power is 280 mW / ASIC For reminder: the value of the signal 1 m.i.p.(Si=300mkm)=4 fC (~24×103 e)

The data of measurements with a radioactive source of electrons 106Ru

Signals from passing through the module of relativistic electrons (106Ru)

The row data of Si-plane measurements on BM@N experiment, march-2017, CH2- target, Ed=4.5 GeV/n Row data: run_1898 (CH2– target), 4.5GeV/n, M8_2 total event 22161.png

Row data: run_1898 (CH2 – target), 4.5GeV/n, M8_1 event 6535.png

Row data: run_1913 (Pb - target), 4.5GeV/n, M8_1

Row data: run_1913 (Pb-target), 4.5GeV/n, M8_1 event 325.png

Row data, Run 1619: direct beam 12C, E=4 Row data, Run 1619: direct beam 12C, E=4.5GeV/n, Field=0 Sp57=350A_no Target.png

Why we use of the VATAG7P : Summary: Why we use of the VATAG7P : Design and main parameters of VATAGP7 to aproach for the our specification of DSSD-modules/tracker BM@N (128 chanels/chip, low noise, low power) VATAGP7 is the commercial ASIC and of the delivery time is (3÷4) month VATAGP7 designed and manufactured by IDEAS (Integrated Detector Electronics AS, Norway), IDEAS is Company with the longtime positive history of the application they ASICs for nuclear physics ASICs for collider experiments: SVX5 - (D0/Fermi-lab, Phenix/BNL, APV26 – CMS, ATLAS/CERN ) – Radiation Hard technology (commercial ?) Plans on future: - To decrease of the readout time (dead time-DT)<30 mks, now (128=128×1) at Fmux=1.25 MHz, DT~100 mks - To discuss of the possibility for increasing Fmux (5 MHz ???) - To discuss of the new structure ASIC (128=32×4)