Plan for future GaAs samples for TestBeam measurements JINR DLNP group (presented Z. Krumshteyn) JINR DLNP group (presented Z. Krumshteyn) FCAL Collaboration.

Slides:



Advertisements
Similar presentations
PAC Nuclear Physics, 1-2 April, 2004 Construction of the IREN source (the theme /2004). Status&perspectives-proposal on the extension W.I.
Advertisements

Photo-Nuclear Physics Experiments by using an Intense Photon Beam Toshiyuki Shizuma Gamma-ray Nondestructive Detection Research Group Japan Atomic Energy.
New hardware and setups New short pulse regime Experimental results TW power Future plans on laser development ATF CO 2 LASER progress Vitaly Yakimenko.
ISS meeting, (1) R. Garoby (for the SPL study group) SPL-based Proton Driver for Facilities SPL-based Proton Driver for Facilities at CERN:
17-May-15Actual problems of microworld physics. Gomel Investigation of radiation hard sensor materials K. Afanaciev on behalf of FCAL collaboration.
17-May-15FCAL collaboration meeting. Krakow.. Radiation hardness of GaAs Sensors K. Afanaciev, Ch. Grah, A. Ignatenko, W. Lange, W. Lohmann, M. Ohlerich.
17-May-15FCAL collaboration workshop, Status of sensor R&D in Minsk K. Afanaciev, M. Baturitsky, I. Emeliantchik, A. Ignatenko, A. Litomin, V. Shevtsov.
GaAs radiation imaging detectors with an active layer thickness up to 1 mm. D.L.Budnitsky, O.B.Koretskaya, V.A. Novikov, L.S.Okaevich A.I.Potapov, O.P.Tolbanov,
Slide 1 Diamonds in Flash Steve Schnetzer Rd42 Collaboration Meeting May 14.
Design and test of a high-speed beam monitor for hardon therapy H. Pernegger on behalf of Erich Griesmayer Fachhochschule Wr. Neustadt/Fotec Austria (H.
Design on Target and Moderator of X- band Compact Electron Linac Neutron Source for Short Pulsed Neutrons Kazuhiro Tagi.
Radiological and Experimental Facilities Based On INR Proton LINAC Institute for nuclear research of RAS, Moscow , Russia Sergey Akulinichev, Leonid.
Precise neutron inelastic cross section measurements A.Negret 1 1 “Horia Hulubei” National Institute for Physics and Nuclear Engineering, Bucharest, ROMANIA.
III. Analytical Aspects Summary Cheetham & Day, Chapters 2, 3 Chemical Characterization of Solid-State Materials Chemical Composition: Bulk, Surface, …
Multiplicity and Energy of Neutrons from 233U(nth,f) Fission Fragments
ELBE Neutron Source IAEA TC Meeting “Nuclear Data for IFMIF”, FZ Karlsruhe, October 4-6, 2005 Klaus Seidel Technische Universität Dresden.
R&D for R3B/EXL silicon spectrometers, ELISe in-ring instrumentation based on planar Si and CVDD Alexander Gorshkov Flerov Laboratory of Nuclear Reactions.
The analysis of element and isotope composition by neutron spectroscopy method N.V. Bazhazhina, Yu. D. Mareev, L.B. Pikelner, P.V. Sedyshev, V.N. Shvetsov.
Applications of neutron spectrometry Neutron sources: 1) Reactors 2) Usage of reactions 3) Spallation sources Neutron show: 1) Where atoms are (structure)
Dubna, January, th session of the JINR Scientific Council Nuclear Physics PAC.
Future usage of quasi-infinite depleted uranium target (BURAN) for benchmark studies Pavel Tichý Future usage of quasi-infinite depleted uranium target.
NEW COMMENTS TO ILC BEAM ENERGY MEASUREMENTS BASED ON SYNCHROTRON RADIATION FROM MAGNETIC SPECTROMETER E.Syresin, B. Zalikhanov-DLNP, JINR R. Makarov-MSU.
CTF3 photo injector laser status CERN 17 July 2009 CLIC meeting.
Interactions of Neutrons
Simulations of Accelerator Driven Systems (ADS) Aleksander Polanski Joint Institute for Nuclear Research, Dubna, Russia. The Andrzej Soltan Institute for.
D ETERMINATION OF ELEMENTAL COMPOSITIONS BY USING NEUTRON RESONANCE SPECTROSCOPIC M AHMOUD G AAFAR T EACHING ASSISTANT, PHYSICS F ACULTY OF SCIENCE, MENOUFIA.
Radiation Test Facilities G. Spiezia. Engineering Department ENEN Radiation tests facilities  Radiation test in the accelerator sector  External facilities.
The Proposed Materials Test Station at LANSCE Eric Pitcher Los Alamos National Laboratory Presented at the Workshop on High-Power Targetry for Future.
High Dose Irradiation of Possible FCAL Sensors at the S-DALINAC Ch.Grah Physics and Detector Meeting DESY HH,
Neutron inelastic scattering measurements at the GELINA facility of EC-JRC-IRMM A. Negret 1, C. Borcea 1, A. Plompen 2 1 NIPNE-HH, Romania 2 EC-JRC-IRMM,
1,2 Tshepo Dinoko, 3 Vasilij Andrianov, 3 Pavel Sedyshev 1 iThemba LABS, Somerset West 7129, South Africa 2 University of the Western Cape, Bellville 7535,
G.Shirkov, Basic Facilities, JINR Scientific Council, Status of the Basic Facilities at JINR G.Shirkov 1.Basic Facilities Operation and development.
Status on 25 Mg(n,  ) and neutron flux in 2012 Bologna, 27 November 2013 C. Massimi.
N. Gubanova 1, V. Kanygin 2, A. Kichigin 3, S. Taskaev 4 1 Institute of Cytology and Genetics, Novosibirsk, Russia 2 Novosibirsk State Medical University,
VIEW on RAD HARDNESS TESTS of STS FEE IN MEPHI. Simakov A.B. – Head of “Special Microelectronics” Lab.
February 21-21, 2008JINR Scientific Council 103-d session IREN project status.
Neutron production study with the thick lead target and uranium blanket irradiated by 1.5 GeV protons Filip Křížek, ÚJF AV ČR.
Beam test possibilities at JINR and Fermilab V. Pronskikh Fermilab 02/15/2012.
Experimental Studies of Spatial Distributions of Neutrons Produced by Set-ups with Thick Lead Target Irradiated by Relativistic Protons Vladimír Wagner.
Neutron inelastic cross section measurement on 28 Si Alexandru Negret Horia Hulubei National Institute for Physics and Nuclear Engineering, Bucharest,
Implementation of an analytical model accounting for sample inhomogeneities in REFIT K. Kauwenberghs EC – JRC – IRMM Standards for Nuclear Safety, Security.
Design and construction of Nuclotron-based Ion Collider fAcility (NICA) and Mixed Phase Detector (MPD) Design and construction of Nuclotron-based Ion Collider.
Neutron cross-sections measurement at the facility at CERN Students’coffee – 26th meeting, Tuesday 28 October 2014, D02-BE Auditorium Prevessin Massimo.
1 Alexey Sissakian Director, Academician of RAS JINR: Results and Prospects R–ECFA meeting 8 – 10 October, 2009.
B. Azadegan, S. A. Mahdipour Hakim Sabzevari University
1 Neutron Effective Dose calculation behind Concrete Shielding of Charge Particle Accelerators with Energy up to 100 MeV V. E Aleinikov, L. G. Beskrovnaja,
1 NICA Project Report of The Group I S.L.Bogomolov, A.V.Butenko, A.V.Efremov, E.D.Donets, I.N.Meshkov, V.A.Mikhailov, A.O.Sidorin, A.V.Smirnov, Round Table.
Albuquerque 1 Wolfgang Lohmann DESY On behalf of the FCAL collaboration Forward Region Instrumentation.
Valery Telnov Budker INP, Novosibirsk IWLC2010, CERN October 21, 2010 A FEL pumped solid state laser system for the photon collider at CLIC.
Antihydrogen Workshop, June , CERN S.N.Gninenko Production of cold positronium S.N. Gninenko INR, Moscow.
Fermilab Test Beam and Irradiation Facilities Erik Ramberg 10 January, 2013.
Experience with Novosibirsk FEL Getmanov Yaroslav Budker INP, Russia Dec. 2012, Berlin, Germany Unwanted Beam Workshop.
Summer Student Practice, 2009, JINR Dubna1 Neutron spectroscopy by time of flight method and determination of neutron beam Prepared by: Sameh Hassan, Yomna.
PSI, Zurich February 29 – March Session classification : Accelerator Concepts Tuesday, March 1, 2016 Introduction Vyacheslav Yakovlev Fermilab,
Studies at BINP Alexander Krasnov
February 6, 2014 CLIC Workshop Switzerland
Radiation hardness tests of GaAs and Si sensors at JINR S. M
Test of Hybrid Target at KEKB LINAC
The nucleosynthesis of heavy elements in Stars: the key isotope 25Mg
Cross-section Measurements of (n,xn) Threshold Reactions
WP11: electron and proton beam testing
Neutron time-of-flight measurements at GELINA
Measurements of the 238U radiative capture cross section using C6D6
Superbeams with SPL at CERN
Injection facility for Novosibirsk Super Charm Tau Factory
The Gas Dynamic Trap (GDT) Neutron Source
Testbeam Results for GaAs and Radiation-hard Si Sensors
O. Svoboda, A. Krása, A. Kugler, M. Majerle, J. Vrzalová, V. Wagner
A.V.Burdakov at al. Plasma transport in linear and helical multiple-mirror systems (EX/P5-26) Budker INP ( Novosibirsk, Russia) developed Gas-Dynamic Multiple-mirror.
Pohang Neutron Facility (First Presentation of Prof. Cho’s Class)
Presentation transcript:

Plan for future GaAs samples for TestBeam measurements JINR DLNP group (presented Z. Krumshteyn) JINR DLNP group (presented Z. Krumshteyn) FCAL Collaboration Meeting, June , 2009, Zeuthen

Batch N carriers n/cm -3 Nplates Darmstadt Beam expired KIAE SI exp. 1 ( )(1-1.5)* ,10,11,12 9 (pad1), 11(pad4) 10(pad1) 2 (AG )(5-6)* ,6,7,8 5(pad4), 7(pad3)? 8(pad1) 3 ( )(1-3)* ,2,31,41 2(pad1), 31(pad4) 41(pad1) 4 (AP )(2-5.5)* ,14,15,16 p-ν-n- structure* bonus(2-3)* , 4, 1-1,2-1 Table 1. GaAs samples 2008 FCAL Collaboration Meeting, June , 2009, Zeuthen

Initial n-GaAsFabrication method №1, n  (1 -1.5)*10 17 см -3,Te Diffusion of Cr under temperatureT2 №2, n  (5 - 6)*10 16 см -3, Te Diffusion of Cr under temperature Tm №3, n  (1 - 3)*10 16 см -3, Sn Diffusion of Cr under temperature T1 №4, n  (2 - 5)*10 16 см -3, Te p-ν-n- structure* Notice T1  Tm<T2. * - presence in the detector n- type low-resistance domain, all other detectors №1, 2, 3 had structure m-i-m: metal- insulator (high-resistance GaAs) –metal. Table 2. GaAs samples 2008(Fabrication method) FCAL Collaboration Meeting, June , 2009, Zeuthen

Table 3. experimental GaAs detectors 2009 FCAL Collaboration Meeting, June , 2009, Zeuthen Initial n-GaAs, n  (2-5)*10 16 см -3 Fabrication methodNumber GaAs, doping Sn Diffusion of Cr under temperature T1 2(?) Diffusion of Cr under temperature T2 2(?) GaAs, doping Te Diffusion of Cr under temperature T1 2(?) Diffusion of Cr under temperature T2 2(?) Total8(?) Notice T1  T2. On the basis study of rad.hardness of batch №3 (2008). Within initial concentration n-GaAs, (2-5)*10 16 см -3, it will be investigate radiation hardness vs impurity (Sn, Te) and temperature (T1, T2)

µm 300 µm Shape of GaAs sample 2008Shape of GaAs sample 2009 FCAL Collaboration Meeting, June , 2009, Zeuthen

In Joint Institute for Nuclear Research (JINR), Dubna the project of new Intense REsonance Neutron source (IREN) is under construction now. The IREN will be used as a neutron source of new generation for research of the broad spectrum of problems in fundamental and applied nuclear physics. The IREN source is intended for nuclear physic investigations by a time-of-flight on a place and in a building of LUE-40 + IBR-30 installation removed from operation, thus the existing infrastructure of eight neutron beams with fly paths from 10 up to 750 m, an experimental hall and measuring pavilions is completely used. The IREN source exploiting a booster principle should provide a fast multiplication of initial neutrons produced by an electron beam from a linear accelerator in electron-neutron converter. So its design has to ensure as short as possible time t <10 ns for one act of neutron multiplication into a subcritical blanket, the total duration of a fast neutron pulse about 400 ns with the repetition rate 150 Hz, and a neutron yield at a level n/s. The project will be implemented in two stages. At the first stage the linear accelerator and nonmultiplying target will be constructed. FCAL Collaboration Meeting, June , 2009, Zeuthen

COMPARISON OF THE IREN SOURCE WITH OTHER NEUTRON SOURCES AIMED FOR NUCLEAR PHYSICS Neutron source(Laboratory), n/s C, 10 7 t, ns dt (at 100 eV), ns FAKEL (IAE, Russia) ORELA (ORNL, USA) GELINA ( IRMM, Belgium) LUE-40+IBR-30 (Dubna, put out of operation) LANSCE (LANL, USA) CERN PS TOF facility IREN (Dubna, project) t – duration of fast neutron burst ; dt – real duration of neutron pulse at E n = 100 eV after moderation of neutrons; С is define by relation φ(En)=C/ En*L2,were φ(En ) – neutron flux with energy Е n (eV) on the 1 cm 2 sample, located on the distance L meter from source, а - total yield of neutrons per second.

LINEAR ACCELERATOR The travelling wave electron linac LUE-200 was designed at the Budker Institute of Nuclear Physics (BINP), Novosibirsk Beam average power10 kW Electron energy200 MeV Pulse current<250ns Repetition rate150 Hz Number of accelerating sections2 IREN 1-st stage parameters Beam average power1.25kW Electron energy100 MeV Pulse current100ns Repetition rate50(150) Hz Peak current (A)2.5 A FCAL Collaboration Meeting, June , 2009, Zeuthen