S.Baccaro, A.Cecilia INFN Rome DPG 6/9/05 July 2005 irradiation test results of SIC & BTCP crystals I.Dafinei, M.Diemoz ENEA-Casaccia & INFN Rome.

Slides:



Advertisements
Similar presentations
Ioan Dafinei Regional Centre ECAL-CMS Rome ITALY Villa Olmo, Como October 2001 Advanced Technology and Particle Physics Lead Tungstate Crystals for.
Advertisements

Evaluation of photothermal effects induced by laser heating of gold nanorods in suspensions and inoculated tumors G.S. Terentyuk, D.S. Chumakov, I.L. Maksimova.
Random Telegraph Signal (RTS) in CMOS Monolithic Active Pixel Sensors (MAPS) for charged particle tracking. Outline Reminder: The operation principle of.
Characterization of primed state of CVD diamond by light and alpha particles C. Manfredotti Experimental Physics Department University of Torino INFN-
Fricke gel dosimeters for the measurement of the anisotropy function of a HDR Ir-192 brachytherapy source Mauro Carrara 1, Stefano Tomatis 1, Giancarlo.
Tests of scintillators CsI, CsI(Na), BGO, NaI(Tl) CsI(Tl)
ECAL Testbeam Meeting, Rome 28 March 2007 Toyoko Orimoto Adolf Bornheim, Chris Rogan, Yong Yang California Institute of Technology Lastest Results from.
Optical Fibre Dosimetry First Thoughts. Goal Target Measuring dose in a distributed way using optical fibres (“active”) Constraints: – Mixed-Radiation.
Clinical application of TCP ・ NTCP. Lyman JT. Complication probability as assessed from dosevolume histograms. Radiat Res Suppl 1985; 8:S13–S19. Because.
24 th ICNTS, Bologna, 1-5 September 2008 Radiation Induced Damage Electron, Gamma Photon and Ion Irradiation Effects in PP/EPR/HDPE Christelle Bergeon.
X-ray radiation damage of silicon strip detectors AGH University of Science and Technology Faculty of Physics and Applied Computer Science, Kraków, Poland.
The Increased Biological Effectiveness of Heavy Charged Particle Radiation: From Cell Culture Experiments to Biophysical Modelling Michael Scholz GSI Darmstadt.
Rutherford Appleton Laboratory CMS ECAL Split 08/09/04 R M Brown - RAL 1 The Status of the CMS Electromagnetic Calorimeter R M Brown On behalf of the CMS.
CMS SLHC workshop, D.J.A. Cockerill (RAL)1 CMS SLHC Workshop The CMS ECAL Detector at SLHC D Cockerill RAL
CERN, July 7 th, 2010 LHCf status report Oscar Adriani Università degli Studi di Firenze INFN Sezione di Firenze On behalf of the LHCf Collaboration.
CMS ECAL Elba May 2006 R M Brown - RAL 1 The Status of the CMS Electromagnetic Calorimeter R M Brown On behalf of the CMS ECAL Group.
Laurie Cuttino MD, Dorin Todor PhD, Douglas Arthur MD, Rohini George, Lynn Pacyna CMD Medical College of Virginia Campus Department of Radiation Oncology.
A Tumour Control Probability based approach to the development of Plan Acceptance Criteria for Planning Target Volume in Intensity Modulated Radiation.
Testing Integrated COTS DC/DC Converters in Hostile Environment Apollo collaboration, funded by I.N.F.N. Italy C. Abbate (a,b), S. Baccaro (c,b), G. Busatto.
CMS ECAL Laser Monitoring System Christopher S. Rogan, California Institute of Technology, on behalf of the CMS ECAL Group High-resolution, high-granularity.
1 Radiation Hardness of Monolithic Active Pixel Sensors Dennis Doering, Goethe-University Frankfurt am Main on behalf of the CBM-MVD-Collaboration Outline.
HF PRR – 16 February Core: 600 ± 10 micron dia Clad: micron dia Buffer: 800 ± 30 micron dia Core material: High OH- sythetic Silica.
SLHC Local Support Requirements Summary M. Gilchriese November 4, 2008.
August 99 E.Auffray CMS/ECAL STATUS on PWO crystals from Bogoroditsk after one year of preproduction for CMS-ECAL Etiennette Auffray SCINT 99, 16 August.
LHC The Large Hadron Collider (LHC) is an accelerator with 27 km circumference. Being built on the France- Switzerland border west of Geneva. It will start.
Chinese Contributions to FAIR Hushan Xu Institute of Modern Physics, CAS, Lanzhou
11/02/04E. Auffray, EP-CMA E. Auffray, CERN PH-CMA Results of the 50 SIC crystals Received in January 2004.
1 P.Rebecchi (CERN) “Monitoring of radiation damage of PbWO 4 crystals under strong Cs 137  irradiation in GIF-ECAL” “Advanced Technology and Particle.
Review for Quiz 1.A light year is a unit of measure for Distance! It is the distance electromagnetic radiation travels in one year.
Remembering PWO Radiation hardness studies at IHEP, Protvino Y. Kubota.
October,05 HCAL Meeting 10/15/05 Quartz Plate Simulation Studies Quartz Plate Simulation Status F. Duru, U. Akgun, A.S. Ayan, J. Olson, Y. Onel The University.
The LHCb Electromagnetic Calorimeter Ivan Belyaev, ITEP/Moscow.
Examples of Good & Bad Practice: Effect of the wedge filter and field size in the skin dose distribution L 9.1.
The CMS electromagnetic calorimeter
Apatity, Bogoroditsk and Shankhai PWO Crystals under Gamma Irradiation (PRELIMINARY RESULTS) Apatity IHEP Khurchatov North Crystals CMS + BTeV Alice Presented.
1 Optical fiber irradiation tests 1.Results from ATLAS LAr 2.Narrow down to Germanium doped GRIN fiber 3.Preliminary tests 4.Tests in the plan Jingbo Ye.
Avalanche Photodiodes from the Start.
Studies on n and p-type MCz and FZ structures of the SMART Collaboration irradiated at fluences from 1.0 E+14 to 5.6E+15 p cm -2 RD50 Trento Workshop ITC-IRST.
Examples A star radiates as a blackbody at a temperature of 1700 K. At what wavelength does the peak of the blackbody spectrum occur? If you were to look.
PbWO 4 crystals Calorimeter Liping Gan University of North Carolina Wilmington.
Beam Profile Monitor for Spot-Scanning System Yoshimasa YUASA.
TEMPLATE DESIGN © Optimization of Cancer Radiation Treatment Schedules Jiafen Gong* and Thomas Hillen Department of Mathematical.
(1/16) 08/05/12 – RadWG meeting G. Spiezia, P. Peronnard, E. Lefteris, P. Oser, J. Mekki PSI tests - Comparator Results Devices under test and beam conditions.
CMS ELECTROMAGNETIC CALORIMETER Jean-Pierre Ernenwein OVERVIEW 6th international conference on advanced technology and particle physics Villa Olmo, Como,
ECAL performance evolution plots Contact: 1.
Radiation Damage Experience: SiPM & QIE Cards Proton Cyclotron - Mass General Hospital (& MIT Research Reactor) Larry Sulak with Sergey Los*, Jim Freeman*,
XI Workshop on Resistive Plate Chambers and Related Detectors, INFN, 5-10 February, Aging test of high rate MRPC Wang Yi Department of Engineering.
HEP2001, Budapest, July 2001 R M Brown - RAL 1 The Vacuum Phototriodes for the CMS Electromagnetic Calorimeter P R Hobson, D C Imrie, O Sharif Brunel University,
Sept 2000E. Auffray, P. Lecoq, EP-CMA Results on the 100 R&D EndCap crystals measured in RCCERN on ACCOCE2 E. Auffray, P. Lecoq CERN EP-CMA.
Ultra Cherenkov based SAC
Mu2e crystals qualification
The Electromagnetic Calorimetry of the PANDA Detector at FAIR
Roman Mizuk (ITEP, Moscow)
Ultra fast SF57 based SAC M. Raggi Sapienza Università di Roma
An extensive aging study of bakelite RPC
Properties of Recent SIC Crystals
PMT/CW Irradiation tests-2010
HF QUARTZ FIBER Y.Onel , J.P.Merlo, K.Cankocak, I.Dumanoglu, I.Schmidt and A.Penzo.
Studies of the effect of the LHC cycle on
Report on radiation test done in Casaccia on January 11, 2006
The Effects of Ionising Radiation on Cell Mechanics
Update on TB 2007 Xtal Irradiation Studies at H4
Studies of the effect of the LHC cycle on
CMS ECAL Endcaps: Fluence/Dose (500 fb-1)
Scintillator tile- SiPM systems R&D
Endcap Crystal Properties
Calorimeter Backgrounds
ELECTROMAGNETIC CALORIMETER
Rotating Spring Problem
Supplementary Material
Presentation transcript:

S.Baccaro, A.Cecilia INFN Rome DPG 6/9/05 July 2005 irradiation test results of SIC & BTCP crystals I.Dafinei, M.Diemoz ENEA-Casaccia & INFN Rome

10 EB crystals made in Russia and 10 EB crystals produced in China (crystals) were irradiated in identical Gy/h dose rate: Gy Gy LTO and TT 3, 9, 15, 21 cm ( distance from FF ) Damage 18 °C followed for 22 days. Standard and Full Saturation tests on BTCP & SIC crystals

Barcode LT360 (%) LT420 (%) LT620 (%) Infl. (nm) S. Infl. (%/nm) TT sp. (nm) TT grad (nm/cm) LY (pe/MeV) FNUF (%/X0) Mean  Qualification parameters of Russian Crystals

Barcode LT360 (%) LT420 (%) LT620 (%) Infl. (nm) S. Infl. (%/nm) TT sp. (nm) TT grad (nm/cm) LY (pe/MeV) FNUF (%/X0) Mean  Qualification parameters of Chinese Crystals

Comparison of Qualification Parameters mean values Barcode LT360 (%) LT420 (%) LT620 (%) Infl. (nm) S. Infl. (%/nm ) TT sp. (nm) TT grad (nm/cm) LY (pe/MeV) FNUF (%/X0) Mean  Barcode LT360 (%) LT420 (%) LT620 (%) Infl. (nm) S. Infl. (%/nm) TT sp. (nm) TT grad (nm/cm) LY (pe/MeV) FNUF (%/X0) Mean  BTCP SIC

 ( ) of all analysed crystals after Gy BTCP SIC

 (420nm) of BTCP & SIC crystals after Gy At Gy radiation hardness parameters are within specifications for 100 % of Russian crystals and 80% for Chinese. BTCP SIC

 ( ) of all analysed crystals after Gy BTCP SIC

 (420nm) of BTCP & SIC crystals after Gy At Gy radiation hardness parameters are within specifications for 50 % of Russian crystals and 70% for Chinese. SIC BTCP

SIC Comparison of Light Yield before and after irradiation

BTCP SIC Fraction of Light Yield lost after irradiation

Comparison of FNUF before and after irradiation BTCP SIC

r = μ SFS / μ FS Saturation level reached in SFS conditions with respect to FS

q = (μ FS - μ Recov )/ μ FS Fraction of recovered colour centres after 22 days from the stop of irradiation

BarcodeLT360LT420LT620SLTODTTOLY8X0FNUF Mean StdDev Min Max IRRADIATION TESTS ON SIC PRODUCTION EB CRYSTALS

Irradiation tests on sic production EB crystals 1h Gy/h

Distribution of radiation 420 nm (1h Gy/h)

Distribution of radiation 420 nm (1h Gy/h) 1.15       0.65 DPG-June05

Some China made crystals (#02, #18) have a remarkably high radiation hardness and fast saturation of the damage. Nevertheless, their overall behaviour is quite non-uniform (possible consequence of large spread of their optical parameters). Russian crystals have a uniform behaviour under irradiation exposure. If SFS conditions are considered, radiation hardness qualification parameters are reliable for 100% of Russian crystals and 80% of Chinese. For FS conditions the reliability drops to 50% in the case of Russian crystals and 70% for Chinese. CONCLUSIONS