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RADMON 15-Feb-071 RPL dosimeter at CERN M. Fuerstner +, I. Brunner +, F. Jaquenod ‡, N. Liaudet ‡, S. Pernecker ‡, M. Tognolini ‡, G. Triscone ‡, H. Vincke + + CERN ‡ Ecole d’ingenieurs de Geneve
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RADMON 15-Feb-072 Overview Principles New RPL reader –Principle –Components –Software RPL Dosimeter China Experiments
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RADMON 15-Feb-073 RPL Dosimeter Material: Silver activated metaphosphate glass Effect: -Ionizing radiation creates radio- photoluminescence centers -Colorization Analysis: -Luminescence intensity after UV-light exposure -Optical density
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RADMON 15-Feb-074 Dosimeter characteristics Increasing the precision ~ 1 M Signal of the RPL reader [arbitrary units] ~1~300~5000 Dose [Gy], log scale
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RADMON 15-Feb-075 New RPL Reader
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RADMON 15-Feb-076 Schematic Photo- Transistor
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RADMON 15-Feb-077 Luminescence 1 2 3 1.UV pulse 2.Chemo-luminescence 3.RPL Signal 4.Predose with long decay t [µs] 4 rel. Light Intensity ns t1t1 t2t2 Dose A(t 1 ) – f(A(t 2 )) UV-Pulse
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RADMON 15-Feb-078 RPL Components Nitrogen Laser –Spectra Physics VSL-337ND-S –Pulse energy: 300 µJ –Pulse duration: 4 ns X-Table –Zaber T-LLS 260 –Resolution: 0.16 µm –Repeatability: < 0.5 µm DAQ card –Acqiris DP308 –Resolution: 12 bit –Sample rate: 200 MS/s
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RADMON 15-Feb-079 Dosimeter holder 42 Samples Collimator Ø 0.7 +0.01 mm
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RADMON 15-Feb-0710 RPL control unit Fast amplifier (420MHz bandwidth) build at EIG Geneve Tailored to our needs
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RADMON 15-Feb-0711 RPL reader
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RADMON 15-Feb-0712 Control Software User friendly GUI Measurement instructions via Excel sheet The measured curves are stored automatically Tracing the efficiency of the System Automatically adjustment of the DAQ input range
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RADMON 15-Feb-0713 Control Software
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RADMON 15-Feb-0714 Conclusion The Reader is designed to be user friendly All components were chosen to guaranty high precision The dosimeter holder is produced in high accuracy and installed The control and analysis software is written
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RADMON 15-Feb-0715 Outlook Comprehensive tests are foreseen to ensure that the Reader is working stable The laser has to be exchanged, since the pulse energy stability does not comply with the specifications given by the company
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RADMON 15-Feb-0716 RPL dosimeter
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RADMON 15-Feb-0717 RPL dosimeter production Cooperation: The Laboratory for laser glass Shanghai Institute of Optical and Fine Mechanics Chinese Academy of Sciences Adjusting: –Melting Temperature and duration –Cooling time –Base components –Predose
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RADMON 15-Feb-0718 Predose
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RADMON 15-Feb-0719 Comparison of China w. Dos2
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RADMON 15-Feb-0720 Conclusion The present Chinese dosimeter are already acceptable for CERN... Nevertheless we push for further improvements
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RADMON 15-Feb-0721 Experiments –CERF 2003 –CERF 2004 –p + Calibration Curve (IRRAD1) –Radiation Source TT40 Beam dump –CNGS –CERF 2006
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RADMON 15-Feb-0722 CERF 2006
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RADMON 15-Feb-0723 IRRAD 1 24 GeV/c proton beam
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RADMON 15-Feb-0724 CERF 2004 (preliminary)
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RADMON 15-Feb-0725 CERF 2003 S1 S2 S3 S4 Al1 Al2 1.094078917861Al2_d 1.094087921958Al2_c 0.984087917862Al2_b 0.854085415724Al2_a 1.02712710130Al1 0.99276775RPL 4 0.9261834169RPL 3 0.9261825168RPL 2 1.041294.430.3RPL 1 Sim/ Meas Measure- ment measured Stat. Simulat -ion Simulation results give Gy in air Gy/pp
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RADMON 15-Feb-0726 Conclusion Various measurement campaigns in mixed high-energy radiation fields were performed in order to improve the knowledge of the HLD systems. Simulations were performed allowing a better understanding of the behavior of the HL dosimeters in mixed radiation fields Further analysis of the measurements and simulations are under way. Results and preliminary results look very promising. RPL and Alanine dosimeter are well suited for High Level Dosimetry at CERN.
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RADMON 15-Feb-0727 Thank you very much for you attention…
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RADMON 15-Feb-0728 PM response
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RADMON 15-Feb-0729 PT response
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RADMON 15-Feb-0730 TT40 450 GeV/c protons More than two hundred dosimeters (RPL and alanine) were installed on various positions on the dump (TED). Analysis of the read out results is ongoing. Preliminary simulations were performed. Accurate simulations will be performed in order to evaluate the various field components at the given detector positions. Measurements will be compared with simulations in order to improve the knowledge of the detector response in mixed fields.
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RADMON 15-Feb-0731 Photon Response
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RADMON 15-Feb-0732 LET response
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RADMON 15-Feb-0733 Neutron response
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