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JSC “Institute in Physical-Technical problems”

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1 JSC “Institute in Physical-Technical problems”
X-ray and gamma ray spectrometers based on cadmium telluride detectors JSC “Institute in Physical-Technical Problems” is a branch company, specializing in the design and manufacture of spectrometers, detection units, and separate nuclear-physics instruments based on semiconductor and scintillation materials! JSC “Institute in Physical-Technical problems” 141980, Dubna, Moscow region, Kurchatova str.4 Tel.: ; fax

2 For the diagnostics of physical processes in the nuclear-energetic installations of JSC IPTP a detection unit BDTK-1K with the cadmium telluride detector with the area of 47mm2 and thickness 1.1mm and with thermoelectric cooling of the head module has been developed. The measuring results of the prototype of BDTK-1K are given below. A digital signal processor (ЦСУ-B-1K) developed at JSC IPTP was used for the detection unit testing.

3 Advantages of the cadmium telluride detectors
High atomic number (Z=50) and high density which implies high efficiency in gamma radiation detection; Sufficiently large band gap width – 1.5 eV (that of silicon is 0.9 eV and of germanium is 0.67 eV) permitting to operate at room temperature with a low level of current noises; Energy resolution is much better than that of scintillation detectors which allows one to use them for applications where a resolution of separate adjacent lines is required;

4 Specifications of the BDTK-1K detection unit
Detected energy range – from 5.9 to keV Energy resolution : by energy 5.9 keV – 0.62 keV; by energy 59.6 keV – 0.93 keV; by energy keV – 1.5 keV; by energy keV – 6.4 keV. Optimum operating voltage of SCD until minus 400 V. Optimum current of the cooler – 0.7 A. Detection unit mass – 0.87 kg. Overall size – 166×106×85 mm.

5 Relative efficiency of the detection depending on radiation energy
Energy, keV counting reduced to output 100 % Fitting at Е > 100 keV count in peak output % 40.5 74 46.2 801830 14.8 122.08 543518 30.8 244.76 277519 285540 21480 7.74 344.14 106646 104137 29221 27.4 410.96 73673 61588 1665 2.26 443.66 53616 49099 1705 3.18 779.03 10469 9276 1340 12.8 964.43 7225 4931 1026 14.2 3750 3465 375 10 2338 3226 311 13.3 1058 1605 218 20.6 Starting from the energy Е>100 keV, the relative efficiency is well approximated by the following dependence: εотн= const / E-2.96

6 Resolution-energy dependence
Energy, keV Resolution, keV 40.55 1.375 46.2 1.599 122.08 1.679 244.76 2.703 344.14 3.551 410.96 4.522 443.66 4.678 779.03 7.025 964.43 8.748 8.824 6.401 8.852

7 Fe-55 and Am-241 spectra Граница шумов – 1,9 keV 5.89 keV 13.94 keV

8 Co-57 and Cs-137 spectra Shaping time – 6 µs
32 keV 37 keV 122 keV 662 keV Shaping time – 6 µs Lines 32 and 37 keV are K-alpha and K–beta series of the Ba-137 isotope generated at the Cs-137 decay.

9 Scintillation detectors
, нм I, отн.ед. Spectrum of radio-luminescence of the detectors Density, g/cm … ….1,05 Maximum of the luminescence spectrum, nm…420

10 Scintillation detectors
Designaiton Purpose T, ns ПС-Н1 Detection of fast neutrons ПС-Б2 Detection of fast neutrons and photon radiation with high time resolution высоким временным разрешением 0.78 ПС-Б3 same 1.0 ПС-Б4 0.67 СПС-С10 Detection of photon radiation due to photoeffect on lead atoms (up to 10% by mass) 1.70 ПС-У14 Detection of photon radiation using the automatic sensitivity control circuit

11 Summary Tellurid cadmium spectrometric systems are small in size and have a low power consumption. CdTe detection units are promising for use in portable instruments and stationary complexes of the technologic parameters control at nuclear power plants and allow one to substantially increase the operation characteristics in applied studies, radiography, and astrophysics. Detectors built with plastic scintillators have showed their advantage in radiation monitoring purposes.


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