Slobodan Jovanović
University of Montenegro
Network
Latest external collaboration on country level. Dive into details by clicking on the dots.
Publication
Featured researches published by Slobodan Jovanović.
Journal of Radioanalytical and Nuclear Chemistry | 1997
Slobodan Jovanović; Aleksandar Dlabac; Nikola N. Mihaljevic; P. Vukotić
AbstractA broadly applicable, flexible and user-friendly PC-code (ANGLE) for calculations of semiconductor detector full energy peak efficiencies (εp) is presented. The physical model behind is the concept of the effective solid angle
Journal of Radioanalytical and Nuclear Chemistry | 1997
P. Vukotić; Nikola N. Mihaljevic; Slobodan Jovanović; S. Dapčević; F. Boreli
Radiation Protection Dosimetry | 2012
Aleksandra Milatović; Olivera Ciraj-Bjelac; Sonja Ivanović; Slobodan Jovanović; Vesna Spasić-Jokić
\overline {(\Omega )}
journal of theoretical and applied physics | 2013
Ahmed M. El-Khatib; Mohamed S. Badawi; Mona M. Gouda; Slobodan Jovanović; Aleksandar Dlabac; Nikola N. Mihaljevic; Sherif S. Nafee; Ekram A. El-Mallah
AIP Advances | 2017
Mohamed S. Badawi; Slobodan Jovanović; Abouzeid A. Thabet; Ahmed M. El-Khatib; Aleksandar Dlabac; Bohaysa A. Salem; Mona M. Gouda; Nikola N. Mihaljevic; Kholud. S. Almugren; Mahmoud I. Abbas
. Written in Pascal, and operating in windows and menus data manipulation mode, ANGLE yields the efficiencies for: (1) HPGe true- and closed-end coaxial (bothn- andp-types), (2) Ge(Li) open- and closed-end, (3) planar LEPD and (4) well-type detectors. Supposing coaxial positioning, cylindrical or Marinelli sources can be treated, regardless of their dimensions (this includes point, disk and ring sources, bulky samples and infinite geometrics). Possible displacement between source and detector axes is treated in our another work, relative to this one. ANGLE input parameters are: (1) reference efficiency curve for the detector used (i.e., efficiency vs. γ-energy for calibrated point sources at a reference distance), (2) detector type and configuration (active body and inactive layers, end cap, windows, housing, shielding, (3) source data (dimension and composition of both container and active material), (4) source-detector geometry (distance, intercepting layers and their composition) and (5) some computational data (Gauss integration coefficients). Gamma-attenuation is calculated upon an extensive (per element and per energy) data file. In the output, efficiency vs. γ-energy is found, both in forms of tables and graphs. In routine applications accuracies of 3–4% are achieved (not worse than 7% for the most unfavourable geometries). Computation times when using recent PC models are of the order of minutes. ANGLE frame is also easily adjustable to other semiempirical or Monte Carlo models for efficiency calculations.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2010
Slobodan Jovanović; Aleksandar Dlabac; Nikola N. Mihaljevic
AbstractWe known activities of two large cylindrical γ-sources (a mixture of radionuclides in solution, and a geological sample) are measured using a semiempirical method for calculating photon detection efficiencies (εp) of Ge-detectors via effective solid angles
Nuclear Technology & Radiation Protection | 2013
Mohamed S. Badawi; Mohamed E. Krar; Ahmed M. El-Khatib; Slobodan Jovanović; Aleksandar Dlabac; Nikola N. Mihaljevic
Nuclear Technology & Radiation Protection | 2012
Nikola N. Mihaljevic; Aleksandar Dlabac; Slobodan Jovanović
\overline {(\Omega )}
Chinese Journal of Physics | 2016
Ahmed M. El-Khatib; Mohamed S. Badawi; Abouzeid A. Thabet; Slobodan Jovanović; Mona M. Gouda; Moustafa M. Mohamed; Aleksandar Dlabac; Mohamed Abd-Elzaher; Nikola N. Mihaljevic; Mahmoud I. Abbas
Archive of Oncology | 2008
Aleksandra Milatović; Sonja Ivanović; Vesna Spasić-Jokić; Slobodan Jovanović
, in order to analyse the feasibility and the accuracy of the method. It is applied here under conditions not favourable to the method itself, which are however quite common in practice: (1) HPGe detector supplied only with standard detector specification and performance data, and (2) large source just above the detector end-cap. The impact of the probable range of uncertainties in knowledge of the detector and source geometrical parameters on the calculated efficiencies is considered. The fact that the crystal of the detector used is not coaxial with the end-cap, discovered by making X-ray radiographs, is of a special concern with respect to the applicability of the method under such conditions. Therefore, the method for the calculations of Ω is extended to cases of parallel but not coincident axes of the cylindrical sources and detectors. True coincidence effects, which introduce typically 5% errors for the counting geometry used, are not dealt with.