Hani H Negm

Dr. Hani H Negm

orcid

Research Focus & Metrics

Academic Career Length

15Years (2012-Present)

(Calculated once Scilit publication data is synced: current year − year of first publication + 1)

Representative Publications

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2 February 2023 in Polymers for Advanced Technologies
Verified
Journal Article
Closed access
AAAli Atta
Ali Atta
Hani H NegmHani H Negm
Hani H Negm
EAE. Abdeltwab
E. Abdeltwab
MRMohamed Rabia
Mohamed Rabia
MAM. M. Abdelhamied
M. M. Abdelhamied

25 August 2024 in Radiation Physics and Chemistry
Verified
Journal Article
Closed access
Hani H NegmHani H Negm
Hani H Negm
EAElhassan A. Allam
Elhassan A. Allam
INIslam M. Nabil
Islam M. Nabil
EAEslam Abdeltwab
Eslam Abdeltwab
MMMassaud Mostafa
Massaud Mostafa
AEAtef El-Taher
Atef El-Taher

16 November 2023 in Radiation Physics and Chemistry
Verified
Journal Article
Closed access
Hani H NegmHani H Negm
Hani H Negm
EAElhassan A. Allam
Elhassan A. Allam
EAEslam Abdeltwab
Eslam Abdeltwab
MMMassaud Mostafa
Massaud Mostafa
MMMohamed E. Mahmoud
Mohamed E. Mahmoud
AEAtef El-Taher
Atef El-Taher

1 January 2019 in Journal of Radiation Research and Applied Sciences
Verified
Journal Article
Open access
HEHany El-Gamal
Hany El-Gamal
Hani H NegmHani H Negm
Hani H Negm
MHMohamed Hasabelnaby
Mohamed Hasabelnaby
Determination of the full-energy peak efficiency of a detection system is significant in the activity calculation of the measured radioactive samples. In this work, we present an experimental method to determine the absolute efficiency calibration of a NaI(Tl) detector, considering that a standard source of interest is unavailable and by using the known specific activity of a standard sample measured using a HPGe detector. The efficiency of a gamma-ray spectrometer that consists of a coaxial HPGe detector is calculated using Canberra ISOCS/LabSOCS software and a fabricated calibration source. To validate our method, environmental samples (rock and soil samples) were analyzed on both the detectors. The obtained activity concentrations were checked by means of the IAEA proficiency test procedure. The performance criteria evaluation results were found to be ‘Acceptable’ for all the analytical determinations of all the radionuclides under study, except for the samples with low activity (<15 Bq kg−1 and <10 Bq kg−1 for 226Ra and 232Th, respectively). The precision of the low-activity samples was not considered ‘Acceptable’ as the results were slightly inaccurate; in this case, the results were considered as ‘Warning’ because the relative bias (RB) was less than the maximum acceptable bias (MAB).

3 May 2024 in Journal of Electronic Materials
Verified
Journal Article
Closed access
PDF file
Hani H NegmHani H Negm
Hani H Negm
ASAsmaa A. Sdeek
Asmaa A. Sdeek
AEAhmed A. Ebrahim
Ahmed A. Ebrahim

17 April 2024 in Physica Scripta
Verified
Journal Article
Closed access
Hani H NegmHani H Negm
Hani H Negm
RERehab M El-Sharkawy
Rehab M El-Sharkawy
EAEslam Abdeltwab
Eslam Abdeltwab
MMMassaud Mostafa
Massaud Mostafa
MMMohamed E Mahmoud
Mohamed E Mahmoud
Atef El-TaherAtef El-Taher
Atef El-Taher
The study investigated new nanocomposites’ γ-ray and neutron shielding properties based on raw attapulgite, a clay matrix intercalated with different weight percentages of mixed nano metal oxides CdO and PbO. The various percentages were as follows: (100–2x)% Attapulgite + x%CdO + x%PbO, abbreviated as (AT100–2x CdxPb x ), where x = 5, 10, 15%. The nanocomposites were characterized using XRD, FTIR, and EDX, confirming their successful preparation. SEM images revealed that the mixed oxide nanoparticles were successfully intercalated into the layers of attapulgite clay, with an average particle size of approximately 31.46 nm. The bulk densities of the prepared nanocomposites were measured to be in the range of 2.034 to 2.555 g/cm3. GEANT4 simulations were employed to evaluate the nanocomposites’ γ-ray and neutron shielding performance in the photon energy range of 0.015 to 15 MeV. Phys-X code was used for verification. The simulation results showed a maximum difference of approximately 9.5% between GEANT4 and Phys-X predictions. To assess the γ-ray shielding performance, various shielding parameters were calculated at selected photon energies. The μ m values ranged from 4.589 to 0.020 cm2.g−1, 6.311 to 0.021 cm2.g−1, 8.350 to 0.022 cm2.g−1 and 10.804 to 0.023 cm2.g−1 for raw attapulgite, AT90Pb5Cd5, AT80Pb10Cd10, AT70Pb15Cd15 across the photon energy range. The AT70Pb15Cd15 nanocomposite exhibited the highest μ m , Z eff , Z eq , and the lowest T 1/2, T 1/10, and MFP values. Notably, it also demonstrated the highest FNRCS (approximately 0.1 cm−1). These findings suggest that clay-based nanocomposites represent a new class of low-cost, locally available advanced materials with potential applications in γ-ray and neutron shielding characteristics.