Ahmed H. Hammad
Current Organizations / Institutes
The organizations/institutes from the scholar's latest article
Previous Organizations / Institutes
The organizations / institutes from the scholar's other articles in the past ten years
Research Subjects
Ahmed H. Hammad has a total of 73 co-authors. Here are the top co-authors by number of shared publications:
- Essam B. Moustafa
Converging Sciences and Emerging Technology (CoSET) Center, Benha National University (BNU), Al Obour 13518, Egypt
11 shared publications Essam Banoqitah
Nuclear Engineering Department, Faculty of Engineering, King Abdulaziz University, Jeddah, Saudi Arabia
6 shared publications- Mohamed Shaaban Abdel Wahab
Materials Science and Nanotechnology Department, Faculty of Postgraduate Studies for Advanced Sciences, Beni-Suef University, Beni-Suef, Egypt
4 shared publications Abdulsalam M. Alhawsawi
Nuclear Engineering Department, Faculty of Engineering, King Abdulaziz University, Jeddah, Saudi Arabia
3 shared publications- Asim Jilani
Clean Energy Technologies Research Institute (CETRI), Process Systems Engineering, Faculty of Engineering & Applied Science, University of Regina, 3737 Wascana Parkway, Regina, SK S4S 0A2, Canada
3 shared publications - Essam Banoqitah
Nuclear Engineering Department, Faculty of Engineering, King Abdulaziz University, 21589 Jeddah, Saudi Arabia
3 shared publications
Latest Publications
- 12 October 2026
- Published by Springer Nature in Optical and Quantum Electronics
- Vol. 58 (12) , 571
Correction: Modification of bismuth borate networks with lithium and molybdenum: effects on structure, optical, and nonlinear optical properties
- 12 October 2026
- Published by Springer Nature in Optical and Quantum Electronics
- Vol. 58 (12) , 571
Correction: Modification of bismuth borate networks with lithium and molybdenum: effects on structure, optical, and nonlinear optical properties
- 8 June 2026
- Published by Taylor & Francis in Phosphorus, Sulfur, and Silicon and the Related Elements
- Vol. 201 (9) , 1-10
Effects of borate substitution on the structural, optical, and physical properties of CuO-Doped sodium zinc phosphate glasses
The phosphate (P2O5) network is a typical glass-forming system, similar to silicate (SiO2), borate (B2O3), and germanate (GeO2) glasses. The phosphate network’s physical and chemical properties are...
- 8 June 2026
- Published by Taylor & Francis in Phosphorus, Sulfur, and Silicon and the Related Elements
- Vol. 201 (9) , 1-10
Effects of borate substitution on the structural, optical, and physical properties of CuO-Doped sodium zinc phosphate glasses
The phosphate (P2O5) network is a typical glass-forming system, similar to silicate (SiO2), borate (B2O3), and germanate (GeO2) glasses. The phosphate network’s physical and chemical properties are...
- 20 May 2026
- Published by Springer Nature in Applied Physics A
- Vol. 132 (6) , 520
Investigation of some structural and spectroscopic characteristics of inverted Alkali–bismuth fluoroborate glass containing holmium ions
- 20 May 2026
- Published by Springer Nature in Applied Physics A
- Vol. 132 (6) , 520
Investigation of some structural and spectroscopic characteristics of inverted Alkali–bismuth fluoroborate glass containing holmium ions
- 30 March 2026
- Published by Springer Nature in Optical and Quantum Electronics
- Vol. 58 (5) , 190
Modification of bismuth borate networks with lithium and molybdenum: effects on structure, optical, and nonlinear optical properties
- 30 March 2026
- Published by Springer Nature in Optical and Quantum Electronics
- Vol. 58 (5) , 190
Modification of bismuth borate networks with lithium and molybdenum: effects on structure, optical, and nonlinear optical properties
- 1 November 2025
- Published by The Electrochemical Society in ECS Journal of Solid State Science and Technology
- Vol. 14 (11) , 113002
Evaluation of Samarium – Doped Bismuth Cadmium Borate Glasses as Radiation Shielding Properties using Empirical Methods
The research has examined the structure, elasticity, and various radiation shielding properties of a bismuth cadmium borate glass system containing samarium ions using empirical methods. The glass density ( D glass ) was experimentally measured by Archimedes’ principles. When 4 mol% of samarium oxide (Sm 2 O 3 ) was introduced to the host glass, the density of the base (free Sm 2 O 3 ) sample dropped from 5.597 g cm −3 to 5.468 g cm −3 . The Makishima-Mackenzie (M–M) model was used to compute the elastic parameters, including Young’s ( E ), shear ( S ), and bulk ( B ) moduli. These parameters increased from 37.009 to 38.003 GPa, from 14.908 to 15.317 GPa, and from 23.827 to 24.410 GPa, respectively. Exposing the base sample to 8.04 keV yielded a mass attenuation coefficient ( MAC ) of 178.048 cm 2 g −1 . Adding 4 mol% Sm 2 O 3 to glass increased its MAC to 188.797 cm 2 g −1 . If the glass thickness is increased to 3 cm, the high radiation energy of 2.506 MeV can be reduced to half its value ( HVL ). The effective atomic number ( Z eff ) for the base sample at 19.63 keV was 77.957, decreasing to 27.071 at 661.7 keV. A similar trend was observed for all other glass samples. Such calculations reveal a promise in radiation shielding protection.
- 1 November 2025
- Published by The Electrochemical Society in ECS Journal of Solid State Science and Technology
- Vol. 14 (11) , 113002
Evaluation of Samarium – Doped Bismuth Cadmium Borate Glasses as Radiation Shielding Properties using Empirical Methods
The research has examined the structure, elasticity, and various radiation shielding properties of a bismuth cadmium borate glass system containing samarium ions using empirical methods. The glass density ( D glass ) was experimentally measured by Archimedes’ principles. When 4 mol% of samarium oxide (Sm 2 O 3 ) was introduced to the host glass, the density of the base (free Sm 2 O 3 ) sample dropped from 5.597 g cm −3 to 5.468 g cm −3 . The Makishima-Mackenzie (M–M) model was used to compute the elastic parameters, including Young’s ( E ), shear ( S ), and bulk ( B ) moduli. These parameters increased from 37.009 to 38.003 GPa, from 14.908 to 15.317 GPa, and from 23.827 to 24.410 GPa, respectively. Exposing the base sample to 8.04 keV yielded a mass attenuation coefficient ( MAC ) of 178.048 cm 2 g −1 . Adding 4 mol% Sm 2 O 3 to glass increased its MAC to 188.797 cm 2 g −1 . If the glass thickness is increased to 3 cm, the high radiation energy of 2.506 MeV can be reduced to half its value ( HVL ). The effective atomic number ( Z eff ) for the base sample at 19.63 keV was 77.957, decreasing to 27.071 at 661.7 keV. A similar trend was observed for all other glass samples. Such calculations reveal a promise in radiation shielding protection.
- 27 March 2025
- Published by IOP Publishing in Physica Scripta
- Vol. 100 (4) , 045956
Impact of TeO2 on the structure, optical, and photoluminescence characteristics of BaO–V2O5 –P2O5 vitreous materials
The objective of the current study is to assess the structural , optical filter property, and photoluminescence of a glass system primarily made of barium phosphate doped with vanadium pentoxide (V2O5), in which the structural units of phosphate (P2O5) are replaced by tellurium oxide (TeO2). The phosphate network consists of PO4 units in Q2 and Q3 modes, while TeO2 exists as trigonal pyramid TeO3 units. Density decreased from 3.263 to 3.046 g cm−3 with TeO2 addition up to 15%, then increased to 3.486 g cm−3 at 20% TeO2. Depending on the TeO2 concentration, the addition of TeO2 to the glass network produces a region with zero transmittance that extends from 672 nm to 998 nm. Furthermore, a cut-off wavelength in the visible and near-infrared (NIR) range was observed in every glass sample. The visible and near-infrared (NIR) cut-off wavelengths of the glass containing 5 mol% TeO2 are 510 nm and 998 nm, respectively. The cut-off wavelengths of the other samples were lower than those of the 5% TeO2 sample. The optical band gap rose from 2.08 to 2.166 eV as the TeO2 content increased from 5 to 20 mol%, while the refractive index dropped from 2.703 to 2.668, respectively. The color purity (CP%) of the glasses is enhanced by the intercalation of TeO2 into the barium phosphate network. The base sample presented a color purity of 19%, which increased to 71% and 82% with a TeO2 contribution of 5 and 10 mol%. However, the color purity decreased to 38% at 20 mol% of TeO2 due to the network former effect of TeO2.
- 27 March 2025
- Published by IOP Publishing in Physica Scripta
- Vol. 100 (4) , 045956
Impact of TeO2 on the structure, optical, and photoluminescence characteristics of BaO–V2O5 –P2O5 vitreous materials
The objective of the current study is to assess the structural , optical filter property, and photoluminescence of a glass system primarily made of barium phosphate doped with vanadium pentoxide (V2O5), in which the structural units of phosphate (P2O5) are replaced by tellurium oxide (TeO2). The phosphate network consists of PO4 units in Q2 and Q3 modes, while TeO2 exists as trigonal pyramid TeO3 units. Density decreased from 3.263 to 3.046 g cm−3 with TeO2 addition up to 15%, then increased to 3.486 g cm−3 at 20% TeO2. Depending on the TeO2 concentration, the addition of TeO2 to the glass network produces a region with zero transmittance that extends from 672 nm to 998 nm. Furthermore, a cut-off wavelength in the visible and near-infrared (NIR) range was observed in every glass sample. The visible and near-infrared (NIR) cut-off wavelengths of the glass containing 5 mol% TeO2 are 510 nm and 998 nm, respectively. The cut-off wavelengths of the other samples were lower than those of the 5% TeO2 sample. The optical band gap rose from 2.08 to 2.166 eV as the TeO2 content increased from 5 to 20 mol%, while the refractive index dropped from 2.703 to 2.668, respectively. The color purity (CP%) of the glasses is enhanced by the intercalation of TeO2 into the barium phosphate network. The base sample presented a color purity of 19%, which increased to 71% and 82% with a TeO2 contribution of 5 and 10 mol%. However, the color purity decreased to 38% at 20 mol% of TeO2 due to the network former effect of TeO2.
- 29 November 2024
- Published by Springer Nature in Applied Physics A
- Vol. 130 (12) , 1-12
Optical and spectroscopic properties of the novel BaO–Al2O3–P2O5: Sm2O3 glass system for orange-red light emission
- 29 November 2024
- Published by Springer Nature in Applied Physics A
- Vol. 130 (12) , 1-12
Optical and spectroscopic properties of the novel BaO–Al2O3–P2O5: Sm2O3 glass system for orange-red light emission
- Open Access
- 1 November 2024
- Published by The Electrochemical Society in ECS Journal of Solid State Science and Technology
- Vol. 13 (11) , 113016
Elastic and Radiation Shielding Properties of Cadmium and Lead-Incorporated Zinc Barium Phosphate Glass
Invert zinc-barium phosphate (ZnO–BaO–P2O5) glass networks were fabricated using the melt-annealing technique. The base glass was modified with cadmium oxide (CdO), lead oxide (PbO), and a mix between CdO and PbO. The elastic parameters were discussed using the Makishima-Mackenzie approach. The calculated values of Young’s (E), bulk (B), and shear (S) moduli decreased after the CdO, CdO+PbO, and PbO were introduced to the network from 53.704 to 52.019 GPa, 34.034 to 32.860 GPa, and 23.184 to 22.473 GPa, respectively. XCOM database was used to compute the mass attenuation coefficient (MAC) and estimate the radiation shielding properties of such glasses. For example, the MAC for the base sample at 0.06 MeV was 3.365 cm2/g, which rose to 3.554 cm2/g for the sample containing PbO. The mean free path (MFP), tenth value layer (TVL), and effective atomic number (Z eff ) were all discussed. The MFP values depend on the glass composition, which decreased from 0.091 cm (the base sample) to 0.082 cm (the glass with PbO) at 0.06 MeV. The phosphate glass, which contains PbO and CdO+PbO, is more suitable for radiation shielding applications.
- 1 November 2024
- Published by The Electrochemical Society in ECS Journal of Solid State Science and Technology
- Vol. 13 (11) , 113016
Open AccessElastic and Radiation Shielding Properties of Cadmium and Lead-Incorporated Zinc Barium Phosphate Glass
Invert zinc-barium phosphate (ZnO–BaO–P2O5) glass networks were fabricated using the melt-annealing technique. The base glass was modified with cadmium oxide (CdO), lead oxide (PbO), and a mix between CdO and PbO. The elastic parameters were discussed using the Makishima-Mackenzie approach. The calculated values of Young’s (E), bulk (B), and shear (S) moduli decreased after the CdO, CdO+PbO, and PbO were introduced to the network from 53.704 to 52.019 GPa, 34.034 to 32.860 GPa, and 23.184 to 22.473 GPa, respectively. XCOM database was used to compute the mass attenuation coefficient (MAC) and estimate the radiation shielding properties of such glasses. For example, the MAC for the base sample at 0.06 MeV was 3.365 cm2/g, which rose to 3.554 cm2/g for the sample containing PbO. The mean free path (MFP), tenth value layer (TVL), and effective atomic number (Z eff ) were all discussed. The MFP values depend on the glass composition, which decreased from 0.091 cm (the base sample) to 0.082 cm (the glass with PbO) at 0.06 MeV. The phosphate glass, which contains PbO and CdO+PbO, is more suitable for radiation shielding applications.
- 30 September 2024
- Published by Elsevier in Optical Materials
- Vol. 157
Utilizing bypass cement dust in the production of radiation shielding bismuth borate glass
- 30 September 2024
- Published by Elsevier in Optical Materials
- Vol. 157
Utilizing bypass cement dust in the production of radiation shielding bismuth borate glass