Youssef, S., N. M. Ali, and N. A. D. I. A. H. RAFAT, Improving the efficiency of kesterite solar cells using semi-ellipsoidal nanostructures, , vol. 6, pp. 100187, 2025. AbstractWebsite

The use of kesterite materials in photovoltaic solar cells holds great promise due to their abundance, non-toxic nature, cost-effectiveness, and excellent optoelectronic properties. However, the power conversion efficiency of kesterite solar cells remains considerably below the Shockley-Queisser limit efficiency. This underscores the need for continuous development of new cell designs to maximize kesterite's potential for solar energy conversion. In this study, we presented a novel design for a kesterite solar cell incorporating semi-ellipsoidal nanostructures into the active layer to overcome its limitations and achieve higher efficiencies. Comprehensive simulations were conducted to study the effect of these nanostructures on solar cell performance. An extensive parametric study was also performed to identify the design parameters for the best performance. The results revealed that the presence of nanostructures significantly enhances power conversion efficiency, reaching a remarkable 17.6%, overcoming many challenging obstacles facing kesterite solar cells and making them more competitive in the ever-expanding solar cell market.

Youssef, S., N.  M. Ali, and N.  H. Rafat, "Analytical Modeling of Solar Cells Having Short Lifetime Materials: Application to Kesterite Solar Cells", Progress in Photovoltaics: Research and ApplicationsProgress in Photovoltaics: Research and Applications, vol. 33, issue 8: John Wiley & Sons, Ltd, pp. 890 - 904, 2025. AbstractWebsite

ABSTRACT Solar cells fabricated from short-carrier lifetime materials face efficiency limitations because of high recombination rates, particularly within the depletion region. Kesterite solar cells offer a promising alternative to conventional solar cells but suffer from short-carrier lifetimes. This work introduces a comprehensive analytical model applicable to such solar cells. We developed a novel approach to accurately represent the recombination rates of the carriers within the depletion region using a Gaussian function. This model overcomes the limitations of existing approximations and enables more precise dark current calculations. Additionally, we employed a fully analytical generation rate calculation based on the transfer matrix method for accurate photocurrent determination. The effectiveness of this model was validated by comparing its results with simulated and experimental data for kesterite solar cells, demonstrating excellent agreement in dark current and photocurrent, with maximum percentage errors of 1.9% and 1.7%, respectively. Beyond accuracy, the model also achieved a 75-fold improvement in computation speed compared to finite element method simulations. This highlights the effectiveness of the model in capturing the complex recombination processes within kesterite solar cells and in providing a valuable tool for understanding and optimizing the performance of solar cells based on short-lifetime materials, particularly kesterite-based devices with one-sided junction characteristics.

Allam, M. A., T. A. Ali, and N. A. D. I. A. H. RAFAT, Mid-infrared supercontinuum generation for WDM applications using chalcogenide photonic crystal fiber, , vol. 57, issue 8, pp. 440, 2025. AbstractWebsite

In this study, the design and characterization of a photonic crystal fiber (PCF) as a light source for a mid-infrared supercontinuum generation (SCG) is presented. This PCF is based on a highly nonlinear chalcogenide $${\text{As}}_{40}{\text{Se}}_{60}$$background material with a hexagonal structure arrangement of air-holes rings. The PCF parameters such as the chromatic dispersion (D), the effective refractive index ($${n}_{eff}$$) and the nonlinear coefficient (γ) have been investigated. We study the stimulated SCG in two types of dispersion regimes: anomalous and all-normal dispersion (ANDi). We initiate the study by sending a 28.4 fs wide optical pulse with a peak power of 10 kW and a central wavelength of 2.8 µm through a 2 cm long PCF. In the anomalous dispersion, we demonstrate the generation of coherent and broadband SCG spectrum spanning the wavelength region from 1.6 to 7.8 µm. While, in the ANDi regime we demonstrate the generation of a broad, ultra-flat-top and highly coherent SCG spectrum extending from 2 to 4 µm at 6 dB spectral flatness. Thus, we achieve ultra-flat SCG spectrum source with a bandwidth as wide as 2400 nm within only 2 cm propagation length of the proposed PCF. This spectrum range is very suitable for variety of applications in mid-infrared region such as optical metrology, frequency comb generation, and optical coherence tomography (OCT). Results further demonstrate that with an applied pump power of 15 kW through the ANDi regime, a flat spectral bandwidth of 380 nm (wavelengths ranging from 1260 to 1640 nm) at just 3 dB spectral flatness is achieved. This band covers the five-telecommunication optical bands O-, E-, S-, C- and L-bands that comply with ITU-T-compliant wavelengths for wavelength division multiplexing (WDM) applications like coarse WDM (CWDM) and dense WDM (DWDM).

Youssef, S., N. M. Ali, and N. A. D. I. A. H. RAFAT, "{Enhancing the performance of lead halide perovskite solar cells and reducing its toxicity using nanostructures}", Journal of Photonics for Energy, vol. 14, no. 3: SPIE, pp. 034501, 2024. AbstractWebsite
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Allam, M. A., T. A. Ali, and N. A. D. I. A. H. RAFAT, Broadband dispersion compensation and high birefringence photonic crystal fiber for CWDM/DWDM networks, , vol. 56, issue 6, pp. 1023, 2024. AbstractWebsite

In this study, we propose a new design based on photonic crystal fibers (PCFs) for broadband dispersion compensation in telecommunication networks. The proposed design has a hexagonal structure arrangement of air-holes rings of different diameters between the silica core and the cladding. The PCF properties like effective area, nonlinearity, dispersion slope, confinement loss, and birefringence are reported and discussed. For the best performance we present three designs A, B and C. Simulation results show that the three designs cover the six-telecommunication optical bands O-, E-, S-, C-, L- and U- bands (wavelengths ranging from 1260 to 1675 nm). Design A achieves a large negative dispersion value of about − 1716 ps/(nm.km) with relative dispersion slope equals to that of conventional single-mode optical fibers (SMFs) of about 0.0036 nm−1, which makes it very suitable for long-haul DWDM transmission systems. With a little modification in the core, designs B and C achieve much higher confinement ability and achieve a very large birefringence value for polarization mode dispersion and sensing applications. Design C is engineered to have exact opposite dispersion of SMF with zero dispersion at the wavelength 1310 nm, which makes it a promising design in CWDM transmission system. The numerical values have been investigated using the full vector finite element method.

Kamal, S. M., T. A. Ali, and N. A. D. I. A. H. RAFAT, New designs of 4 × 2 photonic crystal encoders using ring resonators, , vol. 55, issue 3, pp. 261, 2023. AbstractWebsite

Optical encoders are pivotal elements in optical communication applications. There is much need for ultra-compact and high-speed novel designs. This work proposes two new designs of fast, compact 4 × 2 optical encoders using two dimensional photonic crystals. The proposed structures consist of square lattice silicon rods embedded in an air background. The operation of these encoders is based on the wave interference technique. The encoders are designed to help in achieving better performance through increasing the contrast ratio and decreasing the power loss and the return loss. The PWE method is used to analyze the photonic band gap. We used FDTD simulation to obtain the electric field distribution inside each structure and the normalized output power. We prove that the scattering rods improve the directivity of the light toward the desired paths and decrease the backward reflection. The proposed encoders have small footprint areas of 204.8 and 160.4 μm2 and operate at wavelength 1550 nm. They achieve low response time (254 and 163 fs) and high contrast ratio (6.69 and 12.9 dB). Simplicity and compactness of the designs make them suitable for optical signal processors and photonic integrated circuits. Another advantage of these designs is that low input power is enough for the encoders’ operation, because there is no non-linear materials included. Our designs compete with the published works in the last few years especially in their footprint and response time.

Ali, N. M., T. A. Ali, and N. A. D. I. A. H. RAFAT, "Modeling of Perovskite solar cells containing hexagonal-shaped nanorods", Optical and Quantum Electronics, vol. 54, no. 2: Springer, pp. 1–14, 2022. Abstract
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Mousa, M. A., N. A. D. I. A. H. RAFAT, and A. A. E. Saleh, "Toward spectrometerless instant Raman identification with tailored metasurfaces-powered guided-mode resonances (GMR) filters", Nanophotonics, vol. 10, no. 18: De Gruyter, pp. 4567–4577, 2021. Abstract
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AbdelAziz, H. H., T. A. Ali, and N. A. D. I. A. H. RAFAT, "Plasmonic sphere-cube nano dimer for silicon solar cells power absorbance enhancement", Optical and Quantum Electronics, vol. 53, no. 9: Springer, pp. 1–13, 2021. Abstract
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AbdelAziz, H. H., T. A. Ali, and N. A. D. I. A. H. RAFAT, "Plasmonic Yolk-Shell Nano Structures for Solar Cells Absorbance Enhancement", {IOP} Conference Series: Materials Science and Engineering, vol. 956: {IOP} Publishing, pp. 012018, oct, 2020. AbstractWebsite

In this research we study the enhancement in power absorbance of thin film silicon solar cells by plasmonic yolk-shell (YS) nano particles. Plasmonic YS nano particles are simulated on top/bottom position of thin film Si layers. We suggest different structures of YS and simulate the behaviour of such structures using a FDTD simulations. We calculate the limiting photocurrent taking into consideration the enhanced absorbance of the cell. The simulation results show multi-peaked and broad band power absorbance enhancement all over the solar spectrum. The power absorbance enhanced into solar cell by 64% over planar ultra-thin 300 nm Si cell.

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