Pub Date : 2024-09-11DOI: 10.1007/s11082-024-07348-w
Abdelaziz M. Aboraia, Shoroog Alraddadi, M. Saad, Yasser.A. M. Ismail, E. R. Shaaban
We synthesized the pristine and MoS2 QDs coated the UiO-66 nanostructures employing an eco-friendly drop casting method and studied the physical properties of nanostructures by experimental methods. The X-ray diffraction analysis confirmed that all samples exhibit a singular cubic phase with space group Fm3m. The presence of MoS2 quantum dots coating led to an observed growth in crystalline size and an increase in structural defects. A rise in the optical energy gap (4.02–5.05 eV) and an improvement in transmittance were noted as the concentration of coated MoS2 quantum dots increased. The film thickness of UiO-66@X%MOS2 (X% = 0, 10, 15, 20, and 25) was around 140 ± 5 nm and the increase in the concentration of MoS2QDs was found to be inversely proportional to the decrease in refractive index. The absolute part values of the dielectric constant (ε1) are more significant than the imaginary part (ε2). Optical conductivity decreases with the higher content of embedded MoS2 QDs (from 2.75 × 1010 to 1.75 × 1010) at wavelengths 300–250 nm. Thus, MoS2 QDs-coated UiO-66 nanostructures show suitable potential applications in: optoelectronics, efficient conversion of energy, and numerous other works implemented in the sphere of nanotechnology.
{"title":"Revealing the structural and optical constant of the UiO-66 coated with MoS2 QDs","authors":"Abdelaziz M. Aboraia, Shoroog Alraddadi, M. Saad, Yasser.A. M. Ismail, E. R. Shaaban","doi":"10.1007/s11082-024-07348-w","DOIUrl":"https://doi.org/10.1007/s11082-024-07348-w","url":null,"abstract":"<p>We synthesized the pristine and MoS<sub>2</sub> QDs coated the UiO-66 nanostructures employing an eco-friendly drop casting method and studied the physical properties of nanostructures by experimental methods. The X-ray diffraction analysis confirmed that all samples exhibit a singular cubic phase with space group Fm3m. The presence of MoS<sub>2</sub> quantum dots coating led to an observed growth in crystalline size and an increase in structural defects. A rise in the optical energy gap (4.02–5.05 eV) and an improvement in transmittance were noted as the concentration of coated MoS<sub>2</sub> quantum dots increased. The film thickness of UiO-66@X%MOS<sub>2</sub> (X% = 0, 10, 15, 20, and 25) was around 140 ± 5 nm and the increase in the concentration of MoS<sub>2</sub>QDs was found to be inversely proportional to the decrease in refractive index. The absolute part values of the dielectric constant (ε<sub>1</sub>) are more significant than the imaginary part (ε<sub>2</sub>). Optical conductivity decreases with the higher content of embedded MoS<sub>2</sub> QDs (from 2.75 × 10<sup>10</sup> to 1.75 × 10<sup>10</sup>) at wavelengths 300–250 nm. Thus, MoS<sub>2</sub> QDs-coated UiO-66 nanostructures show suitable potential applications in: optoelectronics, efficient conversion of energy, and numerous other works implemented in the sphere of nanotechnology.</p>","PeriodicalId":720,"journal":{"name":"Optical and Quantum Electronics","volume":null,"pages":null},"PeriodicalIF":3.0,"publicationDate":"2024-09-11","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142201971","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-09-05DOI: 10.1007/s11082-024-07411-6
Mohammad Javad Maleki, Mohammad Soroosh, Gholamreza Akbarizadeh, Shanmuga Sundar Dhanabalan
In this research, a new photonic crystal structure for decoding operation with two inputs and four outputs is introduced. A square array of 28 × 45 silicon rods with a lattice constant of 485 nm has been used as the fundamental structure. Two input signals along with a bias signal reach the four output ports via nine waveguides. Four ring resonators are responsible for coupling light to the output ports. In each ring, a 4 × 4 array of nonlinear rods made of doped glass is used. Depending on the light intensity applied to the rings, one of the resonators couples the signal to one of the output ports. The use of ring resonators increases the coupling efficiency and enhances the light intensity at the output ports. As a result, the structure’s contrast ratio reaches 13.71 dB, and distinguishing between logic 0 and logic 1 for digital applications is well feasible. Calculation of the field components shows that its time response is 194 fs, faster than other structures. This attractive feature allows the designed decoder to be implemented in photonic circuits. Furthermore, the structure area is 296 µm2 which is smaller compared to ring-based 2-to-4 decoders. Based on the obtained results, it can be said that the presented structure performs better compared to other photonic crystal-based decoders.
{"title":"High-performance 2-to-4 decoder using nonlinear ring resonators in photonic crystal platform","authors":"Mohammad Javad Maleki, Mohammad Soroosh, Gholamreza Akbarizadeh, Shanmuga Sundar Dhanabalan","doi":"10.1007/s11082-024-07411-6","DOIUrl":"https://doi.org/10.1007/s11082-024-07411-6","url":null,"abstract":"<p>In this research, a new photonic crystal structure for decoding operation with two inputs and four outputs is introduced. A square array of 28 × 45 silicon rods with a lattice constant of 485 nm has been used as the fundamental structure. Two input signals along with a bias signal reach the four output ports via nine waveguides. Four ring resonators are responsible for coupling light to the output ports. In each ring, a 4 × 4 array of nonlinear rods made of doped glass is used. Depending on the light intensity applied to the rings, one of the resonators couples the signal to one of the output ports. The use of ring resonators increases the coupling efficiency and enhances the light intensity at the output ports. As a result, the structure’s contrast ratio reaches 13.71 dB, and distinguishing between logic 0 and logic 1 for digital applications is well feasible. Calculation of the field components shows that its time response is 194 fs, faster than other structures. This attractive feature allows the designed decoder to be implemented in photonic circuits. Furthermore, the structure area is 296 µm<sup>2</sup> which is smaller compared to ring-based 2-to-4 decoders. Based on the obtained results, it can be said that the presented structure performs better compared to other photonic crystal-based decoders.</p>","PeriodicalId":720,"journal":{"name":"Optical and Quantum Electronics","volume":null,"pages":null},"PeriodicalIF":3.0,"publicationDate":"2024-09-05","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142202013","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-09-05DOI: 10.1007/s11082-024-07382-8
R. A. Almotiri, A. F. Qasrawi, Lara O. Abu Samen
Cadmium sulfide thin films are deposited using the thermal evaporation technique and coated with 50 nm thick Sb nanosheets. Both the coated and uncoated films undergo structural, morphological, and optical investigations to explore potential modifications resulting from the Sb coating. The antimony nanosheets successfully increase the crystallite sizes from 28 to 34 nm and decrease the defect concentration from 4.36 × 1011 lines/cm2 to 3.02 × 1011 lines/cm2. The deposition of Sb nanosheets on CdS films induces the formation of nanowires with a length of 3.0 μm. Sb nanosheet coatings improve visible light absorption by more than nine times, redshift the energy band gap, suppress free carrier absorption in the infrared (IR) range, and increase the optical conductivity of CdS films. Additionally, as optical filters and waveguides, Sb-coated CdS films exhibit a terahertz cutoff frequency range of 0.47–32.06 THz as light energy increases from the IR to ultraviolet ranges. It is also observed that Sb coating alters the third-order nonlinear susceptibility of CdS, making it tunable, more polarizable, and suitable for nonlinear optical applications. Photocurrent measurements showed that Sb nanosheets improved the light responsivity by 330% and significantly enhanced the response time. The enhanced features of CdS achieved through Sb nanosheet coatings position CdS in the preferred group for nonlinear optical waveguides applicable in terahertz and nonlinear optical applications.
{"title":"Enhanced electro-optical properties of CdS thin films through Sb nanosheets coating","authors":"R. A. Almotiri, A. F. Qasrawi, Lara O. Abu Samen","doi":"10.1007/s11082-024-07382-8","DOIUrl":"https://doi.org/10.1007/s11082-024-07382-8","url":null,"abstract":"<p>Cadmium sulfide thin films are deposited using the thermal evaporation technique and coated with 50 nm thick Sb nanosheets. Both the coated and uncoated films undergo structural, morphological, and optical investigations to explore potential modifications resulting from the Sb coating. The antimony nanosheets successfully increase the crystallite sizes from 28 to 34 nm and decrease the defect concentration from 4.36 × 10<sup>11</sup> lines/cm<sup>2</sup> to 3.02 × 10<sup>11</sup> lines/cm<sup>2</sup>. The deposition of Sb nanosheets on CdS films induces the formation of nanowires with a length of 3.0 μm. Sb nanosheet coatings improve visible light absorption by more than nine times, redshift the energy band gap, suppress free carrier absorption in the infrared (IR) range, and increase the optical conductivity of CdS films. Additionally, as optical filters and waveguide<b>s</b>, Sb-coated CdS films exhibit a terahertz cutoff frequency range of 0.47–32.06 THz as light energy increases from the IR to ultraviolet ranges. It is also observed that Sb coating alters the third-order nonlinear susceptibility of CdS, making it tunable, more polarizable, and suitable for nonlinear optical applications. Photocurrent measurements showed that Sb nanosheets improved the light responsivity by 330% and significantly enhanced the response time. The enhanced features of CdS achieved through Sb nanosheet coatings position CdS in the preferred group for nonlinear optical waveguides applicable in terahertz and nonlinear optical applications.</p>","PeriodicalId":720,"journal":{"name":"Optical and Quantum Electronics","volume":null,"pages":null},"PeriodicalIF":3.0,"publicationDate":"2024-09-05","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142202006","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-09-05DOI: 10.1007/s11082-024-07412-5
A. V. Tsukanov
The paper considers an algorithm for entangling the states of an exciton qubit on a single quantum dot and a charge qubit on a double quantum dot. The possibility of performing a conditional two-qubit CNOT operation using laser transitions and the Förster effect is analyzed. Estimates of the system parameters are given for which this operation is implemented with a probability close to unity.
{"title":"Resonant Coulomb interaction of excitonic and charge qubits on quantum dots","authors":"A. V. Tsukanov","doi":"10.1007/s11082-024-07412-5","DOIUrl":"https://doi.org/10.1007/s11082-024-07412-5","url":null,"abstract":"<p>The paper considers an algorithm for entangling the states of an exciton qubit on a single quantum dot and a charge qubit on a double quantum dot. The possibility of performing a conditional two-qubit CNOT operation using laser transitions and the Förster effect is analyzed. Estimates of the system parameters are given for which this operation is implemented with a probability close to unity.</p>","PeriodicalId":720,"journal":{"name":"Optical and Quantum Electronics","volume":null,"pages":null},"PeriodicalIF":3.0,"publicationDate":"2024-09-05","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142202010","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-09-05DOI: 10.1007/s11082-024-07324-4
Abdullah Baz, Jacob Wekalao, Shobhit K. Patel
This study presents a terahertz (THz) resonance gas sensor design incorporating graphene, black phosphorus, and MXene materials in a metasurface structure. The sensor leverages the unique properties of these advanced two-dimensional materials to achieve enhanced sensitivity and versatility in gas detection applications. The proposed design consists of elliptical and square-shaped resonators arranged on a SiO2 substrate with a ground plane back reflector. Comprehensive simulations using COMSOL Multiphysics were conducted to analyze the sensor’s performance across various structural parameters and operating conditions. The sensor demonstrates a maximum sensitivity of 400 GHzRIU−1 and a figure of merit up to 0.816 RIU−1 within a refractive index range of 1–1.07 RIU. Electric field distribution analysis validates the sensor’s transmittance response at different frequencies. Notably, the design shows potential for 2-bit encoding applications based on transmittance characteristics under varying graphene chemical potential values. Compared to existing studies, the senso’s performance is particularly better in terms of sensitivity, offering advantages such as room temperature operation and fast response times. This research contributes to the advancement of THz sensing technology and opens new possibilities for highly sensitive and versatile gas detection in various applications.
{"title":"A novel design of THz resonance gas sensor with advanced 2-bit encoding capabilities","authors":"Abdullah Baz, Jacob Wekalao, Shobhit K. Patel","doi":"10.1007/s11082-024-07324-4","DOIUrl":"https://doi.org/10.1007/s11082-024-07324-4","url":null,"abstract":"<p>This study presents a terahertz (THz) resonance gas sensor design incorporating graphene, black phosphorus, and MXene materials in a metasurface structure. The sensor leverages the unique properties of these advanced two-dimensional materials to achieve enhanced sensitivity and versatility in gas detection applications. The proposed design consists of elliptical and square-shaped resonators arranged on a SiO<sub>2</sub> substrate with a ground plane back reflector. Comprehensive simulations using COMSOL Multiphysics were conducted to analyze the sensor’s performance across various structural parameters and operating conditions. The sensor demonstrates a maximum sensitivity of 400 GHzRIU<sup>−1</sup> and a figure of merit up to 0.816 RIU<sup>−1</sup> within a refractive index range of 1–1.07 RIU. Electric field distribution analysis validates the sensor’s transmittance response at different frequencies. Notably, the design shows potential for 2-bit encoding applications based on transmittance characteristics under varying graphene chemical potential values. Compared to existing studies, the senso’s performance is particularly better in terms of sensitivity, offering advantages such as room temperature operation and fast response times. This research contributes to the advancement of THz sensing technology and opens new possibilities for highly sensitive and versatile gas detection in various applications.</p>","PeriodicalId":720,"journal":{"name":"Optical and Quantum Electronics","volume":null,"pages":null},"PeriodicalIF":3.0,"publicationDate":"2024-09-05","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142225895","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-09-05DOI: 10.1007/s11082-024-07399-z
Muhammad Usman, An Wu, Nazia Bibi, Sara Rehman, Muhammad Awais Rehman, Shakeel Ahmad, Hafeez Ur Rehman, Muhammad Umair Ashraf, Zia ur Rehman, Mohammad Altaf
Our investigation focused on an in-depth examination of the physical properties of KZnH3 and NaZnH3, with lattice parameters of 4.04 and 3.72 Å, respectively. Both compounds exist stably in a cubic structure and exhibit metallic behavior with no band gap. At the Fermi level, the total and partial densities of states exhibit a significant conductivity, confirming the metallic behavior. These materials have brittle and anisotropic properties. Because of their greater bulk modulus, average shear modulus, and Young’s modulus, NaZnH3 appears harder compared to KZnH3. Optical properties indicate significant absorption and optical conductivity in the energy spectrum of 6–9 eV. NaZnH3 has a greater static refractive index and reflectivity as compared to KZnH3. The research on hydrogen storage suggests that both of these materials can store hydrogen, however, NaZnH3 is a more promising candidate due to its higher hydrogen storage capability.
{"title":"Hydrogen storage application of Zn-based hydride-perovskites: a computational insight","authors":"Muhammad Usman, An Wu, Nazia Bibi, Sara Rehman, Muhammad Awais Rehman, Shakeel Ahmad, Hafeez Ur Rehman, Muhammad Umair Ashraf, Zia ur Rehman, Mohammad Altaf","doi":"10.1007/s11082-024-07399-z","DOIUrl":"https://doi.org/10.1007/s11082-024-07399-z","url":null,"abstract":"<p>Our investigation focused on an in-depth examination of the physical properties of KZnH<sub>3</sub> and NaZnH<sub>3</sub>, with lattice parameters of 4.04 and 3.72 Å, respectively. Both compounds exist stably in a cubic structure and exhibit metallic behavior with no band gap. At the Fermi level, the total and partial densities of states exhibit a significant conductivity, confirming the metallic behavior. These materials have brittle and anisotropic properties. Because of their greater bulk modulus, average shear modulus, and Young’s modulus, NaZnH<sub>3</sub> appears harder compared to KZnH<sub>3</sub>. Optical properties indicate significant absorption and optical conductivity in the energy spectrum of 6–9 eV. NaZnH<sub>3</sub> has a greater static refractive index and reflectivity as compared to KZnH<sub>3</sub>. The research on hydrogen storage suggests that both of these materials can store hydrogen, however, NaZnH<sub>3</sub> is a more promising candidate due to its higher hydrogen storage capability.</p>","PeriodicalId":720,"journal":{"name":"Optical and Quantum Electronics","volume":null,"pages":null},"PeriodicalIF":3.0,"publicationDate":"2024-09-05","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142202052","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
In this paper, carrier reservoir semiconductor optical amplifiers (CR-SOAs) are utilized for the first time in designing an all-optical 2 × 1 multiplexer with enable function, operating at 120 Gb/s. Traditional SOAs face challenges with slow carrier recovery, restricting their application in high-speed scenarios. CR-SOA, with a carrier reservoir near the active region, replenishes carriers quickly, enabling faster gain and phase recovery. For the first time, a 2 × 1 multiplexer with an enable input is proposed, adding flexibility and control for dynamic data routing in optical systems. Basic gates such as AND, OR, and NOT gates have been designed using this multiplexer, with the enable input enhancing their versatility. The performance of the multiplexer and gates is evaluated using metrics like quality factor, extinction ratio, contrast ratio, and eye opening factor. The quality factor is analyzed concerning parameters such as amplified spontaneous emission, data rate, carrier transition time, and injection current. Simulation results confirm the functionality of the 2 × 1 multiplexer and logic gates, demonstrating satisfactory performance at high data rates.
{"title":"Design and analysis of carrier reservoir SOA based 2 × 1 MUX with enable input and implementing basic logic gates using MUX at 120 Gb/s","authors":"Vipul Agarwal, Prakash Pareek, Sumit Gupta, Lokendra Singh, Bukya Balaji, Pratap Kumar Dakua","doi":"10.1007/s11082-024-07351-1","DOIUrl":"https://doi.org/10.1007/s11082-024-07351-1","url":null,"abstract":"<p>In this paper, carrier reservoir semiconductor optical amplifiers (CR-SOAs) are utilized for the first time in designing an all-optical 2 × 1 multiplexer with enable function, operating at 120 Gb/s. Traditional SOAs face challenges with slow carrier recovery, restricting their application in high-speed scenarios. CR-SOA, with a carrier reservoir near the active region, replenishes carriers quickly, enabling faster gain and phase recovery. For the first time, a 2 × 1 multiplexer with an enable input is proposed, adding flexibility and control for dynamic data routing in optical systems. Basic gates such as AND, OR, and NOT gates have been designed using this multiplexer, with the enable input enhancing their versatility. The performance of the multiplexer and gates is evaluated using metrics like quality factor, extinction ratio, contrast ratio, and eye opening factor. The quality factor is analyzed concerning parameters such as amplified spontaneous emission, data rate, carrier transition time, and injection current. Simulation results confirm the functionality of the 2 × 1 multiplexer and logic gates, demonstrating satisfactory performance at high data rates.</p>","PeriodicalId":720,"journal":{"name":"Optical and Quantum Electronics","volume":null,"pages":null},"PeriodicalIF":3.0,"publicationDate":"2024-09-05","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142202011","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-09-05DOI: 10.1007/s11082-024-06800-1
Wael W. Mohammed, Naveed Iqbal, S. Bourazza, Elsayed M. Elsayed
In this paper, the fractional Chiral nonlinear Schrödinger equation with time-dependent coefficients (FCNSE-TDCs) is considered. The mapping method is applied in order to get hyperbolic, elliptic, trigonometric and rational fractional solution. These solutions are vital for understanding some fundamentally complicated phenomena. The obtained solutions will be very helpful for applications such as optics, plasma physics and nonlinear quantum mechanics. Finally, the influence of the time-dependent coefficients and the conformable fractional derivative order on the exact solutions of the FCNSE-TDCs is presented.
{"title":"The optical structures for the fractional chiral nonlinear Schrödinger equation with time-dependent coefficients","authors":"Wael W. Mohammed, Naveed Iqbal, S. Bourazza, Elsayed M. Elsayed","doi":"10.1007/s11082-024-06800-1","DOIUrl":"https://doi.org/10.1007/s11082-024-06800-1","url":null,"abstract":"<p>In this paper, the fractional Chiral nonlinear Schrödinger equation with time-dependent coefficients (FCNSE-TDCs) is considered. The mapping method is applied in order to get hyperbolic, elliptic, trigonometric and rational fractional solution. These solutions are vital for understanding some fundamentally complicated phenomena. The obtained solutions will be very helpful for applications such as optics, plasma physics and nonlinear quantum mechanics. Finally, the influence of the time-dependent coefficients and the conformable fractional derivative order on the exact solutions of the FCNSE-TDCs is presented.</p>","PeriodicalId":720,"journal":{"name":"Optical and Quantum Electronics","volume":null,"pages":null},"PeriodicalIF":3.0,"publicationDate":"2024-09-05","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142202007","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-09-05DOI: 10.1007/s11082-024-07378-4
A. A. A. Ebrahim, F. Saad, A. Belafhal
Based on the extended Huygens–Fresnel diffraction integral, the analytical expressions for a finite Airy-Hermite-Hollow Gaussian Beam (FAHHGB) propagating through a gradient-index medium (GRINM) are developed. The characteristics of the normalized intensity for the FAHHGB through the GRINM are theoretically and numerically investigated. The effects of gradient-index parameter β, the mode-orders (beam order (m) and hollow term order (n)), and the Gaussian waist ({omega }_{0}) on the propagation process of the studied beam are numerically discussed in detail. It is found that the normalized intensity distribution of FAHHGB undergo periodic changes during its propagation process in the GRINM. The periodical traits of the normalized intensity distribution of the FAHHGB in a GRINM are strongly affected by the gradient-index parameter. However, the changing of the beam parameters ((m) and (n)) play a clear role in geometrical form of the beam profile in the medium. Finally, the current study included three types of finite Airy Gaussian modes as special cases.
{"title":"Periodic characteristics of a finite Airy-Hermite-Hollow Gaussian beam propagating in a gradient-index medium","authors":"A. A. A. Ebrahim, F. Saad, A. Belafhal","doi":"10.1007/s11082-024-07378-4","DOIUrl":"https://doi.org/10.1007/s11082-024-07378-4","url":null,"abstract":"<p>Based on the extended Huygens–Fresnel diffraction integral, the analytical expressions for a finite Airy-Hermite-Hollow Gaussian Beam (FAHHGB) propagating through a gradient-index medium (GRINM) are developed. The characteristics of the normalized intensity for the FAHHGB through the GRINM are theoretically and numerically investigated. The effects of gradient-index parameter β, the mode-orders (beam order <span>(m)</span> and hollow term order <span>(n)</span>), and the Gaussian waist <span>({omega }_{0})</span> on the propagation process of the studied beam are numerically discussed in detail. It is found that the normalized intensity distribution of FAHHGB undergo periodic changes during its propagation process in the GRINM. The periodical traits of the normalized intensity distribution of the FAHHGB in a GRINM are strongly affected by the gradient-index parameter. However, the changing of the beam parameters (<span>(m)</span> and <span>(n)</span>) play a clear role in geometrical form of the beam profile in the medium. Finally, the current study included three types of finite Airy Gaussian modes as special cases.</p>","PeriodicalId":720,"journal":{"name":"Optical and Quantum Electronics","volume":null,"pages":null},"PeriodicalIF":3.0,"publicationDate":"2024-09-05","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142202009","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-09-05DOI: 10.1007/s11082-024-07225-6
Kiarash Madmeli, Arash Madmeli, Jabbar Ganji
The objective of the present study was to utilize the two-dimensional (2D) structures of silicone (known as silicene) in the structure of solar cells. Its spectacular optical and electronic properties justify its application in solar structures. For this purpose, silicene was involved in the solar cell structure in 3 manners: as silicene1, an n-type semiconductor layer doped with P impurity; silicene2, a p-type semiconductor layer doped with Al; and as the free-standing silicene for the front contact. The former two applications were conducted in the ITO/silicene (1, 2)/(textrm{MoS}_2) (n)/a-SiGe: H (i)/c-Si (P)/Au structure, while the latter was in the Silicene/(textrm{MoS}_2) (n)/a-SiGe: H (i)/c-Si (P)/Au structure. Using the AFORS-HET software, the solar cells were exposed to AM1.5 spectrum radiation at 300 K temperature, and the impacts of 1 sun, 0.1 sun, and 10 sun illumination intensities were evaluated to obtain a better insight into the function of this 2D structure. The highest efficiencies in the mentioned illumination intensities were observed in the proposed cell with the silicene1 layer as the semiconductor, which were 18.96, 17.96, and 19.22%, respectively. Moreover, the efficiencies of the cell with free-standing silicene as the front contact were 27.13, 25.95, and 27.65%, respectively, in the mentioned illumination intensities.
本研究的目的是在太阳能电池结构中利用硅(又称硅烯)的二维(2D)结构。硅具有出色的光学和电子特性,这为其在太阳能结构中的应用提供了理由。为此,我们以三种方式将硅参与到太阳能电池结构中:硅1,掺杂 P 杂质的 n 型半导体层;硅2,掺杂 Al 的 p 型半导体层;以及作为前触点的独立硅。前两种应用是在 ITO/硅烯 (1, 2)/(textrm{MoS}_2) (n)/a-SiGe:H(i)/c-Si(P)/Au结构,而后者是在硅/(textrm{MoS}_2) (n)/a-SiGe.H(i)/c-Si(P)/Au结构中进行的:H (i)/c-Si (P)/Au 结构。利用 AFORS-HET 软件,在 300 K 温度下将太阳能电池暴露在 AM1.5 光谱辐射下,评估了 1 个太阳、0.1 个太阳和 10 个太阳光照强度的影响,以便更好地了解这种二维结构的功能。在上述光照强度下,以硅烯1层为半导体的电池效率最高,分别为18.96%、17.96%和19.22%。此外,以独立硅烯作为前触点的电池在上述照明强度下的效率分别为 27.13%、25.95% 和 27.65%。
{"title":"Simulation of a-SiGe/c-Si solar cell with silicene front contact","authors":"Kiarash Madmeli, Arash Madmeli, Jabbar Ganji","doi":"10.1007/s11082-024-07225-6","DOIUrl":"https://doi.org/10.1007/s11082-024-07225-6","url":null,"abstract":"<p>The objective of the present study was to utilize the two-dimensional (2D) structures of silicone (known as silicene) in the structure of solar cells. Its spectacular optical and electronic properties justify its application in solar structures. For this purpose, silicene was involved in the solar cell structure in 3 manners: as silicene1, an n-type semiconductor layer doped with P impurity; silicene2, a p-type semiconductor layer doped with Al; and as the free-standing silicene for the front contact. The former two applications were conducted in the ITO/silicene (1, 2)/<span>(textrm{MoS}_2)</span> (n)/a-SiGe: H (i)/c-Si (P)/Au structure, while the latter was in the Silicene/<span>(textrm{MoS}_2)</span> (n)/a-SiGe: H (i)/c-Si (P)/Au structure. Using the AFORS-HET software, the solar cells were exposed to AM1.5 spectrum radiation at 300 K temperature, and the impacts of 1 sun, 0.1 sun, and 10 sun illumination intensities were evaluated to obtain a better insight into the function of this 2D structure. The highest efficiencies in the mentioned illumination intensities were observed in the proposed cell with the silicene1 layer as the semiconductor, which were 18.96, 17.96, and 19.22%, respectively. Moreover, the efficiencies of the cell with free-standing silicene as the front contact were 27.13, 25.95, and 27.65%, respectively, in the mentioned illumination intensities.</p>","PeriodicalId":720,"journal":{"name":"Optical and Quantum Electronics","volume":null,"pages":null},"PeriodicalIF":3.0,"publicationDate":"2024-09-05","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142202019","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}