Laser interaction with matter is one of the fundamental fields of the thermophysics.
The problem of heating an isolated finite homogenous silver sulphide slab induced by a laser pulse is studied. Indeed pulsed laser are used in a variety of material processing applications.
The aim of the study is to evaluate quantitatively the thermal effects induced in the irradiated target. The output results will have essential importance in the field of technological applications.
In the present trial, the parabolic heat conduction equation is solved using Laplace integral transform technique which is one of the powerful methods in the field of mathematical physics. An express for the temperature field within the target is obtained.
The functional dependence of the temperature on the parameters of the laser pulse is clarified.
The computations makes it possible to evaluate the critical time required to initiate damage at the front surface, which is a starting point for medical, military, industrial applications.
An illustrative example on silver sulfide slab is given.
{"title":"Analytical modeling of heating effects induced in a finite silver sulfide (Ag2S) slab by a time dependent laser pulse using Laplace integral transform technique","authors":"M.K. El-Adawi, S.A. Shalaby, S.S. Mostafa, S.A. Antar","doi":"10.1016/j.ijleo.2025.172601","DOIUrl":"10.1016/j.ijleo.2025.172601","url":null,"abstract":"<div><div>Laser interaction with matter is one of the fundamental fields of the thermophysics.</div><div>The problem of heating an isolated finite homogenous silver sulphide <span><math><mrow><mfenced><mrow><mspace></mspace><mi>A</mi><msub><mrow><mi>g</mi></mrow><mrow><mn>2</mn></mrow></msub><mi>S</mi></mrow></mfenced></mrow></math></span> slab induced by a laser pulse is studied. Indeed pulsed laser are used in a variety of material processing applications.</div><div>The aim of the study is to evaluate quantitatively the thermal effects induced in the irradiated target. The output results will have essential importance in the field of technological applications.</div><div>In the present trial, the parabolic heat conduction equation is solved using Laplace integral transform technique which is one of the powerful methods in the field of mathematical physics. An express for the temperature field within the target is obtained.</div><div>The functional dependence of the temperature on the parameters of the laser pulse is clarified.</div><div>The computations makes it possible to evaluate the critical time required to initiate damage at the front surface, which is a starting point for medical, military, industrial applications.</div><div>An illustrative example on silver sulfide slab is given.</div></div>","PeriodicalId":19513,"journal":{"name":"Optik","volume":"346 ","pages":"Article 172601"},"PeriodicalIF":3.1,"publicationDate":"2025-11-20","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145584383","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2025-11-20DOI: 10.1016/j.ijleo.2025.172611
Wende Dong , Tianheng Xu , Muhan Ji , Gang Luo , Geng Li , Zhenzhen Zheng
In hazy weather, suspended particles in the air cause significant image degradation by attenuating and scattering light. This degradation poses substantial challenges to subsequent image processing tasks, such as target recognition and positioning. Existing methods often struggle to balance global atmospheric light estimation with fine-detail preservation, leading to residual haze or over-enhancement and color distortion. Inspired by attention mechanisms, we design a hazy image restoration architecture utilizing an improved U-Net based generative adversarial network (GAN), enhanced by a novel hybrid attention mechanism. This mechanism integrates a global attention modulator, a window-based multi-head self-attention module, and a locally enhanced feedforward network, enabling the model to effectively capture both global and local image features while mitigating the artifacts seen in prior work. The network is trained using a tailored loss function that combines pixel loss, adversarial loss, and edge loss, specifically designed for the image dehazing task. Extensive experiments conducted on synthetic and real hazy images demonstrate that the proposed method consistently delivers high-quality dehazed images with exceptional clarity and contrast, outperforming several state-of-the-art methods.
{"title":"Hybrid self-attention aided generative adversarial network for hazy image restoration","authors":"Wende Dong , Tianheng Xu , Muhan Ji , Gang Luo , Geng Li , Zhenzhen Zheng","doi":"10.1016/j.ijleo.2025.172611","DOIUrl":"10.1016/j.ijleo.2025.172611","url":null,"abstract":"<div><div>In hazy weather, suspended particles in the air cause significant image degradation by attenuating and scattering light. This degradation poses substantial challenges to subsequent image processing tasks, such as target recognition and positioning. Existing methods often struggle to balance global atmospheric light estimation with fine-detail preservation, leading to residual haze or over-enhancement and color distortion. Inspired by attention mechanisms, we design a hazy image restoration architecture utilizing an improved U-Net based generative adversarial network (GAN), enhanced by a novel hybrid attention mechanism. This mechanism integrates a global attention modulator, a window-based multi-head self-attention module, and a locally enhanced feedforward network, enabling the model to effectively capture both global and local image features while mitigating the artifacts seen in prior work. The network is trained using a tailored loss function that combines pixel loss, adversarial loss, and edge loss, specifically designed for the image dehazing task. Extensive experiments conducted on synthetic and real hazy images demonstrate that the proposed method consistently delivers high-quality dehazed images with exceptional clarity and contrast, outperforming several state-of-the-art methods.</div></div>","PeriodicalId":19513,"journal":{"name":"Optik","volume":"345 ","pages":"Article 172611"},"PeriodicalIF":3.1,"publicationDate":"2025-11-20","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145570774","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2025-11-20DOI: 10.1016/j.ijleo.2025.172609
Yongkang Yang , Baiang Qu , Hongjie Xu , Manqing Tan , Wentao Guo
The amplified spontaneous emission (ASE) source is widely used in fiber-optic gyroscopes due to its broadband spectrum, which suppresses backscattering- and Kerr-effect–induced phase errors while reducing polarization coupling noise. However, thermally induced wavelength drift remains a critical limitation in ultrahigh-precision systems, as even small spectral shifts introduce non-negligible phase noise. To address this challenge, we propose a wide-temperature wavelength-selective reflection strategy that integrates a wavelength-division multiplexer, optical filter, and reflector into a compact hybrid structure, achieving a mean drift rate below 0.1 ppm/°C across the full operational range. This work presents a significant advance in ASE source technology through the integration of dual fiber Bragg gratings (FBGs) at the 974 nm laser diode (LD) output and a monolithically packaged passive-component module. Comprehensive theoretical modeling and experimental characterization of LD–ASE spectral–power correlations enabled the development of a thermally optimized dual-pass architecture achieving three major performance breakthroughs: (1) ultra-stable wavelength performance with drift below 0.1 ppm/°C over –25°C to + 60°C, (2) ASE output power above 25 mW with < 5 % variation across the temperature cycle, and (3) a record-high optical conversion efficiency exceeding 20 %. These results establish new performance benchmarks for ASE sources used in ultrahigh-precision fiber-optic gyroscopes operating under extreme environmental conditions. The dual-FBG wavelength-stabilization method and hybrid integrated architecture effectively address long-standing challenges in maintaining spectral purity and power efficiency under thermal stress, marking a substantial advancement in photonic light-source technology for precision inertial navigation.
{"title":"High-power wavelength-stabilized amplified spontaneous emission source enabled by 974 nm LD and hybrid integration","authors":"Yongkang Yang , Baiang Qu , Hongjie Xu , Manqing Tan , Wentao Guo","doi":"10.1016/j.ijleo.2025.172609","DOIUrl":"10.1016/j.ijleo.2025.172609","url":null,"abstract":"<div><div>The amplified spontaneous emission (ASE) source is widely used in fiber-optic gyroscopes due to its broadband spectrum, which suppresses backscattering- and Kerr-effect–induced phase errors while reducing polarization coupling noise. However, thermally induced wavelength drift remains a critical limitation in ultrahigh-precision systems, as even small spectral shifts introduce non-negligible phase noise. To address this challenge, we propose a wide-temperature wavelength-selective reflection strategy that integrates a wavelength-division multiplexer, optical filter, and reflector into a compact hybrid structure, achieving a mean drift rate below 0.1 ppm/°C across the full operational range. This work presents a significant advance in ASE source technology through the integration of dual fiber Bragg gratings (FBGs) at the 974 nm laser diode (LD) output and a monolithically packaged passive-component module. Comprehensive theoretical modeling and experimental characterization of LD–ASE spectral–power correlations enabled the development of a thermally optimized dual-pass architecture achieving three major performance breakthroughs: (1) ultra-stable wavelength performance with drift below 0.1 ppm/°C over –25°C to + 60°C, (2) ASE output power above 25 mW with < 5 % variation across the temperature cycle, and (3) a record-high optical conversion efficiency exceeding 20 %. These results establish new performance benchmarks for ASE sources used in ultrahigh-precision fiber-optic gyroscopes operating under extreme environmental conditions. The dual-FBG wavelength-stabilization method and hybrid integrated architecture effectively address long-standing challenges in maintaining spectral purity and power efficiency under thermal stress, marking a substantial advancement in photonic light-source technology for precision inertial navigation.</div></div>","PeriodicalId":19513,"journal":{"name":"Optik","volume":"345 ","pages":"Article 172609"},"PeriodicalIF":3.1,"publicationDate":"2025-11-20","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145570772","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2025-11-20DOI: 10.1016/j.ijleo.2025.172607
J. Arriaga Hernández , B. Cuevas Otahola , A. Diaz Nayotl , A. Jaramillo Núñez , A. Pérez Villegas , O. Valenzuela
We apply new machine learning (ML) technologies to optimize the Hartmann test (HT) and Bi-Ronchi test (BRT) regarding the recognition, identification, and localization of the centroids in experimental Hartmanngrams and Bi-Ronchigrams. We replace the conventional rigid Hartmann screen (Hartmann mask, HM) with structured apertures implemented via a spatial light modulator (SLM), which enables the generation of multiple patterns with different aperture geometries. Based on the classical HM with circular apertures, we build square apertures for the Bi-Ronchi mask (BRM). We designed an experimental setup based on an SLM with a laser illumination system and implemented an unsupervised Centroid Clustering Algorithm (uCCA), based on the ML algorithm -means, to identify the geometries of the centroids, followed by their segmentation and localization by clustering. We compare the experimental and theoretical Bi-Ronchigrams (or Hartmanngrams) to obtain a point cloud of transverse aberrations (). We apply the point cloud method (PCM) to obtain an integrable surface from the points in . Finally, we replace the numerical integration of with transverse aberrations () and a directional derivative approach based on the Eikonal equation, solved using Gaussian quadrature to obtain the wavefront. We compare our results with the Zernike aberration polynomials for sensing optical elements from the aberrations of the system by means of the aberrations of its wavefront .
{"title":"Machine learning K-means algorithm applied to wavefront sensing in Bi-Ronchi/Hartmann tests with SLM","authors":"J. Arriaga Hernández , B. Cuevas Otahola , A. Diaz Nayotl , A. Jaramillo Núñez , A. Pérez Villegas , O. Valenzuela","doi":"10.1016/j.ijleo.2025.172607","DOIUrl":"10.1016/j.ijleo.2025.172607","url":null,"abstract":"<div><div>We apply new machine learning (ML) technologies to optimize the Hartmann test (HT) and Bi-Ronchi test (BRT) regarding the recognition, identification, and localization of the centroids in experimental Hartmanngrams and Bi-Ronchigrams. We replace the conventional rigid Hartmann screen (Hartmann mask, HM) with structured apertures implemented via a spatial light modulator (SLM), which enables the generation of multiple patterns with different aperture geometries. Based on the classical HM with circular apertures, we build square apertures for the Bi-Ronchi mask (BRM). We designed an experimental setup based on an SLM with a laser illumination system and implemented an unsupervised Centroid Clustering Algorithm (uCCA), based on the ML algorithm <span><math><mi>K</mi></math></span>-means, to identify the geometries of the centroids, followed by their segmentation and localization by clustering. We compare the experimental and theoretical Bi-Ronchigrams (or Hartmanngrams) to obtain a point cloud of transverse aberrations (<span><math><mi>P</mi><msub><mi>C</mi><mrow><mi>T</mi><mi>A</mi></mrow></msub></math></span>). We apply the point cloud method (PCM) to obtain an integrable surface from the points in <span><math><mi>P</mi><msub><mi>C</mi><mrow><mi>T</mi><mi>A</mi></mrow></msub></math></span>. Finally, we replace the numerical integration of <span><math><mrow><mi>P</mi><msub><mi>C</mi><mrow><mi>T</mi><mi>A</mi></mrow></msub></mrow></math></span> with transverse aberrations (<span><math><mi>T</mi><mi>A</mi></math></span>) and a directional derivative approach based on the Eikonal equation, solved using Gaussian quadrature to obtain the wavefront. We compare our results with the Zernike aberration polynomials for sensing optical elements from the aberrations of the system by means of the aberrations of its wavefront <span><math><mrow><mrow><mi>W</mi></mrow></mrow><mo>(</mo><mrow><mi>ρ</mi></mrow><mo>,</mo><mrow><mi>θ</mi></mrow><mo>)</mo></math></span>.</div></div>","PeriodicalId":19513,"journal":{"name":"Optik","volume":"346 ","pages":"Article 172607"},"PeriodicalIF":3.1,"publicationDate":"2025-11-20","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145616970","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2025-11-20DOI: 10.1016/j.ijleo.2025.172610
Iman Razmkhah, Zahra Adelpour, Mojtaba Sadeghi
In this work, we present a novel compact plasmonic dual-band bandpass filter based on graphene nanoribbons, tunable through azo-dye-doped liquid crystal and graphene conductivity. Graphene nanoribbons are deposited on a silica substrate and covered with azo-dye-doped liquid crystal. Therefore, the performance of the plasmonic structure can be tuned by a laser pump and the graphene chemical potential. Full-wave simulations are performed in COMSOL Multiphysics using the Finite Element Method (FEM). In addition, Transmission Line Modelling and Electromagnetic Scaling Law are used to validate the numerical simulation results. The proposed filter resonates at 2.45 THz and 9.2 THz when the laser pump is off. However, when the laser pump is on, the resonant frequencies redshift to 2.3 THz and 8.6 THz. The corresponding quality factors are 20 and 31 for the lower and higher resonance frequencies when the laser pump is off. The simulated reflection coefficients (S₁₁) reach −31 dB and −38 dB for the two passbands confirming efficient transmission (S₂₁≈ 0 dB). The effect of graphene chemical potential and geometric variations on our structure is investigated. Finally, the size and performance of our filter are compared with the previously reported designs, demonstrating both practical feasibility and compactness. With a compact footprint of 420 × 350 nm2 and dual-band tunability, the proposed filter is a promising candidate for terahertz sensing and communication systems.
{"title":"The design and TLM analysis of a compact graphene-based dual-band bandpass plasmonic filter with hybrid post-fabrication tunability via liquid crystal in the terahertz regime","authors":"Iman Razmkhah, Zahra Adelpour, Mojtaba Sadeghi","doi":"10.1016/j.ijleo.2025.172610","DOIUrl":"10.1016/j.ijleo.2025.172610","url":null,"abstract":"<div><div>In this work, we present a novel compact plasmonic dual-band bandpass filter based on graphene nanoribbons, tunable through azo-dye-doped liquid crystal and graphene conductivity. Graphene nanoribbons are deposited on a silica substrate and covered with azo-dye-doped liquid crystal. Therefore, the performance of the plasmonic structure can be tuned by a laser pump and the graphene chemical potential. Full-wave simulations are performed in COMSOL Multiphysics using the Finite Element Method (FEM). In addition, Transmission Line Modelling and Electromagnetic Scaling Law are used to validate the numerical simulation results. The proposed filter resonates at 2.45 THz and 9.2 THz when the laser pump is off. However, when the laser pump is on, the resonant frequencies redshift to 2.3 THz and 8.6 THz. The corresponding quality factors are 20 and 31 for the lower and higher resonance frequencies when the laser pump is off. The simulated reflection coefficients (S₁₁) reach −31 dB and −38 dB for the two passbands confirming efficient transmission (S₂₁≈ 0 dB). The effect of graphene chemical potential and geometric variations on our structure is investigated. Finally, the size and performance of our filter are compared with the previously reported designs, demonstrating both practical feasibility and compactness. With a compact footprint of 420 × 350 nm<sup>2</sup> and dual-band tunability, the proposed filter is a promising candidate for terahertz sensing and communication systems.</div></div>","PeriodicalId":19513,"journal":{"name":"Optik","volume":"345 ","pages":"Article 172610"},"PeriodicalIF":3.1,"publicationDate":"2025-11-20","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145681839","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2025-11-19DOI: 10.1016/j.ijleo.2025.172604
Sanjeev Mani Yadav
{"title":"Corrigendum to “A novel PCF-based optical sensor: Design and modeling for early malaria detection” [Optik 342–343, December 2025, 172581]","authors":"Sanjeev Mani Yadav","doi":"10.1016/j.ijleo.2025.172604","DOIUrl":"10.1016/j.ijleo.2025.172604","url":null,"abstract":"","PeriodicalId":19513,"journal":{"name":"Optik","volume":"345 ","pages":"Article 172604"},"PeriodicalIF":3.1,"publicationDate":"2025-11-19","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145839218","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2025-11-17DOI: 10.1016/j.ijleo.2025.172603
Kishore Kumar Venkatesan , Sathiyan Samikannu
The design, fabrication, and development of smart sensors are among the ultimate challenges faced by researchers nowadays in intelligent and real-time monitoring systems. A system for monitoring human breath holds exceptional promise in harsh environments, healthcare, sports, and remote monitoring. Translating this into the real world will be quite challenging as it requires developing unobtrusive and comfortable systems while maintaining high metrological performance. The potential solution for this has been derived from fiber optic sensors due to their compact size, ability to handle multiple inputs, chemical stability, and immunity to electromagnetic (EM) interference. Inclusive of this, a 2D nanomaterial is coated on an optical fiber and used as a sensing medium which detects changes in the breath composition and provides valuable information about the respiratory system because of its high surface-to-volume ratio, high carrier mobility, tunable band gaps, and strong light-matter interactions. This approach can potentially revolutionize the field of breath monitoring, enabling early detection of respiratory diseases and improving patient outcomes. Thus, this system will provide a pathway for exploring new possibilities in the emerging 2D material-based sensing platform. Here, we overview recent developments for monitoring human breath with fiber optic sensors and nanomaterial-based FOS along with various methods of respiratory monitoring and their benefits in real-time monitoring. Also, we summarize the challenges and future perspectives of 2D layered nanomaterial-based fiber optic sensors for human breath monitoring applications.
{"title":"Comprehensive review on 2D nanomaterial-based fiber optic sensor for human breath monitoring application","authors":"Kishore Kumar Venkatesan , Sathiyan Samikannu","doi":"10.1016/j.ijleo.2025.172603","DOIUrl":"10.1016/j.ijleo.2025.172603","url":null,"abstract":"<div><div>The design, fabrication, and development of smart sensors are among the ultimate challenges faced by researchers nowadays in intelligent and real-time monitoring systems. A system for monitoring human breath holds exceptional promise in harsh environments, healthcare, sports, and remote monitoring. Translating this into the real world will be quite challenging as it requires developing unobtrusive and comfortable systems while maintaining high metrological performance. The potential solution for this has been derived from fiber optic sensors due to their compact size, ability to handle multiple inputs, chemical stability, and immunity to electromagnetic (EM) interference. Inclusive of this, a 2D nanomaterial is coated on an optical fiber and used as a sensing medium which detects changes in the breath composition and provides valuable information about the respiratory system because of its high surface-to-volume ratio, high carrier mobility, tunable band gaps, and strong light-matter interactions. This approach can potentially revolutionize the field of breath monitoring, enabling early detection of respiratory diseases and improving patient outcomes. Thus, this system will provide a pathway for exploring new possibilities in the emerging 2D material-based sensing platform. Here, we overview recent developments for monitoring human breath with fiber optic sensors and nanomaterial-based FOS along with various methods of respiratory monitoring and their benefits in real-time monitoring. Also, we summarize the challenges and future perspectives of 2D layered nanomaterial-based fiber optic sensors for human breath monitoring applications.</div></div>","PeriodicalId":19513,"journal":{"name":"Optik","volume":"345 ","pages":"Article 172603"},"PeriodicalIF":3.1,"publicationDate":"2025-11-17","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145570773","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2025-11-17DOI: 10.1016/j.ijleo.2025.172602
Rusul A. Dahab, Hussein A. Jawad
Optical losses represent one of the primary obstacles to increasing the efficiency of silicon solar cells. The recommended solution to minimize optical losses is the use of plasmonic metal nanoparticles; however, they act as recombination centers within the solar cell construction, leading to a decrease in performance. The goal of this article is to introduce cobalt/graphene nanoparticles into the solar cell to minimize the optical losses. An ultra-thin film silicon PIN solar cell of dimensions (400 ×400 ×900) nm3 with ring metal contact shape was designed and numerically investigated using COMSOL Multiphysics software version 6.2 by the finite element method (FEM). Core/shell cobalt-graphene (Co/Gr) nanoparticles are periodically introduced into the cell between two layers (electron transport and active) in a ratio of 50:50 with an inter-spacing of a similar diameter. The Co/Gr parameters, number of nanoparticles (2, 4, 6), radius (10, 20, 30) nm, and shell thickness (1, 2, 4) nm were extensively studied. In addition, the arrangement of the core/shell nanoparticle material was considered. The results manifest the best performance of the proposed cell at 4 nanoparticles of 30 nm radius with 2 nm shell thickness for Co/Gr nanoparticles to get a maximum photocurrent of 26.28 mA/cm2. It is concluded that the optical losses of the Co/Gr core/shell nanoparticles embedded in an ultra-thin film silicon solar cell are significantly reduced owing to the increment in the absorption and hence the photocurrent. This enhancement opens a new avenue for further improvements.
{"title":"Mitigation optical losses via plasmonic core/shell (Co/Gr) nanoparticles introduced in ultra-thin film silicon solar cell","authors":"Rusul A. Dahab, Hussein A. Jawad","doi":"10.1016/j.ijleo.2025.172602","DOIUrl":"10.1016/j.ijleo.2025.172602","url":null,"abstract":"<div><div>Optical losses represent one of the primary obstacles to increasing the efficiency of silicon solar cells. The recommended solution to minimize optical losses is the use of plasmonic metal nanoparticles; however, they act as recombination centers within the solar cell construction, leading to a decrease in performance. The goal of this article is to introduce cobalt/graphene nanoparticles into the solar cell to minimize the optical losses. An ultra-thin film silicon PIN solar cell of dimensions (400 ×400 ×900) nm<sup>3</sup> with ring metal contact shape was designed and numerically investigated using COMSOL Multiphysics software version 6.2 by the finite element method (FEM). Core/shell cobalt-graphene (Co/Gr) nanoparticles are periodically introduced into the cell between two layers (electron transport and active) in a ratio of 50:50 with an inter-spacing of a similar diameter. The Co/Gr parameters, number of nanoparticles (2, 4, 6), radius (10, 20, 30) nm, and shell thickness (1, 2, 4) nm were extensively studied. In addition, the arrangement of the core/shell nanoparticle material was considered. The results manifest the best performance of the proposed cell at 4 nanoparticles of 30 nm radius with 2 nm shell thickness for Co/Gr nanoparticles to get a maximum photocurrent of 26.28 mA/cm<sup>2</sup>. It is concluded that the optical losses of the Co/Gr core/shell nanoparticles embedded in an ultra-thin film silicon solar cell are significantly reduced owing to the increment in the absorption and hence the photocurrent. This enhancement opens a new avenue for further improvements.</div></div>","PeriodicalId":19513,"journal":{"name":"Optik","volume":"345 ","pages":"Article 172602"},"PeriodicalIF":3.1,"publicationDate":"2025-11-17","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145546588","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2025-11-13DOI: 10.1016/j.ijleo.2025.172600
D. Bhadrarao , P. Rakus , A. Venkata Sekhar , V. Chitti Babu , Y. Dana Rao , V. Ravi Kumar , G. Naga Raju , N. Purnachand , N. Venkatramaiah , N. Veeraiah
In this investigation, photo-induced birefringence of Pb3O4-Bi2O3-B2O3 glass ceramics doped with varying content of CuO (ranging from 0.2 to 1.0 mol%) is presented. The photo-induced birefringence (PIB) exhibited a delayed relaxation process lasting few seconds and indicated that the anisotropic photorefractive (PR) effect significantly exceeded the fast Kerr effect. Photorefractive birefringence reached a maximum at a CuO concentration of 0.2 mol%, likely due to enhanced depolymerization of the glass ceramic network that reduces the phonon losses. This is ascribed to the predominant fraction of Cu2 + ions occupying octahedral (Oh) sites and acting as modifiers. Increasing the CuO content further, up to nearly 0.8 mol%, the magnitude of photorefractive birefringence is observed to reduce. Phonon losses increase because a higher proportion of Cu+ ions occupy tetrahedral (Td) positions within the glass ceramic in this concentration range, resulting in stronger interactions between different structural groups in the material. Electrical conductivity and ultrasonic measurements corroborate this finding. Additionally, these glass ceramics were found to be composed of anisotropic CuBi2O4 crystal phases, which enhance their photorefractive (PR) properties. Notably, compositions containing approximately 0.2 mol% CuO demonstrate optimal PR efficiency and are promising candidates for practical applications.
{"title":"Photoinduced birefringence studies in CuO doped Pb3O4-Bi2O3-B2O3 glass ceramics using femtosecond laser","authors":"D. Bhadrarao , P. Rakus , A. Venkata Sekhar , V. Chitti Babu , Y. Dana Rao , V. Ravi Kumar , G. Naga Raju , N. Purnachand , N. Venkatramaiah , N. Veeraiah","doi":"10.1016/j.ijleo.2025.172600","DOIUrl":"10.1016/j.ijleo.2025.172600","url":null,"abstract":"<div><div>In this investigation, photo-induced birefringence of Pb<sub>3</sub>O<sub>4</sub>-Bi<sub>2</sub>O<sub>3</sub>-B<sub>2</sub>O<sub>3</sub> glass ceramics doped with varying content of CuO (ranging from 0.2 to 1.0 mol%) is presented. The photo-induced birefringence (PIB) exhibited a delayed relaxation process lasting few seconds and indicated that the anisotropic photorefractive (PR) effect significantly exceeded the fast Kerr effect. Photorefractive birefringence reached a maximum at a CuO concentration of 0.2 mol%, likely due to enhanced depolymerization of the glass ceramic network that reduces the phonon losses. This is ascribed to the predominant fraction of Cu<sup>2 +</sup> ions occupying octahedral (<em>O</em><sub><em>h</em></sub>) sites and acting as modifiers. Increasing the CuO content further, up to nearly 0.8 mol%, the magnitude of photorefractive birefringence is observed to reduce. Phonon losses increase because a higher proportion of Cu<sup>+</sup> ions occupy tetrahedral (<em>T</em><sub><em>d</em></sub>) positions within the glass ceramic in this concentration range, resulting in stronger interactions between different structural groups in the material. Electrical conductivity and ultrasonic measurements corroborate this finding. Additionally, these glass ceramics were found to be composed of anisotropic CuBi<sub>2</sub>O<sub>4</sub> crystal phases, which enhance their photorefractive (PR) properties. Notably, compositions containing approximately 0.2 mol% CuO demonstrate optimal PR efficiency and are promising candidates for practical applications.</div></div>","PeriodicalId":19513,"journal":{"name":"Optik","volume":"344 ","pages":"Article 172600"},"PeriodicalIF":3.1,"publicationDate":"2025-11-13","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145526858","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2025-11-13DOI: 10.1016/j.ijleo.2025.172599
Dongxin Gao , Minghui Sun , Yunli Yu , Wenyu Wang , Weixin Liu , Yuzhai Pan
We report an experimental investigation into the generation and control of multi-pulse bursts in a passively mode-locked Yb-doped fiber laser based on nonlinear polarization rotation (NPR). By systematically adjusting the polarization controller (PC) at a fixed pump power, we successfully realize controllable pulse bursts with varying pulse numbers and intervals. Notably, distinct pulse interval distributions are observed in the output configurations ranging from 1 to 5 pulses. Additionally, a broadband spectrum with a 20 dB bandwidth extending up to 66 nm is achieved, attributed to the interplay between Raman scattering and polarization state modulation within the laser cavity. These findings demonstrate the potential for precise pulse control and broad spectral generation in NPR based fiber lasers.
{"title":"Generation of pulse bursts and broadband spectrum in a hundred-meter-long Yb-doped fiber laser","authors":"Dongxin Gao , Minghui Sun , Yunli Yu , Wenyu Wang , Weixin Liu , Yuzhai Pan","doi":"10.1016/j.ijleo.2025.172599","DOIUrl":"10.1016/j.ijleo.2025.172599","url":null,"abstract":"<div><div>We report an experimental investigation into the generation and control of multi-pulse bursts in a passively mode-locked Yb-doped fiber laser based on nonlinear polarization rotation (NPR). By systematically adjusting the polarization controller (PC) at a fixed pump power, we successfully realize controllable pulse bursts with varying pulse numbers and intervals. Notably, distinct pulse interval distributions are observed in the output configurations ranging from 1 to 5 pulses. Additionally, a broadband spectrum with a 20 dB bandwidth extending up to 66 nm is achieved, attributed to the interplay between Raman scattering and polarization state modulation within the laser cavity. These findings demonstrate the potential for precise pulse control and broad spectral generation in NPR based fiber lasers.</div></div>","PeriodicalId":19513,"journal":{"name":"Optik","volume":"344 ","pages":"Article 172599"},"PeriodicalIF":3.1,"publicationDate":"2025-11-13","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145526859","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}