Pub Date : 2025-11-09DOI: 10.1016/j.rio.2025.100928
Nur Aida Syahmina Noorbahrin , Nadrahtul Aqilah Mohd Yahaya , Siti Nurul Fatihah Azahan , Muhammad Khudhori Mohd Yusof , Sabrina Mohd Farid , Siti Nurfatinah Mohd Asseri , Retna Apsari , Mohd Zamani Zulkifli
In this work, the fabrication of whispering gallery mode (WGM) microsphere resonators using core-to-core alignment fusion splicer and its application as temperature sensors by optimization of coupling gap is studied and demonstrated. The proposed WGMs microsphere resonators are fabricated using core-to-core alignment fusion splicing technique, and the optimum coupling gap to a tapered fiber is made. Two configurations of coupling gap were tested, which are the 0 µm coupling gap in which both microsphere resonator and tapered fiber contacted, and 10 µm coupling gap. The sensor with 0 µm coupling gap recorded a finesse and Q-factor of 42.792 and 16,069.688 respectively at a resonance wavelength of 1542.69 nm. The sensor with 10 µm coupling gap recorded a finesse and Q-factor of 1.111 and 659.997 respectively at a resonance wavelength of 1544.40 nm. The temperature sensitivity was calculated to be 14.9 pm/°C, with a wavelength resolution of 6.7 × 10−2 m°C and figure of merit (FOM) of 0.11/°C. The smaller gap resulted in a better sensitivity of the temperature sensor. The sensor has a substantial potential as a cost-effective, highly stable, and easy-to-fabricate. The proposed setup has been proven to be extremely sensitive to environmental changes, making them a highly potential alternative temperature sensor, further increasing their appeal for real world applications.
{"title":"Fabrication of Whispering Gallery Mode (WGM) microresonator using core-to-core alignment fusion splicer for high sensitive temperature sensor trough optimum coupling gap with high q-factor","authors":"Nur Aida Syahmina Noorbahrin , Nadrahtul Aqilah Mohd Yahaya , Siti Nurul Fatihah Azahan , Muhammad Khudhori Mohd Yusof , Sabrina Mohd Farid , Siti Nurfatinah Mohd Asseri , Retna Apsari , Mohd Zamani Zulkifli","doi":"10.1016/j.rio.2025.100928","DOIUrl":"10.1016/j.rio.2025.100928","url":null,"abstract":"<div><div>In this work, the fabrication of whispering gallery mode (WGM) microsphere resonators using core-to-core alignment fusion splicer and its application as temperature sensors by optimization of coupling gap is studied and demonstrated. The proposed WGMs microsphere resonators are fabricated using core-to-core alignment fusion splicing technique, and the optimum coupling gap to a tapered fiber is made. Two configurations of coupling gap were tested, which are the 0 µm coupling gap in which both microsphere resonator and tapered fiber contacted, and 10 µm coupling gap. The sensor with 0 µm coupling gap recorded a finesse and Q-factor of 42.792 and 16,069.688 respectively at a resonance wavelength of 1542.69 nm. The sensor with 10 µm coupling gap recorded a finesse and Q-factor of 1.111 and 659.997 respectively at a resonance wavelength of 1544.40 nm. The temperature sensitivity was calculated to be 14.9 pm/°C, with a wavelength resolution of 6.7 × 10<sup>−2</sup> m°C and figure of merit (FOM) of 0.11/°C. The smaller gap resulted in a better sensitivity of the temperature sensor. The sensor has a substantial potential as a cost-effective, highly stable, and easy-to-fabricate. The proposed setup has been proven to be extremely sensitive to environmental changes, making them a highly potential alternative temperature sensor, further increasing their appeal for real world applications.</div></div>","PeriodicalId":21151,"journal":{"name":"Results in Optics","volume":"21 ","pages":"Article 100928"},"PeriodicalIF":3.0,"publicationDate":"2025-11-09","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145525625","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2025-11-09DOI: 10.1016/j.rio.2025.100927
Amir Azizi , Minoo Shariati , Parisa Ahmadi
This study focuses on the UV-assisted synthesis and investigation of Cadmium(II) Diacetate dihydrate [Cd(CH3COO)2·2H2O] (CdDD) it assesses its effectiveness as a liquid photocatalyst for degrading the methylene blue dye (MB). The synthesized compound was characterized using Dynamic Light Scattering (DLS), Ultraviolet–visible (UV–Vis) spectroscopy, Fourier-transform infrared spectroscopy (FT-IR), and Nuclear Magnetic Resonance (NMR) spectroscopy. Using DLS Analysis, the uniform particle size distribution of liquid CdDD was confirmed, and the mean particle size (z-average) was determined to be 101.66 nm with a Polydispersity Index (PdI) of 0.0014. Band gap energy (Eg) of liquid CdDD is estimated to be 3.3 eV. FT-IR and NMR analyses confirm the successful formation of the desired catalyst structure. Liquid CdDD as a photocatalyst for MB degradation was evaluated and optimized. Degradation efficiency of 93 % was achieved under optimum conditions of [MB]o = 20 mg/L, [CdDD] = 10 ml/L, pH of 2, and [30 % H2O2] = 2.5 ml. The kinetic model under optimum conditions, pseudo-first-order, was obtained, with a rate constant of 0.06232 min−1. Also, the half-life values for concentrations of 5, 10, 20, and 40 ppm of MB dye were evaluated and obtained as 26.45, 23.9 min, 20.7 min, and 78.8 min, respectively. Furthermore, the electrical energy consumption (EEC) and the process evaluation criterion (PE) were recorded as 303.8 kWh/m3 and 2.15 × 10−2, respectively, and the results were compared with related reported processes. The most significant outcome of this study is the introduction of CdDD as an effective liquid catalyst in the photodegradation of organic pollutants.
{"title":"UV-assisted synthesis of cadmium(II) diacetate dihydrate for the photocatalytic degradation of methylene blue: kinetics, pathway, and energy consumption","authors":"Amir Azizi , Minoo Shariati , Parisa Ahmadi","doi":"10.1016/j.rio.2025.100927","DOIUrl":"10.1016/j.rio.2025.100927","url":null,"abstract":"<div><div>This study focuses on the UV-assisted synthesis and investigation of Cadmium(II) Diacetate dihydrate [Cd(CH<sub>3</sub>COO)<sub>2</sub>·2H<sub>2</sub>O] (CdDD) it assesses its effectiveness as a liquid photocatalyst for degrading the methylene blue dye (MB). The synthesized compound was characterized using Dynamic Light Scattering (DLS), Ultraviolet–visible (UV–Vis) spectroscopy, Fourier-transform infrared spectroscopy (FT-IR), and Nuclear Magnetic Resonance (NMR) spectroscopy. Using DLS Analysis, the uniform particle size distribution of liquid CdDD was confirmed, and the mean particle size (z-average) was determined to be 101.66 nm with a Polydispersity Index (PdI) of 0.0014. Band gap energy (<em>E<sub>g</sub></em>) of liquid CdDD is estimated to be 3.3 eV. FT-IR and NMR analyses confirm the successful formation of the desired catalyst structure. Liquid CdDD as a photocatalyst for MB degradation was evaluated and optimized. Degradation efficiency of 93 % was achieved under optimum conditions of [MB]<sub>o</sub> = 20 mg/L, [CdDD] = 10 ml/L, pH of 2, and [30 % H<sub>2</sub>O<sub>2</sub>] = 2.5 ml. The kinetic model under optimum conditions, pseudo-first-order, was obtained, with a rate constant of 0.06232 min<sup>−1</sup>. Also, the half-life values for concentrations of 5, 10, 20, and 40 ppm of MB dye were evaluated and obtained as 26.45, 23.9 min, 20.7 min, and 78.8 min, respectively. Furthermore, the electrical energy consumption (<em>E<sub>EC</sub></em>) and the process evaluation criterion (<em>PE</em>) were recorded as 303.8 kWh/m<sup>3</sup> and 2.15 × 10<sup>−2</sup>, respectively, and the results were compared with related reported processes. The most significant outcome of this study is the introduction of CdDD as an effective liquid catalyst in the photodegradation of organic pollutants.</div></div>","PeriodicalId":21151,"journal":{"name":"Results in Optics","volume":"21 ","pages":"Article 100927"},"PeriodicalIF":3.0,"publicationDate":"2025-11-09","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145525626","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2025-11-09DOI: 10.1016/j.rio.2025.100929
Tahani I. Al-Muhimeed , Mostafa Salah , Omar Abdelsamad , Ahmed Shaker , Mohamed Mousa
Lead-free perovskite solar cells (PSCs) are promising for sustainable photovoltaics; however, their performance remains below that of their lead-based counterparts. In this study, we investigate Cs2SnI4Br2 PSCs using SCAPS-1D simulations calibrated to experimental baselines and systematically optimize key design parameters. Some design recommendations are provided for lead-free Cs2SnI4Br2-based PSCs aimed at fostering sustainable and environmentally friendly photovoltaic (PV) solutions. By replacing TiO2 with tungsten disulfide as the electron-transport layer (ETL), the conduction-band offset (CBO) is tuned to a favorable + 0.18 eV, enabling suppressed recombination. The effects of tuning the metal work function of both the front and back electrodes, as well as the doping levels of the transport layers, are also investigated. The thickness and bulk defects of the absorber layer are further studied. Also, the effect of interfacial defects is investigated. Collectively, these design choices raise the simulated PCE from 2.03 % to 9.47 %. Energy loss analysis indicates that absorption remains the dominant loss mechanism. Achieving a PCE exceeding 28 % requires modifications to the optical properties of the photoactive layer, addressing one of the most critical challenges in enhancing overall device performance. These promising findings unveil the potential application of inorganic lead-free Cs2SnI4Br2-based PSCs for sustainable photovoltaic applications.
{"title":"Optimization techniques for power conversion efficiency boosting in lead-free Cs2SnI4Br2-based perovskite solar cell","authors":"Tahani I. Al-Muhimeed , Mostafa Salah , Omar Abdelsamad , Ahmed Shaker , Mohamed Mousa","doi":"10.1016/j.rio.2025.100929","DOIUrl":"10.1016/j.rio.2025.100929","url":null,"abstract":"<div><div>Lead-free perovskite solar cells (PSCs) are promising for sustainable photovoltaics; however, their performance remains below that of their lead-based counterparts. In this study, we investigate Cs<sub>2</sub>SnI<sub>4</sub>Br<sub>2</sub> PSCs using SCAPS-1D simulations calibrated to experimental baselines and systematically optimize key design parameters. Some design recommendations are provided for lead-free Cs<sub>2</sub>SnI<sub>4</sub>Br<sub>2</sub>-based PSCs aimed at fostering sustainable and environmentally friendly photovoltaic (PV) solutions. By replacing TiO<sub>2</sub> with tungsten disulfide as the electron-transport layer (ETL), the conduction-band offset (CBO) is tuned to a favorable + 0.18 eV, enabling suppressed recombination. The effects of tuning the metal work function of both the front and back electrodes, as well as the doping levels of the transport layers, are also investigated. The thickness and bulk defects of the absorber layer are further studied. Also, the effect of interfacial defects is investigated. Collectively, these design choices raise the simulated PCE from 2.03 % to 9.47 %. Energy loss analysis indicates that absorption remains the dominant loss mechanism. Achieving a PCE exceeding 28 % requires modifications to the optical properties of the photoactive layer, addressing one of the most critical challenges in enhancing overall device performance. These promising findings unveil the potential application of inorganic lead-free Cs<sub>2</sub>SnI<sub>4</sub>Br<sub>2</sub>-based PSCs for sustainable photovoltaic applications.</div></div>","PeriodicalId":21151,"journal":{"name":"Results in Optics","volume":"21 ","pages":"Article 100929"},"PeriodicalIF":3.0,"publicationDate":"2025-11-09","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145525624","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2025-10-30DOI: 10.1016/j.rio.2025.100921
Jeremiah O. Abolade , Dominic B.O. Konditi
A terahertz Minkowski Island fractal antenna (MIFA) is presented in this work. The MIFA is etched on a 0.38 × 0.38 substrate with a resonant frequency of 0.29THz. An Artificial Magnetic Conductor (AMC) based on the first iteration Minkowski Island fractal is designed and incorporated to improve antenna performance, such as gain and radiation efficiency at terahertz frequency for the first time in this work. The proposed antenna (MIFA with integrated AMC) footprint is 0.47 × 0.47 . The integration of AMC on the MIFA results in a 287.5 % increase in gain and 50 % increase in radiation efficiency. The bending analysis of the MIFA is investigated, and it was discovered that the proposed MIFA demonstrated a stable response. Therefore, the proposed MIFA is a suitable candidate for Terahertz applications such as body area network and medical diagnostics and telemedicine.
{"title":"Integrated Artificial Magnetic Conductor Minkowski Island fractal terahertz antenna (AMC-MIFA) for future Communications","authors":"Jeremiah O. Abolade , Dominic B.O. Konditi","doi":"10.1016/j.rio.2025.100921","DOIUrl":"10.1016/j.rio.2025.100921","url":null,"abstract":"<div><div>A terahertz Minkowski Island fractal antenna (MIFA) is presented in this work. The MIFA is etched on a 0.38 <span><math><msub><mi>λ</mi><mi>o</mi></msub></math></span> × 0.38 <span><math><msub><mi>λ</mi><mi>o</mi></msub></math></span> substrate with a resonant frequency of 0.29THz. An Artificial Magnetic Conductor (AMC) based on the first iteration Minkowski Island fractal is designed and incorporated to improve antenna performance, such as gain and radiation efficiency at terahertz frequency for the first time in this work. The proposed antenna (MIFA with integrated AMC) footprint is 0.47 <span><math><msub><mi>λ</mi><mi>o</mi></msub></math></span> × 0.47 <span><math><msub><mi>λ</mi><mi>o</mi></msub></math></span>. The integration of AMC on the MIFA results in a 287.5 % increase in gain and 50 % increase in radiation efficiency. The bending analysis of the MIFA is investigated, and it was discovered that the proposed MIFA demonstrated a stable response. Therefore, the proposed MIFA is a suitable candidate for Terahertz applications such as body area network and medical diagnostics and telemedicine.</div></div>","PeriodicalId":21151,"journal":{"name":"Results in Optics","volume":"21 ","pages":"Article 100921"},"PeriodicalIF":3.0,"publicationDate":"2025-10-30","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145473643","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2025-10-30DOI: 10.1016/j.rio.2025.100922
Mingliang Long , Zhibo Wu , Ming Wen , Yan Liang , Haifeng Zhang , Hao Chang , Huarong Deng , Zhongping Zhang
A distributed feedback picosecond (DFB) pulse laser has been designed with a single pulse energy of 5 pJ and a pulse width of 200 ps, resulting in a spectrum width of 0.12 nm. By controlling the time sequence of the DFB picosecond pulse laser and regenerative amplification (RA) at a repetition rate of 5 kHz and pulse width of 200 ps, the single-pulse energy has been amplified to 320 μJ, an amplification factor of 6.4 × 107 is achieved. After frequency doubling, an average power of 0.6 W for the green picosecond laser is obtained, the synchronization accuracy of root mean square (RMS) between the pulse picosecond laser and the external signal is 18.1 ps. Based on the principle of satellite laser ranging (SLR), an external trigger signal has been used to replace the locally collected laser pulse as the local main wave. This new approach has been implemented in the SLR system at the Shanghai Astronomical Observatory, allowing for measurements of low-earth orbit, medium-earth orbit, high-altitude orbit, and geosynchronous (GEO) orbit (∼36000 km) satellites with a measurement accuracy ranging from 6 mm to 20 mm. It is the first successful integration of a DFB + RA-based low jitter picosecond laser with an externally triggered signal as the primary waveform for SLR of multiple satellites,it provides a new and innovative method for laser ranging.
{"title":"A low jitter regenerative amplification picosecond pulse laser with the external trigger signal as local main wave for the SLR","authors":"Mingliang Long , Zhibo Wu , Ming Wen , Yan Liang , Haifeng Zhang , Hao Chang , Huarong Deng , Zhongping Zhang","doi":"10.1016/j.rio.2025.100922","DOIUrl":"10.1016/j.rio.2025.100922","url":null,"abstract":"<div><div>A distributed feedback picosecond (DFB) pulse laser<!--> <!-->has<!--> <!-->been<!--> <!-->designed<!--> <!-->with<!--> <!-->a<!--> <!-->single pulse energy<!--> <!-->of<!--> <!-->5 pJ<!--> <!-->and<!--> <!-->a<!--> <!-->pulse width of 200 ps,<!--> <!-->resulting<!--> <!-->in a<!--> <!-->spectrum width of 0.12 nm.<!--> <!-->By<!--> <!-->controlling<!--> <!-->the time sequence of<!--> <!-->the<!--> <!-->DFB picosecond pulse laser and regenerative amplification<!--> <!-->(RA) at a repetition rate of 5 kHz and pulse width of 200 ps, the single-pulse energy<!--> <!-->has<!--> <!-->been<!--> <!-->amplified to 320 μJ,<!--> <!-->an amplification factor of 6.4 × 10<sup>7</sup> is achieved.<!--> <!-->After<!--> <!-->frequency doubling,<!--> <!-->an average power of 0.6 W<!--> <!-->for the<!--> <!-->green picosecond laser is obtained, the<!--> <!-->synchronization accuracy of root mean square (RMS) between the pulse picosecond laser and the external signal is 18.1 ps.<!--> <!-->Based on the principle of satellite laser ranging (SLR), an external trigger signal<!--> <!-->has<!--> <!-->been<!--> <!-->used to replace the locally collected laser pulse as the local main wave. This new approach<!--> <!-->has<!--> <!-->been<!--> <!-->implemented in the SLR system at the Shanghai<!--> <!-->Astronomical<!--> <!-->Observatory,<!--> <!-->allowing for measurements of<!--> <!-->low-earth orbit, medium-earth orbit, high-altitude orbit,<!--> <!-->and geosynchronous (GEO) orbit (∼36000 km) satellites<!--> <!-->with<!--> <!-->a<!--> <!-->measurement accuracy<!--> <!-->ranging<!--> <!-->from 6 mm to 20 mm.<!--> <!-->It is the first successful integration of a DFB + RA-based low jitter picosecond laser with an externally triggered signal as the primary waveform for SLR of multiple satellites,it provides a new and innovative method for laser ranging.</div></div>","PeriodicalId":21151,"journal":{"name":"Results in Optics","volume":"21 ","pages":"Article 100922"},"PeriodicalIF":3.0,"publicationDate":"2025-10-30","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145473644","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
A sub-MHz frequency stability of the laser is crucial in the quantum-atom experiment where precise atomic transition is required for control and manipulation of atom like in the atom quantum computing. In this work, we have built the frequency stabilization system for the lasers used in our cold Rubidium atom experiment in the magneto-optical trap (MOT) and the optical tweezers. We utilized a Rubidium vapour glass cell as a frequency reference, which provides atomically absolute reference point with low complexity setup. By mean of the absorption of the laser beam by the Rubidium vapour, the saturated absorption spectroscopy (SAS) experiment was setup to produce the D2 line spectra. The acousto-optic modulator (AOM) was used to sinusoidally dither the laser frequency and consequently the resonance peaks in the spectra. Detailing in this work, the AOM sinusoidal dithering and the dithered SAS signal had orthogonality and were processed together to produce the error signal used to stabilize the laser frequency to the resonant peak. This frequency stabilization system achieved the frequency standard deviation below MHz over up to 800 minutes period. The system also allowed for stabilized frequency tunability over a range of MHz about the target resonance peak. This performance is significant for stabilizing the lasers in the MOT experiment and related quantum-atom research.
{"title":"Sub-megahertz laser stabilization by harnessing orthogonality between the acousto-optic modulator dither and atomic spectroscopy","authors":"Phatwarach Siriworakoonchai , Parinya Udommai , Nuttanan Tanasanchai , Waranont Anukool","doi":"10.1016/j.rio.2025.100920","DOIUrl":"10.1016/j.rio.2025.100920","url":null,"abstract":"<div><div>A sub-MHz frequency stability of the laser is crucial in the quantum-atom experiment where precise atomic transition is required for control and manipulation of atom like in the atom quantum computing. In this work, we have built the frequency stabilization system for the lasers used in our cold Rubidium atom experiment in the magneto-optical trap (MOT) and the optical tweezers. We utilized a Rubidium vapour glass cell as a frequency reference, which provides atomically absolute reference point with low complexity setup. By mean of the absorption of the laser beam by the Rubidium vapour, the saturated absorption spectroscopy (SAS) experiment was setup to produce the D2 line spectra. The acousto-optic modulator (AOM) was used to sinusoidally dither the laser frequency and consequently the resonance peaks in the spectra. Detailing in this work, the AOM sinusoidal dithering and the dithered SAS signal had orthogonality and were processed together to produce the error signal used to stabilize the laser frequency to the resonant peak. This frequency stabilization system achieved the frequency standard deviation below <span><math><mrow><mn>0.80</mn></mrow></math></span> MHz over up to 800 minutes period. The system also allowed for stabilized frequency tunability over a range of <span><math><mrow><mn>55</mn><mo>-</mo><mn>60</mn></mrow></math></span> MHz about the target resonance peak. This performance is significant for stabilizing the lasers in the MOT experiment and related quantum-atom research.</div></div>","PeriodicalId":21151,"journal":{"name":"Results in Optics","volume":"21 ","pages":"Article 100920"},"PeriodicalIF":3.0,"publicationDate":"2025-10-27","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145415512","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2025-10-27DOI: 10.1016/j.rio.2025.100923
Xuyu Zhang , Libang Chen , Xuying Zhang , Dawei Zhang , Songlin Zhuang , Shensheng Han , Honglin Liu
Deep learning has been widely applied in imaging through scattering media, showing advantages in penetration depth, resolution, dynamic adaptivity, et al. Due to requirements of network architecture and/or computation efficiency, the recorded speckle pattern is usually cropped or downsampled to reduce the size of the input, which often leads to severely degraded reconstruction under incoherent illumination, when target information is encoded in low-contrast speckles. In this study, we propose a non-symmetric U-Net to enhance information extraction from incoherent speckle patterns while maintaining a low cost in computation resources. The non-symmetric U-Net uses a deeper encoder to match the full-size speckle pattern and extract more feature information but a lightweight decoder to achieve target reconstruction. It has been demonstrated that the deep-contraction-shallow-expansion network structure can selectively enhance information extraction from high-frequency modulations in incoherent speckles that is overwhelmed by noise and can be easily averaged-out by downsampling. The study provides a new architectural paradigm for imaging with deep learning, which has significant research and application values in imaging fields with low coherence illuminations, such as autonomous driving detection and remote sensing.
{"title":"Imaging through scattering media with a non-symmetric U-Net","authors":"Xuyu Zhang , Libang Chen , Xuying Zhang , Dawei Zhang , Songlin Zhuang , Shensheng Han , Honglin Liu","doi":"10.1016/j.rio.2025.100923","DOIUrl":"10.1016/j.rio.2025.100923","url":null,"abstract":"<div><div>Deep learning has been widely applied in imaging through scattering media, showing advantages in penetration depth, resolution, dynamic adaptivity, et al. Due to requirements of network architecture and/or computation efficiency, the recorded speckle pattern is usually cropped or downsampled to reduce the size of the input, which often leads to severely degraded reconstruction under incoherent illumination, when target information is encoded in low-contrast speckles. In this study, we propose a non-symmetric U-Net to enhance information extraction from incoherent speckle patterns while maintaining a low cost in computation resources. The non-symmetric U-Net uses a deeper encoder to match the full-size speckle pattern and extract more feature information but a lightweight decoder to achieve target reconstruction. It has been demonstrated that the deep-contraction-shallow-expansion network structure can selectively enhance information extraction from high-frequency modulations in incoherent speckles that is overwhelmed by noise and can be easily averaged-out by downsampling. The study provides a new architectural paradigm for imaging with deep learning, which has significant research and application values in imaging fields with low coherence illuminations, such as autonomous driving detection and remote sensing.</div></div>","PeriodicalId":21151,"journal":{"name":"Results in Optics","volume":"21 ","pages":"Article 100923"},"PeriodicalIF":3.0,"publicationDate":"2025-10-27","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145415513","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
In this paper, seven surface plasmon-based filters using a single disk resonator (DR) and a DR coupled with one to six ring-shaped resonators (RSRs) are proposed. In these configurations, the resonators are bidirectionally connected to a pair of metal–insulator-metal (MIM) waveguides. The initial filter structure, consisting of only a single DR, functions as a single-mode band-pass filter. By coupling a disk resonator with a ring-shaped resonator (RSR), a dual-mode filter is created. Following this pattern, each additional RSR introduce another mode to the transmission spectrum. Essentially, the innovative method detailed in this work allows for the creation of plasmonic filters capable of operating with one through seven distinct modes. By utilizing a consistent topology, the results for various structural geometries with different numbers of RSRs are achieved, showcasing true scalability. Moreover, the quality factor (Q-factor) of the resulting modes is enhanced by increasing the quantity of RSRs. Consequently, these filters detailed in this study are suitable as foundational designs for optical sensors that require varying levels of sensitivity. The insulator material employed is air, while silver, whose properties are described by the Drude model, is used as the metal. Every result was generated through the finite-difference time-domain method, a technique known for its numerical stability and minimal dispersion error. Due to the remarkable features such as single and multi-mode filtering, tunable resonant frequency, and variable Q-factor, the filter topologies proposed here can find applications in more complex designs, including optical sensors, demultiplexers, splitters, couplers, and so on.
{"title":"Designing scalable single-mode to seven-mode plasmonic filters utilizing disk and ring-shaped resonators","authors":"Saeed Javid, Farzad Tavakkol Hamedani, Pejman Rezaei, Shiva Khani","doi":"10.1016/j.rio.2025.100919","DOIUrl":"10.1016/j.rio.2025.100919","url":null,"abstract":"<div><div>In this paper, seven surface plasmon-based filters using a single disk resonator (DR) and a DR coupled with one to six ring-shaped resonators (RSRs) are proposed. In these configurations, the resonators are bidirectionally connected to a pair of metal–insulator-metal (MIM) waveguides. The initial filter structure, consisting of only a single DR, functions as a single-mode band-pass filter. By coupling a disk resonator with a ring-shaped resonator (RSR), a dual-mode filter is created. Following this pattern, each additional RSR introduce another mode to the transmission spectrum. Essentially, the innovative method detailed in this work allows for the creation of plasmonic filters capable of operating with one through seven distinct modes. By utilizing a consistent topology, the results for various structural geometries with different numbers of RSRs are achieved, showcasing true scalability. Moreover, the quality factor (Q-factor) of the resulting modes is enhanced by increasing the quantity of RSRs. Consequently, these filters detailed in this study are suitable as foundational designs for optical sensors that require varying levels of sensitivity. The insulator material employed is air, while silver, whose properties are described by the Drude model, is used as the metal. Every result was generated through the finite-difference time-domain method, a technique known for its numerical stability and minimal dispersion error. Due to the remarkable features such as single and multi-mode filtering, tunable resonant frequency, and variable Q-factor, the filter topologies proposed here can find applications in more complex designs, including optical sensors, demultiplexers, splitters, couplers, and so on.</div></div>","PeriodicalId":21151,"journal":{"name":"Results in Optics","volume":"21 ","pages":"Article 100919"},"PeriodicalIF":3.0,"publicationDate":"2025-10-14","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145323977","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2025-10-14DOI: 10.1016/j.rio.2025.100917
Ahmed Alqurashi , Sayeeda Khanam , Esam Y.O. Zafar , Ahmed J.A. Al-Gburi
This paper presents a novel dual-band terahertz (THz) metamaterial absorber based on a symmetric dual-ring cross-stub (SDR-CS) resonator, designed for high-sensitivity permittivity sensing. The absorber, composed of aluminum resonators and a polyamide substrate, features a compact unit cell of 80 × 80 μm with rotational symmetry. It exhibits two strong absorption peaks at 1.26 THz and 2.29 THz with near-unity absorption. Detailed electromagnetic simulations reveal the physical mechanisms underpinning the dual-band response and confirm polarization insensitivity and angular stability up to 60° incidence under TE and TM polarizations. Crucially, the device demonstrates excellent sensing performance for refractive indices in the range 1.0–3.162, achieving sensitivities of 0.148 THz/RIU (148 GHz/RIU) and 0.28 THz/RIU (280 GHz/RIU) at the lower and higher resonance frequencies, respectively. The quality factors (Q) are 32.3 and 39.3, resulting in figure-of-merits (FOM) of 39.3 and 32.3 RIU–1, outperforming many reported metamaterial sensors with larger sizes or more complex materials. These attributes underscore the absorber’s potential as a compact, efficient, and highly sensitive platform for THz permittivity sensing with applications in biomedical diagnostics, chemical identification, and environmental monitoring.
{"title":"A symmetric dual-ring cross stub based dual-band THz metamaterial absorber design for permittivity sensing applications","authors":"Ahmed Alqurashi , Sayeeda Khanam , Esam Y.O. Zafar , Ahmed J.A. Al-Gburi","doi":"10.1016/j.rio.2025.100917","DOIUrl":"10.1016/j.rio.2025.100917","url":null,"abstract":"<div><div>This paper presents a novel dual-band terahertz (THz) metamaterial absorber based on a symmetric dual-ring cross-stub (SDR-CS) resonator, designed for high-sensitivity permittivity sensing. The absorber, composed of aluminum resonators and a polyamide substrate, features a compact unit cell of 80 × 80 μm with rotational symmetry. It exhibits two strong absorption peaks at 1.26 THz and 2.29 THz with near-unity absorption. Detailed electromagnetic simulations reveal the physical mechanisms underpinning the dual-band response and confirm polarization insensitivity and angular stability up to 60° incidence under TE and TM polarizations. Crucially, the device demonstrates excellent sensing performance for refractive indices in the range 1.0–3.162, achieving sensitivities of 0.148 THz/RIU (148 GHz/RIU) and 0.28 THz/RIU (280 GHz/RIU) at the lower and higher resonance frequencies, respectively. The quality factors (Q) are 32.3 and 39.3, resulting in figure-of-merits (FOM) of 39.3 and 32.3 RIU–1, outperforming many reported metamaterial sensors with larger sizes or more complex materials. These attributes underscore the absorber’s potential as a compact, efficient, and highly sensitive platform for THz permittivity sensing with applications in biomedical diagnostics, chemical identification, and environmental monitoring.</div></div>","PeriodicalId":21151,"journal":{"name":"Results in Optics","volume":"21 ","pages":"Article 100917"},"PeriodicalIF":3.0,"publicationDate":"2025-10-14","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145360991","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2025-10-14DOI: 10.1016/j.rio.2025.100918
Rania Hamdy Elabd , Ahmed J.A. Al-Gburi , Amany A. Megahed
This research presents a wideband (WB) 1 × 2 tree-shaped fractal antenna (TFA) array designed for sub-6 GHz 5G applications, featuring sidelobe level (SLL) reduction and gain enhancement. The array consists of two linearly arranged TFAs combined with a Wilkinson power divider (WPD) using a single-feed configuration. The WPD is selected due to its wide bandwidth, strong suppression factor, compact size, simple structure, excellent port isolation, and low insertion loss. A single TFA element, fabricated on a Rogers RT5880 substrate with a relative permittivity of 2.2 and a thickness of 1.57 mm, has dimensions of 38.5 × 49.5 mm2. It operates from 2.2 GHz to beyond 5 GHz, achieving a gain of 2.2–4.5 dBi. The proposed 1 × 2 array layout measures 76.5 × 81.36 mm2 and employs defected ground structure (DGS) and stub-loading techniques to suppress SLL and enhance gain. The array achieves a reflection coefficient better than –25 dB and an SLL of –13.2 dB. At the resonance frequency of 3.5 GHz, the gain improves significantly, rising from 3.2 dBi (single element) to 7.5 dBi (array). Simulated and experimental results confirm excellent agreement, validating the effectiveness of the proposed design.
{"title":"Wideband 1 × 2 tree-shaped fractal antenna array with gain enhancement and sidelobe level reduction for sub-6 GHz 5G applications","authors":"Rania Hamdy Elabd , Ahmed J.A. Al-Gburi , Amany A. Megahed","doi":"10.1016/j.rio.2025.100918","DOIUrl":"10.1016/j.rio.2025.100918","url":null,"abstract":"<div><div>This research presents a wideband (WB) 1 × 2 tree-shaped fractal antenna (TFA) array designed for sub-6 GHz 5G applications, featuring sidelobe level (SLL) reduction and gain enhancement. The array consists of two linearly arranged TFAs combined with a Wilkinson power divider (WPD) using a single-feed configuration. The WPD is selected due to its wide bandwidth, strong suppression factor, compact size, simple structure, excellent port isolation, and low insertion loss. A single TFA element, fabricated on a Rogers RT5880 substrate with a relative permittivity of 2.2 and a thickness of 1.57 mm, has dimensions of 38.5 × 49.5 mm<sup>2</sup>. It operates from 2.2 GHz to beyond 5 GHz, achieving a gain of 2.2–4.5 dBi. The proposed 1 × 2 array layout measures 76.5 × 81.36 mm<sup>2</sup> and employs defected ground structure (DGS) and stub-loading techniques to suppress SLL and enhance gain. The array achieves a reflection coefficient better than –25 dB and an SLL of –13.2 dB. At the resonance frequency of 3.5 GHz, the gain improves significantly, rising from 3.2 dBi (single element) to 7.5 dBi (array). Simulated and experimental results confirm excellent agreement, validating the effectiveness of the proposed design.</div></div>","PeriodicalId":21151,"journal":{"name":"Results in Optics","volume":"21 ","pages":"Article 100918"},"PeriodicalIF":3.0,"publicationDate":"2025-10-14","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145360992","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}