Pub Date : 2024-06-22DOI: 10.1016/j.rio.2024.100720
Clyde Varner , Angela Davis , Ashok K. Batra, Padmaja Guggilla
This study explores the impact of CaTiO3 and LiNbO3 crystals on the optical and dielectric properties of polyvinylidene fluoride (PVDF) films. Our investigation employs UV–Visible Spectroscopy to characterize the n-π* C-F related electronic transition within the PVDF matrix. We find that CaTiO3 crystals significantly decrease the composite’s band gap and dielectric properties, enhancing its electronic and optical attributes. Conversely, LiNbO3 crystals increase the band gap energy. These variations align with observed DC conductivity changes, suggesting novel functionalities for optoelectronic, sensing, and energy storage applications.
{"title":"Optical band gap engineering and comparison of conductivity of CaTiO3 and LiNbO3 doped PVDF films","authors":"Clyde Varner , Angela Davis , Ashok K. Batra, Padmaja Guggilla","doi":"10.1016/j.rio.2024.100720","DOIUrl":"https://doi.org/10.1016/j.rio.2024.100720","url":null,"abstract":"<div><p>This study explores the impact of CaTiO<sub>3</sub> and LiNbO<sub>3</sub> crystals on the optical and dielectric properties of polyvinylidene fluoride (PVDF) films. Our investigation employs UV–Visible Spectroscopy to characterize the n-π* C-F related electronic transition within the PVDF matrix. We find that CaTiO<sub>3</sub> crystals significantly decrease the composite’s band gap and dielectric properties, enhancing its electronic and optical attributes. Conversely, LiNbO<sub>3</sub> crystals increase the band gap energy. These variations align with observed DC conductivity changes, suggesting novel functionalities for optoelectronic, sensing, and energy storage applications.</p></div>","PeriodicalId":21151,"journal":{"name":"Results in Optics","volume":"16 ","pages":"Article 100720"},"PeriodicalIF":0.0,"publicationDate":"2024-06-22","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.sciencedirect.com/science/article/pii/S2666950124001172/pdfft?md5=6c1a6aeb0f02fa17be880e241f502307&pid=1-s2.0-S2666950124001172-main.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141444623","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
In this article, we used modern technologies to teach the topic of nanomaterials and nanotechnologies. One of the main tasks of the development of modern nanotechnologies and nanomaterials is one of the main tasks of the development of nanoscale solid, liquid and gas phase structures and systems.
{"title":"Use of educational technologies in teaching the basics of nanophysics, nanomaterials and nanotechnologies","authors":"Dilfuza Begmatova , Husan Eshkuvatov , Nuraddin Abdullayev , Nasiba Xodjayeva , Oqila Suvonova , Javlon Ishtayev","doi":"10.1016/j.rio.2024.100717","DOIUrl":"https://doi.org/10.1016/j.rio.2024.100717","url":null,"abstract":"<div><p>In this article, we used modern technologies to teach the topic of nanomaterials and nanotechnologies. One of the main tasks of the development of modern nanotechnologies and nanomaterials is one of the main tasks of the development of nanoscale solid, liquid and gas phase structures and systems.</p></div>","PeriodicalId":21151,"journal":{"name":"Results in Optics","volume":"16 ","pages":"Article 100717"},"PeriodicalIF":0.0,"publicationDate":"2024-06-21","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.sciencedirect.com/science/article/pii/S2666950124001147/pdfft?md5=83f817babde8cc8e0202b957989afd46&pid=1-s2.0-S2666950124001147-main.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141444642","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-06-18DOI: 10.1016/j.rio.2024.100719
Behnaz Rashidi , Ali Soldoozy , Amir Ali Mohammad Khani , Ilghar Rezaei , Sadegh Biabanifard , Toktam Aghaee
A new geometrical vision for a graphene-based THz wave absorber is investigated in this work. A high-performance THz absorber is proposed to exploit complementary conventional periodic arrays of graphene disks. The equivalent circuit model is modified to take account of the complement pattern. The absorber works in two different operational modes based on chemical potential values. One mode shows absorption around 1 THz while the other one expresses perfect absorption at 6 THz and 9 THz. Such a considerable shifting ability via gate stimulations makes the proposed absorber an ideal block for reconfigurable metasurface. The comparison between the circuit model and full-wave simulation verifies an excellent match while ample sensitivity analysis are reported to show the reliability of the proposed switchable THz absorber.
{"title":"Switchable THz wave absorber based on disks and its complement graphene surfaces","authors":"Behnaz Rashidi , Ali Soldoozy , Amir Ali Mohammad Khani , Ilghar Rezaei , Sadegh Biabanifard , Toktam Aghaee","doi":"10.1016/j.rio.2024.100719","DOIUrl":"https://doi.org/10.1016/j.rio.2024.100719","url":null,"abstract":"<div><p>A new geometrical vision for a graphene-based THz wave absorber is investigated in this work. A high-performance THz absorber is proposed to exploit complementary conventional periodic arrays of graphene disks. The equivalent circuit model is modified to take account of the complement pattern. The absorber works in two different operational modes based on chemical potential values. One mode shows absorption around 1 THz while the other one expresses perfect absorption at 6 THz and 9 THz. Such a considerable shifting ability via gate stimulations makes the proposed absorber an ideal block for reconfigurable metasurface. The comparison between the circuit model and full-wave simulation verifies an excellent match while ample sensitivity analysis are reported to show the reliability of the proposed switchable THz absorber.</p></div>","PeriodicalId":21151,"journal":{"name":"Results in Optics","volume":"16 ","pages":"Article 100719"},"PeriodicalIF":0.0,"publicationDate":"2024-06-18","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.sciencedirect.com/science/article/pii/S2666950124001160/pdfft?md5=777fb9f4bdb911d4479bfdbd2f2bf732&pid=1-s2.0-S2666950124001160-main.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141434014","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-06-12DOI: 10.1016/j.rio.2024.100715
Sandra Martínez , Oscar E. Martínez
In this article we define Discrete SUPPOSe, a new and faster version of the single shot super resolution SUPPOSe (Superposition of virtual point sources) method. The SUPPOSe method for super-resolution of fluorescent microscope images relies in assuming that the sample source distribution can be modeled as a superposition of virtual point sources of equal intensities distributed in a continuous space, converting the ill posed deconvolution problem into a well posed one. In this work we present a faster new method that consists on discretizing the continuum problem, using a normalized covariance instead of a for the fitting function and hence transforming the convolution (the main computational time) into a multiplication, and modifying the mutation step of the genetic algorithm. We compare precision, accuracy, resolution and computation time. It is also shown that despite the spatial discretization in Discrete SUPPOSe similar figures for precision, accuracy and resolution are obtained. The algorithm was implemented in Matlab running on a CPU obtaining with a speed improvement factor of more than 15 for one image of 48 × 48 pixels. Processing images in parallel in a 16 cores CPU a 1Mpixel image is computed 240 times faster than the standard SUPPOSe in a 2600 core GPU. Experimental images were used to validate the method.
{"title":"Discrete SUPPOSe: A new, faster and accurate superresolution method for applications to fluorescence microscopy images","authors":"Sandra Martínez , Oscar E. Martínez","doi":"10.1016/j.rio.2024.100715","DOIUrl":"10.1016/j.rio.2024.100715","url":null,"abstract":"<div><p>In this article we define Discrete SUPPOSe, a new and faster version of the single shot super resolution SUPPOSe (Superposition of virtual point sources) method. The SUPPOSe method for super-resolution of fluorescent microscope images relies in assuming that the sample source distribution can be modeled as a superposition of virtual point sources of equal intensities distributed in a continuous space, converting the ill posed deconvolution problem into a well posed one. In this work we present a faster new method that consists on discretizing the continuum problem, using a normalized covariance instead of a <span><math><msup><mrow><mi>χ</mi></mrow><mrow><mn>2</mn></mrow></msup></math></span> for the fitting function and hence transforming the convolution (the main computational time) into a multiplication, and modifying the mutation step of the genetic algorithm. We compare precision, accuracy, resolution and computation time. It is also shown that despite the spatial discretization in Discrete SUPPOSe similar figures for precision, accuracy and resolution are obtained. The algorithm was implemented in Matlab running on a CPU obtaining with a speed improvement factor of more than 15 for one image of 48 × 48 pixels. Processing images in parallel in a 16 cores CPU a 1Mpixel image is computed 240 times faster than the standard SUPPOSe in a 2600 core GPU. Experimental images were used to validate the method.</p></div>","PeriodicalId":21151,"journal":{"name":"Results in Optics","volume":"16 ","pages":"Article 100715"},"PeriodicalIF":0.0,"publicationDate":"2024-06-12","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.sciencedirect.com/science/article/pii/S2666950124001123/pdfft?md5=da27dde52c5a75c094c1701c0873fd99&pid=1-s2.0-S2666950124001123-main.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141413044","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
The innovative, affordable assembled visible spectrophotometer employed in this study aims to analyze the absorption and emission of colorful metallic blends of colorful samples solution. It features a tungsten white light bulb source, an ammeter as a detection element, a digital voltmeter, a diffraction grating for light dispersion, a converging lens for light collimation, and filters of various wavelengths (blue, red, yellow, and yellow-green). The light bulb source was powered by a standard supply set at 6 V. Using metallic solutions of chromium chloride (CrCl3) and copper sulphate (CuSO4) with different filter wavelengths, the performance was assessed. The transmittance and absorbance of these metallic solution samples exhibit a linear relationship with approximately 3 % deviation compared to results from a commercial UV–VIS spectrophotometer (DR-6000). Similar investigations were conducted with equivalent quantities of CuSO4, CrCl3, and nickel chloride (NiCl2) solutions, showing a discrepancy ranging from 2 % to 8 % when compared with the commercial UV–VIS spectrophotometer. Therefore, in low-income countries like Ethiopia, colorful metallic solution samples can be effectively analyzed using the newly designed low-cost spectrophotometer.
{"title":"Low-cost visible spectrophotometer for detecting absorption and emission in metallic blends of colorful samples solution","authors":"Sewmehon Mengistie Workneh , Gashaw Alemu Dagnaw , Addis Mekonnen Adamu , Getasew Admasu Wubetu","doi":"10.1016/j.rio.2024.100703","DOIUrl":"https://doi.org/10.1016/j.rio.2024.100703","url":null,"abstract":"<div><p>The innovative, affordable assembled visible spectrophotometer employed in this study aims to analyze the absorption and emission of colorful metallic blends of colorful samples solution. It features a tungsten white light bulb source, an ammeter as a detection element, a digital voltmeter, a diffraction grating for light dispersion, a converging lens for light collimation, and filters of various wavelengths (blue, red, yellow, and yellow-green). The light bulb source was powered by a standard supply set at 6 V. Using metallic solutions of chromium chloride (CrCl<sub>3</sub>) and copper sulphate (CuSO<sub>4</sub>) with different filter wavelengths, the performance was assessed. The transmittance and absorbance of these metallic solution samples exhibit a linear relationship with approximately 3 % deviation compared to results from a commercial UV–VIS spectrophotometer (DR-6000). Similar investigations were conducted with equivalent quantities of CuSO<sub>4</sub>, CrCl<sub>3</sub>, and nickel chloride (NiCl<sub>2</sub>) solutions, showing a discrepancy ranging from 2 % to 8 % when compared with the commercial UV–VIS spectrophotometer. Therefore, in low-income countries like Ethiopia, colorful metallic solution samples can be effectively analyzed using the newly designed low-cost spectrophotometer.</p></div>","PeriodicalId":21151,"journal":{"name":"Results in Optics","volume":"16 ","pages":"Article 100703"},"PeriodicalIF":0.0,"publicationDate":"2024-06-06","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.sciencedirect.com/science/article/pii/S2666950124001007/pdfft?md5=5ca9019e5271c1fd93b3fd59bfe10774&pid=1-s2.0-S2666950124001007-main.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141292151","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-06-06DOI: 10.1016/j.rio.2024.100704
Talal M. Abdalkreem, H.C. Swart, R.E. Kroon
A novel technique was created to quickly evaluate the impact of various ratios on the efficiency of up-conversion emission using a combination of up-conversion nanophosphors (UCNPs) and gold nanoparticles (Au NPs). Four different types of Y2O3 UCNPs with different Er3+ or Er3+/Yb3+ doping, which affects the emission colour as well as the up-conversion mechanism, were prepared via the microwave-assisted hydrothermal method. Au NPs were produced independently using the reduction technique. Different ratios of UCNPs were mixed with the Au NPs in water. The mixed powder composites were extracted for analysis. X-ray powder diffraction was utilized to study the structure of UCNPs with and without Au NPs, while transmission electron microscopy was used to study the morphology and size of Au NPs. Absorption and up-conversion measurements were also made. The novel protocol allowed rapid evaluation of four different Y2O3 UCNPs of Er3+ and Er3+/Yb3+ doped with concentrations optimized for red and green emission over a range of Au/UCNP concentrations, which might usually be done in four separate studies. Despite the wide range of variables, only a decrease in UC emission was measured in the presence of Au NPs, suggesting that the conditions for plasmonic enhancement are limited and not easy to attain. In spite of this, in many phosphor/metal NP systems, the innovative prototyping process can enable quick assessment of possible plasmonic enhancement.
利用上转换纳米磷酸盐(UCNPs)和金纳米粒子(Au NPs)的组合,创建了一种新技术来快速评估各种比率对上转换发射效率的影响。通过微波辅助水热法制备了四种不同类型的 Y2O3 UCNPs,它们具有不同的 Er3+ 或 Er3+/Yb3+ 掺杂,这影响了发射颜色以及上转换机制。金纳米粒子是利用还原技术独立制备的。不同比例的 UCNPs 与 Au NPs 在水中混合。提取混合粉末复合材料进行分析。利用 X 射线粉末衍射来研究含有和不含 Au NPs 的 UCNPs 的结构,而透射电子显微镜则用于研究 Au NPs 的形态和尺寸。此外,还进行了吸收和上转换测量。这种新方案可以快速评估四种不同的 Y2O3 UCNPs,其中 Er3+ 和 Er3+/Yb3+ 的掺杂浓度在一定的 Au/UCNP 浓度范围内对红色和绿色发射进行了优化,而这通常需要进行四次单独的研究。尽管变量范围很广,但在 Au NPs 存在的情况下,仅测量到 UC 发射的减少,这表明等离子体增强的条件是有限的,而且不容易达到。尽管如此,在许多荧光粉/金属 NP 系统中,创新的原型制作过程可以快速评估可能的等离子增强效果。
{"title":"Novel protocol for rapid evaluation of plasmonic enhancement for up-converting phosphors applied to Y2O3 doped with Er3+ and Er3+/Yb3+","authors":"Talal M. Abdalkreem, H.C. Swart, R.E. Kroon","doi":"10.1016/j.rio.2024.100704","DOIUrl":"https://doi.org/10.1016/j.rio.2024.100704","url":null,"abstract":"<div><p>A novel technique was created to quickly evaluate the impact of various ratios on the efficiency of up-conversion emission using a combination of up-conversion nanophosphors (UCNPs) and gold nanoparticles (Au NPs). Four different types of Y<sub>2</sub>O<sub>3</sub> UCNPs with different Er<sup>3+</sup> or Er<sup>3+</sup>/Yb<sup>3+</sup> doping, which affects the emission colour as well as the up-conversion mechanism, were prepared via the microwave-assisted hydrothermal method. Au NPs were produced independently using the reduction technique. Different ratios of UCNPs were mixed with the Au NPs in water. The mixed powder composites were extracted for analysis. X-ray powder diffraction was utilized to study the structure of UCNPs with and without Au NPs, while transmission electron microscopy was used to study the morphology and size of Au NPs. Absorption and up-conversion measurements were also made. The novel protocol allowed rapid evaluation of four different Y<sub>2</sub>O<sub>3</sub> UCNPs of Er<sup>3+</sup> and Er<sup>3+</sup>/Yb<sup>3+</sup> doped with concentrations optimized for red and green emission over a range of Au/UCNP concentrations, which might usually be done in four separate studies. Despite the wide range of variables, only a decrease in UC emission was measured in the presence of Au NPs, suggesting that the conditions for plasmonic enhancement are limited and not easy to attain. In spite of this, in many phosphor/metal NP systems, the innovative prototyping process can enable quick assessment of possible plasmonic enhancement.</p></div>","PeriodicalId":21151,"journal":{"name":"Results in Optics","volume":"16 ","pages":"Article 100704"},"PeriodicalIF":0.0,"publicationDate":"2024-06-06","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.sciencedirect.com/science/article/pii/S2666950124001019/pdfft?md5=57129098f401381f844fd9813becf594&pid=1-s2.0-S2666950124001019-main.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141307914","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-06-05DOI: 10.1016/j.rio.2024.100709
Mahdi Rahmanpour, Alireza Erfanian, Ahmad Afifi, Mahdi Khaje, Mohammad Hossein Fahimifar
Single photon avalanche diode (SPAD) is used in quantum detectors. Quantum detectors are widely used in quantum communication. The quality of these detectors strongly affects the optimal performance of the system. The quality of single photon detectors depends on various parameters, which are usually presented in the SPAD specification. If these detectors are made by the manufacturer or evaluated by the user, there is a need for a method to determine and check its main parameters. In this paper, a simple test setup for extracting some of important parameters has been designed and introduced, which can be used practically. These parameters include Dark Count Rate (DCR), Photon Detection Efficiency (PDE), AfterPulse Probability (APP) and Dead time. In the presented design, an FPGA chip is used to measure the parameters. FPGA is responsible for the simultaneous control of the single photon source and the detector. The presented methods specify how to extract the desired parameters. The characterization methods and detailed formulas presented in this paper calculate SPAD parameters.
{"title":"Implementable methods for characterizing single photon avalanche diode parameters","authors":"Mahdi Rahmanpour, Alireza Erfanian, Ahmad Afifi, Mahdi Khaje, Mohammad Hossein Fahimifar","doi":"10.1016/j.rio.2024.100709","DOIUrl":"https://doi.org/10.1016/j.rio.2024.100709","url":null,"abstract":"<div><p>Single photon avalanche diode (SPAD) is used in quantum detectors. Quantum detectors are widely used in quantum communication. The quality of these detectors strongly affects the optimal performance of the system. The quality of single photon detectors depends on various parameters, which are usually presented in the SPAD specification. If these detectors are made by the manufacturer or evaluated by the user, there is a need for a method to determine and check its main parameters. In this paper, a simple test setup for extracting some of important parameters has been designed and introduced, which can be used practically. These parameters include Dark Count Rate (DCR), Photon Detection Efficiency (PDE), AfterPulse Probability (APP) and Dead time. In the presented design, an FPGA chip is used to measure the parameters. FPGA is responsible for the simultaneous control of the single photon source and the detector. The presented methods specify how to extract the desired parameters. The characterization methods and detailed formulas presented in this paper calculate SPAD parameters.</p></div>","PeriodicalId":21151,"journal":{"name":"Results in Optics","volume":"16 ","pages":"Article 100709"},"PeriodicalIF":0.0,"publicationDate":"2024-06-05","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.sciencedirect.com/science/article/pii/S2666950124001068/pdfft?md5=e77043acc9ac710eb3df0d7838764fd9&pid=1-s2.0-S2666950124001068-main.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141292152","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-06-04DOI: 10.1016/j.rio.2024.100710
Alex Midasala
A viable solution to detect the one-way speed of light anisotropy in linear motion is by using an Isosceles triangle-shaped design for the experimental setup, from which two light pulses from both ends of one of the triangle’s sides are sent to the same clock upon the detection of the incident and the reflected pulse, thereby evading the need for synchronization. The relativistic effects are taken into account in the timing measurements by incorporating the Lorentz transformation equations of length contraction and time dilation, which produces a non-null result for the time difference of the incident and the reflected pulse, and testing the equivalence of the one-way speed of light with the average of the roundtrip speed, independent of Einstein’s synchronization convention.
{"title":"Detecting the variance in the one-way light speed for linear motion","authors":"Alex Midasala","doi":"10.1016/j.rio.2024.100710","DOIUrl":"https://doi.org/10.1016/j.rio.2024.100710","url":null,"abstract":"<div><p>A viable solution to detect the one-way speed of light anisotropy in linear motion is by using an Isosceles triangle-shaped design for the experimental setup, from which two light pulses from both ends of one of the triangle’s sides are sent to the same clock upon the detection of the incident and the reflected pulse, thereby evading the need for synchronization. The relativistic effects are taken into account in the timing measurements by incorporating the Lorentz transformation equations of length contraction and time dilation, which produces a non-null result for the time difference of the incident and the reflected pulse, and testing the equivalence of the one-way speed of light with the average of the roundtrip speed, independent of Einstein’s synchronization convention.</p></div>","PeriodicalId":21151,"journal":{"name":"Results in Optics","volume":"16 ","pages":"Article 100710"},"PeriodicalIF":0.0,"publicationDate":"2024-06-04","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.sciencedirect.com/science/article/pii/S266695012400107X/pdfft?md5=e7dd0bb198e32395a9557299461b5e0a&pid=1-s2.0-S266695012400107X-main.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141292153","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-06-04DOI: 10.1016/j.rio.2024.100708
Reem A. Hussien , Safa Salam Radhi , Fareed F. Rashid , Essam N. Abdulla , A.K. Abass
With the increasing demand for image transmission in various fields including medical, military and multimedia, the security of information contained on these images has become a standing problem.. This work provides information security for images transfer for 160 Gbps over 140 km optical fiber link. Image encryption and decryption is maintained by applying blowfish algorithm via MATLAB software with the adaption of OptiSystem software to examine data transmission over 16 channels WDM system.. The proposed algorithm has provide a large key space, resistivity to differential attacks, anti-differential attack, brute-force attack and less correlation between adjacent pixels However, channel dispersion and signal attenuation has been controlled with the adaption of symmetric dispersion compensation map and an erbium doped fiber amplifier (EDFA) at the end of the fiber link. Our WDM system design has reached a high figure of merit of about 22,400 as compared with different previous schemes. Moreover, to provoke the power of the proposed cipher algorithm, key space, correlations, histogram analysis and different security analysis has been studied and compared with other algorithms.
{"title":"Design and performance analysis of secure optical communication system by implementing blowfish cipher algorithm","authors":"Reem A. Hussien , Safa Salam Radhi , Fareed F. Rashid , Essam N. Abdulla , A.K. Abass","doi":"10.1016/j.rio.2024.100708","DOIUrl":"https://doi.org/10.1016/j.rio.2024.100708","url":null,"abstract":"<div><p>With the increasing demand for image transmission in various fields including medical, military and multimedia, the security of information contained on these images has become a standing problem.. This work provides information security for images transfer for 160 Gbps over 140 km optical fiber link. Image encryption and decryption is maintained by applying blowfish algorithm via MATLAB software with the adaption of OptiSystem software to examine data transmission over 16 channels WDM system.. The proposed algorithm has provide a large key space, resistivity to differential attacks, anti-differential attack, brute-force attack and less correlation between adjacent pixels However, channel dispersion and signal attenuation has been controlled with the adaption of symmetric dispersion compensation map and an erbium doped fiber amplifier (EDFA) at the end of the fiber link. Our WDM system design has reached a high figure of merit of about 22,400 as compared with different previous schemes. Moreover, to provoke the power of the proposed cipher algorithm, key space, correlations, histogram analysis and different security analysis has been studied and compared with other algorithms.</p></div>","PeriodicalId":21151,"journal":{"name":"Results in Optics","volume":"16 ","pages":"Article 100708"},"PeriodicalIF":0.0,"publicationDate":"2024-06-04","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.sciencedirect.com/science/article/pii/S2666950124001056/pdfft?md5=0b79e1d9ecad61fe55c1c651cf826296&pid=1-s2.0-S2666950124001056-main.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141292150","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-06-03DOI: 10.1016/j.rio.2024.100701
Farsad Heidari, Ahvan Sharifi
This article introduces a novel two-dimensional photonic crystal biosensor designed for the detection of various cancer cell types and the verification of associated parameters. The proposed structure features a circular resonator nanoring with a sensing region at its center, facilitating the connection with cancer cells. The sensor has been tested with a diverse range of cancer cell types including skin, cervical, blood, adrenal, and two subtypes of breast cancer cells (Sort 1 and Sort 2). All outputs of the structure were studied at two different wavelengths and its parameters were analyzed separately. The best quality factor obtained for normal and abnormal cells of the target structure is 13,353 and 3053, respectively. Due to its high-quality factor and high FOM and low DL, this sensor has an acceptable sensitivity of 214.28(nm/RIU). FOM and DL in this sensor are equal to 172.35(RIU−1) and 5.80 × 10−4(RIU), respectively. The resonant wavelength shift of this structure is a relatively good value due to the coupling distance between the input wave and the resonator nanoring.
{"title":"Design and simulation of a resonant nanoring-based two-dimensional photonic crystal biosensor for cancer cell detection","authors":"Farsad Heidari, Ahvan Sharifi","doi":"10.1016/j.rio.2024.100701","DOIUrl":"10.1016/j.rio.2024.100701","url":null,"abstract":"<div><p>This article introduces a novel two-dimensional photonic crystal biosensor designed for the detection of various cancer cell types and the verification of associated parameters. The proposed structure features a circular resonator nanoring with a sensing region at its center, facilitating the connection with cancer cells. The sensor has been tested with a diverse range of cancer cell types including skin, cervical, blood, adrenal, and two subtypes of breast cancer cells (Sort 1 and Sort 2). All outputs of the structure were studied at two different wavelengths and its parameters were analyzed separately. The best quality factor obtained for normal and abnormal cells of the target structure is 13,353 and 3053, respectively. Due to its high-quality factor and high FOM and low DL, this sensor has an acceptable sensitivity of 214.28(nm/RIU). FOM and DL in this sensor are equal to 172.35(RIU<sup>−1</sup>) and 5.80 × 10<sup>−4</sup>(RIU), respectively. The resonant wavelength shift of this structure is a relatively good value due to the coupling distance between the input wave and the resonator nanoring.</p></div>","PeriodicalId":21151,"journal":{"name":"Results in Optics","volume":"16 ","pages":"Article 100701"},"PeriodicalIF":0.0,"publicationDate":"2024-06-03","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.sciencedirect.com/science/article/pii/S2666950124000981/pdfft?md5=a7a6e65bb73df50fe0ef2b33afdd53bb&pid=1-s2.0-S2666950124000981-main.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141276636","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}