Pub Date : 2024-10-21DOI: 10.1140/epjp/s13360-024-05723-w
Zouhour Rhaim, Fraj Echouchene, Sabra Habli, Mohamed Hichem Gazzah, Mohammed A. Albedah, Hafedh Belmabrouk
This work integrates PC1D simulation, Box–Behnken design (BBD), and machine learning models (artificial neural network—ANN and particle swarm optimization-artificial neural network—PSO-ANN) to optimize monocrystalline silicon solar cells. Using the global desirability function, the optimal efficiency of 23.29% is obtained under certain conditions: p-type doping concentration (3.32 × 1017 cm−3), n-type doping concentration (6 × 1017 cm−3), textured wafer pyramid height (1 µm), textured wafer pyramid angle (80.67°), and temperature (20 °C). Notably, the PSO-ANN model outperforms the ANN model with an RMSE of 0.0149 and a correlation coefficient of 0.9997. This study demonstrates the effectiveness of advanced modeling and machine learning in increasing solar cell efficiency and highlights the superior performance of the PSO-ANN model.
{"title":"Optimization of monocrystalline silicon solar cell using Box–Behnken design and machine learning models","authors":"Zouhour Rhaim, Fraj Echouchene, Sabra Habli, Mohamed Hichem Gazzah, Mohammed A. Albedah, Hafedh Belmabrouk","doi":"10.1140/epjp/s13360-024-05723-w","DOIUrl":"10.1140/epjp/s13360-024-05723-w","url":null,"abstract":"<div><p>This work integrates PC1D simulation, Box–Behnken design (BBD), and machine learning models (artificial neural network—ANN and particle swarm optimization-artificial neural network—PSO-ANN) to optimize monocrystalline silicon solar cells. Using the global desirability function, the optimal efficiency of 23.29% is obtained under certain conditions: <i>p</i>-type doping concentration (3.32 × 10<sup>17</sup> cm<sup>−3</sup>), n-type doping concentration (6 × 10<sup>17</sup> cm<sup>−3</sup>), textured wafer pyramid height (1 µm), textured wafer pyramid angle (80.67°), and temperature (20 °C). Notably, the PSO-ANN model outperforms the ANN model with an RMSE of 0.0149 and a correlation coefficient of 0.9997. This study demonstrates the effectiveness of advanced modeling and machine learning in increasing solar cell efficiency and highlights the superior performance of the PSO-ANN model.</p></div>","PeriodicalId":792,"journal":{"name":"The European Physical Journal Plus","volume":null,"pages":null},"PeriodicalIF":2.8,"publicationDate":"2024-10-21","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://link.springer.com/content/pdf/10.1140/epjp/s13360-024-05723-w.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142453047","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Making use of Hadamard-gate transformations and controlled-NOT transformations, we construct a seven-particle maximally entangled state, and obtain a ((2N+1))-particle ((N>3)) maximally entangled state through this construction method. Then, using this seven-particle entangled state to serve as quantum channel, we suggest a three-party cyclic protocol for cloning three different unknown single-particle states with help of the state preparer and the permission of the controller. The first phase of this protocol needs a controlled cyclic quantu teleportation (CCQT), where Alice transmits an arbitrary unknown single-particle state to Bob, Bob teleports an arbitrary unknown single-particle state to Charlie, meanwhile, Charlie also convey an arbitrary unknown single-particle state to Alice under the consent of the controller. In the second phase, after receiving the three-particle measurement result from the preparer, three different unknown single-qubit states or their orthogonal complement states are cloned simultaneously and probabilistically at the positions of Alice, Bob, and Charlie respectively. Subsequently, we will extend the above three-party cyclic protocol to the case of (2N + 1)-party loops by exploiting the (2N + 1)-particle maximally entangled state act as quantum channel. Additionally, taking the controlled three-party cyclic protocol through non-maximally entangled channel as an example, we analyze the assisted cloning protocol for arbitrary unknown single-particle states from three perspectives: projective measurement, positive operator-value measurement (POVM), and generalized Bell-state measurement. We also point out that by increasing the number of state preparers or controllers, the above schemes can be promoted to meet the needs of future versatile quantum networks.
{"title":"Controlled cyclic assisted cloning of arbitrary unknown single-particle states","authors":"Nueraminaimu Maihemuti, Jiayin Peng, Yimamujiang Aisan, Jiangang Tang","doi":"10.1140/epjp/s13360-024-05698-8","DOIUrl":"10.1140/epjp/s13360-024-05698-8","url":null,"abstract":"<div><p>Making use of Hadamard-gate transformations and controlled-NOT transformations, we construct a seven-particle maximally entangled state, and obtain a <span>((2N+1))</span>-particle (<span>(N>3)</span>) maximally entangled state through this construction method. Then, using this seven-particle entangled state to serve as quantum channel, we suggest a three-party cyclic protocol for cloning three different unknown single-particle states with help of the state preparer and the permission of the controller. The first phase of this protocol needs a controlled cyclic quantu teleportation (CCQT), where Alice transmits an arbitrary unknown single-particle state to Bob, Bob teleports an arbitrary unknown single-particle state to Charlie, meanwhile, Charlie also convey an arbitrary unknown single-particle state to Alice under the consent of the controller. In the second phase, after receiving the three-particle measurement result from the preparer, three different unknown single-qubit states or their orthogonal complement states are cloned simultaneously and probabilistically at the positions of Alice, Bob, and Charlie respectively. Subsequently, we will extend the above three-party cyclic protocol to the case of (2N + 1)-party loops by exploiting the (2N + 1)-particle maximally entangled state act as quantum channel. Additionally, taking the controlled three-party cyclic protocol through non-maximally entangled channel as an example, we analyze the assisted cloning protocol for arbitrary unknown single-particle states from three perspectives: projective measurement, positive operator-value measurement (POVM), and generalized Bell-state measurement. We also point out that by increasing the number of state preparers or controllers, the above schemes can be promoted to meet the needs of future versatile quantum networks.</p></div>","PeriodicalId":792,"journal":{"name":"The European Physical Journal Plus","volume":null,"pages":null},"PeriodicalIF":2.8,"publicationDate":"2024-10-21","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142453050","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 : 2024-10-21DOI: 10.1140/epjp/s13360-024-05722-x
Minxiu Yan, Peng Du
Multibutterfly memristive chaotic systems (MMCSs) exhibit intricate multistable behavior and heightened randomness, making them highly advantageous for secure communications and image encryption. The paper provides a new five-dimensional chaotic system that incorporates two memristors into a 3D chaotic framework, leading to the creation of multibutterfly chaotic attractors. The quantity of multibutterfly chaotic attractors is capable of being managed by varying the parameters (mathrm M) and (mathrm N). We conduct an in-depth analysis of the five-dimensional MMCS dynamics through methods like Lyapunov exponents, Poincare maps, phase diagrams, and bifurcation diagrams. We depicted the basin of attraction for exploring the system’s coexisting attractors. Furthermore, the five-dimensional MMCS exhibits the coexisting attractors through variations in the initial values. By tuning parameters (k_{1}) and (k_{2}), the system’s amplitude can be adjusted. To validate the practical applicability of this system, we design a chaotic circuit based on the five-dimensional MMCS. The system is implemented on a Cyclone IV E series platform with the EP4CE15F23C8N FPGA as the primary chip. The FPGA implementation results align numerical simulations, confirming the practical applicability of the multibutterfly memristive chaotic circuit.
多蝶形忆阻器混沌系统(MMCS)表现出复杂的多稳态行为和更高的随机性,使其在安全通信和图像加密方面极具优势。本文提供了一种新的五维混沌系统,将两个忆阻器纳入三维混沌框架,从而产生了多蝶形混沌吸引子。多蝶形混沌吸引子的数量可以通过改变参数((mathrm M) 和 ((mathrm N) )来管理。我们通过Lyapunov指数、Poincare图、相图和分岔图等方法对五维MMCS动力学进行了深入分析。我们描绘了吸引盆地,以探索系统的共存吸引子。此外,五维 MMCS 通过初始值的变化展示了共存吸引子。通过调整参数 (k_{1}) 和 (k_{2}),可以调整系统的振幅。为了验证该系统的实际应用性,我们设计了一个基于五维 MMCS 的混沌电路。该系统在 Cyclone IV E 系列平台上实现,主芯片为 EP4CE15F23C8N FPGA。FPGA 实现结果与数值仿真结果一致,证实了多蝶形忆阻式混沌电路的实用性。
{"title":"Design and FPGA realization of memristive multibutterfly chaotic system featuring coexisting attractors and complex multistability behavior","authors":"Minxiu Yan, Peng Du","doi":"10.1140/epjp/s13360-024-05722-x","DOIUrl":"10.1140/epjp/s13360-024-05722-x","url":null,"abstract":"<div><p>Multibutterfly memristive chaotic systems (MMCSs) exhibit intricate multistable behavior and heightened randomness, making them highly advantageous for secure communications and image encryption. The paper provides a new five-dimensional chaotic system that incorporates two memristors into a 3D chaotic framework, leading to the creation of multibutterfly chaotic attractors. The quantity of multibutterfly chaotic attractors is capable of being managed by varying the parameters <span>(mathrm M)</span> and <span>(mathrm N)</span>. We conduct an in-depth analysis of the five-dimensional MMCS dynamics through methods like Lyapunov exponents, Poincare maps, phase diagrams, and bifurcation diagrams. We depicted the basin of attraction for exploring the system’s coexisting attractors. Furthermore, the five-dimensional MMCS exhibits the coexisting attractors through variations in the initial values. By tuning parameters <span>(k_{1})</span> and <span>(k_{2})</span>, the system’s amplitude can be adjusted. To validate the practical applicability of this system, we design a chaotic circuit based on the five-dimensional MMCS. The system is implemented on a Cyclone IV E series platform with the EP4CE15F23C8N FPGA as the primary chip. The FPGA implementation results align numerical simulations, confirming the practical applicability of the multibutterfly memristive chaotic circuit.</p></div>","PeriodicalId":792,"journal":{"name":"The European Physical Journal Plus","volume":null,"pages":null},"PeriodicalIF":2.8,"publicationDate":"2024-10-21","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142453046","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 : 2024-10-21DOI: 10.1007/s00340-024-08344-4
Titu Thomas, V. P. N Nampoori, Manu Vaishakh
The investigation of the thermo-optic characteristics of a material is vital in understanding the nonradiative relaxation processes occurring within the sample. Pyrromethene 567 a member of the laser dye family, has gained significant attention due to its excellent photo-physical characteristics, such as excellent laser efficiency, photostability, and quantum yield. The investigation of the photothermal studies in Pyrromethene 567 remains unexplored. Herein, a dual-beam thermal lens technique was performed to analyze the thermal lensing behaviour of Pyrromethene 567 in various solvents. The thermal diffusivity of Pyrromethene 567 in different solvents was calculated. There were no previous reports measuring the thermal diffusivity of Pyrromethene 567 dye. Thermal lens spectroscopy offers several advantages over conventional techniques because of its high sensitivity. The work also discusses the factors that influence the thermal lens signal in Pyrromethene 567. The influence of detector positioning, chopper frequency, and sample positioning, on thermal lens measurements was discussed. Additionally, the thermal lens experiments should be performed at intensities where diffraction patterns due to spatial self-phase modulation are absent to minimise experimental errors.
{"title":"Investigating the thermal diffusivity of Pyrromethene 567 in different solvents using dual beam thermal lens spectroscopy","authors":"Titu Thomas, V. P. N Nampoori, Manu Vaishakh","doi":"10.1007/s00340-024-08344-4","DOIUrl":"10.1007/s00340-024-08344-4","url":null,"abstract":"<div><p>The investigation of the thermo-optic characteristics of a material is vital in understanding the nonradiative relaxation processes occurring within the sample. Pyrromethene 567 a member of the laser dye family, has gained significant attention due to its excellent photo-physical characteristics, such as excellent laser efficiency, photostability, and quantum yield. The investigation of the photothermal studies in Pyrromethene 567 remains unexplored. Herein, a dual-beam thermal lens technique was performed to analyze the thermal lensing behaviour of Pyrromethene 567 in various solvents. The thermal diffusivity of Pyrromethene 567 in different solvents was calculated. There were no previous reports measuring the thermal diffusivity of Pyrromethene 567 dye. Thermal lens spectroscopy offers several advantages over conventional techniques because of its high sensitivity. The work also discusses the factors that influence the thermal lens signal in Pyrromethene 567. The influence of detector positioning, chopper frequency, and sample positioning, on thermal lens measurements was discussed. Additionally, the thermal lens experiments should be performed at intensities where diffraction patterns due to spatial self-phase modulation are absent to minimise experimental errors.</p></div>","PeriodicalId":474,"journal":{"name":"Applied Physics B","volume":null,"pages":null},"PeriodicalIF":2.0,"publicationDate":"2024-10-21","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://link.springer.com/content/pdf/10.1007/s00340-024-08344-4.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142453054","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}