Pub Date : 2024-05-27DOI: 10.1007/s11468-024-02358-6
Avijit Chamoli, Devki Nandan Gupta, Vijay Kumar
The excitation of surface plasma waves (SPWs) by the interaction of lasers with a metal surface can generate terahertz (THz) radiation at metal-free space interface. We present a novel model for THz radiation generation using two lasers, beating at a metal surface in the presence of a magnetic field. This interaction resonantly excites a SPW, leading to the generation of THz plasmon. Two co-planar lasers having frequency difference of effective electron plasma frequency exert a ponderomotive force to the skin layer of the metal, which induces an oscillatory velocity to the surface electrons and drives the surface plasma waves. The transverse component of the SPW leads to the generation of electromagnetic radiation at THz frequency. Furthermore, the applied external magnetic enhances the transverse current associated with the SPWs. As a result, the THz field strength increased significantly. An expression of THz radiation field is obtained and the field scaling with the magnetic field has been estimated. Our results reported a better THz conversion efficiency for an optimized magnetic field strength. The result of this work delivers a plausible approach to generate THz radiation field from a laser interaction with a metallic surface.
{"title":"Terahertz Surface Plasmon Generation from Laser Interaction with a Magnetized Metallic Surface","authors":"Avijit Chamoli, Devki Nandan Gupta, Vijay Kumar","doi":"10.1007/s11468-024-02358-6","DOIUrl":"https://doi.org/10.1007/s11468-024-02358-6","url":null,"abstract":"<p>The excitation of surface plasma waves (SPWs) by the interaction of lasers with a metal surface can generate terahertz (THz) radiation at metal-free space interface. We present a novel model for THz radiation generation using two lasers, beating at a metal surface in the presence of a magnetic field. This interaction resonantly excites a SPW, leading to the generation of THz plasmon. Two co-planar lasers having frequency difference of effective electron plasma frequency exert a ponderomotive force to the skin layer of the metal, which induces an oscillatory velocity to the surface electrons and drives the surface plasma waves. The transverse component of the SPW leads to the generation of electromagnetic radiation at THz frequency. Furthermore, the applied external magnetic enhances the transverse current associated with the SPWs. As a result, the THz field strength increased significantly. An expression of THz radiation field is obtained and the field scaling with the magnetic field has been estimated. Our results reported a better THz conversion efficiency for an optimized magnetic field strength. The result of this work delivers a plausible approach to generate THz radiation field from a laser interaction with a metallic surface.</p>","PeriodicalId":736,"journal":{"name":"Plasmonics","volume":null,"pages":null},"PeriodicalIF":3.0,"publicationDate":"2024-05-27","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141166757","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"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}
We propose and demonstrate a compact optical fiber temperature sensor based on surface plasmon resonance with high sensitivity and high figure of merit. This optical fiber temperature sensor uses a new photonic crystal fiber designed by us, which is realized by coating a gold film on the polished plane of the photonic crystal fiber and coating the high thermo-optical coefficient material polydimethylsiloxane on the outer surface of the fiber. Small changes in the refractive index of the polydimethylsiloxane due to temperature variations will affect the plasmon pattern, which in turn leads to a change in the measured transmission spectrum. Our numerical results show that the maximum achievable temperature sensitivity of this optical fiber temperature sensor in the range of 60–100 °C is 38 nm/°C, and the maximum refractive index sensitivity and figure of merit are 84444.4 nm/RIU and 603.175 RIU−1, respectively. This is better than the existing various types of PCF temperature sensor. The proposed temperature sensor has the advantages of stable structure, ultra-high temperature sensitivity, and small size. It has good application potential in the field of high-precision temperature control, environmental temperature detecting.
{"title":"Ultrahigh Sensitivity Surface Plasmonic Resonance Temperature Sensor Based on Polydimethylsiloxane-Coated Photonic Crystal Fiber","authors":"Shaochun Fu, Wentao Jin, Longsheng Liu, Meng Song, Ying Guo, Hui Qi, Xiaohong Sun","doi":"10.1007/s11468-024-02359-5","DOIUrl":"https://doi.org/10.1007/s11468-024-02359-5","url":null,"abstract":"<p>We propose and demonstrate a compact optical fiber temperature sensor based on surface plasmon resonance with high sensitivity and high figure of merit. This optical fiber temperature sensor uses a new photonic crystal fiber designed by us, which is realized by coating a gold film on the polished plane of the photonic crystal fiber and coating the high thermo-optical coefficient material polydimethylsiloxane on the outer surface of the fiber. Small changes in the refractive index of the polydimethylsiloxane due to temperature variations will affect the plasmon pattern, which in turn leads to a change in the measured transmission spectrum. Our numerical results show that the maximum achievable temperature sensitivity of this optical fiber temperature sensor in the range of 60–100 °C is 38 nm/°C, and the maximum refractive index sensitivity and figure of merit are 84444.4 nm/RIU and 603.175 RIU<sup>−1</sup>, respectively. This is better than the existing various types of PCF temperature sensor. The proposed temperature sensor has the advantages of stable structure, ultra-high temperature sensitivity, and small size. It has good application potential in the field of high-precision temperature control, environmental temperature detecting.</p>","PeriodicalId":736,"journal":{"name":"Plasmonics","volume":null,"pages":null},"PeriodicalIF":3.0,"publicationDate":"2024-05-27","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141173512","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"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 : 2024-05-27DOI: 10.1007/s11468-024-02369-3
Ammar Armghan, Bo Bo Han, Dhruvik Agravat, Khaled Alqiab, Meshari Alsharari, Shobhit K. Patel
The design of surface plasmon resonance solar absorbers with graphene is demonstrated to study the solar absorbers of photonic devices. With the respective properties of each metal in this structure, the tungsten (W) layer is performed as a ground layer, chromium (Cr) is used to create the resonator design, and the titanium nitride (TiN) substrate layer is constructed between Cr and W layers, respectively. According to the advantages of graphene in making absorbers, a thin film of graphene is also constructed above TiN and below the Cr resonator design. To show the radiation effects in spectrums (between UV and NIR), the four highest wavelength numbers (in micrometers) are picked such as 0.4, 1.6, 1.8, and 2. According to the band range, the output absorption observes 97.2% at 0.7 µm, 95.35% at 1.730 µm, and 90.15% at 2.8 µm, respectively. In solar absorber performing, the first important thing before extracting the absorption rate is design construction, and we presented several stages of outputs for each construction to bring the final (complete) step. After exploring the design and thickness of each existing layer in the design, we can change the below and above parameters of the explored thickness in each layer (resonator, substrate, and ground). The variation can also be demonstrated in respective color plots to show the output radiation in different colors. In the calculating section of the absorption percentage in design, the air mass (AM) and graphene equations are also presented with the explanation of each symbol. The proposed sun-shaped design can be used in performing thermal processes such as water heating systems.
利用石墨烯设计表面等离子体共振太阳能吸收器,以研究光子设备的太阳能吸收器。根据该结构中每种金属各自的特性,钨(W)层用作地层,铬(Cr)用于创建谐振器设计,氮化钛(TiN)基底层分别构建在铬层和 W 层之间。根据石墨烯在制作吸收器方面的优势,还在 TiN 的上方和 Cr 谐振器设计的下方构建了一层石墨烯薄膜。为了显示光谱(紫外线和近红外之间)的辐射效应,选取了四个最高波长(以微米为单位),如 0.4、1.6、1.8 和 2。根据波段范围,输出吸收率在 0.7 微米处分别为 97.2%,在 1.730 微米处为 95.35%,在 2.8 微米处为 90.15%。在太阳能吸收器表演中,提取吸收率之前的第一件大事是设计构造,我们为每种构造提出了几个阶段的输出,以实现最后(完整)的步骤。在探索了设计中每个现有层的设计和厚度后,我们可以改变每个层(谐振器、基板和地面)中已探索厚度的下方和上方参数。这种变化还可以通过相应的彩色图来显示不同颜色的输出辐射。在设计中吸收百分比的计算部分,还介绍了空气质量(AM)和石墨烯方程,并对每个符号进行了解释。建议的太阳形状设计可用于热处理,如水加热系统。
{"title":"Graphene-Based Surface Plasmon Resonance–Based Solar Thermal Absorber Using Cr-TiN-W Multilayer Structure","authors":"Ammar Armghan, Bo Bo Han, Dhruvik Agravat, Khaled Alqiab, Meshari Alsharari, Shobhit K. Patel","doi":"10.1007/s11468-024-02369-3","DOIUrl":"https://doi.org/10.1007/s11468-024-02369-3","url":null,"abstract":"<p>The design of surface plasmon resonance solar absorbers with graphene is demonstrated to study the solar absorbers of photonic devices. With the respective properties of each metal in this structure, the tungsten (W) layer is performed as a ground layer, chromium (Cr) is used to create the resonator design, and the titanium nitride (TiN) substrate layer is constructed between Cr and W layers, respectively. According to the advantages of graphene in making absorbers, a thin film of graphene is also constructed above TiN and below the Cr resonator design. To show the radiation effects in spectrums (between UV and NIR), the four highest wavelength numbers (in micrometers) are picked such as 0.4, 1.6, 1.8, and 2. According to the band range, the output absorption observes 97.2% at 0.7 µm, 95.35% at 1.730 µm, and 90.15% at 2.8 µm, respectively. In solar absorber performing, the first important thing before extracting the absorption rate is design construction, and we presented several stages of outputs for each construction to bring the final (complete) step. After exploring the design and thickness of each existing layer in the design, we can change the below and above parameters of the explored thickness in each layer (resonator, substrate, and ground). The variation can also be demonstrated in respective color plots to show the output radiation in different colors. In the calculating section of the absorption percentage in design, the air mass (AM) and graphene equations are also presented with the explanation of each symbol. The proposed sun-shaped design can be used in performing thermal processes such as water heating systems.</p>","PeriodicalId":736,"journal":{"name":"Plasmonics","volume":null,"pages":null},"PeriodicalIF":3.0,"publicationDate":"2024-05-27","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141166758","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"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 : 2024-05-25DOI: 10.1007/s11468-024-02366-6
Uddipan Chowdhury, Shivam Nandy, Pushpak Mandi, Rupam Mukherjee, Amit Ranjan Maity, Samir Kumar, Partha Sona Maji
In this study we present a novel method for constructing a refractive-index sensor utilizing hybrid modes within a dual ‘Ag-photonic quasi-crystal’ geometry, adhering to the conventional Fibonacci sequence. The reflection spectrum of the geometry demonstrates the presence of three interconnected minima in reflectivity, occurring within the photonic-bandgap of a quasi-crystal. These hybrid modes emerge from the interplay between individual Tamm plasmon mode at the metal-photonic quasi crystal interface and the Fabry–Perot resonant cavity mode formed between two metal layers. The low wavelength dip (Mode-2) and high wavelength dip (Mode-3) display pronounced dispersive characteristics due to the substantial presence of mode-field in the sensing medium. Conversely, the mode situated between them (Mode-1) remains largely unaffected by variations in the refractive index of the sensing layer. Thus, our proposed method offers a wide range of wavelengths linked to Mode 2 and Mode 3, facilitating the concurrent utilization of dual wavelengths for sensor parameter analysis. We investigate the foundational parameters of a bio-photonic sensor, laying the foundation for a dual mode refractive-index sensing mechanism. At a normal angle of incidence, Mode -2 exhibits a maximum sensitivity of 401.4 nm/RIU and a Figure of Merit of 42.8 RIU-1. Meanwhile, for Mode -3, the highest sensitivity and Figure of Merit are 448.87 nm/RIU and 28.89 RIU-1, respectively. Additionally, we propose enhancing the hybrid-mode sensor characteristics by strategically optimizing the photonic quasi-crystal structures to increase the dispersion observed in hybrid Tamm plasmon modes, thus improving sensitivity. Utilization of the dual sensitive mode shows potential for enhancing modern biochemical sensors and optoelectronic devices, with possible applications in detecting diverse blood-related disorders distinguished by refractive index fluctuations in blood components.
{"title":"A Theoretical Study On Dual Sensitive Mode Refractive Index Sensor Utilizing Fibonacci Sequence-based Aperiodic Photonic Crystals","authors":"Uddipan Chowdhury, Shivam Nandy, Pushpak Mandi, Rupam Mukherjee, Amit Ranjan Maity, Samir Kumar, Partha Sona Maji","doi":"10.1007/s11468-024-02366-6","DOIUrl":"https://doi.org/10.1007/s11468-024-02366-6","url":null,"abstract":"<p>In this study we present a novel method for constructing a refractive-index sensor utilizing hybrid modes within a dual ‘Ag-photonic quasi-crystal’ geometry, adhering to the conventional Fibonacci sequence. The reflection spectrum of the geometry demonstrates the presence of three interconnected minima in reflectivity, occurring within the photonic-bandgap of a quasi-crystal. These hybrid modes emerge from the interplay between individual Tamm plasmon mode at the metal-photonic quasi crystal interface and the Fabry–Perot resonant cavity mode formed between two metal layers. The low wavelength dip (Mode-2) and high wavelength dip (Mode-3) display pronounced dispersive characteristics due to the substantial presence of mode-field in the sensing medium. Conversely, the mode situated between them (Mode-1) remains largely unaffected by variations in the refractive index of the sensing layer. Thus, our proposed method offers a wide range of wavelengths linked to Mode 2 and Mode 3, facilitating the concurrent utilization of dual wavelengths for sensor parameter analysis. We investigate the foundational parameters of a bio-photonic sensor, laying the foundation for a dual mode refractive-index sensing mechanism. At a normal angle of incidence, Mode -2 exhibits a maximum sensitivity of 401.4 nm/RIU and a Figure of Merit of 42.8 RIU-1. Meanwhile, for Mode -3, the highest sensitivity and Figure of Merit are 448.87 nm/RIU and 28.89 RIU-1, respectively. Additionally, we propose enhancing the hybrid-mode sensor characteristics by strategically optimizing the photonic quasi-crystal structures to increase the dispersion observed in hybrid Tamm plasmon modes, thus improving sensitivity. Utilization of the dual sensitive mode shows potential for enhancing modern biochemical sensors and optoelectronic devices, with possible applications in detecting diverse blood-related disorders distinguished by refractive index fluctuations in blood components.</p>","PeriodicalId":736,"journal":{"name":"Plasmonics","volume":null,"pages":null},"PeriodicalIF":3.0,"publicationDate":"2024-05-25","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141151940","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"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 : 2024-05-25DOI: 10.1007/s11468-024-02367-5
Ishaq Musa, Rahaf Mousa
Pistacia palaestina (P. palaestina) leaf extract was employed in the synthesis of spherical silver (Ag) nanoparticles, serving as a dual-purpose agent for both reduction and stabilization. These nanoparticles exhibited a range of average sizes between 2 and 27 nm. The size of these nanoparticles was observed to change in response to different concentrations of silver nitrate (AgNO3). This indicates that an increase in AgNO3 concentration leads to a reduction in the size of the nanoparticles. The height and morphology were analyzed using scanning probe microscopy (SPM). The crystalline nature of the Ag nanoparticles was confirmed by XRD analysis. Several properties of Ag nanoparticles, including their Raman spectroscopy, UV–visible absorption, and photoluminescence (PL), have been studied. The Raman spectroscopy revealed prominent peaks at 585 cm−1 assigned to skeletal deformation of C-S-C and 1580 cm−1 is linked to symmetric in plane C − C ring stretching. In the UV–visible spectrophotometry analysis, a surface plasmon resonance (SPR) band was observed, ranging between 395 and 398 nm. Additionally, the photoluminescence properties of these nanoparticles were found to vary with the excitation wavelength, marked by a distinct peak at 365 nm, a shoulder peak at 395 nm, and broader peaks observed at 470, 640, 700, and 740 nm. Furthermore, optical analyses of P. palaestina leaf extract indicated the presence of significant active compounds, including polyphenols, glycerol, and chlorophylls.
{"title":"Synthesis and Characterization of Variable-Sized Silver Nanoparticles Using Pistacia palaestina Leaf Extract","authors":"Ishaq Musa, Rahaf Mousa","doi":"10.1007/s11468-024-02367-5","DOIUrl":"https://doi.org/10.1007/s11468-024-02367-5","url":null,"abstract":"<p><i>Pistacia palaestina</i> (<i>P</i>. <i>palaestina</i>) leaf extract was employed in the synthesis of spherical silver (Ag) nanoparticles, serving as a dual-purpose agent for both reduction and stabilization. These nanoparticles exhibited a range of average sizes between 2 and 27 nm. The size of these nanoparticles was observed to change in response to different concentrations of silver nitrate (AgNO<sub>3</sub>). This indicates that an increase in AgNO<sub>3</sub> concentration leads to a reduction in the size of the nanoparticles. The height and morphology were analyzed using scanning probe microscopy (SPM). The crystalline nature of the Ag nanoparticles was confirmed by XRD analysis. Several properties of Ag nanoparticles, including their Raman spectroscopy, UV–visible absorption, and photoluminescence (PL), have been studied. The Raman spectroscopy revealed prominent peaks at 585 cm<sup>−1</sup> assigned to skeletal deformation of C-S-C and 1580 cm<sup>−1</sup> is linked to symmetric in plane C − C ring stretching. In the UV–visible spectrophotometry analysis, a surface plasmon resonance (SPR) band was observed, ranging between 395 and 398 nm. Additionally, the photoluminescence properties of these nanoparticles were found to vary with the excitation wavelength, marked by a distinct peak at 365 nm, a shoulder peak at 395 nm, and broader peaks observed at 470, 640, 700, and 740 nm. Furthermore, optical analyses of <i>P. palaestina</i> leaf extract indicated the presence of significant active compounds, including polyphenols, glycerol, and chlorophylls.</p>","PeriodicalId":736,"journal":{"name":"Plasmonics","volume":null,"pages":null},"PeriodicalIF":3.0,"publicationDate":"2024-05-25","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141151941","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"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 : 2024-05-24DOI: 10.1007/s11468-024-02333-1
T. Shahzadi, Hajra Bibi, T. Riaz, M. Zaib, Tabinda Malik
{"title":"Visual and Sensitive Detection of Milk Adulterant Melamine by Localized Surface Plasmon Resonance Optical Characteristics of Ag-MOF@Fe/SnO2 Nanocomposite","authors":"T. Shahzadi, Hajra Bibi, T. Riaz, M. Zaib, Tabinda Malik","doi":"10.1007/s11468-024-02333-1","DOIUrl":"https://doi.org/10.1007/s11468-024-02333-1","url":null,"abstract":"","PeriodicalId":736,"journal":{"name":"Plasmonics","volume":null,"pages":null},"PeriodicalIF":3.0,"publicationDate":"2024-05-24","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141100796","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"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 : 2024-05-24DOI: 10.1007/s11468-024-02353-x
Roozbeh Negahdari, Z. Kordrostami
{"title":"Opto-fluidic Plasmon Resonance Biosensor Based on Graphene-Black Phosphorous Hybrid for Diabetes Diagnosis","authors":"Roozbeh Negahdari, Z. Kordrostami","doi":"10.1007/s11468-024-02353-x","DOIUrl":"https://doi.org/10.1007/s11468-024-02353-x","url":null,"abstract":"","PeriodicalId":736,"journal":{"name":"Plasmonics","volume":null,"pages":null},"PeriodicalIF":3.0,"publicationDate":"2024-05-24","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141100269","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"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 : 2024-05-24DOI: 10.1007/s11468-024-02355-9
Anush Kannan N. K., Uziel Boaz, Shubhashri Waghmare, Rozalina Zakaria
{"title":"Computational Investigation on Tunability of Optical Absorption in MoS2 Integrated with Mono- and Non-Alloyed AuAg Nanoparticles for Photodetector Application","authors":"Anush Kannan N. K., Uziel Boaz, Shubhashri Waghmare, Rozalina Zakaria","doi":"10.1007/s11468-024-02355-9","DOIUrl":"https://doi.org/10.1007/s11468-024-02355-9","url":null,"abstract":"","PeriodicalId":736,"journal":{"name":"Plasmonics","volume":null,"pages":null},"PeriodicalIF":3.0,"publicationDate":"2024-05-24","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141101613","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"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 : 2024-05-22DOI: 10.1007/s11468-024-02356-8
B. Karki, Partha Sarkar, K. H. Mahmoud, A. S. Alsubaie, Manoj Sharma
{"title":"Detection of Organic Material Using Tungsten Ditelluride Based Surface Plasmon Resonance Sensor","authors":"B. Karki, Partha Sarkar, K. H. Mahmoud, A. S. Alsubaie, Manoj Sharma","doi":"10.1007/s11468-024-02356-8","DOIUrl":"https://doi.org/10.1007/s11468-024-02356-8","url":null,"abstract":"","PeriodicalId":736,"journal":{"name":"Plasmonics","volume":null,"pages":null},"PeriodicalIF":3.0,"publicationDate":"2024-05-22","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141108152","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"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}