Abstract:Plasmonic nanostructures show great promise for sensing because their nanoscale confined light fields are sensitive to the change in the surroundings. Conventional plasmonic sensors based on surface plasmon polaritons (SPPs) and localized surface plasmon resonances (LSPRs) have inspired considerable progress in sensing but still suffer from an oblique incidence or moderate sensitivity. This review focuses on how the rational design of novel plasmonic nanostructures can enable high‐performance sensing. Patterne… Show more
“…Specially, there exists an optimal silver thickness (∼20 nm) for achieving the LPR with a maximum Q -factor up to 610 at 870 nm. Our findings may find potential applications in low-threshold plasmonic band-edge lasing, − ultrasensitive biosensors, strong light-matter coupling, and so on.…”
Section: Discussionmentioning
confidence: 99%
“…This diffraction coupling mechanism can effectively suppress the radiation loss of the LSPs supported by the single metallic nanoparticle and thus obtain ultrahigh- Q plasmonic resonance . According to recent works, the Q -factors as high as 218–2340 of LPRs have been successfully predicted and achieved in various metallic nanostructures array immersed into the uniform environment, − ,,,,− which have found important applications in fields such as high-performance sensing, long-distance resonance energy transfer, low-threshold nanolasers, − and enhancing nonlinear optical processes …”
Section: Introductionmentioning
confidence: 99%
“…This diffraction coupling mechanism can effectively suppress the radiation loss of the LSPs supported by the single metallic nanoparticle and thus obtain ultrahigh-Q plasmonic resonance. 26 According to recent works, the Q-factors as high as 218−2340 of LPRs have been successfully predicted and achieved in various metallic nanostructures array immersed into the uniform environment, 1−3,12,13,21,25−30 which have found important applications in fields such as high-performance sensing, 30 long-distance resonance energy transfer, 31 low-threshold nanolasers, 32−35 and enhancing nonlinear optical processes. 36 In addition, a simple noble metallic (Au/Ag) nanoshell composed of a dielectric nanosphere core and a metallic shell is also demonstrated both theoretically and experimentally to be capable of supporting high-Q cavity plasmon mode (CPM) on the order of ∼200, 37,38 which has been designed for lowthreshold nanolaser, 39 high-performance biosensor, 40 fluorescent shaper, 41 and plasmonic ruler.…”
We theoretically demonstrate a high-Q and intense lattice plasmon resonance supported by the hexagonal nonclose packed thin silver nanoshells array. By introducing the diffraction coupling mechanism, the high-Q and intense lattice plasmon mode stemmed from the coupling between the TM 1 cavity plasmon mode and the diffraction mode of the first-order Wood anomaly is obtained in the thin silver nanoshells array, successfully solving the trade-off between the Q-factor and the resonance intensity of the cavity plasmon mode existed in a single silver nanoshell. In particular, a maximum Q-factor up to 610 of the lattice plasmon resonance is successfully achieved at 870 nm in the silver nanoshell array with an optimal silver thickness of 20 nm.
“…Specially, there exists an optimal silver thickness (∼20 nm) for achieving the LPR with a maximum Q -factor up to 610 at 870 nm. Our findings may find potential applications in low-threshold plasmonic band-edge lasing, − ultrasensitive biosensors, strong light-matter coupling, and so on.…”
Section: Discussionmentioning
confidence: 99%
“…This diffraction coupling mechanism can effectively suppress the radiation loss of the LSPs supported by the single metallic nanoparticle and thus obtain ultrahigh- Q plasmonic resonance . According to recent works, the Q -factors as high as 218–2340 of LPRs have been successfully predicted and achieved in various metallic nanostructures array immersed into the uniform environment, − ,,,,− which have found important applications in fields such as high-performance sensing, long-distance resonance energy transfer, low-threshold nanolasers, − and enhancing nonlinear optical processes …”
Section: Introductionmentioning
confidence: 99%
“…This diffraction coupling mechanism can effectively suppress the radiation loss of the LSPs supported by the single metallic nanoparticle and thus obtain ultrahigh-Q plasmonic resonance. 26 According to recent works, the Q-factors as high as 218−2340 of LPRs have been successfully predicted and achieved in various metallic nanostructures array immersed into the uniform environment, 1−3,12,13,21,25−30 which have found important applications in fields such as high-performance sensing, 30 long-distance resonance energy transfer, 31 low-threshold nanolasers, 32−35 and enhancing nonlinear optical processes. 36 In addition, a simple noble metallic (Au/Ag) nanoshell composed of a dielectric nanosphere core and a metallic shell is also demonstrated both theoretically and experimentally to be capable of supporting high-Q cavity plasmon mode (CPM) on the order of ∼200, 37,38 which has been designed for lowthreshold nanolaser, 39 high-performance biosensor, 40 fluorescent shaper, 41 and plasmonic ruler.…”
We theoretically demonstrate a high-Q and intense lattice plasmon resonance supported by the hexagonal nonclose packed thin silver nanoshells array. By introducing the diffraction coupling mechanism, the high-Q and intense lattice plasmon mode stemmed from the coupling between the TM 1 cavity plasmon mode and the diffraction mode of the first-order Wood anomaly is obtained in the thin silver nanoshells array, successfully solving the trade-off between the Q-factor and the resonance intensity of the cavity plasmon mode existed in a single silver nanoshell. In particular, a maximum Q-factor up to 610 of the lattice plasmon resonance is successfully achieved at 870 nm in the silver nanoshell array with an optimal silver thickness of 20 nm.
“…Several studies illustrate the direct relationship between the Q -factors of plasmonic nanostructure resonances and the associated near-field intensity distribution. , While LSPRs sustained by single metal NPs usually reach a value of Q = 5–10, , SLRs from ordered arrays can largely exceed these numbers, giving rise to sharp resonances that find application in a large number of fields. SLRs are ideal for sensing since they are susceptible to small changes in the refractive index of the surrounding environment with high sensitivity and specificity. − Furthermore, high Q -factor SLRs can be used to enhance the efficiency of light absorption and emission in optoelectronic devices by coupling the SLRs to an emitter, such as a quantum dot or a fluorescent molecule. , …”
Surface lattice resonances (SLRs) sustained by ordered metal arrays are characterized by their narrow spectral features, remarkable quality factors, and the ability to tune their spectral properties based on the periodicity of the array. However, the majority of these structures are fabricated using classical lithographic processes or require postannealing steps at high temperatures to enhance the quality of the metal. These limitations hinder the widespread utilization of these periodic metal arrays in various applications. In this work, we use the scalable technique of template-assisted assembly of metal colloids to produce plasmonic supercrystals over centimeter areas capable of sustaining SLRs with high Q factors reaching up to 270. Our approach obviates the need for any postprocessing, offering a streamlined and efficient fabrication route. Furthermore, our method enables extensive tunability across the entire visible and near-infrared spectral ranges, empowering the design of tailored plasmonic resonant structures for a wide range of applications.
“…4−6 Further, the promise of LSPR-based detections is substantially hindered by their broad resonance widths (typically exceeding 80 nm). 7 Arranging metal NPs into periodical arrays can couple LSPRs of units to the diffracted waves of arrays to support surface lattice resonances (SLRs), where the radiative loss is significantly suppressed to support resonances with line widths down to 10 nm. 8−10 The narrow resonance line widths and strong field enhancement of SLRs lead to potentially high sensitivity and a low limit of detection.…”
Narrow plasmonic resonances in an asymmetric refractive index (RI) environment under normal incidence are desired for miniaturized sensors in clinical evaluation and lab-on-achip devices. We demonstrate that a thin alumina layer between Au nanoparticle (NP) lattices and a quartz substrate can induce total internal reflections and nonvanishing out-of-plane electric fields, resulting in ultranarrow quadrupole surface lattice resonances (SLRs). The SLRs show a line width below 1 nm with high-quality factors up to 1865 in simulations and up to 640 in experiments under normal incidence in the visible range. High-performance RI sensing based on SLRs is demonstrated for glucose in aqueous solutions and DMSO/water mixtures, which show a one magnitude improvement in the figure of merit compared with the Au NP lattices on the bare quartz substrate. This substrate modification opens a new avenue to design and generate high-quality plasmonic resonances for light-matter interactions and sensing applications.
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