Localized Surface Plasmon Resonance of Single Silver Nano-Hemisphere

In this work, we use 3D finite difference time domain (3D-FDTD) to calculate the plasmon resonance effect for a single silver hemisphere in which the palsmon line shape have distinct peaks when the particles are located on a glass substrate. The dependence of the resonance on hemisphere size and the ratio of height over radius are characterized, and it is found that the surface interface effect played an important role on the plasman resonace effect for a single silver hemisphere.

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Finite-Difference Time-Domain Simulation of Localized Surface Plasmon Resonance Adsorption by Gold Nanoparticles

7th WACBE World Congress on Bioengineering 2015 - IFMBE Proceedings ◽

10.1007/978-3-319-19452-3_37 ◽

2015 ◽

pp. 138-141 ◽

Cited By ~ 1

Author(s):

Wen-Chi Lin ◽

Wen-Chen Lin ◽

Cheng-Lun Tsai ◽

Kang-Ping Lin

Keyword(s):

Gold Nanoparticles ◽

Surface Plasmon Resonance ◽

Finite Difference ◽

Surface Plasmon ◽

Time Domain ◽

Plasmon Resonance ◽

Finite Difference Time Domain ◽

Localized Surface Plasmon Resonance ◽

Localized Surface Plasmon ◽

Difference Time

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The effect of size of Au nanodisc on the localized surface plasmon resonance simulated using finite-difference time-domain (FDTD) method

Materials Today Proceedings ◽

10.1016/j.matpr.2018.12.014 ◽

2019 ◽

Vol 7 ◽

pp. 607-611

Author(s):

Nor Ahya Hassan ◽

Abdul Manaf Hashim

Keyword(s):

Surface Plasmon Resonance ◽

Finite Difference ◽

Surface Plasmon ◽

Time Domain ◽

Plasmon Resonance ◽

Finite Difference Time Domain ◽

Localized Surface Plasmon Resonance ◽

Fdtd Method ◽

Localized Surface Plasmon ◽

Difference Time

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Modeling surface plasmon resonance in sensors using finite-difference time-domain analysis

10.1117/12.180749 ◽

1994 ◽

Author(s):

Douglas A. Christensen ◽

David Fowers

Keyword(s):

Surface Plasmon Resonance ◽

Finite Difference ◽

Surface Plasmon ◽

Time Domain ◽

Plasmon Resonance ◽

Finite Difference Time Domain ◽

Time Domain Analysis ◽

Domain Analysis ◽

Difference Time

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Effects of film roughness on surface plasmon resonance sensors: finite-difference time-domain (FDTD) modeling

10.1117/12.190974 ◽

1994 ◽

Cited By ~ 1

Author(s):

Douglas A. Christensen ◽

David Fowers

Keyword(s):

Surface Plasmon Resonance ◽

Finite Difference ◽

Surface Plasmon ◽

Time Domain ◽

Plasmon Resonance ◽

Finite Difference Time Domain ◽

Film Roughness ◽

Difference Time ◽

Surface Plasmon Resonance Sensors

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Finite-Difference Time-Domain (FDTD) design of gold nanoparticle chains with specific surface plasmon resonance

Journal of Molecular Structure ◽

10.1016/j.molstruc.2014.04.086 ◽

2014 ◽

Vol 1072 ◽

pp. 137-143 ◽

Cited By ~ 26

Author(s):

Cristian Tira ◽

Daniela Tira ◽

Timea Simon ◽

Simion Astilean

Keyword(s):

Surface Plasmon Resonance ◽

Finite Difference ◽

Specific Surface ◽

Gold Nanoparticle ◽

Surface Plasmon ◽

Time Domain ◽

Plasmon Resonance ◽

Finite Difference Time Domain ◽

Nanoparticle Chains ◽

Difference Time

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Particle swarm optimization and finite-difference time-domain (PSO/FDTD) algorithms for a surface plasmon resonance-based gas sensor

Journal of Computational Electronics ◽

10.1007/s10825-019-01391-7 ◽

2019 ◽

Vol 18 (4) ◽

pp. 1354-1364 ◽

Cited By ~ 13

Author(s):

Narjes Amoosoltani ◽

Abbas Zarifkar ◽

Ali Farmani

Keyword(s):

Particle Swarm Optimization ◽

Surface Plasmon Resonance ◽

Finite Difference ◽

Gas Sensor ◽

Surface Plasmon ◽

Time Domain ◽

Plasmon Resonance ◽

Finite Difference Time Domain ◽

Swarm Optimization ◽

Difference Time

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Local Electric Field and Scattering Cross Section of Ag Nanoparticles under Surface Plasmon Resonance by Finite Difference Time Domain Method

The Journal of Physical Chemistry B ◽

10.1021/jp022399e ◽

2003 ◽

Vol 107 (31) ◽

pp. 7607-7617 ◽

Cited By ~ 233

Author(s):

M. Futamata ◽

Y. Maruyama ◽

M. Ishikawa

Keyword(s):

Surface Plasmon Resonance ◽

Finite Difference ◽

Electric Field ◽

Cross Section ◽

Surface Plasmon ◽

Time Domain ◽

Plasmon Resonance ◽

Ag Nanoparticles ◽

Finite Difference Time Domain ◽

Difference Time

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Localized Surface Plasmon Resonance Effect of Gold Nanoparticles - TiO2 as Mesoporous Layer for Perovskite Solar Cells

2020 6th International Conference on Applied System Innovation (ICASI) ◽

10.1109/icasi49664.2020.9426330 ◽

2020 ◽

Author(s):

Zi-Heng Lin ◽

Hsueh-Tao Chou ◽

Tien-Ming Wu ◽

Guan-Yu Lin ◽

Jing-Hua Lu

Keyword(s):

Gold Nanoparticles ◽

Solar Cells ◽

Surface Plasmon Resonance ◽

Surface Plasmon ◽

Plasmon Resonance ◽

Localized Surface Plasmon Resonance ◽

Resonance Effect ◽

Perovskite Solar Cells ◽

Localized Surface Plasmon ◽

Surface Plasmon Resonance Effect

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Enhanced photocatalytic hydrogen production over Au/SiC for water reduction by localized surface plasmon resonance effect

Applied Surface Science ◽

10.1016/j.apsusc.2018.06.099 ◽

2018 ◽

Vol 456 ◽

pp. 871-875 ◽

Cited By ~ 8

Author(s):

Da Wang ◽

Lin Huang ◽

Zhongnan Guo ◽

Xue Han ◽

Chunjun Liu ◽

...

Keyword(s):

Surface Plasmon Resonance ◽

Hydrogen Production ◽

Surface Plasmon ◽

Plasmon Resonance ◽

Localized Surface Plasmon Resonance ◽

Resonance Effect ◽

Localized Surface Plasmon ◽

Photocatalytic Hydrogen Production ◽

Water Reduction ◽

Surface Plasmon Resonance Effect

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Performance Analysis of Localized Surface Plasmon Resonance Sensor with and Without Bragg Grating

Journal of Optical Communications ◽

10.1515/joc-2017-0141 ◽

2019 ◽

Vol 41 (1) ◽

pp. 45-50

Author(s):

Ranjit Singh ◽

Sanjeev Dewra

Keyword(s):

Surface Plasmon Resonance ◽

Surface Plasmon ◽

Plasmon Resonance ◽

Localized Surface Plasmon Resonance ◽

Signal To Noise Ratio ◽

Localized Surface Plasmon ◽

Bragg Grating ◽

Surface Plasmon Resonance Sensor ◽

Resonance Sensor ◽

Difference Time

Abstract The performance of localized surface plasmon resonance-based sensor with and without Bragg grating by using finite difference time domain method is evaluated with nanoparticles used at the tip of optical fiber. The proposed sensor has been analyzed in terms of refractive index (RI) sensitivity and signal-to-noise ratio (SNR). It is observed that the RI sensitivity of surface plasmon resonance sensor is 240 nm/RIU with and without grating as RI of surrounding varies from 1.4 to 1.5. It is found that the value of SNR is 0.875 RIU→1 without grating and 2.75 RIU→1 with grating. So there is an improvement in the SNR when the Bragg grating is inscribed within the core of the fiber.

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