three-dimensional simulation of sintering using a continuum modeling approach Search Results


computed tomography (ct) simulator  (TOSHIBA Medical)
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TOSHIBA Medical computed tomography (ct) simulator
Computed Tomography (Ct) Simulator, supplied by TOSHIBA Medical, used in various techniques. Bioz Stars score: 90/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
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computed tomography (ct) simulator - by Bioz Stars, 2026-09
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three-dimensional fem simulations  (COMSOL Inc)
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COMSOL Inc three-dimensional fem simulations
Three Dimensional Fem Simulations, supplied by COMSOL Inc, used in various techniques. Bioz Stars score: 90/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
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three-dimensional fem simulations - by Bioz Stars, 2026-09
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fem simulations comsol multiphysics  (COMSOL Inc)
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COMSOL Inc fem simulations comsol multiphysics
(A) Resonance frequencies as a function of inverse length times mode order (m/L) and (B) average linewidths (Γ) versus frequency for the m = 3 (blue circles) and m = 4 (red squares) Fabry–Pérot resonances of the gold NWs. Data collected from at least three NWs with error bars representing SDs. The dashed black line in A shows the frequencies calculated from Eq. 1. The shaded area in B shows the range of values for the Drude relaxation parameter for Au (55, 56). The solid red and blue lines in A and B are the results from the 3D <t>FEM</t> <t>simulations.</t> (C) Spectra for different length NWs calculated from FEM simulations. The lowest-frequency features are the m = 1 Fabry–Pérot resonances. (Inset) An expanded view of the higher-energy m = 2, 3, and 4 resonances (the spectra have been offset for clarity).
Fem Simulations Comsol Multiphysics, supplied by COMSOL Inc, used in various techniques. Bioz Stars score: 90/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
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fem simulations comsol multiphysics - by Bioz Stars, 2026-09
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imaris software package  (Oxford Instruments)
99
Oxford Instruments imaris software package
(A) Resonance frequencies as a function of inverse length times mode order (m/L) and (B) average linewidths (Γ) versus frequency for the m = 3 (blue circles) and m = 4 (red squares) Fabry–Pérot resonances of the gold NWs. Data collected from at least three NWs with error bars representing SDs. The dashed black line in A shows the frequencies calculated from Eq. 1. The shaded area in B shows the range of values for the Drude relaxation parameter for Au (55, 56). The solid red and blue lines in A and B are the results from the 3D <t>FEM</t> <t>simulations.</t> (C) Spectra for different length NWs calculated from FEM simulations. The lowest-frequency features are the m = 1 Fabry–Pérot resonances. (Inset) An expanded view of the higher-energy m = 2, 3, and 4 resonances (the spectra have been offset for clarity).
Imaris Software Package, supplied by Oxford Instruments, used in various techniques. Bioz Stars score: 99/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
https://www.bioz.com/product/three-dimensional+simulation+of+sintering+using+a+continuum+modeling+approach/Imaris/pm22114708-174-10-13
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imaris software package - by Bioz Stars, 2026-09
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3d fdtd method  (ANSYS inc)
90
ANSYS inc 3d fdtd method
(A) Resonance frequencies as a function of inverse length times mode order (m/L) and (B) average linewidths (Γ) versus frequency for the m = 3 (blue circles) and m = 4 (red squares) Fabry–Pérot resonances of the gold NWs. Data collected from at least three NWs with error bars representing SDs. The dashed black line in A shows the frequencies calculated from Eq. 1. The shaded area in B shows the range of values for the Drude relaxation parameter for Au (55, 56). The solid red and blue lines in A and B are the results from the 3D <t>FEM</t> <t>simulations.</t> (C) Spectra for different length NWs calculated from FEM simulations. The lowest-frequency features are the m = 1 Fabry–Pérot resonances. (Inset) An expanded view of the higher-energy m = 2, 3, and 4 resonances (the spectra have been offset for clarity).
3d Fdtd Method, supplied by ANSYS inc, used in various techniques. Bioz Stars score: 90/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
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maxwell equations solver  (COMSOL Inc)
90
COMSOL Inc maxwell equations solver
(A) Resonance frequencies as a function of inverse length times mode order (m/L) and (B) average linewidths (Γ) versus frequency for the m = 3 (blue circles) and m = 4 (red squares) Fabry–Pérot resonances of the gold NWs. Data collected from at least three NWs with error bars representing SDs. The dashed black line in A shows the frequencies calculated from Eq. 1. The shaded area in B shows the range of values for the Drude relaxation parameter for Au (55, 56). The solid red and blue lines in A and B are the results from the 3D <t>FEM</t> <t>simulations.</t> (C) Spectra for different length NWs calculated from FEM simulations. The lowest-frequency features are the m = 1 Fabry–Pérot resonances. (Inset) An expanded view of the higher-energy m = 2, 3, and 4 resonances (the spectra have been offset for clarity).
Maxwell Equations Solver, supplied by COMSOL Inc, used in various techniques. Bioz Stars score: 90/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
https://www.bioz.com/product/three-dimensional+simulation+of+sintering+using+a+continuum+modeling+approach/maxwell+equations/pmc03797985-53-12-21
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maxwell equations solver - by Bioz Stars, 2026-09
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three-dimensional finite element method (3d-fem) simulations  (COMSOL Inc)
90
COMSOL Inc three-dimensional finite element method (3d-fem) simulations
(A) Resonance frequencies as a function of inverse length times mode order (m/L) and (B) average linewidths (Γ) versus frequency for the m = 3 (blue circles) and m = 4 (red squares) Fabry–Pérot resonances of the gold NWs. Data collected from at least three NWs with error bars representing SDs. The dashed black line in A shows the frequencies calculated from Eq. 1. The shaded area in B shows the range of values for the Drude relaxation parameter for Au (55, 56). The solid red and blue lines in A and B are the results from the 3D <t>FEM</t> <t>simulations.</t> (C) Spectra for different length NWs calculated from FEM simulations. The lowest-frequency features are the m = 1 Fabry–Pérot resonances. (Inset) An expanded view of the higher-energy m = 2, 3, and 4 resonances (the spectra have been offset for clarity).
Three Dimensional Finite Element Method (3d Fem) Simulations, supplied by COMSOL Inc, used in various techniques. Bioz Stars score: 90/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
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three-dimensional finite element method (3d-fem) simulations - by Bioz Stars, 2026-09
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hfss  (Ansoft Corporation)
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Ansoft Corporation hfss
(A) Resonance frequencies as a function of inverse length times mode order (m/L) and (B) average linewidths (Γ) versus frequency for the m = 3 (blue circles) and m = 4 (red squares) Fabry–Pérot resonances of the gold NWs. Data collected from at least three NWs with error bars representing SDs. The dashed black line in A shows the frequencies calculated from Eq. 1. The shaded area in B shows the range of values for the Drude relaxation parameter for Au (55, 56). The solid red and blue lines in A and B are the results from the 3D <t>FEM</t> <t>simulations.</t> (C) Spectra for different length NWs calculated from FEM simulations. The lowest-frequency features are the m = 1 Fabry–Pérot resonances. (Inset) An expanded view of the higher-energy m = 2, 3, and 4 resonances (the spectra have been offset for clarity).
Hfss, supplied by Ansoft Corporation, used in various techniques. Bioz Stars score: 90/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
https://www.bioz.com/product/three-dimensional+simulation+of+sintering+using+a+continuum+modeling+approach/hfss/us08217852-242-7-20
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multiphysics ver  (COMSOL Inc)
90
COMSOL Inc multiphysics ver
(A) Resonance frequencies as a function of inverse length times mode order (m/L) and (B) average linewidths (Γ) versus frequency for the m = 3 (blue circles) and m = 4 (red squares) Fabry–Pérot resonances of the gold NWs. Data collected from at least three NWs with error bars representing SDs. The dashed black line in A shows the frequencies calculated from Eq. 1. The shaded area in B shows the range of values for the Drude relaxation parameter for Au (55, 56). The solid red and blue lines in A and B are the results from the 3D <t>FEM</t> <t>simulations.</t> (C) Spectra for different length NWs calculated from FEM simulations. The lowest-frequency features are the m = 1 Fabry–Pérot resonances. (Inset) An expanded view of the higher-energy m = 2, 3, and 4 resonances (the spectra have been offset for clarity).
Multiphysics Ver, supplied by COMSOL Inc, used in various techniques. Bioz Stars score: 90/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
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multiphysics ver - by Bioz Stars, 2026-09
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multiphysics engineering simulation software  (COMSOL Inc)
90
COMSOL Inc multiphysics engineering simulation software
(A) Resonance frequencies as a function of inverse length times mode order (m/L) and (B) average linewidths (Γ) versus frequency for the m = 3 (blue circles) and m = 4 (red squares) Fabry–Pérot resonances of the gold NWs. Data collected from at least three NWs with error bars representing SDs. The dashed black line in A shows the frequencies calculated from Eq. 1. The shaded area in B shows the range of values for the Drude relaxation parameter for Au (55, 56). The solid red and blue lines in A and B are the results from the 3D <t>FEM</t> <t>simulations.</t> (C) Spectra for different length NWs calculated from FEM simulations. The lowest-frequency features are the m = 1 Fabry–Pérot resonances. (Inset) An expanded view of the higher-energy m = 2, 3, and 4 resonances (the spectra have been offset for clarity).
Multiphysics Engineering Simulation Software, supplied by COMSOL Inc, used in various techniques. Bioz Stars score: 90/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
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multiphysics engineering simulation software - by Bioz Stars, 2026-09
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three-dimensional electromagnetic field simulation  (Ansoft Corporation)
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Ansoft Corporation three-dimensional electromagnetic field simulation
(A) Resonance frequencies as a function of inverse length times mode order (m/L) and (B) average linewidths (Γ) versus frequency for the m = 3 (blue circles) and m = 4 (red squares) Fabry–Pérot resonances of the gold NWs. Data collected from at least three NWs with error bars representing SDs. The dashed black line in A shows the frequencies calculated from Eq. 1. The shaded area in B shows the range of values for the Drude relaxation parameter for Au (55, 56). The solid red and blue lines in A and B are the results from the 3D <t>FEM</t> <t>simulations.</t> (C) Spectra for different length NWs calculated from FEM simulations. The lowest-frequency features are the m = 1 Fabry–Pérot resonances. (Inset) An expanded view of the higher-energy m = 2, 3, and 4 resonances (the spectra have been offset for clarity).
Three Dimensional Electromagnetic Field Simulation, supplied by Ansoft Corporation, used in various techniques. Bioz Stars score: 90/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
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three-dimensional, finite element model  (COMSOL Inc)
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COMSOL Inc three-dimensional, finite element model
(A) Resonance frequencies as a function of inverse length times mode order (m/L) and (B) average linewidths (Γ) versus frequency for the m = 3 (blue circles) and m = 4 (red squares) Fabry–Pérot resonances of the gold NWs. Data collected from at least three NWs with error bars representing SDs. The dashed black line in A shows the frequencies calculated from Eq. 1. The shaded area in B shows the range of values for the Drude relaxation parameter for Au (55, 56). The solid red and blue lines in A and B are the results from the 3D <t>FEM</t> <t>simulations.</t> (C) Spectra for different length NWs calculated from FEM simulations. The lowest-frequency features are the m = 1 Fabry–Pérot resonances. (Inset) An expanded view of the higher-energy m = 2, 3, and 4 resonances (the spectra have been offset for clarity).
Three Dimensional, Finite Element Model, supplied by COMSOL Inc, used in various techniques. Bioz Stars score: 90/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
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Image Search Results


(A) Resonance frequencies as a function of inverse length times mode order (m/L) and (B) average linewidths (Γ) versus frequency for the m = 3 (blue circles) and m = 4 (red squares) Fabry–Pérot resonances of the gold NWs. Data collected from at least three NWs with error bars representing SDs. The dashed black line in A shows the frequencies calculated from Eq. 1. The shaded area in B shows the range of values for the Drude relaxation parameter for Au (55, 56). The solid red and blue lines in A and B are the results from the 3D FEM simulations. (C) Spectra for different length NWs calculated from FEM simulations. The lowest-frequency features are the m = 1 Fabry–Pérot resonances. (Inset) An expanded view of the higher-energy m = 2, 3, and 4 resonances (the spectra have been offset for clarity).

Journal: Proceedings of the National Academy of Sciences of the United States of America

Article Title: Far-field midinfrared superresolution imaging and spectroscopy of single high aspect ratio gold nanowires

doi: 10.1073/pnas.1916433117

Figure Lengend Snippet: (A) Resonance frequencies as a function of inverse length times mode order (m/L) and (B) average linewidths (Γ) versus frequency for the m = 3 (blue circles) and m = 4 (red squares) Fabry–Pérot resonances of the gold NWs. Data collected from at least three NWs with error bars representing SDs. The dashed black line in A shows the frequencies calculated from Eq. 1. The shaded area in B shows the range of values for the Drude relaxation parameter for Au (55, 56). The solid red and blue lines in A and B are the results from the 3D FEM simulations. (C) Spectra for different length NWs calculated from FEM simulations. The lowest-frequency features are the m = 1 Fabry–Pérot resonances. (Inset) An expanded view of the higher-energy m = 2, 3, and 4 resonances (the spectra have been offset for clarity).

Article Snippet: Three-dimensional FEM simulations (performed using COMSOL Multiphysics) are used to calculate the IR absorption of the NWs, as well as the time dependence of the heat transfer process.

Techniques:

FEM simulation maps of the resistive heating and time-dependent temperature changes for an L = 3.1-μm-long Au NW on a glass substrate for the (A) m = 3 and (B) m = 4 Fabry–Pérot modes. (Top) Images in each panel shows maps of the IR absorption of the NWs. (Bottom) Images show the time-dependent temperature changes in the system. The excitation wavelength for the simulations is chosen to be at the maximum for each resonance. Note that the temperature profiles in the right-hand panels in A and B have been offset for clarity.

Journal: Proceedings of the National Academy of Sciences of the United States of America

Article Title: Far-field midinfrared superresolution imaging and spectroscopy of single high aspect ratio gold nanowires

doi: 10.1073/pnas.1916433117

Figure Lengend Snippet: FEM simulation maps of the resistive heating and time-dependent temperature changes for an L = 3.1-μm-long Au NW on a glass substrate for the (A) m = 3 and (B) m = 4 Fabry–Pérot modes. (Top) Images in each panel shows maps of the IR absorption of the NWs. (Bottom) Images show the time-dependent temperature changes in the system. The excitation wavelength for the simulations is chosen to be at the maximum for each resonance. Note that the temperature profiles in the right-hand panels in A and B have been offset for clarity.

Article Snippet: Three-dimensional FEM simulations (performed using COMSOL Multiphysics) are used to calculate the IR absorption of the NWs, as well as the time dependence of the heat transfer process.

Techniques: