wave optical module Search Results


90
COMSOL Inc wave optics module
Wave Optics Module, 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/wave+optical+module/wave+optics+module/10__1063_slash_5__0196982-32-7-16
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90
COMSOL Inc wave optics module of comsol version 6.22
Wave Optics Module Of Comsol Version 6.22, 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/wave+optical+module/wave+optics+module+of+comsol+multiphysics/pm40075176-62-7-7
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90
COMSOL Inc wave optics module of comsol multiphysics v5.5
Wave Optics Module Of Comsol Multiphysics V5.5, 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/wave+optical+module/wave+optics+module+of+comsol+multiphysics+v5+5/pmc10690780-166-13-12
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wave optics module of comsol multiphysics v5.5 - by Bioz Stars, 2026-11
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90
COMSOL Inc fem package wave optical module comsol multiphysics
Fem Package Wave Optical Module 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
https://www.bioz.com/product/wave+optical+module/fem+package++the+wave+optical+module+of+comsol+multiphysics++v+5+1+/pmc08229787-41-24-24
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fem package wave optical module comsol multiphysics - by Bioz Stars, 2026-11
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90
COMSOL Inc electromagnetic waves, frequency domain interface of the wave optics module
Electromagnetic Waves, Frequency Domain Interface Of The Wave Optics Module, 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/wave+optical+module/electromagnetic+waves++frequency+domain+interface+of+the+wave+optics+module/pmc11501110-168-10-14
Average 90 stars, based on 1 article reviews
electromagnetic waves, frequency domain interface of the wave optics module - by Bioz Stars, 2026-11
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90
Verlag GmbH guided-wave acousto-optic modulator (aom)
Guided Wave Acousto Optic Modulator (Aom), supplied by Verlag GmbH, 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/wave+optical+module/guided+wave+acousto+optic+modulator++aom+/us08149265-73-15-34
Average 90 stars, based on 1 article reviews
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COMSOL Inc fem package, wave optical module multiphysics
( a ) <t>FEM</t> simulations of the E-field intensity in the proximity of a AgNW laying on a graphene surface. The E-field intensity is visualized for the plane corresponding to the G-paper surface while the wire is pictured as uniform grey color for better clarity. ( b ) The E-field intensity is visualized for two <t>crossed</t> <t>AgNWs</t> in the air. In this case, the E-field intensity on the wire surface is visualized. ( c ) Maximum E-field variation within the visible spectral range as simulated at the interfaces between a AgNW and graphene (blue), PTFE (red) and cellulose (black).
Fem Package, Wave Optical Module 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
https://www.bioz.com/product/wave+optical+module/fem+package++wave+optical+module+multiphysics/pmc08229787-41-17-24
Average 90 stars, based on 1 article reviews
fem package, wave optical module multiphysics - by Bioz Stars, 2026-11
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90
COMSOL Inc multphysics wave optics module
( a ) <t>FEM</t> simulations of the E-field intensity in the proximity of a AgNW laying on a graphene surface. The E-field intensity is visualized for the plane corresponding to the G-paper surface while the wire is pictured as uniform grey color for better clarity. ( b ) The E-field intensity is visualized for two <t>crossed</t> <t>AgNWs</t> in the air. In this case, the E-field intensity on the wire surface is visualized. ( c ) Maximum E-field variation within the visible spectral range as simulated at the interfaces between a AgNW and graphene (blue), PTFE (red) and cellulose (black).
Multphysics Wave Optics Module, 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/wave+optical+module/multphysics+wave+optics+module/10__1007_slash_s13320___019___0543___z-50-4-3
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90
COMSOL Inc wave-optics and multiphysics simulations
( a ) <t>FEM</t> simulations of the E-field intensity in the proximity of a AgNW laying on a graphene surface. The E-field intensity is visualized for the plane corresponding to the G-paper surface while the wire is pictured as uniform grey color for better clarity. ( b ) The E-field intensity is visualized for two <t>crossed</t> <t>AgNWs</t> in the air. In this case, the E-field intensity on the wire surface is visualized. ( c ) Maximum E-field variation within the visible spectral range as simulated at the interfaces between a AgNW and graphene (blue), PTFE (red) and cellulose (black).
Wave Optics And Multiphysics 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
https://www.bioz.com/product/wave+optical+module/multiphysics+wave+optics+module/10__1103_slash_physrevlett__130__083802-113-11-16
Average 90 stars, based on 1 article reviews
wave-optics and multiphysics simulations - by Bioz Stars, 2026-11
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90
Electro-Optical Systems Inc modulation of a continuous wave laser light
( a ) Schematic of the OFC generation using a mode-locked laser. The top panel shows a train of optical pulses with a period 1 / f r e p . The bottom panel depicts the spectrum of narrow frequency peaks corresponding to the train of pulses in the time domain. The phase shift Δ ϕ of the carrier wave with respect to the pulse envelope induces a translation f 0 = f r e p Δ ϕ / π of spectral peaks from their harmonic frequencies n f r e p . Reproduced from with permission from Elsevier. ( b ) Sketch of an OFC-based spectroscopy technique. The OFC as a broadband light source interrogates an absorbing sample and a spectrometer analyses the transmission spectrum. ( c ) Artist’s rendition of a Kerr effect-based OFC generation in a micro-photonic disc resonator. A continuous-wave (CW) input pump wave creates a pattern of optical whispering-gallery modes (WGMs) inside the disc resonator, thereby inducing a periodic light intensity <t>modulation</t> and thus producing an output signal with an OFC-like spectrum. The bottom panel shows the sketch of a simplified experimental setup for the generation of a Kerr OFC and its further processing using a photodetector (PD). Reproduced from published by De Gruyter Open under a Creative Commons License.
Modulation Of A Continuous Wave Laser Light, supplied by Electro-Optical Systems 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/wave+optical+module/modulation+of+a+continuous+wave+laser+light/pmc09143010-63-11-10
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modulation of a continuous wave laser light - by Bioz Stars, 2026-11
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Electro-Optical Systems Inc carrier wave modulator 320
( a ) Schematic of the OFC generation using a mode-locked laser. The top panel shows a train of optical pulses with a period 1 / f r e p . The bottom panel depicts the spectrum of narrow frequency peaks corresponding to the train of pulses in the time domain. The phase shift Δ ϕ of the carrier wave with respect to the pulse envelope induces a translation f 0 = f r e p Δ ϕ / π of spectral peaks from their harmonic frequencies n f r e p . Reproduced from with permission from Elsevier. ( b ) Sketch of an OFC-based spectroscopy technique. The OFC as a broadband light source interrogates an absorbing sample and a spectrometer analyses the transmission spectrum. ( c ) Artist’s rendition of a Kerr effect-based OFC generation in a micro-photonic disc resonator. A continuous-wave (CW) input pump wave creates a pattern of optical whispering-gallery modes (WGMs) inside the disc resonator, thereby inducing a periodic light intensity <t>modulation</t> and thus producing an output signal with an OFC-like spectrum. The bottom panel shows the sketch of a simplified experimental setup for the generation of a Kerr OFC and its further processing using a photodetector (PD). Reproduced from published by De Gruyter Open under a Creative Commons License.
Carrier Wave Modulator 320, supplied by Electro-Optical Systems 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/wave+optical+module/carrier+wave+modulator+320/us09310552-58-0-7
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carrier wave modulator 320 - by Bioz Stars, 2026-11
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90
COMSOL Inc multiphysics® 5.6.0.401 (electromagnetic waves, frequency domain wave optics module
( a ) Schematic of the OFC generation using a mode-locked laser. The top panel shows a train of optical pulses with a period 1 / f r e p . The bottom panel depicts the spectrum of narrow frequency peaks corresponding to the train of pulses in the time domain. The phase shift Δ ϕ of the carrier wave with respect to the pulse envelope induces a translation f 0 = f r e p Δ ϕ / π of spectral peaks from their harmonic frequencies n f r e p . Reproduced from with permission from Elsevier. ( b ) Sketch of an OFC-based spectroscopy technique. The OFC as a broadband light source interrogates an absorbing sample and a spectrometer analyses the transmission spectrum. ( c ) Artist’s rendition of a Kerr effect-based OFC generation in a micro-photonic disc resonator. A continuous-wave (CW) input pump wave creates a pattern of optical whispering-gallery modes (WGMs) inside the disc resonator, thereby inducing a periodic light intensity <t>modulation</t> and thus producing an output signal with an OFC-like spectrum. The bottom panel shows the sketch of a simplified experimental setup for the generation of a Kerr OFC and its further processing using a photodetector (PD). Reproduced from published by De Gruyter Open under a Creative Commons License.
Multiphysics® 5.6.0.401 (Electromagnetic Waves, Frequency Domain Wave Optics Module, 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/wave+optical+module/multiphysics++5+6+0+401++electromagnetic+waves++frequency+domain+wave+optics+module/pm38052773-325-15-17
Average 90 stars, based on 1 article reviews
multiphysics® 5.6.0.401 (electromagnetic waves, frequency domain wave optics module - by Bioz Stars, 2026-11
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Image Search Results


( a ) FEM simulations of the E-field intensity in the proximity of a AgNW laying on a graphene surface. The E-field intensity is visualized for the plane corresponding to the G-paper surface while the wire is pictured as uniform grey color for better clarity. ( b ) The E-field intensity is visualized for two crossed AgNWs in the air. In this case, the E-field intensity on the wire surface is visualized. ( c ) Maximum E-field variation within the visible spectral range as simulated at the interfaces between a AgNW and graphene (blue), PTFE (red) and cellulose (black).

Journal: Nanomaterials

Article Title: Cost Effective Silver Nanowire-Decorated Graphene Paper for Drop-On SERS Biodetection

doi: 10.3390/nano11061495

Figure Lengend Snippet: ( a ) FEM simulations of the E-field intensity in the proximity of a AgNW laying on a graphene surface. The E-field intensity is visualized for the plane corresponding to the G-paper surface while the wire is pictured as uniform grey color for better clarity. ( b ) The E-field intensity is visualized for two crossed AgNWs in the air. In this case, the E-field intensity on the wire surface is visualized. ( c ) Maximum E-field variation within the visible spectral range as simulated at the interfaces between a AgNW and graphene (blue), PTFE (red) and cellulose (black).

Article Snippet: The electric field distribution in the near proximity of the AgNWs had been evaluated using a commercial FEM package, the wave optical module of COMSOL multiphysics (Stockholm, Sweden, v 5.1), and the MNPBEM MATLAB (Natick, MA, USA) toolbox for the simulation of metallic nanoparticles, using a boundary element method approach [ ].

Techniques:

( a ) Schematic of the OFC generation using a mode-locked laser. The top panel shows a train of optical pulses with a period 1 / f r e p . The bottom panel depicts the spectrum of narrow frequency peaks corresponding to the train of pulses in the time domain. The phase shift Δ ϕ of the carrier wave with respect to the pulse envelope induces a translation f 0 = f r e p Δ ϕ / π of spectral peaks from their harmonic frequencies n f r e p . Reproduced from with permission from Elsevier. ( b ) Sketch of an OFC-based spectroscopy technique. The OFC as a broadband light source interrogates an absorbing sample and a spectrometer analyses the transmission spectrum. ( c ) Artist’s rendition of a Kerr effect-based OFC generation in a micro-photonic disc resonator. A continuous-wave (CW) input pump wave creates a pattern of optical whispering-gallery modes (WGMs) inside the disc resonator, thereby inducing a periodic light intensity modulation and thus producing an output signal with an OFC-like spectrum. The bottom panel shows the sketch of a simplified experimental setup for the generation of a Kerr OFC and its further processing using a photodetector (PD). Reproduced from published by De Gruyter Open under a Creative Commons License.

Journal: Sensors (Basel, Switzerland)

Article Title: Acoustic, Phononic, Brillouin Light Scattering and Faraday Wave-Based Frequency Combs: Physical Foundations and Applications

doi: 10.3390/s22103921

Figure Lengend Snippet: ( a ) Schematic of the OFC generation using a mode-locked laser. The top panel shows a train of optical pulses with a period 1 / f r e p . The bottom panel depicts the spectrum of narrow frequency peaks corresponding to the train of pulses in the time domain. The phase shift Δ ϕ of the carrier wave with respect to the pulse envelope induces a translation f 0 = f r e p Δ ϕ / π of spectral peaks from their harmonic frequencies n f r e p . Reproduced from with permission from Elsevier. ( b ) Sketch of an OFC-based spectroscopy technique. The OFC as a broadband light source interrogates an absorbing sample and a spectrometer analyses the transmission spectrum. ( c ) Artist’s rendition of a Kerr effect-based OFC generation in a micro-photonic disc resonator. A continuous-wave (CW) input pump wave creates a pattern of optical whispering-gallery modes (WGMs) inside the disc resonator, thereby inducing a periodic light intensity modulation and thus producing an output signal with an OFC-like spectrum. The bottom panel shows the sketch of a simplified experimental setup for the generation of a Kerr OFC and its further processing using a photodetector (PD). Reproduced from published by De Gruyter Open under a Creative Commons License.

Article Snippet: For some practical applications, OFCs can be generated using an electro-optical modulation of a continuous wave laser light.

Techniques: Spectroscopy, Transmission Assay

( a ) Measured time-domain acoustic response of gas bubbles. The time between the vertical dashed lines is Δ T = 1 / f n a t ≈ 0.6 ms, where f n a t is the natural frequency of the bubble oscillations (see for details). The insets show a closeup of the waveforms and demonstrate the amplitude modulation. ( b ) Experimental AFC spectra obtained using gas bubbles in water insonated with an f 0 = 24.6 kHz sinusoidal signal of increasing pressure amplitude α = 1.15, 3.75, 4, 4.2, 4.3, 7.5 and 11.5 kPa. The scattered pressure values (in dB) are shown along the vertical axis with a vertical offset of 30 dB between the spectra. Reproduced from published by Springer Nature under the terms of the Creative Commons CC BY license.

Journal: Sensors (Basel, Switzerland)

Article Title: Acoustic, Phononic, Brillouin Light Scattering and Faraday Wave-Based Frequency Combs: Physical Foundations and Applications

doi: 10.3390/s22103921

Figure Lengend Snippet: ( a ) Measured time-domain acoustic response of gas bubbles. The time between the vertical dashed lines is Δ T = 1 / f n a t ≈ 0.6 ms, where f n a t is the natural frequency of the bubble oscillations (see for details). The insets show a closeup of the waveforms and demonstrate the amplitude modulation. ( b ) Experimental AFC spectra obtained using gas bubbles in water insonated with an f 0 = 24.6 kHz sinusoidal signal of increasing pressure amplitude α = 1.15, 3.75, 4, 4.2, 4.3, 7.5 and 11.5 kPa. The scattered pressure values (in dB) are shown along the vertical axis with a vertical offset of 30 dB between the spectra. Reproduced from published by Springer Nature under the terms of the Creative Commons CC BY license.

Article Snippet: For some practical applications, OFCs can be generated using an electro-optical modulation of a continuous wave laser light.

Techniques:

( a ) Experimental average response of an ethanol drop subjected to vertical vibration at 70 Hz plotted as a function of the vibration amplitude. The inset shows the power spectra obtained by Fourier-transforming the measured signals. The parenthetical labels relate the spectra to the experimental points in the main panel. ( b ) Experimental average response of a canola oil drop subjected to vertical vibration at 70 Hz plotted as a function of the vibration amplitude. The modulation sidebands (the spectrum label 7) are present in the ethanol drop spectra and absent in the spectra of a canola oil drop. The shaded regions in the main panels correspond to the chaotic oscillations, resulting in strong diffuse scattering leading to a decrease in the optical intensity of the detected signal. Reproduced from . Copyright 2019 by the American Physical Society.

Journal: Sensors (Basel, Switzerland)

Article Title: Acoustic, Phononic, Brillouin Light Scattering and Faraday Wave-Based Frequency Combs: Physical Foundations and Applications

doi: 10.3390/s22103921

Figure Lengend Snippet: ( a ) Experimental average response of an ethanol drop subjected to vertical vibration at 70 Hz plotted as a function of the vibration amplitude. The inset shows the power spectra obtained by Fourier-transforming the measured signals. The parenthetical labels relate the spectra to the experimental points in the main panel. ( b ) Experimental average response of a canola oil drop subjected to vertical vibration at 70 Hz plotted as a function of the vibration amplitude. The modulation sidebands (the spectrum label 7) are present in the ethanol drop spectra and absent in the spectra of a canola oil drop. The shaded regions in the main panels correspond to the chaotic oscillations, resulting in strong diffuse scattering leading to a decrease in the optical intensity of the detected signal. Reproduced from . Copyright 2019 by the American Physical Society.

Article Snippet: For some practical applications, OFCs can be generated using an electro-optical modulation of a continuous wave laser light.

Techniques: