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Nicolas Large
Приєднався 1 жов 2011
Travels to Deep-Space: The Colors of Nebulae
Travels to Deep-Space: The Colors of Nebulae
Переглядів: 70
Відео
Nanophotonics & Plasmonics - Ch. 2 | Wave equations
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Chapter 2 | Theoretical Foundations: Electrodynamics Part 2: Derivation of the wave equations Derivations: drive.google.com/file/d/1uU5KGuFnbCq8C6vQ1eq4hzR3UHF55L78/view?usp=sharing by Dr. Nicolas Large, Department of Physics and Astronomy, The University of Texas at San Antonio physics.utsa.edu/nlarge
Nanophotonics & Plasmonics - Ch. 2 | Helmholtz equations
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Chapter 2 | Theoretical Foundations: Electrodynamics Part 3: Derivation of the Helmholtz equations Derivations: drive.google.com/file/d/1uU5KGuFnbCq8C6vQ1eq4hzR3UHF55L78/view?usp=sharing by Dr. Nicolas Large, Department of Physics and Astronomy, The University of Texas at San Antonio physics.utsa.edu/nlarge
Nanophotonics & Plasmonics - Ch. 4 | Green tensor
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Chapter 4 | Optical Interactions Part 1: Derivation Green Tensor Derivations: drive.google.com/file/d/1uU5KGuFnbCq8C6vQ1eq4hzR3UHF55L78/view?usp=sharing by Dr. Nicolas Large, Department of Physics and Astronomy, The University of Texas at San Antonio physics.utsa.edu/nlarge
Nanophotonics & Plasmonics - Ch. 2 | Reciprocity theorem
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Chapter 2 | Theoretical Foundations: Electrodynamics Part 3: Derivation of the Reciprocity theorem Derivations: drive.google.com/file/d/1uU5KGuFnbCq8C6vQ1eq4hzR3UHF55L78/view?usp=sharing by Dr. Nicolas Large, Department of Physics and Astronomy, The University of Texas at San Antonio physics.utsa.edu/nlarge
Nanophotonics & Plasmonics - Ch. 2 | Green Tensor Symmetry
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Chapter 2 | Theoretical Foundations: Electrodynamics Part 3: Proof of Green Tensor Symmetry Derivations: drive.google.com/file/d/1uU5KGuFnbCq8C6vQ1eq4hzR3UHF55L78/view?usp=sharing by Dr. Nicolas Large, Department of Physics and Astronomy, The University of Texas at San Antonio physics.utsa.edu/nlarge
Nanophotonics & Plasmonics - Ch. 11 | Optical Spectroscopies & Sensing (2/2)
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Nanophotonics & Plasmonics - Ch. 11 | Optical Spectroscopies & Sensing (2/2)
Nanophotonics & Plasmonics - Ch. 4 | Optical Interactions (2/2)
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Nanophotonics & Plasmonics - Ch. 4 | Optical Interactions (2/2)
Nanophotonics & Plasmonics - Ch. 6 | Photonic Crystals (1/3)
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Nanophotonics & Plasmonics - Ch. 6 | Photonic Crystals (1/3)
Nanophotonics & Plasmonics - Ch. 13 | Electron Spectroscopies (1/2)
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Nanophotonics & Plasmonics - Ch. 13 | Electron Spectroscopies (1/2)
Nanophotonics & Plasmonics - Ch. 8 | Surface Plasmons (1/2)
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Nanophotonics & Plasmonics - Ch. 8 | Surface Plasmons (1/2)
Nanophotonics & Plasmonics - Ch. 3 | Nanoscale Optical Microscopy (1/2)
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Nanophotonics & Plasmonics - Ch. 3 | Nanoscale Optical Microscopy (1/2)
Nanophotonics & Plasmonics - Ch. 8 | Surface Plasmons (2/2)
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Nanophotonics & Plasmonics - Ch. 8 | Surface Plasmons (2/2)
Nanophotonics & Plasmonics - Ch. 9 | Localized Surface Plasmons (1/3)
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Nanophotonics & Plasmonics - Ch. 9 | Localized Surface Plasmons (1/3)
Nanophotonics & Plasmonics - Ch. 12 | Photonic vs Plasmonic Waveguides (2/2)
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Nanophotonics & Plasmonics - Ch. 12 | Photonic vs Plasmonic Waveguides (2/2)
Nanophotonics & Plasmonics - Ch. 3 | Nanoscale Optical Microscopy (2/2)
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Nanophotonics & Plasmonics - Ch. 3 | Nanoscale Optical Microscopy (2/2)
Nanophotonics & Plasmonics - Ch. 7 | Introduction to Numerical Methods
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Nanophotonics & Plasmonics - Ch. 7 | Introduction to Numerical Methods
Nanophotonics & Plasmonics - Ch. 10 | Optical Nano-Antennas (1/2)
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Nanophotonics & Plasmonics - Ch. 10 | Optical Nano-Antennas (1/2)
Nanophotonics & Plasmonics - Ch. 11 | Optical Spectroscopies & Sensing (1/2)
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Nanophotonics & Plasmonics - Ch. 11 | Optical Spectroscopies & Sensing (1/2)
Nanophotonics & Plasmonics - Ch. 9 | Localized Surface Plasmons (3/3)
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Nanophotonics & Plasmonics - Ch. 9 | Localized Surface Plasmons (3/3)
Nanophotonics & Plasmonics - Ch. 9 | Localized Surface Plasmons (2/3)
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Nanophotonics & Plasmonics - Ch. 9 | Localized Surface Plasmons (2/3)
Nanophotonics & Plasmonics - Ch. 2 | Theoretical Foundations (3/3)
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Chapter 2 | Theoretical Foundations: Electrodynamics Part 3: Dyadic Green functions, Reciprocity theorem, Evanescent fields. Lecture Notes: drive.google.com/file/d/1evZm3QZZvsu84VS1AoF5vk9hfLUh0I1v/view?usp=sharing Derivations: drive.google.com/file/d/1uU5KGuFnbCq8C6vQ1eq4hzR3UHF55L78/view?usp=sharing 0:24 - Dyadic Green functions 4:01 - Scalar Green function & spherical waves 8:09 - Reciprocit...
Nanophotonics & Plasmonics - Ch. 14 | Nonlinear Plasmonics
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Chapter 14 | Nonlinear Plasmonics Nonlinear optical processes, Polarization, Anharmonicity, Electric susceptibility, Optical Kerr effect, Second harmonic generation. Lecture Notes: drive.google.com/file/d/1Z3m4YsaYDC5Q9LnBFfbBuIzE9hITlRWK/view?usp=sharing 0:23 - Nonlinear optical processes 5:23 - Anharmonicity 8:31 - Polarization & electric susceptibility 13:10 - Examples 20:05 - Key Points Sum...
Nanophotonics & Plasmonics - Ch. 6 | Photonic Crystals (3/3)
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Chapter 6 | Photonic Crystals: From Nature to Applications Part 3: Fabrication 3D photonic crystals, Line and point defects, Waveguiding and Localization, Applications, Metamaterials. Lecture Notes: drive.google.com/file/d/1Nz_QMKuVcOGqdArXHA1vOQghvW51aSRP/view?usp=sharing 0:21 - Fabrication of a 3D photonic crystal 4:50 - Examples of 3D photonic crystals 6:40 - Defects in photonic crystals 16:...
Nanophotonics & Plasmonics - Ch. 13 | Electron Spectroscopies (2/2)
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Chapter 13 | Electron Spectroscopies Part 2: 3D EELS mapping, Comparison EELS/NF/LDOS/Potential, Cathodoluminescence (CL), 3D CL, Comparison Optical Spectroscopy/CL/EELS. Lecture Notes: drive.google.com/file/d/1GZZgfnfcwg5yS8Sg_Kd9tx4cgkzQz-BC/view?usp=sharing 0:27 - 3D EELS mapping 3:07 - Comparison EELS/NF/LDOS/Potential 9:31 - Light emission from swift electrons 10:49 - Cathodoluminescence (...
Nanophotonics & Plasmonics - Ch. 4 | Optical Interactions (1/2)
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Chapter 4 | Optical Interactions Part 1: Multipole expansion, Particle-field interaction, Radiating dipole. Lecture Notes: drive.google.com/file/d/1buLB1oBcubdvkOrYdWDVu4HWEPdKGmu5/view?usp=sharing 1:14 - Multipole expansion 8:08 - Classical particle-field Hamiltonian 12:24 - Radiating electric dipole & Green formalism 15:35 - Near, intermediate, and far fields 22:14 - Poynting's theorem by Dr....
Nanophotonics & Plasmonics - Ch. 10 | Optical Nano-Antennas (2/2)
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Chapter 10 | Optical Nano-Antennas Part 2: Plasmonic nano-antennas, Dipole antenna, Yagi-Uda antenna, Quantum emitter, Quenching and fluorescence enhancement, Multipoles. Lecture Notes: drive.google.com/file/d/1oe3fcJFrkLiM5GR9gQM-TLf1ePBE0WCD/view?usp=sharing 0:18 - Plasmonic nano-antennas 1:42 - Dipole antenna 3:42 - Yagi-Uda antenna 7:58 - Probes 8:27 - Quantum emitter & fluorescence enhance...
Nanophotonics & Plasmonics - Ch. 12 | Photonic vs Plasmonic Waveguides (1/2)
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Chapter 12 | Photonic vs Plasmonic Waveguides Part 1: Optical Waveguide classification, single mode, Optical fiber, Dispersion, Nonlinearity, Loss, Noise, Photonic Crystals, SPP at planar interface, Figure of Merit. Lecture Notes: drive.google.com/file/d/1VbI1M20KCeG8fuvNn070qegfdti-yfyC/view?usp=sharing 0:50 - Optical Waveguide classification 2:28 - Optical fiber 4:56 - Dispersion, Nonlinearit...
Nanophotonics & Plasmonics - Ch. 5 | Quantum Emitters
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Chapter 5 | Quantum Emitters: Molecules & Quantum Dots Quantum dots, Fluorescent molecules, Defects in diamonds, Absorption cross-section, Single molecule near-field probe. Lecture Notes: drive.google.com/file/d/1YjOb5xV8HpBptd1Yej_1YLAuT-h4BzLs/view?usp=sharing 1:05 - Fluorescent molecules 11:19 - Quantum dots 16:52 - Color centers in diamond 19:42 - Absorption cross-section 22:14 - Single mol...
Nanophotonics & Plasmonics - Ch. 6 | Photonic Crystals (2/3)
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Chapter 6 | Photonic Crystals: From Nature to Applications Part 2: Photonic bandgap, Photonic band diagrams, Optical properties. Lecture Notes: drive.google.com/file/d/1Nz_QMKuVcOGqdArXHA1vOQghvW51aSRP/view?usp=sharing 0:27 - Photonic bandgap 10:53 - Photonic band diagram 14:45 - Optical properties 16:34 - Optical spectra vs band structure 20:06 - FDTD simulations by Dr. Nicolas Large, Departme...
this is so helpful! thank you for making these explanations accessible to everyone :))
Thanks for this set of lectures! Preparing for my masters degree exam and thats a great refresher of ED!
Thanks. I'm glad you find it useful to you. Best of luck for your exam.
is MM a simulation method ? i am searching for method based on pure coding without any reliance on simulation for calculating the electromagnetic response.
By MM I'm guessing you're referring to the Method of Moments (MoM). By definition it is computational method as it solves Electromagnetic problems using mathematical methods. Now I'm not to understand what you mean by "method based on pure coding without any reliance on simulation"". Any computational method will be coded using mathematical methods to run on a computer. By definition any method that will run on a computer is a computer simulation. Now if you're referring to Analytical models, the only pure analytical solution of Maxwell's equation will be Mie theory but it is limited to spheres. Anything deviating from a sphere in a uniform medium will require computation simulations.
a huge thank you for making this video, because i was so doomed while choosing the right method to be used for scattering problem
Design antenna with this theory so that practically helpful
The preamble is redundant.
Great explanations. Thank you very much. We would appreciate it if you could do videos on Metastructures & Metamaterials. 11:10 is it the retardation effect due to the back and forth movement of the electrons (dipole moment) or the light?
Retardation effect is due to the time it takes for light to travel. If you imagine a sinusoidal wave passing onto a NP, the electrons on one side may experience an electric field pointing upward at a time t, while the electrons on the other side will experience the same field a later time because the wave it takes time for light to travel from one side to another. Even if this time is very short it's not instantaneous.
thank for your nice presentation. But I have Questions, How can simulate and calculate the optical absorption of Active layer of organic solar cells?
21:36 What instrument was used to image these waves?
These maps are not obtained experimentally. There are obtained from theory/simulation. There is no experimental optical setup that would allow you to map the spatial distribution of em waves inside a material (substrate). A SNOM (Sanning Near field Optical Microscope) can be used to map out the evanescent fields at the surface of the substrate.
@@nicolaslarge8622 Okay, thank you.
I would be glad if the lectures notes for each videos are added to the description.
Thanks. This is a great suggestion. I've just added a link to the lecture notes for all the videos.
6:07 Do the bolden E,H, B and D hats indicate unit vectors?
No, they are not unit vectors. They are the complex vector fields.
Prof. can you share the links to the website where you said the derivations of the equations will be posted? Thank you
You can download the notes from this Google Drive link: drive.google.com/file/d/12UzEIHvjVv4cpSepag4c5ZDne5SqAf1v
@@nicolaslarge8622 Thank you
excellent presentation.
hello professor, my research area is plasmonic, could you guide me in a proper way, from the very beginning to advance
If you were to focus only on plasmonics, I would recommend going though Ch. 1 (intro), 2 (electrodynamics), 4 (Optical Interactions), 7 (numerical methods), 8-9 (plasmonics). Chapters 10-14 are more related to specific applications of Plasmonics.
Thank you!
Great lecture professor, thanks!
thanks for breaking these equations down by terms
In 13:20 you said its an harmonic oscillator model but eq of motion has no restoring force. I think HO model is for Lorentz model which is for dielectric material.
That is partly correct. The generalized model (Drude-Lorentz-Sommerfield model) describe an harmonic oscillator with restoring force. This is the more rigorous description of the electron gas oscillation as these electrons do experience the Coulomb attraction from the ion background. However, because the electrons are only weakly bound to the nuclei, this Coulomb attraction can be neglected and the model reduce to a simple Drude-Sommerfeld model, which indeed contains no restoring force. The Lorentz model is later introduced to account for the Interband transitions (25:25). So as you can see it does not only apply to dielectric materials. Hope this clarifies.
Please make more videos on optical antennas. Thanks for making such a helpful video.
Thanks! Great! :)
Will you keep this online. Would love to take the time to absorb it all.
Yes, the whole course will remain online. Take all the time you need to go through.
nice video!
Thanks
Outstanding lecture! Thank you for sharing this!
professor, could you please provide the name of the text book for this course?
This course is not associated with a single textbook but it does mostly follow the structure of "Principles of Nano-Optics" by Novotny and Hecht.
amazing explanation!
Thanks. I'm Glad you liked it.
Hi Nicolas. Thank you for the detailed information! Liked your way of explaining things.