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When optical components are reduced to the nanoscale, they exhibit interesting properties that can be harnessed to create new devices. For example, imagine a block of material with thin layers of alternating materials. This creates a periodic arrangement of alternating dielectric constants, forming a "photonic crystal" that is analogous to the electronic crystals used in semiconductor devices. Photonic crystals, along with quantum dots and other devices patterned at the nanoscale, may form the basis for sensors and switches used in computers and telecommunications. More information on Nanophotonics can be found here.
Towards Light-Spin Interface for NV Center in Diamond
17 Mar 2015 | | Contributor(s):: Alexey V Akimov
In this work we present our efforts on using CMOS compatible hyperbolic metamaterials and optical fibers to construct efficient single-photon sources and sensing elements using NV center in diamond.
Quantum Optics in New Systems: From Plasmonics to Cold Atoms
In my talk I will describe our activities in both field on quantum interfaces and cold atoms
Generation Model with Coupled Mode Theory
20 Jul 2012 | | Contributor(s):: yujie guo, Peter Bermel, Roman Shugayev
Models generation of an optical comb in a multiple-resonance cavity coupled to a single waveguide, using coupled mode theory to represent linear and nonlinear dynamics
Spaser in Quantum Regime
02 Feb 2015 | | Contributor(s):: Mark I Stockman
The spaser have been introduced theoretically and discovered experimentally. We briefly consider quantum theory and latest results on spaser as an ultrafast quantum generator and amplifier of nanoplasmonic fields, ultrabright nanolabel, and highly-efficient nanosensor. We present latest original...
Optical Properties of Single Coaxial Nanowires
06 May 2014 | | Contributor(s):: Sarath Ramadurgam, Tzu-ging Lin, Katherine Elizabeth Hansen, Chen Yang
Computes various optical properties of a single nanowire with up to 2 shell layers using Mie-formalism
PhotonicsPOS: Particle on Substrate
13 Mar 2014 | | Contributor(s):: Rohith Chandrasekar, Urcan Guler, Ludmila Prokopeva, Alexander V. Kildishev
Scattering solutions for a core-shell spherical particle on a planar lamellar substrate
[Illinois] Spectral Method for Linear and Nonlinear Phenomena in Nanophotonics
23 Dec 2014 | | Contributor(s):: Qing Huo Liu
Modeling of Optical Multilayers for Both Spectra and Admittance Loci
03 Aug 2014 | | Contributor(s):: Joel che email@example.com, kuo-ping chen
simulate spectra and admittance loci of multilayer structures
Thermophotonic Selective Emitter Simulation
14 Jul 2014 | | Contributor(s):: Anubha Mathur, Enas Sakr, Peter Bermel, Namrata Vivek Raghavan
Simulate Thermophotovoltaics With Rare Earth-Based Selective Emitters
Addressing the Inverse Problem of Optical Imaging
19 Aug 2014 | | Contributor(s):: Aaron Lewis
"Addressing the inverse problem of imaging" by Prof. Aaron Lewis from the Nanonics NanoPhotonics workshop.
TPV efficiency simulation
22 Jul 2013 | | Contributor(s):: Qingshuang Chen, Peter Bermel, Roman Shugayev, Masayoshi Sumino, Zhou Zhiguang, Omar R Yehia, Evan L Schlenker
Simulate the efficiency of a thermophotovoltaic system
19 Aug 2013 | | Contributor(s):: Xin Tze (Joyce) Tee, Haejun Chung, Peter Bermel
Finite-difference Time-Domain Simulations for photovoltaic cells
DDSCAT Convert: A Target Generation Tool
17 Jul 2013 | | Contributor(s):: John Feser, AbderRahman N Sobh
Convert .obj files to DDSCAT shape files
Perfect Absorber Metamaterial simulator
19 Dec 2012 | | Contributor(s):: sainath gupta, Bala Krishna Juluri
perfect absorber matametrial
PHYS 620 Lecture 14 : Surface Plasmons
13 Feb 2013 | | Contributor(s):: Roberto Merlin
PHYS 620 Lecture 8: Phonons
PHYS 620 Lecture 15: Plasmons in Nanoparticles
PHYS 620 Lecture 12: Excitons III
S4: Stanford Stratified Structure Solver
11 Sep 2012 | | Contributor(s):: Jiarui Kang, Xufeng Wang, Peter Bermel, Chang Liu
S4 is a frequency domain code to solve layered periodic structures. Internally, it uses Rigorous Coupled Wave Analysis (RCWA; also called the Fourier Modal Method (FMM)) and the S-matrix algorithm.
PHYS 620 Lecture 5: Diamond and Zincblende Semiconductors: Band Structure