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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.
Raghunandan Mohan Rao
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
German Felipe Giraldo
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
PHYS 620 Lecture 7: Effective-Mass Theory, Landau Levels and Franz-Keldysh Oscillations
PHYS 620 Lecture 10: Excitons I
PHYS 620 Lecture 11: Excitons II