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2010 Nano-Biophotonics Summer School @ UIUC Lecture 2 - 2D/3D Fourier transforms & Electromagnetic fields/ Lorentz-Drude model
25 Sep 2010 | | Contributor(s):: Gabriel Popescu
So far, we have discussed Fourier transformations involving one-dimensional functions. Of course, in studying imaging, the conceptmust be generalized to 2D and 3D functions. For example, diffraction and 2D image formation are treated efficiently via 2D Fouriertransforms, while light scattering...
2010 Nano-Biophotonics Summer School @ UIUC Lecture 5 - Biomedicine - A tour of the Cell
25 Sep 2010 | | Contributor(s):: Marina Marjanovic
Edited and Uploaded by Omar Sobh, University of Illinois at Urbana-Champaign
2010 Nano-Biophotonics Summer School @ UIUC Lecture 3 - Fourier optics - Nonlinear optics - Microscopy
25 Sep 2010 | | Contributor(s):: Kimani C Toussaint
Ray optics-Limit of wave optics when wavelength isinfinitesimally smallWave optics-provides a description of opticalphenomena using scalar wave theoryElectromagnetic optics- provides most completetreatment of light within classical opticsQuantum optics-provides a quantum mechanicaldescription of...
2010 Nano-Biophotonics Summer School @ UIUC Lecture 4 - Gaussian beam propagation - Elastic light scattering - Dynamic light scattering
Often, experiments involve light beams. A light beam can be defined as a distribution of field that fulfills the approximation in Eq. 20,i.e. is characterized by a dominant wave vector component, k(z) >> k(x) , k(y) . A beam is, therefore, the spatial equivalent of quasimonochromaticlight, where...
2010 Nano-Biophotonics Summer School @ UIUC Lecture 1 - Introduction
20 Sep 2010 | | Contributor(s):: Rashid Bashir, Stephen Boppart