SCOUT tutorial 2

- A -

	Step 1: Homogeneous silver layers
	Configuration of the PL object

anisotropic layer

anisotropic optical properties

automatic fit

	Step 4: Determination of tilt angles from experiments
	Fitting PL spectra

autoscale

averaging

averaging formulas

- B -

back-scattered radiation

backside

Bergman representation

	The problem
	Step 2: Testing simple effective medium models
	Step 3: The Bergman representation

Bergman representation object

- C -

- D -

	The problem
	Step 2: Testing simple effective medium models
	Step 1: Optical constants
	Reflectance analysis

dielectric function model

dipole approximation

dipole resonance

drag

- E -

effective dielectric function

effective medium

	The problem
	Step 2: Testing simple effective medium models

Effective Medium Approxiamtion

electric field

electronic transition

	Configuration of the PL object
	Fitting PL spectra

electronic transitions

- F -

	Step 3: Tilt angle as master parameter
	Fitting PL spectra

- G -

geometry

	Step 2: Testing simple effective medium models
	Step 3: The Bergman representation

glass

	The problem
	Step 1: Homogeneous silver layers

- H -

- I -

interband transitions

	Introduction
	Configuration of the PL object
	Fitting PL spectra

island films

islands

- K -

Kim oscillator

	Step 1: Optical constants
	Configuration of the PL object
	Fitting PL spectra

- L -

layer stack

	Step 2: Layer stack and spectra
	Configuration of the PL object

layer thickness

light wavelength

list of fit parameters

list of layer stacks

list of spectra

	Step 2: Layer stack and spectra
	Configuration of the PL object
	Fitting PL spectra

list of susceptibilities

- M -

Maxwell Garnett formula

metal islands

microgeometry

molecular orientation

- N -

- O -

	Step 1: Optical constants
	Introduction
	Reflectance analysis

optical model

orientation

	Introduction
	Step 3: Tilt angle as master parameter

- P -

	Introduction
	Configuration of the PL object
	Fitting PL spectra

Percolation

percolation strength

	Step 2: Testing simple effective medium models
	Step 3: The Bergman representation

	Configuration of the PL object
	Fitting PL spectra

PL spectrum object

	Introduction
	Configuration of the PL object

PL spectrum window

polarization

	Step 2: Layer stack and spectra
	Configuration of the PL object

porous silicon

	Introduction
	Reflectance analysis
	Fitting PL spectra

- R -

random

random orientation

Range

	Step 2: Layer stack and spectra
	Configuration of the PL object

re-absorption

real part

Reflectance

	Step 1: Homogeneous silver layers
	Reflectance analysis
	Configuration of the PL object

	Introduction
	Step 3: Tilt angle as master parameter

rough

- S -

sample inhomogeneities

silicon

	Step 1: Optical constants
	Introduction

silver

	The problem
	Step 1: Homogeneous silver layers

	Configuration of the PL object
	Fitting PL spectra

spectral density

	The problem
	Step 2: Testing simple effective medium models
	Step 3: The Bergman representation

spectral range

	Step 1: Homogeneous silver layers
	Step 2: Testing simple effective medium models
	Step 2: Layer stack and spectra

- T -

	Step 2: Testing simple effective medium models
	Step 4: Determination of tilt angles from experiments
	Reflectance analysis
	Fitting PL spectra

thickness variation

tilt angle

	Introduction
	Step 3: Tilt angle as master parameter

	Step 1: Homogeneous silver layers
	Configuration of the PL object

- U -

- V -

	The problem
	Step 2: Testing simple effective medium models
	Step 3: The Bergman representation

- W -

wavelength

	The problem
	Configuration of the PL object

- X -

x-y-plane

- Z -

z-direction