- A -

About

absorption

angle of incidence

IconStep 1: Homogeneous silver layers
IconConfiguration of the PL object

anisotropic layer

anisotropic optical properties

automatic fit

IconStep 4: Determination of tilt angles from experiments
IconFitting PL spectra

autoscale

averaging

averaging formulas

- B -

back-scattered radiation

backside

Bergman representation

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

Bergman representation object

broadening

Bruggeman formula

- C -

Conversion

current transport

- D -

database

decimals

definition points

density gradient

dielectric function

IconThe problem
IconStep 2: Testing simple effective medium models
IconStep 1: Optical constants
IconReflectance analysis

dielectric function model

dipole approximation

dipole resonance

drag

- E -

effective dielectric function

effective medium

IconThe problem
IconStep 2: Testing simple effective medium models

Effective Medium Approxiamtion

electric field

electronic transition

IconConfiguration of the PL object
IconFitting PL spectra

electronic transitions

EMA

embedded particle

Emission

Excitation

- F -

film thickness

fit

fit parameters

IconStep 3: Tilt angle as master parameter
IconFitting PL spectra

- G -

geometry

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

glass

IconThe problem
IconStep 1: Homogeneous silver layers

- H -

halfspace

Help&Manual

host

hypertext jumps

- I -

infrared

inhomogeneities

inhomogeneous

insulator

interactions

interband transitions

interference

interference effects

interference fringes

internal efficiency

IconIntroduction
IconConfiguration of the PL object
IconFitting PL spectra

island films

islands

- K -

Kim oscillator

IconStep 1: Optical constants
IconConfiguration of the PL object
IconFitting PL spectra

- L -

layer stack

IconStep 2: Layer stack and spectra
IconConfiguration of the PL object

layer thickness

light wavelength

list of fit parameters

list of layer stacks

list of spectra

IconStep 2: Layer stack and spectra
IconConfiguration of the PL object
IconFitting PL spectra

list of susceptibilities

list of transitions

Looyenga formula

luminescent layer

- M -

magic angle

master parameter

matrix

matrix material

Maxwell Garnett formula

metal islands

microgeometry

molecular orientation

molecules

multiphase-composite

- N -

network

- O -

observation angle

OJL

optical constants

IconStep 1: Optical constants
IconIntroduction
IconReflectance analysis

optical model

orientation

IconIntroduction
IconStep 3: Tilt angle as master parameter

orientation angles

oscillator

oscillator strength

oscillators

Overview

- P -

parameter variation

Parameters

peak

IconIntroduction
IconConfiguration of the PL object
IconFitting PL spectra

Percolation

percolation strength

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

photoluminescence

PL

PL active layer

PL interpretation

PL layer

PL model

PL radiation

PL sources

PL spectrum

IconConfiguration of the PL object
IconFitting PL spectra

PL spectrum object

IconIntroduction
IconConfiguration of the PL object

PL spectrum window

polarization

IconStep 2: Layer stack and spectra
IconConfiguration of the PL object

porous silicon

IconIntroduction
IconReflectance analysis
IconFitting PL spectra

- R -

random

random orientation

Range

IconStep 2: Layer stack and spectra
IconConfiguration of the PL object

re-absorption

real part

Reflectance

IconStep 1: Homogeneous silver layers
IconReflectance analysis
IconConfiguration of the PL object

reflection

resonance

resonance frequency

response

IconIntroduction
IconStep 3: Tilt angle as master parameter

rough

- S -

sample inhomogeneities

silicon

IconStep 1: Optical constants
IconIntroduction

silver

IconThe problem
IconStep 1: Homogeneous silver layers

slave parameter

slider

sliders

spectra list

IconConfiguration of the PL object
IconFitting PL spectra

spectral density

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

spectral range

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

spectral unit

spectrum simulation

sputtering

sputtering rate

substrate

superposition

susceptibility list

- T -

technical manual

thickness

IconStep 2: Testing simple effective medium models
IconStep 4: Determination of tilt angles from experiments
IconReflectance analysis
IconFitting PL spectra

thickness variation

tilt angle

IconIntroduction
IconStep 3: Tilt angle as master parameter

transition

transitions

transmission

Transmittance

IconStep 1: Homogeneous silver layers
IconConfiguration of the PL object

- U -

unit

- V -

vibrational mode

vibrational modes

volume fraction

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

- W -

wavelength

IconThe problem
IconConfiguration of the PL object

- X -

x-y-plane

- Z -

z-direction