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Photoluminescence is the optical emission obtained by photon excitation (usually a laser) and is commonly observed with III-V semiconductor materials. This type of analysis allows non-destructive characterization of semiconductors (material composition, qualitative investigations, etc.

Description

An Argon laser beam is focused on the sample which is located in the center of the sample compartment. If the energy of photons coming from the laser source is greater than the energy gap of the semiconductor, the sample emits photons. These are collected and analyzed with a dual flat field spectrograph. Two detectors are used, a CCD and an InGaAs array. This system allows investigations from 0.75 to 2.4 eV.

Measurement Procedure

We identify the position of one or several photoluminescence lines, and with the help of mathematical models, determine the composition of the material.

Example: GaAlAs sample.

The following expression gives the AlAs composition as a function of the photoluminescence line position (*):

E(x) = 1.424 + 1.247 x (at T = 300K)

with

E(x): line position (in eV units)

x: AlAs composition

Measured line position: 1.643 eV

then x = 0.18 (18% of AlAs)

Applications

• Qualitative investigations for semiconductors.
• Fast determination of alloy composition in ternary compounds (GaAlAs, GaInAs, AlInAs...)

System Advantages

The two array detectors, CCD and InGaAs, offer high sensitivity and speed. They can both be mounted simultaneously on a Dual Flat Field Spectrograph allowing full characterization of the sample with ease.