PhotoluminescenceW is the process where a substance absorbs photons and re-emits photons. The incident photons excite electrons from a lower energy level to a higher energy level. As the electrons relax from the higher energy level to the lower energy level a photon is released. For a semiconductor, the electrons are excited from a set of energy levels called the valence band to a higher set of energy levels called the conduction band. The energy area between the valence band and the conduction band is called the band gap, and no electrons can be energetically found here.

Photoluminescence (PL) Spectroscopy is a type of contactless and nondestructive probing method for determining the electronic structure of a sample. In PL Spectroscopy, a laser is fired at a sample and the resulting fluorescence is measured by a spectrometer. The measured fluorescence can be used to determine the band gap of a semiconductor sample, impurity levels and possible defects in the sample, and the recombination mechanisms within the sample [1]. The determination of the electronic band gap for a semiconductor is the primary focus of this work.

As previously stated, in a semiconductor the electrons are excited from the valence to the conduction band. When electrons relax from the conduction band back down to the valence band, photons will be released. These photons will have energy that matches the transition from the conduction band to the valence band. Measuring the emitted photons' wavelength with a spectrometer will reveal the energy of the photon and therefore the size of the bandgap.

Design[edit | edit source]

Equipment List[edit | edit source]

  • Pavilion Integration Corp W445-40FS 445 nm laser - 500mW
Laser linear response

Design Schematic[edit | edit source]

Open-source-PL setup.png

Fig 1. The PL Test Bench
Fig 2. The PL Setup

Design Considerations and Explanations[edit | edit source]

The first step to using of PL spectroscopy is to have a powerful enough laser to excite the electrons from the valence band to the conduction band for all the different samples you wish to examine. We used at 450 nm (2.755 eV) laser to test samples. This will only work for semiconductors with bandgaps smaller than 2.755eV. When choosing a laser, it is the wavelength that is important with intensity being a secondary concern since it is the wavelength that determines if the electrons jump the band gap.

The setup of the PL system was designed from two separate works from the University of Colorado [2] and from the University of Ohio [3]. While researching the design of a PL system, it became obvious that researchers in general do not share their exact PL system design. Both of the works feature explicit diagrams of their photoluminescence spectroscopy setups. This open source PL spectroscopy setup is largely based on their previous work.

Both of the setups from Colorado and OSU used a neutral density filter. We do not use one here because our laser has a variable intensity dial on it. The use of a mirror to bounce the laser onto the sample instead of direct illumination from the laser offers more flexibility. It is much easier to adjust the mirror than the laser. The laser is incident on the sample at a glancing angle so that specular reflection from the sample does not go near the fiber optic cable. This will reduce the laser signal read on the spectrometer and thus the noise. The spectrometer will still read some of the laser signal from diffuse reflection. The focusing lens is used to gather the fluorescence from the sample and focus it onto the fiber optic cable. Thus the fiber optic cable must be placed away from the lens at a distance equal to the focal length of the lens. The whole PL experiment is done within a dark box to limit the effect of outside light on the spectrometer.

The mirror, sample, lens, and fiber optic cable are held in place with open source optics holders, which can be printed on an open source 3D printer. These open source optic holders allow us greater flexibility of placement than an optical bread board or lab bench would. However, it does lower the overall stability of the system, but such fined tuned stability is not needed for a simple PL system like this.

Improvements[edit | edit source]

There many improvements to this simple system that could be implemented.

Fig. 3. Open-source sample holder v3

Fig. 4. Open-source fiber switcher
Fig. 5. Open-source rail
  • Shown on the left is an improved open-source sample holder for pieces of semiconductor wafers. Instead of the clamping a sample, it provides a 2mm lip that allows samples to fluently sink into the slot. The purpose of the design is to make sample switching faster and easier, and reduce abrasion caused by frequent sample switch. Also notice the hemisphere hole in the backside makes it easier for tweezers work. The design can be applied to variety of wafer-like material, we also use it as a mirror holder since it works fine with our appropediately sized mirror.
  • On the right is the improved fiber holder is a dual-channel fiber switcher, which attaches two fiber optic cable to a 8mm smooth rod and allow easy switching between cables for optical experiments.
  • In order to smoothly move each parts in our PL system, we've designed an optical rail that helps accurately align our system in a line and make lens focusing much easier. Installed with strong magnet the rail is clinging to the platform firmly. Now the system works in a fixed X-Y plane with measurable precision.

Further improvement[edit | edit source]

  • A component for a low temperature liquid to cool the sample during data taking.
  • The addition of a optical chopper and lock-in amplifier would improve signal to noise ratio
  • A monochromator would allow the system to focus on a small range of wavelengths at a time instead of looking a wide range of wavelengths.

As part of the open source optics project we will be designing all of these components.

To operate[edit | edit source]

See also[edit | edit source]

Discussion[View | Edit]

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