light emitting diodes
DESCRIPTION
Light Emitting Diodes. NanoLab 2003. Outline. Motivation/Applications: Why LED’s? Background Fabrication Testing Conclusions. Motivation/Applications: Why LED’s?. Wide range of colors Efficient and Reliable Saves money Requires less money to operate Generates less heat - PowerPoint PPT PresentationTRANSCRIPT
Light Emitting Diodes
NanoLab 2003
Outline
• Motivation/Applications: Why LED’s?• Background• Fabrication• Testing• Conclusions
Motivation/Applications: Why LED’s?
• Wide range of colors • Efficient and Reliable
– Saves money• Requires less money to operate• Generates less heat
– Good for electronics– Reduced AC costs
• Last longer
Why Do We Care? Efficiency (lumens/watt)
Light Bulbs vs LED’s•Light Bulbs
–Filament• Sudden
Failure-Breaks/Burns down
–Recent bulbs last up to two years at ~20 lumens/watt
–Fluorescent tubes last about 7500 hrs at ~80 lumens/watt
•LED’s–No filament
• Gradual Failure-Intensity decrease over time
–Last from 50,000 to 100,000 hrs (5-10 yrs)
–Recent LED’s (orange,red) have efficiency of ~100 lumens/watt
– Generate little heat• Reduced A/C costs
Applications•Communication (fiber optics)•Blue Laser Diodes
–Video Recording–Data Storage–Televisions–Video Games–High Density DVD’s–DVD-ROM drive
•Extra Motivation:–First company to produce efficient, reliable, cost-
effective WHITE LED’s will make lots of money.
Isolated Atoms > Crystal > Artificial Atom
isolated atom
Diamond lattice
Background-Band Gaps and Lattice Constants
• Lattice mismatch reduces efficiency
Background-Band Gaps and Lattice Constants
Bandgap energy vs lattice constant of various III-semiconductors at room temperature.
What are the III-Vs
Background-Band Gaps and Lattice Constants
Room-temperature bandgap energy vs lattice constant of common elemental and binary semiconductors.
Background -Lattice Mismatch
• Lattice mismatch reduces efficiency
Two crystals with mismatched lattice constants resultion in dislocation at or near the interface between the two semiconductors.
Background: pn Junctions and Recombination• Electron from
donor material recombines with hole in acceptor material.
• Produces photon with energy hv equal to that of the band gap.
• Smaller band gaps give infrared/red light; larger band gaps give blue/UV light
Carrier distribution in pn homojunctionsCarrier distribution in pn homojunctions
Background: pn Junctions and Recombination
• Electron and holes are trapped in the quantum wells.• Such spatial overlap gratly enhances the
recombination rate - brightness, efficiency.
Heterojunction under forward biasHeterojunction under forward bias
Background: Ohmic Contacts
• http://nina.ecse.rpi.edu/shur/Ch3/sld043.htm
Contacts
Relatively little resistance
DopingHole in lower energy band allows for easier travel for electrons
Electrons forced to higher, partially filled band electron moves easier
Making our Samples• We are working with two
different samples– GaAsP/GaAs– GaAs/GaAs
• We dope the sample with ZnAs (p-type) using the quartz ampoule method– ZnAs and our sample are cleaned
using TCE, Acetone, and Methanol
– Our quartz is cleaned using 2.5% HF
– Seal the ZnAs and our sample in quartz with vacuum
– Bake for 15 minutes for roughly 2 m of diffusion
Making the Samples• We use a black wax (softening point at
T~140oC) and 1% Bromine in Methanol etch to make contacts
Test LED’s using curve tracer• Check to see that
device actually works
• Find turn-on voltage
• P=VI, the less power it takes to operate the device, the better
Red LED at 1.5V, 16mA
Current I (mA)
Voltage V (V)
The Setup
SpectraPro
Sample
Laser
Optic cable
Lens
The Setup Continued
SpectraPro Setup Curve tracer
Gratings for SpectraPro
One of our LED’s
Red LED, 1.5V,15mA
Current (mA)
Voltage (V)
Testing Our Sample• Use SpectraPro-150 to test wavelength, relative
intensity, and spectral length of our LED
Red LED Testingwithlasers
Some LED’s
Intensity v Wavelength
0500010000150002000025000300003500040000
400 450 500 550 600 650 700 750
Wavelength (nm)
Inte
nsity
Intensity
White LED: RGB
Conclusions
• Several samples were made– Most did not reach a turn-on voltage when
applying a current using the curve tracer– One LED was in the infrared range the other red – The two LEDs that did turn on were not all that
efficient.
References
• Photos from Jason Rausch• E. Fred Schubert
– www.lightemittingdiodes.org• Craford, M.George and Stringfellow, G.B.
High Brightness Light Emitting Diodes. Academic Press, 1997.
• Professor Colin J Humphreys– www.sterlinggroup.org.uk/lecture2001.htm