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| May 17, 2006 |
Aluminum Nitride Light Emitting Diodes with the Shortest Wavelength |
| -Towards Dioxin, PCB Decomposition Technology- |
Nippon Telegraph and Telephone Corporation (NTT) has observed light of 210-nm wavelength from aluminum nitride (AlN) light emitting diodes (LED). This is the shortest wavelength ever observed from any semiconductor, and confirms the long-held theoretical expectation that AlN could emit light in the deep ultraviolet (DUV) region (*1) (wavelengths from 200 to 300 nanometers; nano is 10-9).
Light emitted at wavelengths in the DUV can efficiently decompose persistent toxic substances such as dioxin and PCBs (*2), which have caused serious environmental problems all over the world. Therefore, our AlN LED promises to have a major environmental impact. In addition, AlN semiconductor itself is harmless, unlike the mercury lamp. Replacing gas lasers with high-power AlN DUV lasers could lead to small, highly reliable, and highly efficient nanometer fabrication.
The major problem in AlN LED fabrication had been high densities of crystalline
defects and high impurity concentrations. NTT has overcome these problems by
developing technologies for high-purity AlN crystal fabrication and for p-type
and n-type doping (*3), which are essential for LED fabrication.
This achievement
is the first step towards practical AlN LEDs, but is a giant step in science,
and will be reported in "Nature" magazine, May 18 issue. |
[Features]
| 1) |
Fabrication technology of high-pure AlN semiconductor. |
| 2) |
p-type and n-type doping technologies essential for LEDs. |
| 3) |
Observation of deep ultraviolet light, 210nm, the shortest in the world. |
| 4) |
AlN LEDs will replace conventional gas sources such as mercury lamp. |
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[Background]
Aluminum nitride (AlN) has the widest direct band gap among semiconductors (*4),
Therefore, it has always been expected theoretically that an AlN light-emitting
device would emit light with the shortest wavelength among semiconductors (Fig.
1). However, AlN has had a high density of crystalline defects and the p-type
and n-type doping technologies essential for LEDs were not available. Of course,
AlN LEDs have not been achieved.
At present, blue and ultra-violet gallium nitride
(GaN) LEDs and laser diodes are commercially available, but their shortest wavelength
is 365nm, still in the near-ultraviolet region (*1).
The deep ultraviolet (DUV)
light sources available at present are only gas sources, such as mercury lamps
or gas lasers. Mercury lamps and gas lasers use toxic substances, and gas lasers
have practical problems: the gas has to be supplied often and the lasers are
large and inefficient. Replacing these light sources with semiconductor devices
will save space and greatly improve reliability and efficiency.
DUV light has
very short wavelength, and can be focused to spots only tens of nanometers in
diameter (Fig. 2). It therefore can be applied to nanometer-scale fabrication
and to submicron-particle detection. In addition, the energy of DUV light is
high enough to decompose very stable substances. Therefore, DUV LEDs are expected
to have a wide range of applications, such as in environmental protection, nanotechnology,
information technology, medical treatment, sanitation, and biology. |
[Technology]
(1) High-purity AlN fabrication technology
NTT noticed that the purity could be improved by reducing crystalline defects
and impurities (*5). Therefore, NTT constructed AlN fabrication
system that could endure fabrication temperatures as high as 1100°C and prevent
secondary reactions of composite aluminum and nitrogen sources. As a result,
we were able to decrease defect density and impurity concentration by one order
and produce high-purity AlN crystal (Fig. 3).
(2) AlN p-type and n-type doping technologies
In this high-purity AlN, by doping magnesium (Mg) to AlN we achieved p-type AlN,
and, similarly, by doping silicon (Si) to AlN, we achieved n-type AlN (Fig.
4).
(3) AlN deep-ultraviolet (DUV) light-emitting diodes (LEDs)
Next, we formed a high-purity AlN light-emitting layer sandwiched by p-type and
n-type AlN layers and fabricated AlN LEDs (Fig. 5).
When current flowed through the AlN LEDs, we observed 210-nm DUV light (Fig.
6). |
[Future plan]
By further decreasing crystalline defects and impurities and by improving doping
technologies, NTT intends to improve the output power of AlN LEDs, which should
lead to practical use. |
[Terminology]
*1 Deep ultraviolet (DUV) light, Neat ultraviolet light
Light at wavelengths shorter than 400nm is called ultraviolet light. Ultraviolet
light in the wavelength region from 200 to 300nm is called deep ultraviolet
(DUV) light, and ultraviolet light in the wavelength region from 300 to 400nm
is called near ultraviolet light. Ultraviolet light with a wavelength shorter
than 200nm is absorbed by air, and therefore cannot be used in air. Therefore,
it is called vacuum ultraviolet light. Thus, the wavelengths of DUV light are
shortest at which light can be used in air. The shorter the wavelength is, the
smaller the area in which light can be concentrated and the higher the energy
becomes.
*2 Dioxin, PCB
Dioxin and PCB (polychlorinated biphenyls) are very toxic but very stable chemically.
One way to decompose them chemically and to make them harmless is to expose them
to DUV light. Conventional DUV light sources are gas sources, and therefore are
not practical. But if practical AlN LEDs can be built, we will have an invaluable
light source for the decomposition of harmful chemical substances.
*3 p-type, n-type doping technologies
Adding a small amount of dopant to pure semiconductors can drastically change
their electric properties. With p-type doping, holes, positively charged carriers,
can be supplied, and with n-type doping, electrons, negatively charged carriers,
can be supplied. In LEDs or semiconductor lasers, holes are supplied from a p-type
layer and electrons from an n-type layer to the light-emitting layer, and when
holes and electrons combine, light is emitted. Therefore, p-type and n-type doping
technologies are essential for LEDs or semiconductor lasers.
*4 Direct band gap semiconductor
From its physical properties, any semiconductor has either a direct band gap
or an indirect band gap. In direct band gap semiconductors, electrons and holes
combine directly, and the efficiency of light emitting is therefore very high.
Therefore, direct band gap semiconductor is suitable for LEDs and semiconductor
lasers. In contrast, in indirect band gap semiconductors, electrons and holes
combine indirectly, and efficiency of light emission is very low. Therefore,
indirect band gap semiconductor is not suitable for light-emitting devices.
For example, diamond and boron nitride (BN) have wide band gap energies similar
to that of AlN, but because they are indirect band gap semiconductors, they are
not suitable for LEDs.
Band gap
In a semiconductor, there is forbidden energy gap between the electron-allowed
and hole-allowed bands. The band gap energy is inversely proportional to the
wavelength of light emitted from a semiconductor. AlN has the widest band gap
energy among direct band gap semiconductors and can therefore emit the shortest
light.
*5 Crystalline defect, impurity
Ideally in AlN crystal, aluminum (Al) and nitrogen (N) atoms order periodically.
However, if the crystal has any anomalies, there will be vacancies at which an
Al or N atom sit and these vacancies become crystalline defects. If there are
atoms other than Al or N, such as oxygen, those atoms become impurities. When
crystalline defects or impurities exist and p-type or n-type doping is tried,
the dopants capture generated holes or electrons, and p-type or n-type semiconductor
is not formed.
In the case of AlN, because Al and N atoms are attracted strongly to each other,
during crystal fabrication, secondary reactions between Al and N sources can
easily occur. As a result, in AlN, crystalline defects and impurities occur very
easily.
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- Fig.1 Aluminum Nitride, "Shortest Light-Emitting Semiconductor"
- Fig.2 AlN's Superior Physical Properties and its Ability in Devices
- Fig.3 Technology (1): High-Purity AlN Crystal Fabrication Technology
- Fig.4 Technology (2): p-type, n-type Doping Technologies
- Fig.5 Technology (3): AlN Deep-Ultraviolet Light-Emitting Diode
- Fig.6 Technology (4): 210-nm Light Emission; World's
Shortest
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For further information, contact:
NTT Science and Core Technology Laboratory Group
Planning department
Tamechika
Tel: 046-240-5152
http://www.ntt.co.jp/sclab/contact_e/ |
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Copyright (c) 2006 Nippon telegraph and telephone corporation |
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