January 31, 2005... In 1970 I was working at the David Sarnoff Research Center
in Princeton, New Jersey. These Laboratories were named previously the R.C.A.
Laboratories. I was a Research Chemist and my area of work, at the time, involved
materials development, with novel and potentially valuable materials for developing
light emitting diodes (LEDs) and solid state lasers. Around September 1970
I was asked by my group head supervisor, David Richman, if I would take on the
task of growing Gallium Nitride (GaN) for Dr. Jacques I Pankove, who was a staff
member at the laboratories at the time. They needed someone to take over the work
from Herb Maruska who had gone back to Graduate School. The semiconductor Gallium
Nitride was a material that was of interest at the time because of its high band
gap with the potential for developing a blue LED or laser. Dr. James J Tietjen,
who was our Lab Director, envisioned using the GaN blue LEDs to make a flat panel
television display, one which could be hung on the wall like a picture. The project
that I would begin to work on was the gas phase growth of GaN as previously reported
by Maruska and Tietjen.[1] Dr. Tietjen had started this project at RCA Labs in
May 1968.
This program consisted of growing GaN, which was then a candidate
semiconductor for blue LEDs or lasers because of its high band gap at about 3.4
eV, and which would require making p-type material. This blue emitter was greatly
sought after because the other primary colors, red and green, had already been
established with GaAsP and GaP:N. Blue was the one primary color that was missing
an emitter material in order to be used in future full color flat panel displays.
Previous work at RCA Labs had established the method of growth by Vapor Phase
Epitaxy (VPE) and had made some initial investigations of doping. The work entailed
the growth of GaN in a horizontal quartz system originally designed for the growth
of GaAs, using chlorides to transport vapors containing Ga, and a hydride gas
(arsine) to transport the Group-V element. Zinc for p-type doping was transported
as its own vapor from a vertical sidearm tube. To grow GaN, the arsine source
was replaced with ammonia.
The VPE growth system consisted of a complex of
quartz and pyrex tubes. The upstream section consisted of two parallel horizontal
quartz tubes each about two feet long and one inch in diameter. They were joined
to a single quartz tube, two inches in diameter and about two feet long. Films
were deposited in the upstream end of this two inch diameter tube. In one of the
narrower tubes, gallium metal (a liquid) would be placed in a quartz boat. At
the entrance to this tube was a ground quartz joint coated with halocarbon stopcock
grease, and through this joint hydrogen chloride gas and hydrogen were allowed
to flow over the gallium. This reaction would form gallium chloride, a gas that
can be transported by the hydrogen flow into the reaction zone. The other narrow
tube also began with a ground joint, and served to admit gaseous anhydrous ammonia
to the growth chamber, also with hydrogen as a carrier gas. When the two components
ammonia and gallium chloride mixed in the growth chamber, GaN was formed.
Downstream
of the growth zone, the two inch tube divided into two perpendicular tubes, with
the original tube terminating at a large pyrex stopcock. The other sidearm served
to conduct the effluent gases to the exhaust system. The stopcock created a loadlock.
Beyond the stopcock, which was also lubricated with halocarbon stopcock grease,
was a pyrex forechamber. This allowed samples to be inserted and removed from
the growth chamber without opening that part of the reactor to the ambient. The
forechamber received the substrate placed on a quartz sled attached to a true-bore
quartz rod. The rod was positioned through a true-bore pyrex bearing that was
filled with flowing inert gas. The rod could be inserted and withdrawn through
the bearing.
The procedure was to place a sapphire substrate upon the sled
at the front end of the true-bore rod. The stopcock was of course closed at this
time. The true-bore gas bearing featured a ground glass joint which was then affixed
to the forechamber. The forechamber would then be flushed with inert gas to remove
all traces of air. If desired, it could also be flushed with hydrogen. Meanwhile,
hydrogen was also flowing through the main growth tube.
The growth system
was contained in a furnace with multiple zones. Each zone had an independent temperature
control. Typically there were two zones for the dual one inch diameter inlet tubes,
followed by a short mixing zone, and then the growth zone. There was also a sidearm
for doping coming up out of the mixing zone, with its own temperature control.
In the sidearm was located a small quartz bucket loaded with zinc metal. The bucket
was held on the end of another true-bore quartz rod, which allowed the position
of the bucket to be moved within the sidearm furnace. The zinc vapor and hence
the delivery rate for zinc was determined by the temperature of the bucket. At
first it was necessary to establish a calibration graph for zinc concentration
in the grown film versus temperature. The zinc would be evaporated in a flow of
hydrogen gas.
As the growth system came on line, the products of GaN both
undoped and doped with zinc would be passed on to Dr. Pankove for his evaluation.
It was only a short time following my earliest growth run that the exciting news
came over the phone from Dr. Pankove that he had observed for the first time electroluminescence
in GaN.[2]
This news caused a modest amount of excitement in the Laboratories
and I particularly recall the stimulating urgency of the work I was involved with.
Now each new growth run was made to try to modify the temperature or a flow rate
or some other variable to optimize a particular property of the GaN product. As
time went by, new results were coming out of Dr. Pankoves measurements and
evaluations of the devices that he made from the GaN crystal films that I supplied.
This was a very exciting time indeed!
Thick films of GaN were required to
obtain free standing GaN wafers without the substrate attached for evaluation
of the effect of stress in the film. On the thicker films an uneven thickness
was obtained across the wafer. A quick room temperature test was designed and
used to reveal the gas flow patterns within the growth tube. This was accomplished
with the furnaces open to permit observations. By admitting both HCl and ammonia
simultaneously into the growth tube (in the absense of any liquid gallium) at
the typical flow rates for a run, a flow of white smoke was generated which showed
us the gas flow patterns.
These tests established a need for better positioning
of the substrate facing the gas flow. When this was accomplished by having the
substrate facing the flow at a sloping angle, the growth of the thicker films
became more uniform in thickness and satisfactory for testing the diodes.[3]
This
period of time in 1971 and 1972 gave me what everyone who is involved with basic
research would dream of, ie, a hectic, exciting productive effort to advance the
frontier of science.
As 1973 arrived, new advances continued to be made with
the GaN material.[4,5] Maruska and Pankove introduced Mg doping.[6] But each new
advance became longer to achieve, as with any project as it matures, and obtaining
a really bright blue LED became a harder goal to obtain.[7] The tide of interest
began to wane at the Laboratories, and I had the feeling that we had better do
something soon or support would dry up for GaN. While new results were being reported
such as Li and Be doping,[8] the highly sought after quest for p-type doping was
not accomplished.[9] But it seemed to us that if enough time were permitted, results
would be forth coming.
I envied Bell Labs at this time because I had heard
that they had a group of about 10 staff researchers working to make p-type GaN.
I was just waiting for the "big shoe" to drop and read that they
were successful. If only we could have enough time to do all of the various tests
that we were thinking of, I was sure that we would succeed in beating them to
the elusive goal.
It was at this time, in the summer of 1973, that I attended
a Gordon Conference in New Hampshire featuring nitride research. At this meeting
I was at a table one evening with the head of the Bell Labs Materials Group, and
I did not hesitate to ask him about the GaN work at his laboratory. I was astonished
at his answer. He said that they were shutting down the work on GaN and moving
on to other more promising work, because they were unable to make p-type GaN.
Well, I thought, so be it. Except for the fact that Dr. David Richman, my group
head at the time, was also at the table and heard what was said, I do not think
that I would have mentioned it again for some time.
As it turned out, our
nitride work continued for about another 6 months. Herb Maruska returned from
graduate school at the end of the year, expecting to rejoin the project. Then
in January 1974, Dr. Tietjen called us into his office and explained that spending
money on the GaN work with no results that could lead to a commercial product
in the near term was exhausting his budget. "You guys have bled me dry
with nothing useful to show for it," he said. Then he phased out the project.
What else could he do?
A scientist is fortunate if at some time in his or
her career, an exciting project comes along and the adrenalin rises. I had such
a time with the GaN project and I will always remember it as a good time.
References
H. P. Maruska and J. J. Tietjen, "The preparation and properties
of vapor-deposited single crystal GaN," Appl. Phys. Lett., 15, 327 (1969).
2. J. I. Pankove, E. A. Miller, D. Richman, J. E. Berkeyheiser, "Electroluminescence
in GaN," J. Luminescence, 4, 63 (July 1971).
3. J. I. Pankove, E. A. Miller, J. E. Berkeyheiser, "GaN yellow light-emitting
diodes," J. Luminescence, 6, 54 (Jan 1973).
4. J. I. Pankove, E. A. Miller, J. E. Berkeyheiser, "GaN electroluminescent
diodes," RCA Review, 32, 383 (Sept 1971).
5. J. I. Pankove, E. A. Miller, J. E. Berkeyheiser, "GaN blue light-emitting
diodes," J. Luminescence, 5, 84 (Mar 1972)
6. H.P. Maruska, D.A. Stevenson, J.I Pankove "Violet Luminescence of Mg-doped
GaN," Appl. Phys. Lett., 22, 303 (1973).
7. J. I. Pankove, E. A. Miller, J. E. Berkeyheiser, "Electroluminescence
in GaN," Proc. Of Luminescence Conf. Leningrad, Ferd Williams, editor,
Plenum Publishing Corp, New York, pp. 426-430 (1972).
8. J. I. Pankove, M. T. Duffy, E. A. Miller, J. E. Berkeyheiser, "Luminescence
of insulating Be-doped and Li-doped GaN," J. Luminescence, 8, 89 (Sept
1973).
9. J. I. Pankove, J. E. Berkeyheiser, E. A. Miller, "Properties of Zinc-doped
GaN," J. Appl. Phys., 45, 1280 (Mar 1974).