Messrs. Brattain, Shockley, and Bardeen, are credited
with inventing the first working transistor per their announcement in December of 1947. This article
provides what was for many people an introduction to the operational specifics of transistors. Although
its crude point contact ('cat's whisker') emitter and collector arrangement against the doped germanium
base element was still in a configuration that did not yet represent a significant challenge to the
domain of vacuum tubes, people of vision recognized its superior potential. As with most technologies,
progress occurred quickly and within a year the first commercial transistor was on the market. C.E.
Atkins, a frequent author in Radio & Television News magazine, related this story of his
own attempts to develop a transistor and offers the opinion that transistor might indeed someday replace
tubes as amplifiers, oscillators, and frequency converters.
A Crystal That Amplifies
Details of experiments with a double-contact germanium type crystal having transconductance.
By C. E. Atkins
Tung-Sol Lamp Works, Inc.
Bell Telephone Laboratories' recent announcement of a new electronic
component - the "Transistor" has started many "back of the shop" experiments. Like any other new design,
complete technical details on the product are withheld for a time. In view of this we believe it to
be appropriate to publish this report of an independent experiment that was, however, suggested by the
announcement of the "Transistor" - Editor.
Rumors of a recent sensational development in crystal transducers led the writer to explore a field
he had not touched since the early 1920's. Like thousands of other boys, he built the usual crystal
receivers and tinkered endlessly with "cat-whiskers" and coils. The very words "silicon" and' "galena"
evoke nostalgia for the halcyon days now, alas, so rapidly receding into a dim and remote era. Even
in that day the electron tube had largely supplanted the crystal detector, once the mainstay of wireless
reception. In addition to its role as a detector, amplification and oscillation were also attempted
without much success. Radio News in 1923 carried articles on the Zincite crystal, wherein feeble oscillations
were developed because of a small negative resistance exhibited under certain rather critical conditions.
This was elaborated on in further articles in September and October, 1924. This was referred to as the
"Crystodyne Principle," a term copyrighted by Radio News.
Nothing much came of these developments and with the increasing availability and lower cost of vacuum
tubes, crystal devices of this kind were largely relegated to the historical museum. However, during
the second World War, vast strides were made in the development of fixed crystal detectors for use in
radar where at ultra-high frequencies they were, in many instances, superior to electron tubes.
Spurred on by the fragmentary press releases and general trade gossip regarding a three terminal
crystal transducer using a germanium crystal, the writer undertook the fabrication of such a device
himself. A 1N34 crystal diode was procured and used as the source of a ready mounted germanium crystal.
By holding the 1N34 with a pair of long-nosed pliers gripping the cathode or negative lead (which is
clearly marked) the crystal may be exposed by chopping the ceramic adjacent the metal cap at the negative
end with side-cutters. The ceramic will shatter, and there is a brass stud inside against which the
cutting force expends itself. The germanium crystal is mounted on the stud and, with ordinary care and
good fortune, it is possible to strip the ceramic away without impairing the crystal.
Fig. 1. (A) Voltage-current characteristics of a single cat-whisker for two different
positions (a and b) on a germanium crystal. (B) Detail of (A) in the region of the elbow to show high
conductance characteristic in the forward direction.
The writer's attempts to utilize the cat-whisker used with the 1N34 were unsuccessful, so this part
of the assembly was discarded. Workable cat-whiskers can be made from the heater wire of almost any
150 ma. radio tube. The tubes can be defective for almost any cause - even heater failure, if in the
right place. The average radio shop generally has many of these at hand. The writer used type 35W4 because
several defective ones were currently available. By breaking the glass bulb and clipping the support
leads to all elements except the heater, it is possible in most cases to slide the heater out of the
cathode sleeve. The structure can be further disassembled by gripping one of the base pins with a pair
of long-nosed pliers while all the glass around the pin is chipped away with side-cutters. One then
has a base pin and lead welded to a segment of coated heater wire. It is necessary to leave the ceramic
coating on the heater wire in order to give it sufficient rigidity. It may be trimmed to suitable length
with a small pair of sharp scissors and a short tip (say one-sixteenth or one-thirty-second of an inch)
of bare wire can be exposed by gently and adroitly crushing the ceramic coating with a small pair of
tweezers. It is advisable to prepare several of these cat-whiskers, inasmuch as they are quite fragile
and several may be needed before a workable device is obtained.
As the photograph shows, the experimental assembly is mounted on a block of wood approximately 5
1/2" x 3 1/2" x 3/4". The lead from the germanium crystal mounting is saddled onto a brass nut in such
a way that this assembly will turn concentrically about a 6-32 machine screw. The machine screw, in
turn, is bolted to a soldering lug bent at right angles and soldered to a piece of No. 16 tinned bus
wire. As can be seen from the photograph, the wire is held by a Fahnestock clip mounted on the wood
block with a wood screw and spacer. This crude but effective arrangement facilitates adjustment of the
Two cat-whiskers are brought to bear on the crystal surface. Clips, extracted from a wafer type miniature
socket by cutting the bakelite away, are soldered to short lengths of No. 16 tinned bus wire. These
wires slide into binding posts mounted on brackets by means of which electrical connections and a measure
of adjustment are obtained. Since the cat-whiskers were prepared attached to the radio tube pins, they
can be readily fitted into the socket clips. After suitable forming with tweezers or small pliers and
the exercise of considerable cautious diligence, two cat-whiskers may be brought to bear upon the surface
of the crystal. They should engage the crystal with a light pressure and should be as close together
as feasible without contacting each other (the separation is only a few thousandths of an inch at most).
A magnifying glass is essential and considerable juggling artistry must be exercised before good characteristics
Fig. 1 shows a voltage current characteristic of a single cat-whisker (either one of them). It has
the shape typical of a barrier type rectifier. The curves a and b are from data for different cat-whisker
settings. Fig. 1B is a detail of Fig. 1A in the region of the elbow in order to show with greater clarity
the high conductance characteristic in the forward direction. This data indicates that in the forward
direction the impedance is approximately 100 ohms, while in the backward direction it is approximately
3000 ohms. These curves are typical of many taken. In the backward direction voltage breakdown is likely
to occur at above 50v, while in the forward direction burnout takes place in the neighborhood of 60
or 70 ma.
Fig. 2. Two curves relating the transfer or control parameters of the device.
Fig. 2 shows two curves relating the transfer or control parameters of the device. With a back voltage
of approximately -50v. on one cat-whisker, the control effect on current to this cat-whisker of the
application of small forward potentials to the other cat-whisker is shown. Curve a, indicating a transconductance
of 15,000, was about the best the writer was able to do. Characteristics of the order shown by curve
b are more readily obtainable. As Fig. 1 indicates, small forward potentials on the cat-whisker result
in rather substantial forward current so that unlike typical vacuum tube operation the input electrode
does require appreciable amounts of power for control purposes. However, since the output electrode
potential is much higher than the control electrode potential, a favorable ratio of controlled power
to controlling power may result even in cases where the input current is actually greater than the output
current! The writer's nomenclature designates the output circuit as the "B" circuit, while that associated
with the control cat-whisker is called "C" circuit. This is in rough accord with ancient usage.
Fig. 3A is a schematic diagram of a test circuit for measurements of amplication with the three terminal
crystal and for obtaining the data of the foregoing characteristic curves. Since the control electrode
impedance is only about 100 ohms, a stepdown transformer is needed to couple a signal into the device.
The d.c. resistance of the transformer secondary is only a few ohms and its effect on input circuit
current is negligible. The output load resistor RL can be shorted out while data for the
static characteristics is taken, although it is generally advisable to have a hundred ohms or so at
this point in order to prevent runaway at high current levels. In fact, the writer's data set forth
in Figs. 1 and 2 is in error to the extent of the IR drop in a protective resistor in series with the
The best conditions the writer has so far managed resulted in a change of 15 ma. Ip at
-50v. Eb with a control potential change of +1v. at 15 ma. This is a power ratio of 50 to
1. Unfortunately this condition was very unstable. More reliable and more readily obtainable adjustments
gave power ratios of approximately 15 to 1.
As an amplifier, a load of 500 ohms seemed to give the best results even though the curves apparently
call for 1500 ohms or more. A typical favorable adjustment of the cat-whiskers gave a maximum power
output of 200 mw. at Eb -40v., Ib 22 ma. (B power .88 watts), a C bias of + 2.0v.
and rectified Ic of 15 ma. ("C" circuit standby power 30 mw.) a likely a.c. input power of
approximately 22 mw., giving a power gain of 10 to 1. The small positive bias on the input cat-whisker
is necessary for relative linearity in output current. The waveform looked reasonably good on an oscilloscope
and the response was constant from 20 cycles to 30,000 cycles. Substantial voltage amplification should
be possible, if the resistor RL is replaced by a properly designed' step-up transformer.
Fig. 3. (A). Schematic diagram of test circuit used for measurements of amplification
with the three-terminal crystal and for obtaining data of curves of Fig. 2. (B) Circuit diagram of an
oscillator using double cat-whisker germanium crystal.
Fig. 3B is a circuit diagram of an oscillator using the double cat-whisker germanium crystal. A 15v.
r.m.s. signal was developed across either of the tank circuits at frequencies from 20 to 100 kc. depending
upon the L-C ratio. Eb was -35v., Ib 4 ma., Ic 1.5 ma. and Ec,
probably around -1.5v. due to the d.c. resistance of the transformer winding. These figures are considerably
different than the amplifier case. The oscillatory condition apparently has a marked influence on the
behavior of the crystal.
The writer has not as yet succeeded in operating the double contact crystal at high frequencies but
expects to do so at a later date.
Why does the device function as it does? An exact answer is doubtless couched in terms of mathematical
physics. Any purely verbal description is likely to be a generalized approximation at best. Barrier
rectifier characteristics stem from the fact that when dissimilar metals are extremely close together
without actually touching (100 atomic diameters or so) electrons from the more electropositive metal,
i.e., the one with the lowest work function, spill over into the other metal. That is to say, they actually
jump the barrier. Enough of them will do this and equilibrium is established when a back-potential equal
to the difference in work functions of the two metals is reached. If a positive external potential is
applied to absorb the electrons across the barrier the process continues and a current can flow in the
"forward" direction. A potential in the reverse direction, however, results in but little current since
electrons merely pile up at the barrier unless, of course, the potential difference is great enough
for breakdown. In the case of the germanium crystal and the tungsten contact a suitable barrier is supplied,
as it were, by the atomic structure of the germanium crystal because it is a certain type of semi-conductor.
As Fig. 1 indicates, electrons pass through the junction more readily in one direction than the other.
If a back voltage is applied to such a germanium-tungsten junction and a second tungsten cat-whisker
is positioned very close to the first one with a small forward potential applied to it the equilibrium
conditions are upset and it is possible for electrons to flow from the first cat-whisker in spite of
the backward potential.
What good is it? Prophesy is always hazardous, but it would seem that devices of this kind might
certainly supplant vacuum tubes as oscillators, amplifiers, and frequency converters in many applications.
While the writer's working model is admittedly crude - one could not sneeze in the same room without
substantially altering its characteristics - one can readily see how the necessary mechanical and electrical
refinements might be worked out as in all likelihood is already the case. New components and new circuit
techniques must of course be developed to use them in radio, television, and industrial electronics.
Posted October 26, 2016