The Transistor |




The first transistor (germanium is at the bottom of the
triangel)
(the pictures above
were taken over from http://www.lucent.com/ideas/heritage/transistor/history.html)
The first step to the explication of the physical fundaments of the transistor were made by Shockles´ formulation of the Theory of positive-negative conversions. Important was also the role of emitting the moving charge-carriers on one side and their receiving (collecting) on the opposite side. He brilliantly concluded his analysis with the invention of a junction transistor. According to his conceptions it was a sandwich adjustment of a small tablet made from the n-material between two p-type areas (or conversely). One month later – in February 1948 – John Shive did the experiment of principle: he put two phosphor-bronze contacts to the opposite sides of the Germanium tablet (0,1 mm thick). The behaviour of this transistor corresponded with Shockley´s theory. Then Shockley continued in another team of fellow-workers and after many experiments he finished his junction theory and so he created solid fundaments of the “transistor” phenomenon (he published this theory in 1950 in – today well known - classical text Electrons and Holes in Semiconductors).
The brief principle of Shockley´s junction theory consists in the apposite adjustment of the p and n areas. What are these areas? Absolutely clean semiconductors´ material (type of material, where only 1 atom of dirt comes to 100 millions atoms of clean semiconductor) has got at least 35million times bigger resistance then the copper has. (by Germanium and Silicon it is even 4000 times bigger). But when we add just futile amount of admixture (10.000.000 : 1) the conductivity grows several times and especially the new qualitative attributes appear. E.g. a semiconductor type n arises, if we add slight tingle of quinquevalent Arsen to chemical quadrivalent Germanium. Its conductivity is caused by the surplus of electrons (so called electron conductivity). Conversely a semiconductor type p arises if we add only trivalent Indium. Its conductivity is caused by the absence of electrons (so called holes conductivity). If these areas are combined e.g. in this order: n-p-n and if we advisably apply the poles of voltage sources (-,+,+), the electrons will freely float from the left n area (emitter) do the central p area (base) and from here to the right n area (collector). The current flowing through the collector will be many times bigger then the current in the emitter. That way attached transistor works as an amplifier The theory was clear, however two types of transistor designs existed at that time, but none of them was good enough for the manufacturing. The first one was the dotted transistor (this type was created as the first one). The second one is the junction transistor created by Shockley. The dotted one was could have been manufactured at that time but had had many insufficiencies. Mainly the great dispersion of the electric attributes. With some exaggeration we could say, that each piece was an original. But despite these problems this type was being manufactured for more then 10 years, e.g. like the telephone oscillators or the ear-trumpets for the hard of hearing – their production had to be quitted because of their bad quality). In the second case the question were the junction transistors. Their attributes were in the expected limits but they were more complicated to manufacture and were material-purity demanding.As we enunciated at the beginning, two materials were used: Germanium and Silicon. Already since the beginning it was known, that Silicon has got more suitable attributes. E.g. it is energetically more advantageous, is less dependent on the temperature changes and the current in the back circuit is smaller. But at the beginning the manufacturing of Silicon with the demanded quality was aggravated with the demanding chemical and metallurgical process. E.g. the smelting temperature of Silicon is 1415 °C and of Germanium only 937 °C. The right way of Silicon manufacturing, which would assure the cleanliness comparable with Germanium was not found untill 1953.
In the meantime (1952) the Bell’s labs sold the patent-rights for transistor to
everyone who was ready to pay 25.000 $ for it.
The first commercially manufactured
Silicon transistors (1954)
The mass manufacturing of transistor could begin. In 1952 the thickness of the base-tablet was cut back to 10 micromilimeters and so the marginal frequency of the transistor was increased up to 10 MHz. The first diffuse Germanium mesa transistor with the marginal frequency 500 MHz was manufactured in 1954. A year later a Silicon one was produced. In 1956 the original “transistor” team gets a Nobel prize …
The first consumer goods (ear-trumpet) with a
integrated circuit (1964)
(fig. from page http://www.ti.com/corp/docs/history/1960snf.htm)

