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basics of semiconductor

Basics of semiconductor

basics of semiconductor


It is not easy to define a semiconductor if we want to take into account all its physical

However, generally, a semiconductor is defined on the basis of electrical
conductivity as under:

A semiconductor is a substance which has resistivity (10 -4 to 0.5 Ωm) in between
conductors and insulators e.g. germanium, silicon, selenium, carbon etc.
The reader may wonder, when a semiconductor is neither a good conductor nor
an insulator, then why not to classify it as a resistance material? The answer shall be
readily available if we study the following table:

basics of semiconductor
basics of semiconductor

Comparing the resistivities of above materials, it is apparent that the resistivity of
germanium (semiconductor) is quite high as compared to copper (conductor) but it is
quite low when compared with glass (insulator).

This shows that resistivity of a
semiconductor lies inbetween conductors and insulators. However, it will be wrong to
consider the semiconductor as a resistance material. For example, nichrome, which is
one of the highest resistance materials, has resistivity much lower than germanium.
This shows that electrically germanium cannot be regarded as conductor or insulator or
a resistance material. This gave such substances like germanium the name of
It is interesting to note that it is not the resistivity alone that decides whether a
substance is semiconductor or not. For example, it is just possible to prepare an alloy
whose resistivity falls within the range of semiconductors but the alloy cannot be
regarded as a semiconductor. In fact, semiconductors have a number of peculiar
properties which distinguish them from conductors, insulators and resistance materials.

Properties of Semiconductors

(i) The resistivity of a semiconductor is less than an insulator but more than a
(ii) Semiconductors have negative temperature co-efficient of resistance i.e.
the resistance of a semiconductors decreases with the increase in
temperature and vice-versa. For example, germanium is actually an
insulator at low temperatures but it becomes a good conductor at high
(iii) When a suitable metallic impurity (e.g. arsenic, gallium etc.) is added to
semiconductor, its current conducting properties change appreciably. This
property is most important and is discussed later in detail.

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