N Type Semiconductor
Before understanding what is n-type semiconductor we should focus on some basic theories of atomic science. We all know that each atom of any substance requires eight electrons at its outermost orbit. But it is also true that all atoms do not have eight electrons at their outermost orbit. But all the atoms have an ultimate goal to have eight electrons at their outermost orbit. The electrons at an outermost orbit of an atom are called valence electrons. If the outermost orbit of an atom does not have eight electrons, then there will be as many vacancies as the lack of electrons in orbit. These vacancies are always ready to accept electrons to fulfil eight electrons in the outermost orbit of the atom. The most commonly used semiconductors are silicon and germanium. The Silicon has 14 electrons which have been configured as 2, 8, 4. Germanium has 32 electrons which have been configured as 2, 8, 18, 4. Both of the semiconductors have 4 electrons at their outer-most orbit. Hence, there are vacancies for more 4 electrons.
Four valence electrons fulfil these vacancies each of which is from four individual neighbouring semiconductor atom. Actually, in this way, all atoms of a semiconductor crystal make a covalent bond with their nearest most neighbourhood atoms. Ideally, all valence electrons in a semiconductor crystal are involved in forming of covalent bonds. Hence, there should not be any free electron in the crystal. But this is not the actual case. At absolute 0o Kelvin there would not be any free electron in the crystal, but when the temperature rises from absolute zero to room temperature, numbers of valence electrons in the bonds are thermally excited and come out from the bond and generate a number of free electrons in the crystal. These free electrons cause the conductivity of the semiconductor materials at any temperature higher than absolute zero. There is a method of increasing conductivity of semiconductors at any temperature greater than absolute zero. This method is called doping. In this method is pure or intrinsic semiconductor is doped with pentavalent impurities like antimony, arsenic and phosphorus. These impurity atoms replace some of the semiconductor atoms in the crystal and occupy their positions. As the impurity atoms have five valence electrons in the outermost orbit 4 of them will create the covalent bond with four adjacent semiconductor atoms.
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One valance electron of impurity atom does not get chance to involve in covalent bonding and becomes more loosely bounded with parent impurity atom. At room temperature, these loosely attached fifth valence electrons of impurity atoms can come out from its position due to thermal excitation. Due to this phenomenon, there will be a considerable number of free electrons, but still, there are breakdowns of covalent bonds in the crystal due to thermal excitation at room temperature. The free electrons in addition to free electrons created due to the breakdown of a semiconductor to semiconductor and semiconductor to impurities covalent bonds cause the total of free electrons in the crystal. Although whenever a free electron gets created during the breakdown of a semiconductor to semiconductor covalent bond, there is a vacancy created in the broken bond. These vacancies are referred to as holes. Each of these holes is considered as a positive equivalent of a negative electron as it gets created due to lack of one electron. Here electrons are main mobile charge carriers. In an n-type semiconductor there will be both free electrons and holes. But the number of holes is quite smaller than that of electrons because holes are created only due to the breakdown of the semiconductor to semiconductor covalent bond whereas free electrons are created both due to loosely bounded non-bonded fifth valence electron of impurity atoms and breakdown of the semiconductor to semiconductor covalent bonds.