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III–V and II–VI compounds                       137

            excitations, that is electrons can be excited into the conduction band. The only
            difference relative to Ge and Si is that III–V compounds have an ionic contribu-
            tion to the bonding as well. This is not particularly surprising. We mentioned in
            Chapter 5 that the ionic bond of NaCl comes about because the one outer elec-
            tron of sodium is happy to join the seven outer electrons of chlorine to make up
            a completed ring—so it is easy to see that, with Ga having three outer electrons
            and As having five outer electrons, they will also strike up a companionship in
            order to complete the ring.
               Which are the most important III–V materials? The oldest one, and  Note, however, that a III–V ionic
            technologically the best developed, is GaAs, to which serious attention has  bond is weaker than a I–VII
            been paid since the middle of the 1950s and which has been the preferred ma-  ionic bond.
            terial for a host of devices. Why? One might expect that arsenic was the last
            thing anyone in any laboratory would have wanted to work on. However, some
            of the rivals, for example AlSb, fell by the wayside because of a tendency to
            decompose quickly, and, most importantly, GaAs was the material that offered
            high mobility relative to Ge and Si. For measured curves of electron and hole
            mobilities against impurity concentration, see Fig. 8.8.
               What can we say about the energy gap of GaAs? It is, 1.42 eV, a lot higher
            than that of Ge, the element between them in the periodic table. The energy
            gap is higher which means that it is more difficult to break a bond in GaAs
            than in Ge. Why? Because of the presence of ionic bonding. We can also say
            something definite about the energy gaps of some other compounds relative to
            that of GaAs. If we combine with Ga the element in the periodic table above
            As, we obtain GaP with an energy gap of 2.24 eV. If we choose for the other
            element in the compound Sb, which is below As in the periodic table, then we
            obtain GaSb with an energy gap of 0.67 eV. The same is true if we combine
            various elements from column III with As. The energy gap of AlAs is 2.2 eV,
            whereas the energy gap declines to 0.36 eV for InAs. The general rule is easy to
            remember: the lower you go in the periodic table in your choice of the elements
            the smaller is the gap. What is the reason? The farther down the columns of the
            periodic table (Table 4.1) the higher are both the nuclear charge (Ze) and the
            number of filled electronic inner shells. Hence, the valency electrons are farther
            from the nucleus and so more loosely bound. Thus, the bonding force between
            atoms is weaker (lower melting point) and the energy to promote electrons
            into the conduction band is less (lower energy gap). This is shown in Table 8.2
            where also we have omitted the heaviest group III–V elements thallium (atomic
            number 81) and bismuth (83) as their compounds have a very narrow gap and
            so are almost metallic.


                      1
                                                 e
                    Mobility (m 2 V –1 s –1 )  10 –1  h






                                                                             Electron and hole mobilities in GaAs
                    10 –2                                                    Fig. 8.8
                       10 20    10 21   10 22    10 23    10 24    10 25     as a function of impurity
                                                      –3
                                     Impurity concentration (m )             concentration.
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