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Semiconductors Semiconductor Elements 1 EE141 © 2009 Associate Professor PhD. T.Vasileva Silicon Atom Structure W WGe< WSi < WGaAs Nucleus and electrons Conduction band W Bandgap energy Valence band As a whole the atom is neutral. Energy Bands 2 EE141 © 2009 Associate Professor PhD. T.Vasileva 1 Intrinsic Semiconductors Free electron ni = pi Energy ni.pi= ni2 Hole niGe > ni Si > niGaAs W Covalent bonds Equal numbers of free electrons and holes are created in the covalent bonds breaking up. Heat from the surrounding air is the primary source for the required energy. EE141 Exitation of an electron from the valence to the conductive 3band. © 2009 Associate Professor PhD. T.Vasileva Electron and Hole Currents Drift movement vE = µE µn > µp Holes move slower than electrons by drifting from one covalent bond to another. The movement of one hole requires the movement of many more valence electrons. Jp Jn J = Jn +Jp Free electrons and holes are referred to as mobile carriers. Carriers flow 4 EE141 © 2009 Associate Professor PhD. T.Vasileva 2 Current Direction The direction of the hole's flow is opposite to that of the free electrons. The electric current is conventionally represented by the flow of positive charges. 5 EE141 © 2009 Associate Professor PhD. T.Vasileva Impure Semiconductors – n-Type Covalent bonds Neutral phosphorus (P) atom Donor atom – V valence electrons Majority carriers n >> p Free electron Minority carriers Positively charged ion A donor atom will easily donate an extra electron to the silicon crystal. 6 EE141 © 2009 Associate Professor PhD. T.Vasileva 3 Carriers in n-Type Semiconductor Majority carriers are formed in donor ionisation process. One free electron will be created, but without a hole. Minority carriers are created by breaking covalent bonds. nno = ND Whenever a neutral donor atom looses one electron, it will become a positively charged ion. 7 EE141 © 2009 Associate Professor PhD. T.Vasileva Carriers Concentration T = const Relation between majority/minority carriers’ concentrations nno.pno= ni2 Carrier type Semiconductor type nno = ND pno= ni2 Intrinsic concentration nno = const (T) pno = f (T) nno 8 EE141 © 2009 Associate Professor PhD. T.Vasileva 4 p-Type Semiconductors Covalent bonds Majority carriers Neutral boron (B) atom Acceptor atom – III valence electrons EE141 Hole p >> n Minority carriers Negatively charged ion When a neutrally charged acceptor gains an extra electron it will become 9 a fixed negatively charged ion. © 2009 Associate Professor PhD. T.Vasileva Carriers in p-Type Semiconductor Majority carriers are formed in accepror ionisation process. One hole will be created, but without an electron. Minority carriers are created by breaking covalent bonds. ppo = NA Whenever a neutral boron atom gains an extra electron, it will become a negatively charged ion. 10 EE141 © 2009 Associate Professor PhD. T.Vasileva 5 Currents in Impurity Semiconductors In n-type semiconductors, electrons are the majority carriers. In p-type semiconductors, holes are the majority carriers. The value of the electron current In will far exceed the value of the hole current Ip. In p-type semiconductors the hole current Ip will far exceed the electron current In. 11 EE141 © 2009 Associate Professor PhD. T.Vasileva 6