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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
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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
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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.
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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.
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EE141
© 2009 Associate Professor PhD. T.Vasileva
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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.
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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
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EE141
© 2009 Associate Professor PhD. T.Vasileva
4
p-Type Semiconductors
Covalent bonds
Majority
carriers
Neutral boron (B) atom
Acceptor atom – III valence
electrons
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Hole
p >> n
Minority
carriers
Negatively charged ion
When a neutrally charged acceptor
gains an extra electron it will become
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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.
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EE141
© 2009 Associate Professor PhD. T.Vasileva
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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.
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EE141
© 2009 Associate Professor PhD. T.Vasileva
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