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impurities{}
Specifications that define imputities
impurities{
donor{ name =
"n-P-in-Si" energy = 0.045 degeneracy =
2 }
donor{ name =
"n-As-in-Si" energy =
0.054 degeneracy = 2 }
acceptor{ name =
"p-B-in-Si" energy =
0.045 degeneracy =
4 }
Note: To fully ionize the impurity atoms,
just specify a large negative number for the energy level.
donor{ name = "fully-ionized"
energy = -1000 degeneracy
= 2 }
charge{ name =
"positive-charge" type =
positive } #
can be used to put positive charges into the device (e.g. to describe interface
charges)
charge{ name =
"negative-charge" type =
negative }
# can be used to put negative charges
into the device (e.g. to describe interface charges)
}
Donors/acceptors
The energy separation from the conduction or valence band edge is given in
units of [eV] .
These energies are meant as ionization
energies, e.g. a donor with an energy level right below the conduction
band edge would be specified by a small positive energy level.
When impurity levels are relatively deep compared to the thermal energy kBT/e
at room temperature, incomplete ionization must be considered. (This is done
automatically).
(Cheat parameter: energy = -1000
(for instance), that means, all electrons are fully ionized from
the donors (similar for holes/acceptors). This might be useful for low temperatures like 4
K where usually the degree of ionization is very small. By using -1000
one can force them to be completely ionized.)
Degeneracy of the specified energy levels
Degeneracy of impuritiy levels affects their degree of ionization.
The degeneracy of donors is usually assumed to be equal to
2 , for acceptors it is equal to
4 .
shallow donors: degeneracy factor 2
Outer s orbital is onefold occupied (neutral state). There is one
possibility to get rid of one electron but there are two to incorporate
one (spin up, spin down).
shallow acceptors: degeneracy factor 4
The sp3 orbital is threefold occupied. Thus, one possibility
to incorporate an electron, four possibilities to get rid of one.
More details on degenerate impurity levels can be found in e.g. "Physics of
Optoelectronic Devices" by Shun Lien Chuang.
Note that in nitride semiconductors crystallizing in the wurtzite structure the
degeneracy factor may vary from 4 to 6 because of a small valence
band splitting.
If full ionization is assumed, i.e. energy =
-1000 , then the degeneracy
factor effectively becomes irrelevant. This can be seen from eqs. (1.4) - (1.7)
in PhD thesis of S. Birner.
Donor levels (n-type) in units of [eV] relative to conduction band edge
n-As-in-Si
= 0.054 # DESSIS
n-As-in-Si
= 0.049 # American Institute of
Physics Handbook, 3rd ed., McGraw-Hill, New York (1972)
n-P-in-Si
= 0.045 # DESSIS, American Institute
of Physics Handbook, 3rd ed., McGraw-Hill, New York (1972)
n-Sb-in-Si
= 0.039 # DESSIS
n-N-in-Si
= 0.045 # DESSIS
n-As-in-Ge
= 0.013 # American Institute of
Physics Handbook, 3rd ed., McGraw-Hill, New York (1972)
n-P-in-Ge
= 0.012 # American Institute of
Physics Handbook, 3rd ed., McGraw-Hill, New York (1972)
n-N-in-SiC
= 0.10 # DESSIS
n-Si-in-GaAs
= 0.0058 #
n-Si-in-AlAs
= 0.007 # 300 K, Landolt-Boernstein
n-Si-in-Al0.27Ga0.73As =
0.006 # Landolt-Boernstein
More parameters can be found in the nextnano³ database file
database.in or at this website:
http://www.ioffe.ru/SVA/NSM/Semicond/
Acceptor levels (p-type) in units of [eV] relative to valence band edge
p-In-in-Si
= 0.16 # DESSIS
p-B-in-Si
= 0.045 # DESSIS, American Institute
of Physics Handbook, 3rd ed., McGraw-Hill, New York (1972)
p-Al-in-Si
= 0.057 # American Institute of
Physics Handbook, 3rd ed., McGraw-Hill, New York (1972)
p-B-in-Ge
= 0.010 # American Institute of
Physics Handbook, 3rd ed., McGraw-Hill, New York (1972)
p-Al-in-Ge
= 0.010 # American Institute of
Physics Handbook, 3rd ed., McGraw-Hill, New York (1972)
p-Al-in-SiC
= 0.20 # DESSIS
p-C-in-GaAs
= 0.027 # Landolt-Boernstein 1982
More parameters can be found in the nextnano³ database file
database.in or at this website:
http://www.ioffe.ru/SVA/NSM/Semicond/
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