Title: Ione Implantasjon
1Ione Implantasjon
FYS4310
Doping
2
I
Ion Implantation
2Fys4310 I2, Program
What is I2
How it is done
Characteristics
Ranges
Rf(?), Sn(E), Se(E)- qualitatively
LSS
Impulse approximation
Examples, measurements
Disorder
Channelling
Annealing of disorder
3What is I2
How See next slide
Characteristics
Energy 15 keV - 250 keV, ( 5 keV.. MeV )
Dose 1e12 - 1e15(1e18) cm-2
The benefits of I2 technology
Control, reproducibility, uniformity, flexibility
Dose ( QT) measured accurately by integrating
current
High purity obtainable by mass separation
The less ideal things about I2 technology
Cost of an ion implanter machine
High throughput even more expensive Radiation
damage Impossible to implant delta function/the
ultimate shallow profile
4The Ion Implanter
Ion implanter in a FAB
5Ranges, Rprojected range Rp
Rp
Straggling ? Rp
Nuclear (elastic)
electron (inelestic
Concentration
?Rp
Depth
6S(E), Sn Se
LSS
s
n
e
e0.5
7Binary collision
Projectile
Impact parameter
8Impulse-approximation
M1, E0
q
x
a
r
b
M2
The force F acts on the projectile through the
traveled distance dx
The time it takes is
Integrate -inf. inf.
(Momentum change parallel path 0)
perpendicular
9Impulse-approximation, exampleCoulomb potential
10Impulse-approximation, example Coulomb potensial
Enter this in expression for b
Impulse approximation gives analytical results
for potentials of the type 1/r, 1/r2, 1/rs,
11LSS Impulse approx. with Thomas Fermi potential
Thomas-Fermi screening func.
e
s
n
e0.5
12LSS nuclear and electronic stopping
13Implant profiles
14Implant profiles
15Implant profiles
16Implant profiles
17Implant profiles through masks
18Implant profiles through masks
19Rp As,P,B,O,..
20Rp C,Zn,..
21SRIM
22Channeling
Steering of ion, small angle correlations between
collisions
Also feed in is possible
Range becomes larger than in an amorphous material
Critical angle - dependence on E, Z
Low energy largest problem/challenge
Implant in pre-amorphised Si with Si, Si with Ge
23Critical angle channeling
24Critical angle channeling
25Implantation disorder
Caused by elastic collisions
?t 10-13 sec, 10-12 thermal equilibrium, 10-9
reordering
Boron loss -mostly inelastic at start of
trajectory. Most displacement close to
the end
Arsenic starts large elastic loss, disorder
similar to As distribution
Density displaced atoms Dose/Energy Sn
FdisordergtFamorphous -gt amorph
Buried amorphous layer
26Damage profile
27Damage distribution
28Damage distribution
29RBS implant B
30Critical dose amorphous
31Annealing
Amorphous anneals different than non amorphous
Amorphous -SPEG
Epi growth , ?x prop. T, ?Ea 2.3 eV,
collective bond flipping
Two-stage annealing
Ion straggling disorder
32Annealing P
33Annealing B
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36Equipment/Limitation, implant angle
37Equip./limitations, scan angle
38Equip., sector magnet
39Equip., Mass separation
40Equip., Scanning