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Ione Implantasjon

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Range becomes larger than in an amorphous material ... Buried amorphous layer. Arsenic starts large elastic loss, disorder similar to As distribution ... – PowerPoint PPT presentation

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Title: Ione Implantasjon


1
Ione Implantasjon
FYS4310
Doping
2
I
Ion Implantation
2
Fys4310 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
3
What 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
4
The Ion Implanter
Ion implanter in a FAB
5
Ranges, Rprojected range Rp
Rp
Straggling ? Rp
Nuclear (elastic)
electron (inelestic
Concentration
?Rp
Depth
6
S(E), Sn Se
LSS
s
n
e
e0.5
7
Binary collision
Projectile
Impact parameter
8
Impulse-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
9
Impulse-approximation, exampleCoulomb potential
10
Impulse-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,
11
LSS Impulse approx. with Thomas Fermi potential
Thomas-Fermi screening func.
e
s
n
e0.5
12
LSS nuclear and electronic stopping
13
Implant profiles
14
Implant profiles
15
Implant profiles
16
Implant profiles
17
Implant profiles through masks
18
Implant profiles through masks
19
Rp As,P,B,O,..
20
Rp C,Zn,..
21
SRIM
22
Channeling
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
23
Critical angle channeling
24
Critical angle channeling
25
Implantation 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
26
Damage profile
27
Damage distribution
28
Damage distribution
29
RBS implant B
30
Critical dose amorphous
31
Annealing
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
32
Annealing P
33
Annealing B
34
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35
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36
Equipment/Limitation, implant angle
37
Equip./limitations, scan angle
38
Equip., sector magnet
39
Equip., Mass separation
40
Equip., Scanning
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