Title: On the Influence of Substrate Temperature
1On the Influence of Substrate Temperature on the
Ion Energy Distribution Function
M.M. de Jong MsC. Final Talk 9-9-08
2Outline
- Introduction
- Thin film solar cells
- Plasma-Enhanced chemical vapor deposition
- Ion energies
- Why?
- How?
- Results
- Pressure variations
- Power variations
- Dilution variations
- Temperature variations
- Restore high T energy flux
- Conclusions
3Thin Film Solar Cells
- Positive, neutral and negative doped layers
- Thickness 1µm
- Deposite on any substrate
- Holy grail
- Roll to Roll on plastics
- Low T!
4Plasma Enhanced Chemical Vapour Deposition
- Plasma ingredients
- Gas
- Oscillating field
- Free electron
- Ionization
- e- A ? A 2e-
- Dissociation
- SiH4 e- ? SiH3 H
- Ambipolar diffusion leads to positive plasma
bulk and plasma sheaths
5Introduction Why?
- Ions contribute to growth rate and create growth
sites - Ions transfer energy to the substrate (both
kinetic and potential (10eV)) - Ions enhance surface diffusion, densifying the
film
From Hamers, 1998, PhD thesis
6Retarding Field Ion Energy Analyzer (RFIEA)
- Retarding field ion energy analyzer
- V1 -30V to repel electrons
- V2 sweeps from 0V to 75V
- V3 -30V to repel secondary electrons
7RFIEA II
8Ion Energy Distributions Function (IEDF)
- Measures I as a function of V2
- Ion current
- Energy flux
- In a collisionless plasma
- heavy positive ions gain eVpl
- Light ions gain eVpl
- Elastic collisions will decrease ion energy
- Chemical reactions will broaden the IEDF
12.2W, 280C, FH225 sccm, 0.10 mbat
9RFIEA vs. MS
- Equally sensitive to ions with different masses
- No chromatic abberation, enabling calculation of
average ion energies - Less failure due to clogging (low T ? dust)
- Therefore better reproducibility
12.4W, 280C, FH245.5 sccm, FSi2H44.5 sccm,
0.10 mbar
10Results Pressure variations(in pure hydrogen)
- Increasing pressure will increase number of
collisions and reduce ion energy and ion current
12.0W, 200C, FH220 sccm
11Results Dilution variations
- Increasing silane flow decreases ion energies and
ion current - Silane has a lower ionization energy
- Hydrogen atoms go faster, increasing ion current
12.3W, 280C, Ftotal50sccm, 0.13 mbar
12Results Power Variations(in pure hydrogen)
- Increasing dissipated power will increase Vpl
- Increasing power will increase ionization rate
25C, FH210 sccm, 0.10 mbar
13Results Temperature Variations
- Direct influence of substrate T on IEDF
- Therefore it is even harder to compensate for
reduced surface mobility at low T - Change in particle density?
12.3W, Ftotal50sccm, 0.10 mbar
14Results Temperature Variations II
- Constant p/T
- But still T dependent
- Overcompensation
- Sticking coefficients depend on T
- Check growth rate?
12.3W, Ftotal50sccm
15Results Restore High T Conditions
- Ion current is easily restored
- Ion energy is hard to restore
50C, Ftotal50sccm, 0.10 mbar
16Results Restore High T Conditions II
- Ion current can be restored
- Ion energy can be increased, not restored
12.4W, 50C, Ftotal50sccm
17Results Restore High Temp Conditions III
- Energy flux can be restored by both increasing
power and decreasing pressure
18Results Restore High Temp Conditions IIII
- Although the energy flux can be reacquired at low
T, the IEDF changes shape
FH245.5 sccm, FSi2H44.5 sccm
19Conclusions
- Decreasing substrate temperature will decrease
energy flux to the substrate - Therefore it is more difficult to compensate for
decreased surface mobility at low T - When going from 280C to 50C, this decrease can
be compensated by reducing the pressure or
increasing the power coupled into the plasma. - Although the energy flux can be repaired, the
IEDFs have a different shape. - Increasing the power will mainly increase ion
current. - Decreasing the plasma pressure will both increase
ion energies and ion current.