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Identification of Defects and Secondary Phases in Reactively Sputtered Cu2ZnSnS4 Thin Films
Vardaan Chawla, Stacey Bent, Bruce Clemens
April 7th, 2010
Center on Nanostructuring for Efficient Energy Conversion
Materials Science and Engineering
Stanford University
2
Outline
• Motivation• Problems with characterization of thin films
• Experimental approach
• Results• X-ray diffraction• Raman Spectroscopy• Transmission Electron Microscopy• Scanning Auger Microscopy
• Summary & Acknowledgements
3
Motivation – Phase Equilibrium
• CZTS is a line compound between Cu2SnS3 and ZnS
• Theoretically even a 2-3% compositional variation could lead to phase separation
Ternary Phase Diagram Binary Phase Diagram
Cu2S ZnS
SnS2
Cu2SnS3
Olekseyuk, I.D. "Phase Equilibria in the Cu2S-ZnS-SnS2 System." Journal of Alloys and Compounds. 368. (2004): 135-143. Print.
CZ
TS
4
Motivation – Crystal Structure
• Crystal structures of secondary phases similar to CZTS• All primary peaks overlap and hard to separate• Low intensity peaks cannot be seen easily in thin films
Theoretical XRD Patterns of CZTS, Cu2SnS3, and ZnS
5
Experimental Approach
Substrate
CuZn
Sn
H2S H2S
H2SH2S
H2S
H2S
4H2S + 2Cu + Zn + Sn Cu2ZnSnS4 + 4H2
CZTS
• Introduce H2S into chamber during sputter deposition
• Sulfur is incorporated into the film in one step (no anneal)• Expect to see higher densities and improved film quality
Reactive Sputtering
6
Characterization - XRD
Cu2S ZnS
SnS2
Cu2SnS3
Varying Zn/(Cu+Sn) Ratio
• Zn/(Cu+Sn) ratio is varied while holding Cu/Sn ratio constant• Impossible to determine difference between CZTS, CTS, and
ZnS from XRD pattern
(101
)
(200
)
(220
)
(312
)
(112
)
Olekseyuk, I.D. "Phase Equilibria in the Cu2S-ZnS-SnS2 System." Journal of Alloys and Compounds. 368. (2004): 135-143. Print.
7
Characterization - XRD
Cu2S ZnS
SnS2
Cu2SnS3
Varying Cu/(Zn+Sn) Ratio
• Cu/(Zn+Sn) ratio is varied while holding Zn/Sn ratio constant
• Need to get very far off 2:1:1 stoichiometry before any CuxS phases can be seen
• CuxS can be removed with KCN etch
CuS Cu2S
(101
)
(200
)
(220
)
(312
)
(112
)Olekseyuk, I.D. "Phase Equilibria in the Cu2S-ZnS-SnS2 System." Journal of Alloys and Compounds. 368. (2004): 135-143. Print.
8
Characterization – Raman
Varying Zn/(Cu+Sn) Ratio
• Raman spectra show only minor changes even though composition is varied dramatically
• No evidence of the CuxS phase shown by other groups at growth temperatures higher than 500C
Varying Cu/(Zn+Sn) Ratio
9
500nm
Device Fabrication
Glass Substrate3000 µm
Molybdenum Layer1 µm
1.75 µm
CdS (n-type)55 nm
ZnO:Al (n-type)340 nm
Aluminum Grid
CZTS Absorber (p-type)
CZTS Device Stack
• Zn-rich films incorporated into standard CIGS device stack for testing
ZnO85 nm ZnO
ZnO:Al
CdS
CZTS
Mo
SEM Image
10
Device Characterization
I-V Measurement EQE Measurement
• First CZTS devices grown by a reactive sputtering process• Efficiency = 1.35%• Degraded EQE clearly points to undetected defects in
the absorber
11
Characterization - TEM
500nm
200nm
CZTS
Secondphase
5nm
CZTS
Secondphase
• Detrimental secondary phase interspersed in CZTS matrix
• Stacking faults in the secondary phase point to a transition between cubic and hexagonal crystal structures
12
Characterization - Auger
• Raster beam over sputtered surface of sample and scan for Cu, Zn, Sn
• Overlay Cu, Zn, Sn signal• Composition variation points to
CZTS / ZnS (Zn-rich)
2 um
Cu
Zn
Sn
CZTS
ZnS
13
Characterization - CdZnS
• Cd penetration into ZnS lowers the cubic-hexagonal transition temperature
• Stacking faults in TEM images are created during CBD of CdS layer
CdS – ZnS Phase Diagram
(101
)
H-Z
nS
(220
)
(312
)
(112
)
XRD before and after CBD
C
C + H
H
Chen et al.“Solid State Phase Equilibria in the ZnS-CdS System." Materials Research Bulletin. 23. (1988): 1667-1673. Print.
14
Characterization - Auger
Sn
Cd • Overlay Sn and Cd signal• Cd ion exchanges with Zn during
bath deposition and penetrates the ZnS phase
CZTS
CdZnS
2 um
15
Summary
• CZTS thin films were grown using Reactive Sputtering
• Films were characterized using X-ray Diffraction and Raman Spectroscopy
• Full devices have been grown and tested but are limited due to secondary phases in the films
• Transmission Electron Microscopy and Scanning Auger Microscopy can be used to identify these secondary phases
16
Acknowledgements
• US Department of Energy, Office of Basic Energy Sciences as part of an Energy Frontier Research Center• http://www.er.doe.gov/bes/EFRC/index.html
• Applied Quantum Technologies• Local thin film solar startup• http://www.aqtsolar.com
17
Questions
Questions?