A Robust and Low-Cost Strategy to Prepare Cu2ZnSnS4 Precursor

0 downloads 0 Views 609KB Size Report
Electronic supplementary information. A Robust and Low-Cost Strategy to Prepare Cu2ZnSnS4. Precursor Solution and Its Application in Cu2ZnSn(S,Se)4 Solar.
Electronic Supplementary Material (ESI) for RSC Advances. This journal is © The Royal Society of Chemistry 2014

Electronic supplementary information

A Robust and Low-Cost Strategy to Prepare Cu2ZnSnS4 Precursor Solution and Its Application in Cu2ZnSn(S,Se)4 Solar Cells Qingwen Tian,a Yong Cui,b Gang Wang,a* and Daocheng Pana* a: State Key Laboratory of Rare Earth Resource Utilization, Changchun Institute of Applied Chemistry, Chinese Academy of Sciences, 5625 Renmin Street, Changchun, Jilin, 130022, China

b: Shenyang R&D Center Laboratory for Material Science, Institute of Metal Research, Chinese Academy of Sciences. Wenhua Road 72, Shenyang, 110016, China

E-mail: [email protected] and [email protected].

2 cm

Figure S1. A digital photograph of graphite box.

1   

2.0 cm

Figure S2. A digital photograph of CZTSSe solar cells.

a Cu 2p1/2

1020

940 950 960 Binding Energy(eV) Sn 3d5/2

Intensity (a.u.)

Sn 3d3/2

485

490 495 Binding Energy(eV)

Zn 2p1/2

c

1030 1040 1050 Binding Energy(eV) S2p

500

160 165 Binding Energy(eV)

Figure S3. XPS spectra of the as-fabricated CZTS thin film. 2   

d

Intensity (a.u.)

930

b

Zn 2p3/2 Intensity (a.u.)

In te n s ity (a .u .)

Cu 2p3/2

170

a Cu 2p1/2

940 950 Binding Energy(eV)

Intensity (a.u.)

Sn 3d5/2

485

960

Sn 3d3/2

490 495 Binding Energy(eV)

1030 1040 1050 Binding Energy(eV)

c

d

500

S 2p Se 3p

160 165 Binding Energy(eV)

e

Intensity (a.u.)

Se3d

Zn 2p1/2

1020

Intensity (a.u.)

930

50

55 60 Binding Energy(eV)

65

Figure S4. XPS spectra of the selenized CZTSSe thin film. .

3   

b

Zn 2p3/2 Intensity (a.u.)

Intensity (a.u.)

Cu 2p3/2

170

K/S (a.u.) 400

Eg=1.03 eV

600

800

1000

1200

1400

Wavelength (nm) Figure S5. The band gap of selenized CZTSSe thin film was calculated by extrapolating the Kubelka-Munk function to K/S=0.

4