Synthesis, characterization and photovoltaic properties of phase pure Cu2SnSe3 nanostructures using molecular precursors

被引:11
|
作者
Tyagi, Adish [1 ,2 ]
Shah, Alpa Y. [1 ]
Kedarnath, G. [1 ,2 ]
Wadawale, Amey [1 ]
Singh, Vishal [3 ]
Tyagi, Deepak [1 ]
Betty, C. A. [1 ]
Lal, Champa [4 ]
Jain, Vimal K. [1 ,5 ]
机构
[1] Bhabha Atom Res Ctr, Chem Div, Mumbai 400085, Maharashtra, India
[2] HomiBhabha Natl Inst, Mumbai 400094, Maharashtra, India
[3] Bhabha Atom Res Ctr, Mat Sci Div, Mumbai 400085, Maharashtra, India
[4] Bhabha Atom Res Ctr, Tech Phys Div, Mumbai 400085, Maharashtra, India
[5] Univ Mumbai, UM DAE Ctr Excellence Basic Sci, Kalina Campus, Mumbai 400098, Maharashtra, India
关键词
COLLOIDAL SYNTHESIS; CHALCOGENIDE NANOCRYSTALS; SELENOLATES SYNTHESIS; UTILITY; CONVERSION; COMPLEXES; PYRIDYL; GROWTH; FILMS;
D O I
10.1007/s10854-018-8912-8
中图分类号
TM [电工技术]; TN [电子技术、通信技术];
学科分类号
0808 ; 0809 ;
摘要
Phase pure Cu2SnSe3 (CTSe) nanostructures have been synthesized using metal selenolates, [Me2Sn{SeC5H3(Me-3)N}(2)] (molecular structure of [Me2Sn{SeC5H3(Me-3)N}(2)] has been established by single crystal X-ray analysis) and [Cu{SeC5H3(Me-3)N}](4) as molecular precursors in oleylamine (OLA) and tri-n-octylphosphine oxide (TOPO). The effect of temperature on final composition of nanostructures has also been investigated. Powder X-ray diffraction, Raman and X-ray photoelectron spectroscopy (XPS) were used to investigate the crystal structure, phase purity and homogeneity of the nanostructures while the electron microscopy revealed the morphology of the nanostructures. Superconducting quantum interference device (SQUID) measurements of CTSe nanostructures showed weak magnetic ordering at low temperature (below 50 K) attributed to the presence of some defect centres in the sample. The CTSe nanostructure possess an optical band gap of 1.7 eV deduced from diffuse reflectance spectroscopy (DRS) and showed photo response which makes them promising candidate for alternative low cost photon absorber material.
引用
收藏
页码:8937 / 8946
页数:10
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