Photo-electrochemical properties of Cd1−xHgxSe thin films
Introduction
The use of photo-electrochemical cells (PEC) utilizing thin film semiconductor material, as a direct route to harness solar energy has become a subject of intensive research due to its overriding advantages over the other conventional devices. The photo-electrochemical cells are much cheaper, simple to construct and need no complicated processing steps. Unlike semiconductor–semiconductor junction in solar cells, the semiconductor–electrolyte junction in PEC is readily established so that the study of junction energetics becomes easy [1], [2], [3]. A PEC utilizing a polycrystalline aggregate can achieve 70% efficiency of the same material in a single crystal form [4]. The efficiency and stability of PEC depends strongly on the preparation conditions of the photoelectrodes, electrolytes and the experimental conditions set during the experimentation [5]. The alloyed/mixed ternary semiconductor materials are known to function effectively in conversion of solar energy into electrical energy [6], [7]. This is because the properties of the ternary material can be easily tailored to the desired level by variation of the compositional parameter ‘x’ (i.e. the relative compositions of the two binary systems selected).
The chalcogenides, especially of cadmium group, find applications in the photovoltaic devices [8], [9], [10]. These compounds have been shown to form a solid solution over an appreciable range. However, the scope and study was limited to bulk form only and studies in thin film form are quite limited. A few of the ternary selenide series consisting of Cd1−xZnxSe [11], CdS1−xSex [12], Cd1−xMnxSe [13], etc. have been prepared and studied. In this context, Cd1−xHgxSe seems to be promising due to following reasons (i) CdSe is a semiconductor material with a band gap of 1.7 eV while, HgSe is low band gap (∼0.6 eV in thin film form) material, so the ternary system with a proper composition can be engineered to cope with the maximum of visible spectrum (∼1.4 eV), (ii) the addition of Hg in CdSe reduces the resistance of the film, (iii) the ternary material has better absorptivity and higher spectral sensitivity over a considerable range of photon energies and (iv) CdSe and HgSe exist in cubic as well as hexagonal forms. Their lattice constants (in cubic phase) do not differ greatly, so a solid solution is possible in almost the whole range of compositions. It was, therefore, proposed to prepare Cd1−xHgxSe thin film photoelectrodes and study their photo-electrochemical properties with special reference to the PEC parameters namely open-circuit voltage (Voc), short-circuit current (Isc), efficiency (η), fill factor (ff), Barrier height (Φb), flat band potential (Vfb), etc.
Section snippets
Preparation of photoelectrode
The photoelectrodes of the type Cd1−xHgxSe with (0 ≤ x ≤ 1) were prepared onto a smooth, polished, stainless steel substrates. A well-known chemical bath deposition method utilizing AR grade cadmium acetate, mercuric nitrate and sodium selenosulphate was used. The values of composition parameter (x) were adjusted by maintaining the volume concentrations of Cd2+, Hg2+ and Se2− ions in solution state. The detail of the deposition process is described elsewhere [14].
Fabrication and characterization of a PEC cell
A photo-electrochemical cell was
Results and discussion
When a semiconductor material is immersed into the solution of a redox electrolyte, the movement of charge occurs at semiconductor–electrolyte (S/E) interface in order to equilibrate the two phases, generating an electric field at the interface. The excess charge that is located on semiconductor usually extends into the bulk of electrode for a significant distance; this region is referred to as ‘space charge region’ or ‘depletion region’. When this interface is illuminated with a light having
Conclusions
The PEC cells with the photoanode of the type Cd1−xHgxSe have been constructed and investigated for various cell properties as a function of photoelectrode composition parameter x. The results indicated that for Cd0.6Hg0.4Se the efficiency and the fill factor were increased to 1.03 and 41.0, respectively. The observed enhancement is due to increased open-circuit voltage, improved grain quality and improved photoelectrode absorption. The increase in photocurrent is attributed to reduction in
Acknowledgements
The author (V.M. Bhuse) thankfully acknowledges UGC for providing financial assistance through a Minor research scheme [F. No. 47-97/2002/WRO, dated 22/03/2002].
References (27)
- et al.
Mater. Chem. Phys.
(1998) - et al.
Sol. Energy Mater.
(1990) - et al.
Mater. Chem. Phys.
(2000) - et al.
Sol. Energy Mater. Sol. Cells
(1994) - et al.
Mater. Chem. Phys.
(2004) - et al.
Mater. Chem. Phys.
(2001) - et al.
J. Electrochem. Soc.
(1977) - et al.
Chemical and Electrochemical Energy Systems
(1997) - et al.
J. Indian Chem. Soc.
(1993) - et al.
Int. J. Electron.
(1999)
Int. J. Ionics
Ind. J. Pure Appl. Phys.
Ind. J. Pure Appl. Phys.
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