Abstract:Copper sulfide thin films have been fabricated by various deposition techniques, such as chemical vapor deposition, [15] sputtering, spray pyrolysis, [16,17] chemical bath deposition, [18,19] and electrochemical methods. [20][21][22] However, in most cases the required control over the film stoichiometry and phase composition is poorly achieved due to the coexistence of several stable and metastable copper sulfide phases. [23] Moreover, fabrication of continuous copper sulfide coatings with a well-controlled m… Show more
“…CuS thin films are generally grown by methods like spray pyrolysis [8], the hydrothermal method [9], chemical-vapor deposition [10], atomic-layer deposition [11], and sputtering [12]. Among these, radio-frequency (RF) magnetron sputtering, which is one of the physical vapor-deposition methods, employs simple equipment and can form a strong adhesive force between the as-sputtered thin films and the substrate.…”
Copper sulfide (CuS) thin films were deposited on a glass substrate at room temperature using the radio-frequency (RF) magnetron-sputtering method at RF powers in the range of 40–100 W, and the structural and optical properties of the CuS thin film were investigated. The CuS thin films fabricated at varying deposition powers all exhibited hexagonal crystalline structures and preferred growth orientation of the (110) plane. Raman spectra revealed a primary sharp and intense peak at the 474 cm−1 frequency, and a relatively wide peak was found at 265 cm−1 frequency. In the CuS thin film deposited at an RF power of 40 W, relatively small dense particles with small void spacing formed a smooth thin-film surface. As the power increased, it was observed that grain size and grain-boundary spacing increased in order. The binding energy peaks of Cu 2p3/2 and Cu 2p1/2 were observed at 932.1 and 952.0 eV, respectively. Regardless of deposition power, the difference in the Cu2+ state binding energies for all the CuS thin films was equivalent at 19.9 eV. We observed the binding energy peaks of S 2p3/2 and S 2p1/2 corresponding to the S2− state at 162.2 and 163.2 eV, respectively. The transmittance and band-gap energy in the visible spectral range showed decreasing trends as deposition power increased. For the CuS/tin sulfide (SnS) absorber-layer-based solar cell (glass/Mo/absorber(CuS/SnS)/cadmium sulfide (CdS)/intrinsic zinc oxide (i-ZnO)/indium tin oxide (ITO)/aluminum (Al)) with a stacked structure of SnS thin films on top of the CuS layer deposited at 100 W RF power, an open-circuit voltage (Voc) of 115 mA, short circuit current density (Jsc) of 9.81 mA/cm2, fill factor (FF) of 35%, and highest power conversion efficiency (PCE) of 0.39% were recorded.
“…CuS thin films are generally grown by methods like spray pyrolysis [8], the hydrothermal method [9], chemical-vapor deposition [10], atomic-layer deposition [11], and sputtering [12]. Among these, radio-frequency (RF) magnetron sputtering, which is one of the physical vapor-deposition methods, employs simple equipment and can form a strong adhesive force between the as-sputtered thin films and the substrate.…”
Copper sulfide (CuS) thin films were deposited on a glass substrate at room temperature using the radio-frequency (RF) magnetron-sputtering method at RF powers in the range of 40–100 W, and the structural and optical properties of the CuS thin film were investigated. The CuS thin films fabricated at varying deposition powers all exhibited hexagonal crystalline structures and preferred growth orientation of the (110) plane. Raman spectra revealed a primary sharp and intense peak at the 474 cm−1 frequency, and a relatively wide peak was found at 265 cm−1 frequency. In the CuS thin film deposited at an RF power of 40 W, relatively small dense particles with small void spacing formed a smooth thin-film surface. As the power increased, it was observed that grain size and grain-boundary spacing increased in order. The binding energy peaks of Cu 2p3/2 and Cu 2p1/2 were observed at 932.1 and 952.0 eV, respectively. Regardless of deposition power, the difference in the Cu2+ state binding energies for all the CuS thin films was equivalent at 19.9 eV. We observed the binding energy peaks of S 2p3/2 and S 2p1/2 corresponding to the S2− state at 162.2 and 163.2 eV, respectively. The transmittance and band-gap energy in the visible spectral range showed decreasing trends as deposition power increased. For the CuS/tin sulfide (SnS) absorber-layer-based solar cell (glass/Mo/absorber(CuS/SnS)/cadmium sulfide (CdS)/intrinsic zinc oxide (i-ZnO)/indium tin oxide (ITO)/aluminum (Al)) with a stacked structure of SnS thin films on top of the CuS layer deposited at 100 W RF power, an open-circuit voltage (Voc) of 115 mA, short circuit current density (Jsc) of 9.81 mA/cm2, fill factor (FF) of 35%, and highest power conversion efficiency (PCE) of 0.39% were recorded.
“…Prototypical ALD processes include those for binary metal oxides (e.g., Al 2 O 3 , HfO 2 , TiO 2 , ZnO) , and sulfides (e.g., ZnS), but ternary and even quaternary processes are possible as well, though more challenging to optimize. − Organometallic compounds such as trimethylaluminum (TMA) and diethylzinc (DEZ) or metal halides such as TiCl 4 or HfCl 4 are usually used as the metal precursors, as they have much lower sublimation/evaporation temperatures than, for example, elemental metals, thus allowing for the reactor to be operated at a reasonably low temperature. The second precursor is then typically the source of oxygen (e.g., H 2 O, O 3 ), sulfur (e.g., H 2 S, S), , or nitrogen (e.g., NH 3 ) …”
Section: Ald and
Mld Techniques In Briefmentioning
Atomic layer deposition
(ALD) is the fastest growing thin-film
technology in microelectronics, but it is also recognized as a promising
fabrication strategy for various alkali-metal-based thin films in
emerging energy technologies, the spearhead application being the
Li-ion battery. Since the pioneering work in 2009 for Li-containing
thin films, the field has been rapidly growing and also widened from
lithium to other alkali metals. Moreover, alkali-metal-based metal–organic
thin films have been successfully grown by combining molecular layer
deposition (MLD) cycles of the organic molecules with the ALD cycles
of the alkali metal precursor. The current literature describes already
around 100 ALD and ALD/MLD processes for alkali-metal-bearing materials.
Interestingly, some of these materials cannot even be made by any
other synthesis route. In this review, our intention is to present
the current state of research in the field by (i) summarizing the
ALD and ALD/MLD processes so far developed for the different alkali
metals, (ii) highlighting the most intriguing thin-film materials
obtained thereof, and (iii) addressing both the advantages and limitations
of ALD and MLD in the application space of these materials. Finally,
(iv) a brief outlook for the future perspectives and challenges of
the field is given.
“…These sample are p-type films, band gap values in the ranges of 2.4 to 2.54 eV. Higher growth arte and flake like morphology could be observed when the temperature was increased above 160°C [52]. H 2 S was used to provide sulphur ion [53] during the deposition process at 130 to 200°C.…”
Nano material is an important field in world of science and technology. In this work, activated carbon and metal chalcogenide thin films were discussed. Activated carbon has high surface area and porosity structure. Basically, it could be synthesized by using various raw materials under carbonization and chemical activation process. Utilization of activator such as KOH, NaOH, zinc chloride, phosphoric acid, sulphuric acid could improve texture properties and adsorption capacity. On the other hand, metal chalcogenide thin films have been prepared by using various deposition techniques including physical and chemical method. These materials have great potential in solar cell, sensor device, laser device and optoelectronic applications. Characterization of metal sulfide, metal selenide and metal telluride thin films was studied by using different tools.
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