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Dive into the research topics where Chitra Agashe is active.

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Featured researches published by Chitra Agashe.


Thin Solid Films | 2003

Modified Thornton model for magnetron sputtered zinc oxide: film structure and etching behaviour

Oliver Kluth; Gunnar Schöpe; J. Hüpkes; Chitra Agashe; J. Müller; Bernd Rech

ZnO:Al films were prepared on glass substrates with different sputter techniques from ceramic ZnO:Al2O3 target as well as metallic Zn:Al targets using a wide range of deposition parameters. Independent of the sputter technique, sputter pressure and substrate temperature were found to have a major influence on the electrical and structural properties of the ZnO:Al films. With an increasing deposition pressure, we observed a strong decrease in the carrier mobility and also an increase of the etching rate. The surface morphology obtained after etching of RF sputtered ZnO:Al systematically changes from crater-like to hill-like surface appearance with increasing pressure. The correlation of sputter parameters, film growth and structural properties is discussed in terms of a modified Thornton model.


Journal of Applied Physics | 2004

Efforts to improve carrier mobility in radio frequency sputtered aluminum doped zinc oxide films

Chitra Agashe; Oliver Kluth; J. Hüpkes; U. Zastrow; Bernd Rech; Matthias Wuttig

This study addresses the electrical and optical properties of radio frequency magnetron sputtered aluminum doped zinc oxide (ZnO:Al) films. The main focus was on the improvement in carrier mobility μ to achieve simultaneously high transparency for visible and particularly near-infrared light and low resistivity. The influence of Al concentration in the target, film thickness, sputter power, deposition pressure, and substrate temperature on material properties was investigated. The structural, compositional, electrical and optical properties were studied using x-ray diffraction, secondary ion mass spectrometry (SIMS), room temperature Hall effect measurements and spectral photometry, respectively. All ZnO:Al films were polycrystalline and preferentially oriented along [002]. The grain size along the direction of growth increased with higher Al doping and with increasing film thickness. The SIMS measurements revealed that the Al concentration in the film was nearly the same as in the target. Carrier concent...


Thin Solid Films | 2003

Optimization of the electrical properties of magnetron sputtered aluminum-doped zinc oxide films for opto-electronic applications

Chitra Agashe; Oliver Kluth; Gunnar Schöpe; H. Siekmann; J. Hüpkes; Bernd Rech

Abstract Magnetron sputtered ZnO:Al films are promising candidates as front electrode in a variety of opto-electronic devices. Here we report on efforts to obtain highly conductive and transparent ZnO:Al films using different deposition conditions for RF, DC and MF (mid frequency) sputtering. Investigations were made to see the effect of target doping concentration (TDC), film thickness, sputter pressure and deposition temperature. RF sputtering from ceramic targets yields low resistivities between 3 and 5×10−4 Ω cm for target doping concentrations between 4 and 0.5%. With decreasing TDC to 0.5% carrier mobilities up to 44 cm2/Vs were obtained, accompanied by the extension of the region of high transmission to the near infrared, due to a reduction in free carrier absorption and corresponding shift in plasma wavelength. DC and MF sputtering from metallic targets yielded similar low resistivities at deposition rates up to 200 nm/min. An analysis of mobility (μ) data of all films as function of the corresponding carrier densities (N) showed that the μ–N values obtained in this study are in the vicinity to limits suggested in the literature.


Journal of Materials Research | 1993

Dopant induced modifications in the physical properties of sprayed ZnO : In films

D. J. Goyal; Chitra Agashe; M. G. Takwale; V.G. Bhide; Shailaja Mahamuni; S. K. Kulkarni

Indium-doped zinc oxide (IZO) films were prepared by the spray pyrolysis technique. The effect of gradual incorporation of indium cations on the structural, electrical, and compositional properties of IZO films was studied in detail. It was observed that even a small addition of indium modifies the preferred growth of IZO film from the [002] direction to the [101] direction. Such a modification in growth pattern is a result of more nucleating centers created by indium doping. Indium dopant improves the electrical properties of the films. The carrier concentration depends mainly on the indium dopant level while the mobility is affected by the changes in crystal orientation that take place due to addition of dopants. X-ray photoelectron spectroscopy results show that indium doping does not lead to any stoichiometric changes in the IZO films and the dopant incorporation in the film is linearly proportional to that in the solution.


Journal of Applied Physics | 1991

Effect of Sn incorporation on the growth mechanism of sprayed SnO2 films

Chitra Agashe; M. G. Takwale; V.G. Bhide; Shailaja Mahamuni; Sulabha K. Kulkarni

In order to probe into the growth mechanism of sprayed SnO2 films, the films were deposited with different Sn concentrations in the precursor solution. The orientational properties were determined using grazing incidence x‐ray diffraction. The preferred growth changed from [110] to [200] direction as the Sn incorporation was increased. Such a change in growth can be anticipated from structure factor calculations. The compositional analysis was done using x‐ray photoelectron spectroscopy. The Hall effect measurements indicated that the carrier concentration and mobility are sensitively dependent on the orientation and composition of the films.


Journal of Applied Physics | 1993

Effect of dopant incorporation on structural and electrical properties of sprayed SnO2:Sb films

D. J. Goyal; Chitra Agashe; B.R. Marathe; M. G. Takwale; V.G. Bhide

Antimony‐doped tin oxide films were deposited by spray pyrolysis technique. The effect of antimony doping on structural and electrical properties was investigated in detail using the x‐ray diffraction technique and room‐temperature Hall measurements. Antimony doping did not affect the preferred growth along [200] to a considerable extent. These results were analyzed on the basis of structure factor calculations. From the Hall measurements, the lowest electrical resistivity, i.e., 5.2×10−4 Ω cm was observed for the films with a doping level of 2.3 at. % in the solution. This value of electrical resistivity is the lowest reported so far in the case of spray deposited antimony‐doped SnO2 films. The grain boundary and ionized impurity scattering were observed to be prevalent in governing the electronic transport of lightly and heavily doped films, respectively.


Thin Solid Films | 1988

Structural properties of SnO2: F films deposited by spray pyrolysis technique

Chitra Agashe; B.R. Marathe; M. G. Takwale; V.G. Bhide

Abstract Thin films of SnO 2 and SnO 2 : F were deposited by a spray pyrolysis technique. The effect of substrate temperature on the structural and electrical transport properties of these films was investigated. The standard deviation of these films from ASTM data explains the growth mechanism with other process parameters at optimum values.


Journal of Applied Physics | 2008

Al-doped ZnO nanocrystals

Pratibha Kadam; Chitra Agashe; Shailaja Mahamuni

Al3+-doped ZnO nanocrystals were differently obtained by wet chemical and an electrochemical route. An increase in forbidden gap due to change in crystal size and also due to Al3+ doping in ZnO is critically analyzed. The Moss–Burstein type shift in Al3+-doped ZnO nanocrystals provides an evidence of successful Al3+ doping in ZnO nanocrystals. The possibility of varying the carrier concentration in ZnO nanocrystals is the indirect implication of the present investigations.


Semiconductor Science and Technology | 1995

Doping-induced changes in the physical properties of In2O3:Sn films

Chitra Agashe; Shailaja Mahamuni

Here we report studies carried out on heavily tin-doped and undoped indium oxide films. Structural, electronic transport and compositional properties of the sprayed films deposited with different doping levels of tin (0-110 at.% in solution), were investigated. X-ray diffraction, room-temperature Hall effect measurements, conductivity measurements at low temperatures and x-ray photoelectron spectroscopy were used for these studies. The films were polycrystalline and the preferred growth showed systematic changes with dopant incorporation from (400) to (222). The carrier mobility was very sensitive to these changes in orientation of preferred growth as well as the grain size. The high carrier concentration ( approximately 1020 cm-3) implied that the films belong to the class of degenerate semiconductors. Such a high carrier concentration was a result of increased non-stoichiometry and increased dopant incorporation. The conductivity measurements at low temperatures show that with increased Sn incorporation, electronic transport is governed by ionized impurity scattering and acoustic lattice scattering.


Solar Energy Materials and Solar Cells | 1993

Cobalt oxide selective coatings for all glass evacuated collectors

Sushama Pethkar; M. G. Takwale; Chitra Agashe; V.G. Bhide

Abstract Black cobalt deposits were formed on glass substrates for use in all glass evacuated collectors. Glass was made conducting by depositing fluorine doped tin oxide films using spray pyrolysis. The reflectivity of this glass was further improved by electroplating a thin nickel layer (0.35 μm) on it. Cobalt oxide thin films were deposited on these nickel coated conducting glass substrates using spray pyrolysis. The effect of cobalt acetate concentration in the precursor solution on the performance of these multilayer coatings was studied. Solar absorptances as high as 0.93–0.94 and thermal emittances as low as 0.09 were obtained for films deposited with lower concentrations. For films deposited with higher concentrations the selectivity significantly reduces from ~ 33 to ~ 3.0. Structural analysis confirms the presence of Co 3 O 4 .

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Shailaja Mahamuni

Savitribai Phule Pune University

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J. Hüpkes

Forschungszentrum Jülich

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Oliver Kluth

Forschungszentrum Jülich

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Bernd Rech

Helmholtz-Zentrum Berlin

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Gunnar Schöpe

Forschungszentrum Jülich

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J. Müller

Forschungszentrum Jülich

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H. Siekmann

Forschungszentrum Jülich

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Pratibha Kadam

Savitribai Phule Pune University

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B. Rech

Forschungszentrum Jülich

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