Effect of Lanthanum Doping on the Optical Properties of Hematite (α-Fe2O3) Thin Film

DOI : 10.17577/IJERTCONV1IS05007

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Effect of Lanthanum Doping on the Optical Properties of Hematite (-Fe2O3) Thin Film

Pawan Kumar and Rajesh Kumar*

Jaypee University of Information Technology, Waknaghat, Solan-173234, H.P., India E-mail: rajeshkumarf11@gmail.com, rajesh.kumar@juit.ac.in


Hematite (-Fe2O3) thin films are formed on the surface of the precursor solution. The effect of lanthanum (La) doping on the optical property and an effect of deposition conditions of the film morphology has been studied. The -Fe2O3 films formed on the surface of solution were transferred to the glass substrate. XRD, SEM and UV-Vis spectroscopy techniques have been used for the structural, morphological and optical characterizations of the films. The as deposited films were observed crystalline as analyzed by XRD. Depending upon the deposition conditions the films have thickness 400 nm, and are optically transparent and smooth surface morphology. Also, a variation in the optical band gap with the La concentration in the film has been observed.

Keywords: Hematite thin films, Band gap, lanthanum

  1. Introduction

    Hematite (-Fe2O3) is a thermodynamically stable iron oxide with corundum hexagonal closed packed crystal structure. It is a semiconducting material with an optical band gap around 2.0 eV [1]. The nanocrystalline -Fe2O3 has attracted a great deal of attention over the past decade due to a wide range of applications in chemical industry as active catalytic, non linear optical material, as photo electrode and gas sensors to detect combustible gases like CH4 and C3H8 [2]. Although, the physical preparation method such as chemical vapor deposition (CVD) and laser assisted CVD result into excellent thin films quality, they have some shortcoming from the point of view of wide usage for e.g. lack of flexibility and cost effectiveness [3].

    Now a days, great attention has to be drawn to miniaturization of electronic devices. For this reason, surface and interfacial phenomena play an important role in the device performance. One of the main characteristics of the electronic state of the surface is the energy band gap. Thin film of – Fe2O3 (with no added metal dopants) has been extensively studied with reported photo conversion efficiency of up to 2% for water splitting. So,

    adding element such as B, Al, In and Ga, Mo, Cr, Si improve the range of solar radiation absorption and conductivity of -Fe2O3 film [3-7]. In the present paper, the -Fe2O3 film is doped with La and variation in the optical properties has been studied.

  2. Experimental

    Iron salts FeCl2 and FeCl3 each in with 24 mM were added in a flask containing 32 M solution of PVA. The solution was heated at 70oC for 30 minutes on magnetic stirrer and then transferred in a petri dish placed inside an argon (Ar) gas chamber with a volume of 2 litres. A measured volume (120 cm3) of the NH3 vapor was poured deliberately inside the chamber containing solution filled petri dish. In this process, the NH3 vapors react with the surface of the solution and a floating film was formed on the solution surface within 15 minutes after the NH3 was poured. After the formation of film, it was transferred to the glass substrate and annealed at argon gas environment at 500oC temperature. The film was doped with 5% concentration of Lanthanum by adding Lanthanum

    (III) chloride heptahydrate in initial precursor solution. Thus formed film (-Fe2O3) was characterized by Field Emission Electron Microscopy (FESEM), X-ray Diffractometer (XRD) and UV-Vis-NIR spectrophotometer.

  3. Result and Discussion

Figure 1 shows the XRD patterns of – Fe2O3 and La-doped -Fe2O3 thin films annealed at 500oC temperature. All the peaks in the figure 1 matched the standard data for -Fe2O3 (JCPDS 33- 664). The XRD pattern shows no phase change with the lanthanum doping although the peak become sharper with La doping. The increase in the peak intensity with lanthanum doping shows increase in crystallinity and grain size within the thin film due to La doping.

Intensity (a. u.)



La- doped


25 30 35 40

Bragg Angle (2)

Figure 1 XRD patterns of the -Fe2O3 and La doped -Fe2O3 thin film.

Figure 2(a) & (b) shows the SEM micrograph of the -Fe2O3 and La-doped -Fe2O3 thin film deposited on the glass substrate and annealed at 500 oC temperature respectively. Figure 2(a) is the SEM image of the -Fe2O3 thin film which shows very small grain of the particles with smooth surface. Figure 2b is the La doped -Fe2O3 film shows increase in the grain size and clustering of the particles with La doping in -Fe2O3 thin film

The thickness of the all film is measured with the profillometer and found to be 400 nm. The optical property of the -Fe2O3 film deposited on the glass substrate and annealed at 500oC temperature has been studied by the UV-Vis-NIR spectrophotometer. With the doping of La in – Fe2O3 thin film a red shift is observed.

Figure 2 (a) SEM images of the undoped – Fe2O3 thin film and (b) the -Fe2O3 film doped with 5% La.

Figure 3(a) shows the transmission spectra of – Fe2O3 and La doped -Fe2O3 thin film and all the samples have high transmission in the visible and IR region. The results shows a decrease in transmission with La doping this is due to large absorption resulting from the large grain size in La doped thin film.

The optical absorption coefficient can be calculated as

= (1/t) ln (1/T) (1)

Where T is the transmission & t is the thickness of the film. Further, the optical band gap (Eg) was determined using the following Tauc,s relation[8]:

h = C1 (h-Eg)n (2)

Where h is Plancks constant, C1 is a constant and prefix n has values 0.5 and 2, respectively for a direct and indirect band gap transitions.

Figure 3(a) Transmission spectra, (b) band gap (Eg) of the -Fe2O3 and La-doped – Fe2O3 thin films.

The direct band gap values (Fig 3b.) of the undoped and La doped -Fe2O3 films are 2.47 and 2.30 eV, respectively. This indicates that the optical band gap decreases with the La doping in -Fe2O3 thin film. The decrease in the band gap with La doping can be explained on the basis of increase in particle size of the thin film with La doping as seen in the

potential candidate for many nanotechnology based application.

  1. Acknowledgements

    This work was supported by the Nanotechnology research grant of Jaypee University of Information Technology (JUIT).

  2. References

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    S.C. Katyal, H. Jang, H.N. Lee, R. Kumar. A novel method for controlled synthesis of nanosized hematite (- Fe2O3) thin film on liquidvapor interface. J. Nanopart. Res. 15, 2013, 1532.

  3. C. Aydin, S.A. Mansour, Z.A. Alahmed, F. Yakuphanoglu. Structural and optical characterization of sol-gel derived boron doped Fe2O3 nanostructured films. J Sol-Gel Sci. Technol. 62, 2012, 397.

  4. G. Wang, Y. Ling, D.A. Wheeler, K.E.N. George, K. Horsley, C. Heske, J.Z. Zhang, Y. Li, Facile synthesis of highly photoactive -Fe2O3 based films for water oxidation.Nano Lett. 11, 2011, 3503.

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    SEM images. Further, as observed from the XRD 2 3

    and SEM results, the size of particles and crystalline inside the film is changed with La doping.

    4. Conclusion

    Doped and undoped -Fe2O3 thin film are prepared by using simple chemical method. The band gap variation is found with the La doping in -Fe2O3 thin film. The band gap measured from optical properties shows variation in values which are found to be related to size of the nanoparticles inside the film. In this study the size of -Fe2O3 grain also increase with the La doping. The band gap tunability and strong optical absorption with high chemical stability make this material a

    water splitting by sunlight: Nanostructure-directing effect of Si doping. J Am. Chem. Soc. 128, 2006, 4582.

  7. P. Lio, M.C. Toroker, E.A. Carter. Electron transport in pure and doped hematite. Nano Lett. 11, 2011, 1775.

  8. G.P. Joshi, N.S. Saxena, R. Mangal, A. Mishra, T.P. Sharma. Band gap determination of NiZn ferrites.Bull. Mater. Sci. 26, 2003, 387.

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