Elsevier

Thin Solid Films

Volume 520, Issue 1, 31 October 2011, Pages 497-500
Thin Solid Films

F-doped SnO2 thin films grown on flexible substrates at low temperatures by pulsed laser deposition

https://doi.org/10.1016/j.tsf.2011.07.025Get rights and content

Abstract

Fluorine-doped tin oxide (SnO2:F) films were deposited on polyethersulfone plastic substrates by pulsed laser deposition. The electrical and optical properties of the SnO2:F films were investigated as a function of deposition conditions such as substrate temperature and oxygen partial pressure during deposition. High quality SnO2:F films were achieved under an optimum oxygen pressure range (7.4–8 Pa) at relatively low growth temperatures (25–150 °C). As-deposited films exhibited low electrical resistivities of 1–7 mΩ-cm, high optical transmittance of 80–90% in the visible range, and optical band-gap energies of 3.87–3.96 eV. Atomic force microscopy measurements revealed a reduced root mean square surface roughness of the SnO2:F films compared to that of the bare substrates indicating planarization of the underlying substrate.

Introduction

There is a growing need for transparent conducting oxides (TCOs) in the field of organic optoelectronics — specifically in applications such as substrates for flat panel organic light-emitting devices (OLEDs) and organic photovoltaic (OPV) devices. In general, glass substrates are widely used for most optoelectronic and electro-optic devices. However, glass substrates are unsuitable for many applications such as ultra-thin displays, electronic maps, smart cards and portable computers where flexibility, weight and/or safety issues are critical, and especially true for large area applications due to the inherent rigidity, brittleness and weight of the glass. These disadvantages can be overcome by using flexible substrates, which are robust, light-weight, and cost effective. For these reasons, optically transparent plastics, such as polyethersulfone (PES; Tg = 223 °C), polycarbonate (Tg = 150 °C), and polyethylene terephthalate (Tg = 70 °C), where Tg is the glass transition temperature, have been explored as substrate materials for the growth of transparent conducting oxide thin films in passive and active matrix display applications [1], [2], [3], [4], [5]. Among these substrates, PES is an excellent candidate because it exhibits ~ 90% of optical transmission in the visible and near-infrared spectrum with a high glass transition temperature (Tg = 223 °C), which allows for the growth of metal oxide films at relatively high temperatures (up to 150 °C) without compromising the mechanical and optical stability of the substrate.

Thin films of F-doped SnO2 (SnO2:F, or abbreviated as FTO) are commonly used as transparent conducting electrodes for many devices such as solar cells and flat panel displays because SnO2 films are inexpensive as well as chemically and thermally stable [6], [7], [8]. There are numerous deposition techniques used to grow FTO films on glass substrates including chemical vapor deposition [9], [10], spray pyrolysis [11], [12], thermal evaporation [13], sol–gel [14] and sputtering [15], [16]. However, there have been very few reports of deposition of FTO films on flexible polymer substrates. Previously, high quality FTO films have been grown on glass substrates using pulsed laser deposition (PLD) and the deposition conditions were optimized for highly conductive films [17]. In general, the films grown by PLD crystallize at relatively lower substrate temperatures compared to those grown by other physical vapor deposition techniques due to the high kinetic energies (> 1 eV) of the ejected species in the laser-produced plasma [18]. Thus, TCO films grown on plastic substrates by PLD can achieve relatively lower resistivity compared to those grown by other techniques at low temperatures. In this paper, we report our study on the electrical and optical properties of FTO films deposited on flexible PES substrates by PLD without a postdeposition anneal. Film properties were measured as a function of the substrate temperature and oxygen pressure during deposition.

Section snippets

Experimental details

FTO thin films were deposited on PES substrates (200 μm, Sumilite®, courtesy of Sumitomo Bakelite) using a KrF excimer laser (Lambda Physik LPX 305, 248 nm, 30 ns full width half maximum). Details of the film deposition conditions are presented elsewhere [17], [19]. Briefly, the laser beam, operating at 10 Hz, was focused by a 50-cm focal length lens through a quartz window into a vacuum chamber onto a rotating target at a 45° angle of incidence. The energy density of the laser beam at the target

Results and discussion

Fig. 1 shows a plot of the electrical resistivity as a function of oxygen deposition pressure (Po2) for FTO films grown on PES substrates at three different substrate temperatures, (Ts = 25, 100 and 150 °C). For the films grown at 25 °C, the resistivity is highly responsive to the oxygen deposition pressure. Low resistivity values can be obtained only in a small range of oxygen deposition pressures between 7.4 and 8 Pa. As the Ts increases, the resistivity of the FTO films becomes less dependent on

Conclusion

In summary, SnO2:F thin films have been deposited on PES plastic substrates by pulsed laser deposition. FTO films (300 nm thick) grown at Ts = 25 °C and 8 Pa of oxygen exhibited a resistivity of 6.9 × 10 3 Ω-cm and an average transmittance of 80% in the visible range with an optical band-gap of 3.88 eV. For a 320 nm thick FTO film deposited at Ts = 150 °C and 8 Pa of oxygen, an electrical resistivity of 1.3 × 10 3 Ω-cm, an average transmittance of 89% in the visible range, and an optical band-gap of 3.96 eV were

Acknowledgments

This work was supported by the Office of Naval Research (ONR).

References (23)

  • B. O'Regan et al.

    Nature

    (1991)
  • B. Thangaraju

    Thin Solid Films

    (2002)
  • D. Das et al.

    Thin Solid Films

    (1987)
  • O. Varghese et al.

    J. Appl. Phys.

    (2000)
  • R. Eason

    Pulsed Laser Deposition of Thin Films, 239–260

    (2006)
  • G.P. Kushto et al.

    Appl. Phys. Lett.

    (2005)
  • H.-K. Kim et al.

    Appl. Phys. Lett.

    (2007)
  • H. Kim et al.

    Appl. Phys. Lett.

    (2001)
  • G. Gu et al.

    Optics Lett.

    (1997)
  • G. Gustafsson et al.

    Nature

    (1992)

    Synth. Metals

    (1993)
  • T. Fukano et al.

    J. Appl. Phys.

    (2005)
  • Cited by (20)

    • Highly transparent conductive F-doped SnO<inf>2</inf> films prepared on polymer substrate by radio frequency reactive magnetron sputtering

      2022, Thin Solid Films
      Citation Excerpt :

      It has been widely used in solar cells [1], organic light emitting diodes [2], low emission glass [3] and other fields [4,5]. In general, FTO films can be prepared on the surface of rigid glass substrates by methods such as sol-gel [6], chemical vapor deposition (CVD) [7–9], spray pyrolysis [10–13], magnetron sputtering [14] and pulsed laser deposition (PLD) [15,16]. However, with the development of wearable devices and curved display screens, it is necessary to prepare FTO films on surface of flexible substrates.

    • Physical properties of rare earth metal (Gd<sup>3+</sup>) doped SnO<inf>2</inf> thin films prepared by simplified spray pyrolysis technique using nebulizer

      2019, Optik
      Citation Excerpt :

      As the ionic radius of Gd3+ (0.94 Å) is slightly larger than the ionic radius of Sn4+ (0.69 Ǻ), the Sn4+ ions could be easily substituted by Gd ions without provoking any significant variation in lattice parameters and crystalline nature. Undoped and doped SnO2 thin films can be synthesized by numerous methods such as dip coating [16], pulsed laser deposition [17], DC reactive sputtering [18], Spray pyrolysis [19], and chemical vapour deposition [20], etc. Amongst, nebulizer used spray pyrolysis (NSP) is one of the unique technique possess similar advantages of spray pyrolysis technique in addition to this, it is a low-cost and non-vacuum technique for wider range of applications and also yield good quality film with minimum precursor volume, nevertheless the rate of deposition and film thickness could be easily controlled for large area deposition that are desirable for industrial applications.

    View all citing articles on Scopus
    View full text