Elsevier

Thin Solid Films

Volume 473, Issue 1, 1 February 2005, Pages 35-40
Thin Solid Films

Transport phenomena in high performance nanocrystalline ZnO:Ga films deposited by plasma-enhanced chemical vapor deposition

https://doi.org/10.1016/j.tsf.2004.06.154Get rights and content

Abstract

Nanocrystalline gallium doped zinc oxide (ZnO:Ga) thin films were synthesized by plasma-enhanced chemical vapor deposition (PECVD). A statistical design of experiments (DOE) was employed to optimize electrical conductivity. A carrier concentration of 5.5×1020/cm3 and a mobility of 15 cm2/V s yielding a resistivity of 7.5×10−4 Ω cm resulted from the conditions of high pressure, rf power, and electrode gap. X-ray diffraction showed that gallium doping had a profound impact on film orientation. Atomic force microscopy (AFM) revealed that the films were nanostructured, with an average grain size of 80 nm and a surface roughness of ∼2 nm. This unique morphology benefited optical transmission, but limited electrical performance. Average transmission across the visible spectrum was ∼93% as scattering losses were minimized. Temperature dependent Hall and optical transmission measurements demonstrated that structural defects and ionized impurities were equal contributors to electron scattering.

Introduction

Zinc oxide is a versatile wide bandgap semiconductor that is widely used in numerous applications including solar cells, displays, surface acoustic wave devices, and sensors. Zinc oxide is a promising alternative to indium tin oxide in transparent conducting oxide (TCO) applications, due to its low cost and ease of patterning. As a TCO, ZnO is commonly doped with aluminum and deposited by physical vapor deposition techniques such as sputtering [1] or pulsed laser deposition [2]. Plasma-enhanced chemical vapor deposition (PECVD) has found limited use for ZnO synthesis, with most work focused on intrinsic zinc oxide for structural properties [3] and more recently for UV emission [4]. The electrical properties of PECVD ZnO were the focus of a recent report [5], and ZnO:Al has been fabricated by injecting metallorganic precursor downstream of a cascaded thermal plasma [6]. However, some of the best zinc oxide films have been gallium doped, usually produced by chemical vapor deposition [7], [8].

In this paper, we discuss the fabrication of ZnO:Ga by PECVD. A statistical design of experiments (DOE) was used to optimize film conductivity. High conductivity films have a unique orientation and morphology relative to films deposited by other techniques. Excellent transmission in the visible spectrum and low resistivity were obtained. Both optical and electrical performances were related to microstructure. The nanocrystalline morphology resulted in exceptionally smooth films; however, electrical conductivity was limited in part by grain boundary and structural defects.

Section snippets

Experimental details

The films were deposited in a parallel plate, capacitively coupled RF plasma that has been described previously [5]. Corning 1737 glass was used as substrates. Diethyl zinc (DEZ, Strem, >95% purity) and trimethyl gallium (TMG, Strem, 99% purity) were carried into the reactor using argon and reacted with oxygen. The total metallorganic precursor flow rate was 2 sccm. This work derives from a study that interrogated the entire phase space from ZnO to Ga2O3[9]. In that work, it was found that both

Synthesis and characterization

Previous work on intrinsic ZnO PECVD demonstrated that high conductivity was achieved under highly oxidizing conditions [5]. The increased conductivity was attributed to higher surface mobility during growth, which yielded preferentially (002) oriented films. This study found that fuel-rich conditions (low O2/DEZ ratio) produced insulating films with random orientations. A recent study of gallium incorporation showed that the electrical conductivity and rate were optimized at a DEZ/TMG ratio of

Conclusions

Transparent and uniform conducting ZnO:Ga films with a fine grain size in the range of 50–100 nm were fabricated by PECVD. Statistically designed experiments used to optimize electrical conductivity demonstrated the strong interactions among plasma operating parameters. Optimized films had a unique crystal orientation as well as a smooth morphology. Optimized films had resistivity values of 7.5×10−4 Ω cm and 93% transmission across the visible. The electrical performance was limited by electron

Acknowledgements

The authors gratefully acknowledge the National Science Foundation for support for this work through award CTS-0093611.

References (19)

  • T. Minami et al.

    Thin Solid Films

    (1984)
  • R. Groenen et al.

    Thin Solid Films

    (2001)
  • J.J. Robbins et al.

    J. Cryst. Growth

    (2004)
  • J. Proscia et al.

    Thin Solid Films

    (1992)
  • J. Bruneaux et al.

    Thin Solid Films

    (1991)
  • M. Hiramatsu et al.

    J. Vac. Sci. Technol., A

    (1998)
  • T. Shiosaki et al.

    Appl. Phys. Lett.

    (1981)
  • B.S. Li et al.

    J. Appl. Phys.

    (2002)
  • J.J. Robbins et al.

    J. Electrochem. Soc.

    (2003)
There are more references available in the full text version of this article.

Cited by (62)

  • Pyrosol-deposited Ga-doped ZnO (GZO) transparent electrodes in GZO/(p<sup>+</sup>nn<sup>+</sup>)c-Si solar cells

    2015, Vacuum
    Citation Excerpt :

    Doping with Ga seems preferable, because the resistance of GZO films is more stable in comparison with other ZnO-based films of the same thickness and produced under the same conditions [14]. GZO films can be prepared by a variety of techniques, including atmospheric pressure chemical vapour deposition (APCVD) [15,16], plasma-enhanced chemical vapour deposition (PECVD) [17], ion plating [18], sputtering [19–26], plasma-assisted molecular beam epitaxy (PAMBE) [27,28], pulsed laser deposition (PLD) [29–35], sol–gel processing [36,37], vacuum arc plasma evaporation (VAPE) [38], and spray pyrolysis [39–46]. Among these techniques, spray pyrolysis is the simplest and the most economically attractive.

  • The electrical properties of low pressure chemical vapor deposition Ga doped ZnO thin films depending on chemical bonding configuration

    2014, Applied Surface Science
    Citation Excerpt :

    There have been reports on ZnO:Ga thin film deposition using various deposition techniques including sputtering [3], pulsed laser deposition (PLD) [8], molecular beam epitaxy (MBE) [9], sol–gel method [10], spray pyrolysis [11] and chemical vapor deposition (CVD) [12,13]. As for Ga doping precursor for CVD, triethyl gallium (TEG) [13–15], triisopropyl gallium (TIPGa) [16], trimethyl gallium (TMGa) [17] and mixtures [18] were reported. Especially, TEG and TMGa have been familiar precursors for GaAs deposition [19–21].

  • Tuning of TCO properties of ZnO by silver addition

    2014, Superlattices and Microstructures
    Citation Excerpt :

    Infect, Ag is not only a good electric conductor with relatively low optical absorption coefficient in the visible region but also an important optical material in the visible region and the near infrared region. While the doping of the different metals was successful for tuning the electrical properties of ZnO in thin films [14–16] and in bulk forms which has been widely reported [17,18]. But the reports on the systematic studies of the optical and electrical properties of Ag–ZnO, either in bulk or in thin film forms are still very scarce.

  • Using SiO <inf>x</inf> nano-films to enhance GZO Thin films properties as front electrodes of a-Si solar cells

    2013, Applied Surface Science
    Citation Excerpt :

    The defects inside thin films, such as grain boundaries, vacancies, and interstitials, result in the scattering of the carriers and reduce the carrier concentration. At a high electron density (>1020 cm−3), the dominant scattering effect of mobility measured by the Hall equipment was regarded as ionized impurity scattering [19,20]. An enhancement in the crystallinity of the bilayer GZO/SiOx thin films could reduce ionized impurity scattering, further increasing both the carrier mobility and the carrier concentration.

View all citing articles on Scopus
View full text