Journal of Young Investigators
    Undergraduate, Peer-Reviewed Science Journal
Volume Ten 
    RESEARCH ARTICLE
RECENT ISSUES | ARCHIVES | RESOURCES | JYI NEWS | ABOUT JYI 
Issue 3, March 2004

Biological & Biomedical Sciences

Synthesis of Single Phase SrCu2O2 from Liquid Precursors

Alex Martinson
Luther College
Advisor: David Ginley, Ph.D.
National Renewable Energy Laboratory
Discuss this article!

Abstract

We report on the first successful non-vacuum deposition of single phase SrCu2O2 from liquid precursors by spray deposition and experiments on the deposition of SrCu2O2 thin films by inkjet printing. Liquid precursors for SrCu2O2 were made by dissolving copper formate and strontium acetate in water. Bulk single-phase powdered SrCu2O2 was synthesized through the spray deposition of liquid precursors at 180° C followed by a four-hour anneal at 775° C and 2.0 x 10-5 Torr vacuum. Additionally, CaCO3 was successfully added to the precursor solution above and subsequently incorporated after annealing. This was a critical demonstration of the ability to perform cation substitutions by this approach. Employing the liquid precursor for thin films resulted in mixed phase SrCu2O2 and Cu2O due to Sr loss during annealing. The liquid precursor was also successfully inkjet printed.

 

Introduction

Transparent conducting oxides (TCOs) are widely used in solar cells, flat panel displays, electrochromic windows, and various other opto-electronic devices (Ginley and Bright 2000). TCOs are metal oxides that are optically transparent throughout most of the visible range of wavelengths. Unlike most metal oxides, this special class of materials can conduct electricity will relative ease. A TCO may be further classified by its major charge-carrying species. Most TCOs are n-type, which means that the major charge carriers are electrons. In contrast, TCOs are said exhibit p-type conduction when holes are the major carriers. While many n-type TCOs are known and currently in use, TCOs that exhibit p-type conduction are still rare.

Recently, several copper oxides, including SrCu2O2, CuAlO2, and CuGaO2, have been found to demonstrate p-type conductivity (Kawazoe et al. 1997, Yanagi et al. 2000, Kudo et al. 1998a). SrCu2O2 is of particular interest, because recent studies have shown it to have wide band gap and relatively low deposition temperatures (Kudo et al. 1998b). These properties give it tremendous potential for the next generation of high performance photovolatics (PV) as a contact to p-type semiconductors and as a component in a tunnel junction (Coutts et al. 2000). In addition, a working transparent diode composed completely of TCOs has now also been fabricated (Kudo et al. 1999). This transparent diode, the only one of its kind, is composed of p-SrCu2O2 and n-ZnO. SrCu2O2 has been synthesized through conventional ceramic processing followed by vacuum-based pulsed laser deposition to create thin films.

In this work, we report on a new method of SrCu2O2 synthesis that is more economical, potentially environmentally friendly, and more conducive to rapid exploration of process and compositional phase space. We report the non-vacuum synthesis of SrCu2O2 from liquid precursors. The precursors are synthesized inexpensively and are amenable to ready compositional substitution.

The liquid precursor approach was chosen with the intention that they could readily be incorporated into inkjet printing in the future. Inkjet printing allows for control of the deposition space as well as a relatively inexpensive method of deposition. Greater control of deposition space allows scientists to deposit materials only where needed, thus reducing the amount of material used for certain applications. Multiple inkjet head printing may allow for elemental substitution gradients similar to the way color inkjet printers can create a gradient of colors. For example, a Ca liquid precursor may be simultaneously printed with the SrCu2O2 precursor just as yellow is simultaneously printed with cyan in conventional inkjet printing. This method could create gradients of cation substitution, altering the p-type characteristics of the TCO throughout the sample.

The first step toward inkjet printing of thin film SrCu2O2 is the synthesis of the correct phase using the non-vacuum processing and the liquid precursors. We report the synthesis and substitution of bulk phase SrCu2O2 through spray deposition of liquid precursors. Spin casting allows similar precursors to be spun into thin films. The viability of inkjet printing liquid precursors has also been explored.

Materials and Methods

Liquid precursors to SrCu2O2 were made by dissolving organometallic powders into liquid solvents. Stoichiometrically correct 1 M solutions were prepared by dissolving Cu(OOCH)2•4H2O and Sr(CH3CO2)2 into water. In some samples, CaCO3 were substituted for the Sr(CH3CO)2 by 10% (atomic ratio).

As an initial test of the ink formulations, bulk powder samples were made by spray deposition. A fused-silica substrate was mounted on a resistive heater positioned 30° from horizontal and heated to 180° C. The precursor solution was passed through a 0.2 µm syringe filter and sprayed with an artist’s airbrush. Approximately 3 ml of solution were deposited over five minutes, yielding a thin brown powder. The fused-silica substrates were then secured to a resistive heating element with silver paste and sealed in a vacuum chamber with a base pressure 2.0 x 10-6 Torr. The samples were annealed in vacuum with a controlled oxygen partial pressure to bring the total chamber pressure to 2.0 x 10-5 Torr. After four hours of heating at 775° C, the temperature was quickly dropped to 650° C, and the oxygen bleed was eliminated before allowing the sample to cool to room temperature.

Multiple liquid precursors in various solvents were successfully spin cast onto fused silica substrates. The 4 cm2 substrates were mounted onto a spin caster (photoresist spinner, Headway Research Inc.). Liquid precursor was filtered through a 0.2 µm syringe filter and 2 drops were deposited onto the substrate. Samples were spun at 2000 rpm for 30 seconds at room temperature. The samples were warmed to 100° C for 30 minutes and then heated to 400° C for 30 minutes. In some cases, multiple layers were deposited by repeating the same process. The same annealing conditions are used as for the spayed case above.

Several liquid precursors in multiple solvents were also inkjet printed onto fused-silica substrates. A 50-micron inkjet print head (50 µm MicroJet™, MicroFab Technologies Inc.) was used to print the liquid precursors.

A second batch of samples was prepared using the exact same method; however, these were annealed in the vacuum chamber at 775° C in 2.0 x 10-5 Torr O2, a decrease from the original pressure.

Samples from both batches were characterized using X-ray diffraction (XRD, Scintag Model X1, Cu Kα) and inductively coupled plasma emission spectroscopy (ICP, Varian Liberty 150).

Results

Figure 1 shows the XRD θ/2θ pattern for a spray deposited sample annealed at 775° C under argon flow. The XRD pattern allows one to ascertain the composition and purity of a mixture by examining each compounds characteristic diffraction pattern. The XRD pattern for samples annealed at 775° C in 2.0 x 10-5 Torr O2 is shown in Figure 2. Pattern “a” is the water-based precursor spray deposited on fused silica at 180° C after annealing. Pattern “b” represents the liquid precursor with CaCO3 substituted for 10 atomic % of the Sr and annealed under the same conditions. Table 1 shows the composition of each sample as determined by ICP.

figure 1

Figure 1. XRD θ/2θ spectra for bulk phase SrCuO2. Liquid precursor spray was deposited on fused silica substrate and annealed at 775° C under argon flow for 20 hours. Bottom panel: expected powder pattern intensities (JCPDS 38-1179).

 

figure 1

Figure 2. XRD θ/2θ spectra of bulk phase (a) SrCu2O2 and (b) Ca substituted SrCu2O2. Samples were annealed at 775° C and 2.0 x 10-5 Torr for 4 hours. Bottom panel: expected powder pattern intensities (JCPDS 38-1178).

 

table 1

Table 1. Precursor* and Annealed Powder† Ratios

*Ratio calculated according to preparation of liquid precursor
†Ratio measured by ICP emission spectroscopy

The spin-cast films were similarly characterized. The precursor is a 0.5 M solution of copper formate and strontium acetate in a 70:30 mix of water and 2-propanol. This spectra was taken from a film deposited by spinning two layers of 0.5 M precursor. ICP results for the films are shown in Table 2.

table 2
Table 2. Thin Film Annealed Samples Showing Sr Deficiency

The viability of inkjet printing of the liquid precursors was also explored. The water-based precursor could be consistently printed under conditions given in Table 3.

table 3
Table 3. Stable Inkjet Printer Conditions with Water-Based Liquid Precursor

Discussion and Conclusion

The aim of this work was to provide an alternative synthesis technique for SrCu2O2 that would be easily and affordably implemented. To our knowledge, this is the first report of synthesis of SrCu2O2 through liquid precursors. One main advantage of this method of deposition is its potential to explore compositional phase space in the SrCu2O2 system. Future work includes the optimization of spin-cast deposition synthesis as well as inkjet printing of thin film SrCu2O2 precursors.

The first batch of samples, annealed at 775° C under argon flow, resulted in a mixed phase made primarily of SrCuO2 and CuO. The development of this phase distribution can be understood by examining the phase space for the (Sr-Cu-O) system, shown as Figure 3. This phase diagram, based on the work of Suzuki et al. (1992), shows the various Sr-Cu-O phase fields as a function of oxygen pressure and temperature for a fixed metals ratio of Cu/Sr = 2 as is appropriate for SrCu2O2. Taken together, this phase diagram and the XRD results from Figure 1 suggest that to reach the correct phase, the O2 partial pressure needed to be decreased.

figure 1

Figure 3. Sr-Cu-O phase space for Cu/Sr = 2.

 

The XRD pattern for samples annealed at 775° C in 2.0 x 10-5 Torr O2 show that they appear to be highly crystalline and phase pure. From Table 1 it is clear that the Ca source added to the liquid precursor has survived the annealing process. This suggests that elemental substitution may be achieved using liquid precursors. Facile elemental substitution will allow for greater control of p-type conduction.

XRD patterns and ICP results for the spin-cast films indicate that the sample is less pure and less crystalline than the spray deposited counterparts (Table 2). Note the presence of Cu2O in addition to SrCu2O2. This suggests that, after annealing, the thin film samples are Sr-deficient. The ICP results given in Table 2 show further evidence of the incorrect stoichiometry after annealing of several thin film samples. The loss of Sr from the precursor during anneal was unexpected and demonstrates a potential problem for the thin film samples. Mixed phase thin films will exhibit physical properties unlike those of the desired phase of pure TCO. Additional Sr may need to be added to the precursor or Sr vapor pressure may need to be controlled during anneal.

The inkjet printing of liquid precursors has developed as a viable option for the deposition of SrCu¬2O2. The time and cost of preparing these samples appear to be less than other popular methods such as sputtering. Additionally, as the technique develops, composition gradients and control of deposition space may further prove inkjet printing to be a valuable to tool for solid-state chemists.

We have demonstrated the synthesis of phase-pure bulk SrCu2O2 through the use of liquid precursors for the first time. Ca has been substituted through the use a liquid precursor and been shown to endure the annealing process. Spin-cast thin films have been created using water based liquid precursors. Annealing of the thin films results in a mixed phase of SrCu2O2 and CuO. The ability to inkjet print the precursors to SrCu2O2 has also been demonstrated. This work suggests that p-type TCOs may be derived from liquid precursors and easily substituted to allow greater control of p-type conductivity. These methods may open doors to new and better solar cells, flat panel displays and various other opto-electronic devices.

 

Acknowledgements

This work was supported by the National Renewable Energy Laboratory and Department of Energy. Special thanks to David Ginley, Tanya Kaydanova, Alex Miedaner, and John Perkins for all their assistance that made this work a productive and rewarding experience.

Discuss this article!

References

Coutts, T.J. et al. (2000) Characterization of Transparent Conducting Oxides. Materials Research Society Symposium Proceedings 623:199.

Ginley, D.S. and C. Bright (2000). Transparent Conducting Oxides. Materials Research Society Bulletin 25:15

Kawazoe, H. et al. (1997) P-type Electrical Conduction in Transparent Thin Films of CuAlO2. Nature 389:939

Kudo, A. et al. (1998a) SrCu2O2: A p-type conductive oxide with wide band gap Applied Physics Letters 73:220.

Kudo, A. et al. (1998b) A New p-type Conductive Transparent Oxide: Cu2SrO2. Materials Research Society Symposium Proceedings 526:299

Kudo, A. et al. (1999) Fabrication of transparent p–n heterojunction thin film diodes based entirely on oxide semiconductors. Applied Physics Letters 75:2851

Suzuki, R.O. et al. (1992) Thermodynamics and Phase-Equilibria in the SR-CU-O System. Journal of the American Ceramics Society 75:2833.

Yanagi, H. et al. (2000) Chemical Design and Thin Film Preparation of p-Type Conductive Transparent Oxides. Journal of Electroceramics 4:407.

Journal of Young Investigators. 2004. Volume Ten.
Copyright © 2004 by Alex Martinson and JYI. All rights reserved.
 
SEARCH   |   SITE MAP   |   RECENT WEB SITE ADDITIONS          PRIVACY POLICY  |    CONTACT US

JYI is supported by: The National Science Foundation, The Burroughs Wellcome Fund, Glaxo Wellcome Inc., Science Magazine, Science's Next Wave, Swarthmore College, Duke University, Georgetown University, and many others.
Copyright ©1998-2004 The Journal of Young Investigators, Inc.