Overview study on the characterization of zirconia as a function of calcination temperature

Chemical and biological agents continue to pose a threat to U.S. national security. The development of next generation of devices to sense, detect, filter, and remove these threats remains a priority of the U.S. Department of Defense. Zr(OH)4 is currently being developed as a decontaminant and is being engineered into suitable forms capable of removing chemical warfare agents. As such, having a detailed understanding of the local structure of amorphous Zr(OH)4 and heat treated ZrO2 analogs is a crucial step in developing these compounds as suitable countermeasures against chemical threats. In this study, zirconium hydroxide powders were calcined at various temperatures to study the effects of porosity, surface area, structure, and electronic properties as a function of temperature. Different characterization techniques were used to demonstrate that the surface area and porosity decreased as the material changed from an amorphous phase to a monoclinic crystal structure. Analysis of X-ray pair distribution function data provided a detailed representation of the local structure of amorphous Zr(OH)4 and its thermal decomposition into ZrO2. Impedance analysis showed both the dielectric constants and capacitance decreased by two orders of magnitude as crystallinity increased, correlating to a lowered concentration of defects, such as surface hydroxyl groups that contribute to leakage current.

[1]  B. Thibeault,et al.  High Dielectric Constant ZrO2 Films by Atomic Layer Deposition Technique on Germanium Substrates , 2016, Silicon.

[2]  R. D. Levie,et al.  On porous electrodes in electrolyte solutions: I. Capacitance effects☆ , 1963 .

[3]  C. Bark,et al.  Characteristics of the Dye-Sensitized Solar Cells Using TiO2 Nanotubes Treated with TiCl4 , 2014, Materials.

[4]  G. Peterson,et al.  Surface Chemistry and Morphology of Zirconia Polymorphs and the Influence on Sulfur Dioxide Removal , 2011 .

[5]  D. Vanderbilt,et al.  Structural and dielectric properties of crystalline and amorphous ZrO2 , 2005 .

[6]  R. Stroud,et al.  Structural Impact on Dielectric Properties of Zirconia , 2016 .

[7]  P. Barnes,et al.  A Dynamic High Temperature XRPD Study of the Calcination of Zirconium Hydroxide , 1988, Powder Diffraction.

[8]  Juan Bisquert,et al.  Doubling Exponent Models for the Analysis of Porous Film Electrodes by Impedance. Relaxation of TiO2 Nanoporous in Aqueous Solution , 2000 .

[9]  Wai Kin Chim,et al.  Interfacial and bulk properties of zirconium dioxide as a gate dielectric in metal–insulator–semiconductor structures and current transport mechanisms , 2003 .

[10]  W. Gordon,et al.  Local Structure of Zr(OH)4 and the Effect of Calcination Temperature from X-ray Pair Distribution Function Analysis. , 2018, Inorganic chemistry.

[11]  K. Honkala,et al.  Review: monoclinic zirconia, its surface sites and their interaction with carbon monoxide , 2015 .

[12]  E. Sasaoka,et al.  Effect of SO2 on the low-temperature selective catalytic reduction of nitric oxide with ammonia over TiO2, ZrO2, and Al2O3 , 2001 .

[13]  S. Sengupta,et al.  Sulfur Dioxide and Nitrogen Dioxide Adsorption on Zinc Oxide and Zirconium Hydroxide Nanoparticles and the Effect on Photoluminescence , 2012 .

[14]  Rosario A. Gerhardt,et al.  Impedance and dielectric spectroscopy revisited: Distinguishing localized relaxation from long-range conductivity , 1994 .

[15]  Jane P. Chang,et al.  Ultrathin zirconium oxide films as alternative gate dielectrics , 2001 .

[16]  J. Hanson,et al.  In situ study of the crystallization from amorphous to cubic zirconium oxide : Rietveld and reverse monte carlo analyses , 2007 .

[17]  Richard W. Siegel,et al.  Impedance spectroscopy of grain boundaries in nanophase ZnO , 1995 .

[18]  N. Mukherjee,et al.  Electrochemically synthesized microcrystalline tin sulphide thin films: high dielectric stability with lower relaxation time and efficient photochemical and photoelectrochemical properties , 2014 .

[19]  A. Guerrero-Ruíz,et al.  Interaction of Carbon Dioxide with the Surface of Zirconia Polymorphs , 1998 .

[20]  Simon J. L. Billinge,et al.  PDFgetX2: a GUI-driven program to obtain the pair distribution function from X-ray powder diffraction data , 2004 .

[21]  J. Ross Macdonald,et al.  Electrode kinetics, equivalent circuits, and system characterization: Small-signal conditions , 1977 .

[22]  S J L Billinge,et al.  PDFfit2 and PDFgui: computer programs for studying nanostructure in crystals , 2007, Journal of physics. Condensed matter : an Institute of Physics journal.

[23]  R. Gerhardt,et al.  Grain‐Boundary Effect in Ceria Doped with Trivalent Cations: I, Electrical Measurements , 1986 .

[24]  I. Danilenko,et al.  Impedance Spectroscopy of Concentrated Zirconia Nanopowder Dispersed Systems Experimental Technique , 2012 .

[25]  G. Colón,et al.  Effects of H2O2 and SO42- Species on the Crystalline Structure and Surface Properties of ZrO2 Processed by Alkaline Precipitation , 1997 .

[26]  Piero Pianetta,et al.  Interfacial properties of ZrO2 on silicon , 2003 .

[27]  R. Gerhardt,et al.  Grain‐Boundary Effect in Ceria Doped with Trivalent Cations: II, Microstructure and Microanalysis , 1986 .

[28]  A. Nowick,et al.  The “grain-boundary effect” in doped ceria solid electrolytes , 1980 .

[29]  Y. Gogotsi,et al.  Structure–activity relationship of Au/ZrO2 catalyst on formation of hydroxyl groups and its influence on CO oxidation , 2013 .

[30]  Brian H. Toby,et al.  EXPGUI, a graphical user interface for GSAS , 2001 .

[31]  G. Peterson,et al.  Zirconium Hydroxide as a Reactive Substrate for the Removal of Sulfur Dioxide , 2009 .

[32]  Qun Hui,et al.  RMCProfile: reverse Monte Carlo for polycrystalline materials , 2007, Journal of physics. Condensed matter : an Institute of Physics journal.

[33]  J. Jorcin,et al.  CPE analysis by local electrochemical impedance spectroscopy , 2006 .

[34]  G. Peterson,et al.  Reactions of VX, GD, and HD with Zr(OH)4: Near Instantaneous Decontamination of VX , 2012 .

[35]  K. Bowman,et al.  Crystallization of metastable tetragonal zirconia from the decomposition of a zirconium alkoxide derivative , 1995 .

[36]  M. Caymax,et al.  Characterisation of ALCVD Al2O3–ZrO2 nanolaminates, link between electrical and structural properties , 2002 .

[37]  M. Zaki,et al.  HT-XRD, IR and Raman characterization studies of metastable phases emerging in the thermal genesis course of monoclinic zirconia via amorphous zirconium hydroxide: impacts of sulfate and phosphate additives , 2002 .

[38]  E. Barsoukov,et al.  Impedance spectroscopy : theory, experiment, and applications , 2005 .

[39]  W. A. Adams,et al.  Electrochemical efficiency in multiple discharge/recharge cycling of supercapacitors in hybrid EV applications , 1999 .

[40]  Robert B. Balow,et al.  Environmental Effects on Zirconium Hydroxide Nanoparticles and Chemical Warfare Agent Decomposition: Implications of Atmospheric Water and Carbon Dioxide. , 2017, ACS applied materials & interfaces.

[41]  Udo Weimar,et al.  Investigations of conduction mechanism in Cr2O3 gas sensing thick films by ac impedance spectroscopy and work function changes measurements , 2008 .