Crossref journal-article
American Association for the Advancement of Science (AAAS)
Science (221)
Abstract

It has recently been shown that zirconium tungstate (ZrW 2 O 8 ) exhibits isotropic negative thermal expansion over its entire temperature range of stability. This rather unusual behavior makes this compound particularly suitable for testing model predictions of a connection between negative thermal expansion and pressure-induced amorphization. High-pressure x-ray diffraction and Raman scattering experiments showed that ZrW 2 O 8 becomes progressively amorphous from 1.5 to 3.5 gigapascals. The amorphous phase was retained after pressure release, but the original crystalline phase returned after annealing at 923 kelvin. The results indicate a general trend between negative thermal expansion and pressure-induced amorphization in highly flexible framework structures.

Bibliography

Perottoni, C. A., & Jornada, J. A. H. da. (1998). Pressure-Induced Amorphization and Negative Thermal Expansion in ZrW 2 O 8. Science, 280(5365), 886–889.

Authors 2
  1. C. A. Perottoni (first)
  2. J. A. H. da Jornada (additional)
References 20 Referenced 242
  1. See, for example, J. S. Tse, D. D. Klug, Phys. Rev. Lett. 70, 174 (1993); J. S. Tse, J. Chem. Phys. 96, 5482 (1992); F. Sciortino, et al., Phys. Rev. E 52, 6484 (1995); Lyapin A. G., Brazhkin V. V., Phys. Rev. B 54, 12036 (1996). (10.1103/PhysRevB.54.12036) / Phys. Rev. B by Lyapin A. G. (1996)
  2. See, for example, M. B. Kruger, R. Jeanloz, Science 249, 647 (1990); J. S. Tse, D. D. Klug, J. A. Ripmeester, S. Desgreniers, K. Lagarec, Nature 369, 724 (1994); O. Mishima, ibid 384, 546 (1996); C. Meade, R. J. Hemley, H. K. Mao, Phys. Rev. Lett. 69, 1387 (1992); G. C. Serghiou, R. R. Winters, W. S. Hammack, ibid 68, 3311 (1992); J. H. Nguyen, M. B. Kruger, R. Jeanloz, ibid. 78, 1936 (1997); Gillet P., Badro J., Varrel B., McMillan P. F., Phys. Rev. B 51, 11262 (1995). (10.1103/PhysRevB.51.11262) / Phys. Rev. B by Gillet P. (1995)
  3. Y. G. Gogotsi A. Kailer K. G. Nickel Mater. Res. Innovat. 1 3 (1997). (10.1007/s100190050011)
  4. Speedy R. J., J. Phys. Condens. Matter8, 10907 (1996). (10.1088/0953-8984/8/50/017) / J. Phys. Condens. Matter by Speedy R. J. (1996)
  5. Martinek C., Hummel F. A., J. Am. Ceram. Soc.51, 227 (1968). (10.1111/j.1151-2916.1968.tb11881.x) / J. Am. Ceram. Soc. by Martinek C. (1968)
  6. 10.1126/science.272.5258.90
  7. Evans J. S. O., Mary T. A., Vogt T., Subramanian M. A., Sleight A. W., Chem. Mater.8, 2809 (1996). (10.1021/cm9602959) / Chem. Mater. by Evans J. S. O. (1996)
  8. Evans J. S. O., et al., Science275, 61 (1997). (10.1126/science.275.5296.61) / Science by Evans J. S. O. (1997)
  9. Pryde A. K. A., et al., J. Phys. Condens. Matter8, 10973 (1996). (10.1088/0953-8984/8/50/023) / J. Phys. Condens. Matter by Pryde A. K. A. (1996)
  10. For reviews on RUMs, see M. T. Dove, Am. Mineral. 82, 213 (1997); Hammonds K. D., Dove M. T., Giddy A. P., Heine V., Winkler B., ibid 81, 1057 (1996); M. T. Dove, V. Heine, K. D. Hammonds, Mineral. Mag. 59, 629 (1995). / ibid by Hammonds K. D. (1996)
  11. J. Graham, A. D. Wadsley, J. H. Weymouth, L. S. Williams, J. Am. Ceram. Soc. 42, 570 (1959); Chang L. L. Y., Scroger M. G., Phillips B., ibid 50, 211 (1967). . ZrW2O8 was prepared by heating a mixture of ZrO2 and WO3 in the correct stoichiometric proportion in a sealed platinum tube at 1473 K for 48 hours. Cubic ZrW2O8 was retained metastably at ambient conditions by quenching the sample in water. Rietveld analysis of the x-ray diffraction pattern of the product revealed essentially pure cubic ZrW2O8, with a residual amount of less than 1.7% of ZrO2. / ibid by Chang L. L. Y. (1967)
  12. EDXRD experiments were done with a liquid nitrogen–cooled, intrinsic germanium detector from Princeton Gamma Tech, with measured resolution of 163 eV at 5.894 keV. Radiation from a conventional tungsten x-ray tube, operating at 45 kV and 20 mA, was collimated to a beam of 160-μm diameter before reaching the sample in the DAC. The diffraction angle was kept fixed at 7.62°, and acquisition time was typically 24 hours for each spectrum. After each spectrum acquisition, the energy scale was calibrated against an241Am radioactive source to compensate for any drift of the amplifier electronics. Peak positions in the EDXRD spectra were determined by fitting the peaks to Gaussian profiles, with the program XRDA [Desgreniers S., Lagarec K., J. Appl. Crystallogr. 27, 432 (1994)]. (10.1107/S0021889893012610) / J. Appl. Crystallogr. by Desgreniers S. (1994)
  13. Raman spectra were obtained with a Raman microprobe consisting of an Olympus BH-2 microscope equipped with a holographic beam splitter and a super notch filter a Jobin-Yvon HR320 monochromator and a EG&G Princeton Applied Research charge-coupled device detector cooled with liquid nitrogen. A nominal 10-mW HeNe laser (632.8 nm) was used as the excitation source.
  14. A Piermarini-Block DAC was used to generate high pressures [Piermarini G. J., Block S., Rev. Sci. Instrum. 46, 973 (1975)]. The powder sample, together with a small ruby chip as a pressure gauge, was conditioned inside a hole of 250-μm diameter drilled in a Waspaloy gasket preindented to 80 μm. No pressure medium was used. The low deviatoric stress condition inside the gasket hole was monitored by observing the broadening of the ruby peaks as pressure increased. Experiments performed with either methanol-ethanol-water (16:3:1) or silicon oil as the pressure medium yielded essentially the same results. (10.1063/1.1134381) / Rev. Sci. Instrum. by Piermarini G. J. (1975)
  15. Piermarini G. J., Block S., Barnett J. D., Forman R. A., J. Appl. Phys.46, 2774 (1975). (10.1063/1.321957) / J. Appl. Phys. by Piermarini G. J. (1975)
  16. A sample of ZrW 2 O 8 of about 12 mm 3 was encapsulated into hexagonal boron nitride and put inside a gasket to guarantee quasi-hydrostatic conditions during the experiment. Pressure was calibrated with the fixed points of bismuth [W. F. Sherman and A. A. Stadtmüller Experimental Techniques in High Pressure Research (Wiley New York 1987) chap. 6]. After compression the pellet of ZrW 2 O 8 was carefully ground in an agate mortar to provide a powder sample suitable for x-ray diffractometry.
  17. L. G. Khvostantsev High Temp. High Pressures 16 165 (1984).
  18. X-ray powder diffraction data for the cubic and amorphous samples of ZrW 2 O 8 at ambient conditions were obtained with a Siemens D500 diffractometer equipped with Soller slits in the incident beam a 1° divergence slit a 0.15-mm receiving slit and a graphite monochromator in the secondary beam. Data were collected with Cu Kα radiation in the angular range from 10° to 100° (2θ°) with a step scan of 0.05° and an acquisition time of 2 s by step (1 s for the cubic zirconium tungstate sample).
  19. A similar mechanism of pressure-induced amorphization can be found in the review by S. M. Sharma and S. K. Sikka [ Prog. Mater. Sci. 40 1 (1996)].
  20. We thank J. Haines from the Laboratoire de Physico-Chimie des Matériaux–CNRS Meudon (France) for a critical review of the paper and M. Sasso for help with the toroidal chamber. This work was supported by Conselho Nacional de Desenvolvimento Cientı́fico e Tecnológico (CNPq) Financiadora de Estudos e Projetos (FINEP) Fundação de Amparo à Pesquisa do Estado do Rio Grande do Sul (FAPERGS) and Perto S.A. (Brazil).
Dates
Type When
Created 23 years ago (July 27, 2002, 5:42 a.m.)
Deposited 1 year, 7 months ago (Jan. 12, 2024, 10:34 p.m.)
Indexed 2 weeks, 4 days ago (Aug. 2, 2025, 12:58 a.m.)
Issued 27 years, 3 months ago (May 8, 1998)
Published 27 years, 3 months ago (May 8, 1998)
Published Print 27 years, 3 months ago (May 8, 1998)
Funders 0

None

@article{Perottoni_1998, title={Pressure-Induced Amorphization and Negative Thermal Expansion in ZrW 2 O 8}, volume={280}, ISSN={1095-9203}, url={http://dx.doi.org/10.1126/science.280.5365.886}, DOI={10.1126/science.280.5365.886}, number={5365}, journal={Science}, publisher={American Association for the Advancement of Science (AAAS)}, author={Perottoni, C. A. and Jornada, J. A. H. da}, year={1998}, month=may, pages={886–889} }