Search for content and authors
 

High-pressure phase transitions in AI3 (A = Rb, Cs, Tl, NH4) Triiodides

Joseph A. Hriljac 1Richard H. Jones 2Alistair Lennie 3William G. Marshall 4

1. School of Chemistry, University of Birmingham, Edgbaston, Birmingham B152TT, United Kingdom
2. School of Physical and Geographical Sciences, Keele University, Keele ST55BG, United Kingdom
3. Daresbury Laboratory (DL), Daresbury, Warrington WA4 4AD, United Kingdom
4. ISIS Facility, Rutherford Appleton Laboratory (ISIS), Oxon, Chilton Didcot OX110QX, United Kingdom

Abstract

The high pressure behaviour of molecular diatomic iodine is perhaps one of the most fascinating, with a gradual shortening of the intramolecular I-I contacts until they become near in value to the intermolecular I-I bonding distances.  At ~18 GPa metallization occurs1,2 even though the system remains a molecular solid.3  With continuing pressure the distances continue to approach a similar value, finally at ~30 GPa the iodine bonds break and an extended monoatomic solid forms.4  To date, there have been no reports of the high pressure chemistry of related simple polyhalide salts, such as the well known AI3 (A = Rb, Cs, Tl, NH4) systems, to explore the possibilities of similar metallisation and/or phase transitions.  We have recently collected synchrotron X-ray and neutron powder diffraction data on these materials and observe phase transitions from orthorhombic to trigonal systems at very low pressures, in the range of 0.7-3 GPa.  We have solved the structure of the high pressure phase, it is compared to the ambient pressure phase in Figure 1.  Although the phase transition does not involve loss of triiodide units, there are drastic changes in the packing of the cations and polyhalides precluding a simple correspondence between the two polymorphs.  It also appears that the phases are approaching a simple cubic AX3 system with the A15 (Cr3Si) structure type.  In this talk, details of the novel high pressure phases and correlations between the nature of the A cation and phase transition pressure and measured bulk moduli  will be presented.

ambient_HP_views.jpg

Fig. 1.Views of the ambient (left) and high (right) pressure phases

1. Balchan, A. S. & Drickamer, H., J. Chem. Phys. 34, 1948 (1961).
2. Riggleman, B. M. & Drickamer, H. G., J. Chem. Phys. 38, 2721 (1963).
3. Shimomura, O. et al., Phys. Rev. B 18, 715 (1978).
4. Takemura, K., Minomura, S., Shimomura, O. & Fujii, Y., Phys. Rev. Lett. 45, 1881 (1980).

 

Legal notice
  • Legal notice:
 

Related papers

Presentation: Oral at 11th European Powder Diffraction Conference, Microsymposium 14, by Joseph A. Hriljac
See On-line Journal of 11th European Powder Diffraction Conference

Submitted: 2008-04-30 00:30
Revised:   2009-06-07 00:48