Skip to main content

Thank you for visiting nature.com. You are using a browser version with limited support for CSS. To obtain the best experience, we recommend you use a more up to date browser (or turn off compatibility mode in Internet Explorer). In the meantime, to ensure continued support, we are displaying the site without styles and JavaScript.

  • Letter
  • Published:

New T3B7 Compounds

Abstract

IN the course of a study on transition-element compounds of composition TB2 (T = transition element, B = phosphorus-group element) two compounds with a body-centred cubic structure were found, a semiconducting one in the system Re–As and a metallic one in the system Mo–Sb. Both compounds formed on reacting, at 600°–900° C, the powdered elements in various ratios. A crude analysis of ReAsx by thermal dissociation at 1,000° C gave x ≈ 2.4. Our arsenide, therefore, must be identical to the phase Re As2.3 reported by Wiechmann et al.1. The non-metallic behaviour as well as the diamagnetism of rhenium arsenide confirmed the suspected stoichiometry Re3As7 which corresponds to the normal valencies of Re and As. From density measurements, the unit cell [a = 8.722 ± 2 Å] was found to contain four formula units of Re3As7. Since in the X-ray diagram only the general extinctions for body-centred cubic symmetry are observed, seven space groups are possible. However, the striking resemblance between the diagram of Re3As7 and that of Ir3Ge7 led me to postulate a D8f structure for Re3As7. Best agreement between calculated and observed intensities was obtained for the following parameter values: Assuming the D8f type to be correct* for Re3As7, the coordination is as follows: This proximity is, in fact, reasonable since it makes allowance for saturated covalent bonds as can readily be seen by invoking a charge transfer Re3+As3As4 and by allowing half-bonds to form between Re and AsI. The non-metallic character of Re3As7 was established by resistivity measurements on sintered samples at temperatures above 300° C. Assuming ρ ≈ exp (δE/2kT), an energy gap δE ≈ 0.7 eV was derived. At room temperature the samples were n-type with a thermoelectric power of about 100 μV/°C. The magnetic susceptibility χM was found to be −210 and −250×10−6 cgs units/mole at liquid-nitrogen and room temperature, respectively.

This is a preview of subscription content, access via your institution

Access options

Buy this article

Prices may be subject to local taxes which are calculated during checkout

Similar content being viewed by others

References

  1. Wiechmann, F., Heimberg, M., and Biltz, W., Z. Anorg. Chem., 240, 129 (1939).

    Article  CAS  Google Scholar 

  2. Schubert, K., Kristallstrukturen zweikomponentiger Phasen, 316 (Springer-Verlag, 1964).

    Book  Google Scholar 

  3. Hellner, E., Z. Metallkde., 41, 480 (1950).

    CAS  Google Scholar 

Download references

Author information

Authors and Affiliations

Authors

Rights and permissions

Reprints and permissions

About this article

Cite this article

HULLIGER, F. New T3B7 Compounds. Nature 209, 500–501 (1966). https://doi.org/10.1038/209500a0

Download citation

  • Issue Date:

  • DOI: https://doi.org/10.1038/209500a0

Comments

By submitting a comment you agree to abide by our Terms and Community Guidelines. If you find something abusive or that does not comply with our terms or guidelines please flag it as inappropriate.

Search

Quick links

Nature Briefing

Sign up for the Nature Briefing newsletter — what matters in science, free to your inbox daily.

Get the most important science stories of the day, free in your inbox. Sign up for Nature Briefing