Abstract

Structural transformations caused by coarse-grained powdering and fine-grained mechanochemical milling in a dry mode were probed in high-temperature modification of tetra-arsenic tetra-sulfide known as β-As4S4. In respect to X-ray diffraction analysis, the characteristic sizes of β-As4S4 crystallites in these coarse- and fine-grained powdered pellets were 90 and 40 nm, respectively. Positron annihilation lifetime spectroscopy was employed to characterize transformations occurred in free-volume structure of these nanoarsenicals. Experimentally measured positron lifetime spectra were parameterized in respect to three- or two-term fitting procedures and respectively compared with those accumulated for single crystalline realgar α-As4S4 polymorph. The effect of coarse-grained powdering was found to result in generation of large amount of positron and positronium Ps trapping sites inside arsenicals in addition to existing ones. In fine-grained powdered β-As4S4 pellets, the positron trapping sites with characteristic free volumes close to bi- and tri-atomic vacancies were evidently dominated. These defects were supposed to originate from grain boundary regions and interfacial free volumes near aggregated β-As4S4 crystallites. Thus, the cumulative production of different positron traps with lifetimes close to defect-related lifetimes in realgar α-As4S4 polymorph was detected in fine-grained milled samples.

Highlights

  • Positron annihilation lifetime (PAL) spectroscopy is highinformative tool in studying sub-atomistic free-volume imperfections in solids affected by different nanostructurization routes [1,2,3,4,5]

  • The X-ray powder diffraction (XRPD) patterns of β-coarse-grained powdered (CGP) and β-fine-grained powder (FGP) pellets are shown in Fig. 1, top and bottom, respectively

  • The same β-As4S4 phase of C2/c space group was obviously dominated in both pellets (β-CGP and β-FGP), giving two different sets of crystallographic lattice parameters: a = 9.9200(2), b = 9.3946(2), c = 8.9505(2) Å, and β = 101.968(2)° for β-CGP and a = 9.9047(5), b = 9.4173(5), c = 9.0133(5) Å, and β = 101.246(4)° for β-FGP

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Summary

Background

Positron annihilation lifetime (PAL) spectroscopy is highinformative tool in studying sub-atomistic free-volume imperfections in solids affected by different nanostructurization routes [1,2,3,4,5]. With complementary mathematical algorithms allowing correct parameterization of mixed positron-electron annihilation paths in structurally complicated substances, this method (the positronics [6]) can be successfully motivated as a nanoscale alternative for conventional micro-meso-scale porosimetry exemplified by such well-approbated techniques as gas (nitrogen) sorption, mercury intrusion, and small-angle X-ray scattering [7,8,9]. Further progress in this field relies on stretching possibilities for positronics to be applied for a great diversity of known nanomaterials.

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