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JOURNALS // Fizika Tverdogo Tela // Archive

Fizika Tverdogo Tela, 2021 Volume 63, Issue 8, Pages 1120–1125 (Mi ftt8072)

This article is cited in 2 papers

Mechanical properties, strength physics and plasticity

Fracto- and photoluminescence of quartz during its fracture

V. I. Vettegren, A. G. Kadomtsev, I. P. Shcherbakov, R. I. Mamalimov

Ioffe Institute, St. Petersburg, Russia

Abstract: The fractoluminescence (FL) spectra at the destruction of the quartz surface by “micro-cutting” of diamond micro crystals and impact on its surface with a steel striker and photoluminescence (PL) spectra after “micro-cutting” are obtained. Band of 2.12 eV in the FL spectra was attributed to excited $\equiv$ Si-O$^\bullet$ radicals. FL consist from a set of signals whose duration was $\sim$ 50 ns, and their intensity varies by an order of magnitude. The time interval between the signals varies from $\sim$ 0.1 to several $\mu$s. Signals generated at impact contain five, and at “micro-cutting” contain four superimposed maxima. It is assumed that the FL signals appear when the barriers that prevent the movement of dislocations along the sliding planes breaks, and the smallest “primary” cracks are formatted. The rate constants of growth the cracks and fading of FL after the cracks stops are determined. The average size of the “primary” cracks surfaces after impact is $\sim$ 5 nm$^2$, and after “micro-cutting” is $\sim$ 25 nm$^2$. In the PL spectra after the fracture, a band of 2.4 eV was observed, which is attributed to non excited $\equiv$ Si-O- radicals on the cracks surface after their stop.

Keywords: fractoluminescence, photoluminescence, quartz, nanocracks, fracture.

Received: 25.03.2021
Revised: 30.03.2021
Accepted: 30.03.2021

DOI: 10.21883/FTT.2021.08.51165.060


 English version:
DOI: 10.1134/S1063783421080308

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© Steklov Math. Inst. of RAS, 2026