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A vivid analogy with the photo- and radioluminescence immediately comes to mind. A direct photoexcitation of luminescent centers (photoluminescence) is known to be much more efficient than the radiation-induced excitation of the crystalline lattice (radioluminescence); see, for example:;;; Zinatne: Riga,; p [in Russian].
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A vivid analogy with the photo- and radioluminescence immediately comes to mind. A direct photoexcitation of luminescent centers (photoluminescence) is known to be much more efficient than the radiation-induced excitation of the crystalline lattice (radioluminescence); see, for example: Aluker, E. D.; Lusis, D. Y.; Chernov, S. A. Electronic Excitation and Radioluminescence of Alkali Halide Crystals; Zinatne: Riga, 1979; p 251 [in Russian].
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200 (Zababakhin Scientific Talks - 2005: International Conference on High Energy Density Physics). As was shown, the fragmentation of the heavy metal azide samples occurs already at a sufficiently low temperature (∼200 K), and most of the energy release and heating (∼3500 K) occur at the stage of expansion of explosion products. Perhaps, something similar can also take place in PETN. See also ref 3.
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Aluker, E. D.; Belokurov, G. M.; Krechetov, A. G.; Aduev, B. P.; Loboyko, B. G.; Filin, V. P. Two Stages of the Energy Release of Explosive Decomposition of Heavy Metals Azides. AIP Conf. Proc. 2006, 849, 196 - 200 (Zababakhin Scientific Talks-2005: International Conference on High Energy Density Physics). As was shown, the fragmentation of the heavy metal azide samples occurs already at a sufficiently low temperature (∼200 K), and most of the energy release and heating (∼3500 K) occur at the stage of expansion of explosion products. Perhaps, something similar can also take place in PETN. See also ref 3.
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0003862715
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It is also possible that the fracture of the sample is caused by the gaseous reaction products that destroy the crystalline lattice due to their high kinetic energy rather than due to heating. The analogy with radiation blistering is appropriate here; see, for example:; Cambridge Univ. Press: New York,; p.
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It is also possible that the fracture of the sample is caused by the gaseous reaction products that destroy the crystalline lattice due to their high kinetic energy rather than due to heating. The analogy with radiation blistering is appropriate here; see, for example: Thompson, M.W. Defects and radiation damage in metals; Cambridge Univ. Press: New York, 1969; p 384.
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Attention is drawn to the sufficiently deep analogy between this process and a well-known process in radiation physics of solid state, an exciton decay into a pair of Frenkel defects (see ref 18).
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Attention is drawn to the sufficiently deep analogy between this process and a well-known process in radiation physics of solid state, an exciton decay into a pair of Frenkel defects (see ref 18).
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79953746610
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Since PETN absorption spectra in the near-infrared region are insufficiently studied, it is difficult to propose a well-justified model of the nature of this state at this time.
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Since PETN absorption spectra in the near-infrared region are insufficiently studied, it is difficult to propose a well-justified model of the nature of this state at this time.
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-
-
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39
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79953747931
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We would like to reiterate that the idea of a pronounced correlation between the observed absorption band at 1020 nm and the band gap narrowing of an ideal PETN molecule is hypothetical and requires complex and computationally demanding ab initio calculations to refine and accept or reject this model. We are grateful to a reviewer of this manuscript who suggested an alternative explanation based on a possible extrapolation of the vibrational overtone sequence as partially observed in:; Portland; Office of Naval Research: Washington, DC, 1989; pp - 1117, Figure 3. A difficulty with this model is the lack of a reasonable explanation of why there is a dramatic difference in absorption caused by overtone(s) near 1020 nm and other overtones in the sequence.
-
We would like to reiterate that the idea of a pronounced correlation between the observed absorption band at 1020 nm and the band gap narrowing of an ideal PETN molecule is hypothetical and requires complex and computationally demanding ab initio calculations to refine and accept or reject this model. We are grateful to a reviewer of this manuscript who suggested an alternative explanation based on a possible extrapolation of the vibrational overtone sequence as partially observed in: Paisley, D.L. 9th Symposium on Detonation Proceedings; Portland; Office of Naval Research: Washington, DC, 1989; pp 1110-1117, Figure 3. A difficulty with this model is the lack of a reasonable explanation of why there is a dramatic difference in absorption caused by overtone(s) near 1020 nm and other overtones in the sequence.
-
9th Symposium on Detonation Proceedings
, pp. 1110
-
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Paisley, D.L.1
|