Radiation-stimulated processes under interaction of ions with porous structures

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For objects with topological and fractal dimensions (using the example of a “Coulomb explosion”), the physics of modification of electron-stimulated processes in porous media under irradiation with multiply charged ions is considered. A quasi-one-dimensional model has been constructed, which is a convenient methodological approach that describes characteristic phenomena in various media. The results obtained are assessed within the framework of the “complexity” concept.

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作者简介

N. Nikiforova

Arifov Institute of Ion Plasma and Laser Technologies, Academy of Sciences of the Republic of Uzbekistan; Institute of Materials Science, Academy of Sciences of the Republic of Uzbekistan, Scientific and Production Association “Physics-Sun”

Email: oksengendlerbl@yandex.ru
乌兹别克斯坦, Tashkent; Tashkent

B. Oksengendler

Institute of Materials Science, Academy of Sciences of the Republic of Uzbekistan, Scientific and Production Association “Physics-Sun”; Institute of Polymer Chemistry and Physics, Academy of Sciences of the Republic of Uzbekistan

编辑信件的主要联系方式.
Email: oksengendlerbl@yandex.ru
乌兹别克斯坦, Tashkent; Tashkent

Kh. Ashurov

Arifov Institute of Ion Plasma and Laser Technologies, Academy of Sciences of the Republic of Uzbekistan

Email: oksengendlerbl@yandex.ru
乌兹别克斯坦, Tashkent

B. Kutlimurotov

Arifov Institute of Ion Plasma and Laser Technologies, Academy of Sciences of the Republic of Uzbekistan

Email: oksengendlerbl@yandex.ru
乌兹别克斯坦, Tashkent

S. Maksimov

Arifov Institute of Ion Plasma and Laser Technologies, Academy of Sciences of the Republic of Uzbekistan

Email: oksengendlerbl@yandex.ru
乌兹别克斯坦, Tashkent

О. Galkina

Institute of Polymer Chemistry and Physics, Academy of Sciences of the Republic of Uzbekistan

Email: oksengendlerbl@yandex.ru
乌兹别克斯坦, Tashkent

参考

  1. Oksengendler B.L., Maksimov S.E., Turaeva N.N., Djurabekova F.G. // Nucl. Instrum. Methods Phys. Res. B. 2014. V. 326. P.45. https://doi.org/10.1016/j.nimb.2013.09.040
  2. Максимов С.Е., Оксенгендлер Б.Л., Тураев Н.Ю. // Поверхность. Рентген., синротр. и нейтрон. исслед. 2013. № 4. С. 42. https://doi.org/10.7868/S0207352813040161
  3. Оксенгендлер Б.Л., Зацепин А.Ф., Аширметов А.Х., Тураева Н.Н., Сулейманов С.Х., Никифорова Н.Н., Ашуров Х.Б. // Поверхность. Рентген., синротр. и нейтрон. исслед. 2022. № 6. С. 53. https://doi.org/10.31857/S1028096022060139
  4. Бак П. Как работает природа. М.: УРСС, 2013. 276 с.
  5. Parilis E.S., Kishinevsky L.M., Turaev N.Y., Baklitzky B.E., Umarov F.F., Verleger V.Kh., Nizhnaya S.L., Bitensky I.S. Atomic Collisions on Solid Surfaces. Amsterdam: North-Holland, 1993. 664 p.
  6. Auger P. // Comptes Rendus de l’Académie des Sciences. 1923. V. 177. P. 169.
  7. Meitner L. // Z. Physik. 1922. B. 9. № 1. S. 131. https://doi.org/10.1007/BF01326962
  8. Парилис Э.С. Эффект Оже. Ташкент: Фан, 1969. 205 с.
  9. Szilard L., Chalmers C.A. // Nature. 1934. V. 134. P. 462. https://doi.org/10.1038/134462b0
  10. Cooper J.W. // Phys. Rev. 1962. V. 128. P. 681. https://doi.org/10.1103/PhysRev.128.681
  11. Platsman R.L. // Radiat. Res. 1955. V. 2. P. 1. https://doi.org/10.2307/3570224
  12. Varley J.A. // Nature. 1954. V. 174. P. 886. https://www.nature.com/articles/174886a0
  13. Dexter D.L. // Phys. Rev. 1960. V. 118. P. 934. https://doi.org/10.1103/PhysRev.118.934
  14. Yunusov M.S., Zaikovskaya M.A., Oksengendler B.L., Tokhirov K.R. // Phys. Stat. Sol. A. 1976. V. 35. P. 145. https://doi.org/10.1002/pssa.2210350260
  15. Turaeva N.N., Oksengendler B.L., Ruban I.N., Rashidova S. // Dokl. Chem. 2002. V. 387. P. 302. https://doi.org/10.1023/A:1021174422477
  16. Suleymanov S.X., Oksengendler B.L., Kulagina N.A. // Crystallogr. Rep. 2021. V. 66. № 6. P. 1066. https://doi.org/10.1134/S1063774521060419
  17. Fleischner R., Price P., Walker R. Nuclear Tracks in Solids. Berkeley: University of California Press, 1975. 605 p.
  18. Оксенгендлер Б.Л., Тураева Н.Н. Радиационная физика конденсированных сред. Т. 1. Ташкент: Фан, 2006. 136 с.
  19. Oksengendler B.L., Ashirmetov A.Kh., Turaeva N.N. et al. // Nucl. Instrum. Methods Phys. Res. B. 2022. V. 512. P. 66. https://doi.org/10.1016/j.nimb.2021.12.009
  20. Yokoya A., Ito T. // Int. J. Radiat. Biol. 2017. V. 93. № 8. P. 743. https://doi.org/10.1080/09553002.2017
  21. Gharibkandi N.A., Gieraltowska J., Wawrowicz K., Bilewicz A. // Materials. 2022. V. 15. № 3. P. 1143. https://doi.org/10.3390/ma15031143
  22. Anderson P.W. // Phys. Rev. 1958. V. 109. P. 1492. http://refhub.elsevier.com/S0168-583X(21)00419-5/h0255
  23. Тихомиров В.П., Горленко О.А., Измеров М.А. // Изв. Самарского науч. центра РАН. 2011. Т. 13. № 4(3). С. 879.
  24. Федер Е. Фракталы. М.: Мир, 1991. 254 с.
  25. Nicolis G., Prigogine I. Exploring Complexity, Аn Introduction, New York: W. H. Freeman & Company, 1989. 328 р.
  26. Чукбар К.В. // ЖЭТФ. 1995. Т. 108. Вып. 5 (11). С. 1875.
  27. Олемской А.И., Флат А.Я. // УФН. 1993. Т. 13. Вып. 12. С. 1.

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2. Fig. 1. Scheme of the extended concept 'Complexity' applied to radiation effects in complex media.

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3. Fig. 2. Atomic structures with different topological dimensionality: a — three-dimensional; b — two-dimensional; c — one-dimensional chain.

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4. Fig. 3. Characteristic dependence of destruction cross-section on topological dimensionality.

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5. Fig. 4. Scheme of superposition of the Coulomb field of the Auger charge on the potential relief of electrons in the case of: a — strictly periodic relief of the electron potential; b — Anderson aperiodic chain.

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6. Fig. 5. Fractal pore containing both concave surface regions α, where the interaction of neighboring atoms is suppressed, and convex region β, where the interaction of neighboring atoms is enhanced.

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7. Fig. 6. Areas of a fractal surface with different curvature of local regions and, accordingly, with different overlap of the wave functions of neighboring atoms: ΔEV0 — corresponds to the width of the allowed valence band for flat surface areas; ΔEV — for concave surface areas with increased valence band width; — for convex areas with reduced overlap of the wave functions of neighboring atoms and narrowing of the valence band. This corresponds to both lower and higher radiation susceptibility, respectively.

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