American Journal of Nano Research and Applications

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Acoustic Detection of Resonance Plasticizing of LiF Crystals Under the Influence of Crossed Magnetic Fields in the EPR Scheme

Received: 03 February 2017    Accepted: 04 February 2017    Published: 28 February 2017
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Abstract

For the first time, the possibility of acoustic detection of resonance plasticizing of non-magnetic crystals when exposed to magnetic fields in EPR scheme was demonstrated. It is experimentally observed the sharp leap of dislocation internal friction in LiF crystals in crossed magnetic fields: constant field B0 = 340 µT and HF field B~ = 10 µT at the frequency of 9.525 MHz, corresponding to the paramagnetic resonance condition hv= BB0 for g = 2 (h is the Planck’s constant, g is the Lande factor, and μB is the Bohr magneton).

DOI 10.11648/j.nano.s.2017050301.19
Published in American Journal of Nano Research and Applications (Volume 5, Issue 3-1, May 2017)

This article belongs to the Special Issue Nanotechnologies

Page(s) 37-41
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This is an Open Access article, distributed under the terms of the Creative Commons Attribution 4.0 International License (http://creativecommons.org/licenses/by/4.0/), which permits unrestricted use, distribution and reproduction in any medium or format, provided the original work is properly cited.

Copyright

Copyright © The Author(s), 2024. Published by Science Publishing Group

Keywords

Magnetoplastic Effect, Internal Friction, Dislocation, Resonance Plasticizing, EPR

References
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Author Information
  • E. Andronikashvili Institute of Physics, I. Javakhishvili Tbilisi State University, Tbilisi, Georgia

  • E. Andronikashvili Institute of Physics, I. Javakhishvili Tbilisi State University, Tbilisi, Georgia

  • E. Andronikashvili Institute of Physics, I. Javakhishvili Tbilisi State University, Tbilisi, Georgia

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  • APA Style

    D. Driaev, M. Galustashvili, S. Tsakadze. (2017). Acoustic Detection of Resonance Plasticizing of LiF Crystals Under the Influence of Crossed Magnetic Fields in the EPR Scheme. American Journal of Nano Research and Applications, 5(3-1), 37-41. https://doi.org/10.11648/j.nano.s.2017050301.19

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    ACS Style

    D. Driaev; M. Galustashvili; S. Tsakadze. Acoustic Detection of Resonance Plasticizing of LiF Crystals Under the Influence of Crossed Magnetic Fields in the EPR Scheme. Am. J. Nano Res. Appl. 2017, 5(3-1), 37-41. doi: 10.11648/j.nano.s.2017050301.19

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    AMA Style

    D. Driaev, M. Galustashvili, S. Tsakadze. Acoustic Detection of Resonance Plasticizing of LiF Crystals Under the Influence of Crossed Magnetic Fields in the EPR Scheme. Am J Nano Res Appl. 2017;5(3-1):37-41. doi: 10.11648/j.nano.s.2017050301.19

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  • @article{10.11648/j.nano.s.2017050301.19,
      author = {D. Driaev and M. Galustashvili and S. Tsakadze},
      title = {Acoustic Detection of Resonance Plasticizing of LiF Crystals Under the Influence of Crossed Magnetic Fields in the EPR Scheme},
      journal = {American Journal of Nano Research and Applications},
      volume = {5},
      number = {3-1},
      pages = {37-41},
      doi = {10.11648/j.nano.s.2017050301.19},
      url = {https://doi.org/10.11648/j.nano.s.2017050301.19},
      eprint = {https://download.sciencepg.com/pdf/10.11648.j.nano.s.2017050301.19},
      abstract = {For the first time, the possibility of acoustic detection of resonance plasticizing of non-magnetic crystals when exposed to magnetic fields in EPR scheme was demonstrated. It is experimentally observed the sharp leap of dislocation internal friction in LiF crystals in crossed magnetic fields: constant field B0 = 340 µT and HF field B~ = 10 µT at the frequency of 9.525 MHz, corresponding to the paramagnetic resonance condition hv= gµBB0 for g = 2 (h is the Planck’s constant, g is the Lande factor, and μB is the Bohr magneton).},
     year = {2017}
    }
    

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    AB  - For the first time, the possibility of acoustic detection of resonance plasticizing of non-magnetic crystals when exposed to magnetic fields in EPR scheme was demonstrated. It is experimentally observed the sharp leap of dislocation internal friction in LiF crystals in crossed magnetic fields: constant field B0 = 340 µT and HF field B~ = 10 µT at the frequency of 9.525 MHz, corresponding to the paramagnetic resonance condition hv= gµBB0 for g = 2 (h is the Planck’s constant, g is the Lande factor, and μB is the Bohr magneton).
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