1 / 19

Anisotropic Physical Properties of Decagonal Quasicrystals Janez Dolinšek

Anisotropic Physical Properties of Decagonal Quasicrystals Janez Dolinšek Jožef Stefan Institute, University of Ljubljana, Slovenia. Slovenia. Ljubljana. area: 20.000 km 2 population: 2 million. Adriatic sea. Lipizaner horses. Julian Alps. Lake Bled.

juana
Télécharger la présentation

Anisotropic Physical Properties of Decagonal Quasicrystals Janez Dolinšek

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. Anisotropic Physical Properties of Decagonal Quasicrystals Janez Dolinšek Jožef Stefan Institute, University of Ljubljana, Slovenia

  2. Slovenia Ljubljana area:20.000 km2 population: 2 million Adriatic sea Lipizaner horses Julian Alps Lake Bled

  3. “Jožef Stefan” Institute, Ljubljana, Slovenia staff: 850 revenues (2012): 52 MEur physics chemistry biology

  4. Structure of decagonal quasicrystals Geometrical description: periodic stacking of quasiperiodic atomic layers quasiperiodic atomic layers periodic 10-fold direction P

  5. Investigated phase Decagonalquasicrystald-Al-Co-Ni: - symmetry: decagonal - chemicalcomposition (at. %): Al70Co10Ni20 2 atomiclayerswithin one periodicunitof 0.4 nmalong105axis 5

  6. Physical properties investigated: • electrical resistivityρ(T) • magnetism χ(T), M(H) • thermoelectric power S(T) • - Hall coefficient RH(T) • thermal conductivity κ(T)

  7. Anisotropic physical properties of d-Al-Co-Ni measurements performed along four crystallographic directions (three “in-plane” and the stacking “10-fold” direction) P ... stacking direction P

  8. d-Al-Co-Ni: samples preparation P P P. Gille, G. Meisterernst, N. Faber, J. Crystal Growth 275, 224 (2005) 8

  9. Symmetry analysis General form of a tensorial physical property (2nd rank tensor) for a decagonal point group: P 9

  10. d-Al70Co10Ni20: symmetry analysis by 27Al NMR 27Al NMR spectrum central line central line satellites M. Bobnar et al., Phys. Rev. B 85, 024205 (2012) 10

  11. d-Al70Co10Ni20: orientation-dependent 27Al NMR spectra 11

  12. d-Al70Co10Ni20: orientation-dependent 27Al NMR satellite intensity 12

  13. d-Al70Co10Ni20: orientation-dependent 27Al NMR satellite intensity 13

  14. d-Al70Co10Ni20: electrical resistivity T-dependent resistivity in the Q plane P P Theory: Model of slow charge carriers G. Trambly de Laissardièreet al., Phys. Rev. Lett. 97, 026601 (2006)

  15. d-Al70Co10Ni20 :Hall coefficient P M. Bobnar et al., Phys. Rev. B 85, 024205 (2012) 15

  16. : d-Al70Co10Ni20 : thermal conductivity P M. Bobnar et al., Phys. Rev. B 85, 024205 (2012) 16

  17. Magnetization vs. magnetic field and magnetic susceptibility Stronger diamagnetism for the field along 10-fold axis: atomic rings in the Q plane form diamagnetic circular current loops P P W. Steurer et al., Acta Cryst. B 49, 661 (1993)

  18. Conclusions • electrical, thermal and magnetic properties of d-Al-Co-Ni decagonal quasicrystal are highly anisotropic; • stacking direction is the most conducting direction for the electricity and heat; • origin of anisotropy is the anisotropic stacked-layer atomic structure.

  19. Coworkers and cooperation J. Stefan Institute, Ljubljana Stane Vrtnik Matej Bobnar Zvonko Jagličić Institute of Physics, Zagreb Ana Smontara Ludwig-Maximilian University, Munich Peter Gille

More Related