1 / 17

Nonlinear transport in  Na 0.33 V 2 O 5

S.Sirbu 1 , P.H.M. van Loosdrecht 1 , T.Yamauchi 2 , and Y.Ueda 2. 1 Optical Condensed Matter Physics, Material Science Centre, University of Groningen. 2 Institute for Solid State Physics, University of Tokyo, Japan. Nonlinear transport in  Na 0.33 V 2 O 5. Charge ordering T  136 K.

Download Presentation

Nonlinear transport in  Na 0.33 V 2 O 5

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. S.Sirbu1, P.H.M. van Loosdrecht1, T.Yamauchi2, and Y.Ueda2 1Optical Condensed Matter Physics, Material Science Centre, University of Groningen 2 Institute for Solid State Physics, University of Tokyo, Japan Nonlinear transport in Na0.33V2O5

  2. Charge ordering T136 K S.C. under pressure Yamada, Ueda JPSJ 68, 2735 (1999) T. Yamauchi, Y. Ueda, N. Mori, PRL, 89, (2002). Magnetic ordering T24 K b-Na0.33V2O5 Phase Transitions

  3. b-Na0.33V2O5 T = 65 K TNa = 240K b-Na0.33V2O5 TMI = 136K 125K 105K 90K 65K Nonlinear transport

  4. Brazovskii, Sov.Phys.JETP 51, 342 (1980) Quasiparticles Quasiparticles + midgap solitons QP & Soliton transport b-Na0.33V2O5

  5. Quasiparticles Quasiparticles + midgap solitons QP & Soliton transport K0.3MoO3

  6. CDW transport models b-Na0.33V2O5 65K

  7. Simple classical model Charge q, applied field E Friction force: q·ET (E>ET) Damping: h Current:  Conductivity

  8. domain conductivity Domains considerations H. Fukuyama and P. Lee, Phys. Rev. B 17 , 535 (1978) Network of series and parallel domains Series  same functional form for conductivity Parallel  sum over domain contributions

  9. Series domains All paths in series can be replaced by an effective conductivity

  10. Parallel domains Taking a Lorentzian domain distribution:

  11. b-Na0.33V2O5 CO transport–simple model

  12. after percolation b-Na0.33V2O5 CO transport–simple model

  13. Conclusions • Highly nonlinear transport below MI transition. Charge density wave like conductivity. • Low field transport: quasiparticles + midgap solitons. • Domain model more adequately describes non-linear conduction of CDW like systems.

  14. x V z O y one Na1+ per two sites Na0.33V2O5 at 300K • Quasi 1D • Sodium ordering 240 K • Charge ordering 136 K • Spin ordering 24 K Space group C2/m (C2h3), a = 16.4 Å; b = 3.6 Å; c = 10.1Å; ß=109.6

  15. Simple classical model Log(s) Log(E) Variants by Grüner, Mihaly,…

  16. Domain model Log(s) Log(E)

  17. Properties of Na0.33V2O5 Charge ordering T=136 K Magnetic ordering T=24 K Yamada, Ueda JPSJ 68, 2735 (1999) T. Yamauchi, Y. Ueda, N. Mori (2002).

More Related