html5-img
1 / 8

SPIN EXCITATIONS IN La 2 CuO 4 : CONSISTENT DESCRIPTION BY INCLUSION OF RING EXCHANGE

SPIN EXCITATIONS IN La 2 CuO 4 : CONSISTENT DESCRIPTION BY INCLUSION OF RING EXCHANGE. A.A.Katanin a,b and A.P.Kampf a a Instit u t f ü r Physik, Universit ä t Augsburg, Augsburg, Germany b Institute of Metal Physics, Ekaterinburg, Russia. Magnetic structure of La 2 CuO 4.

luke-owen
Télécharger la présentation

SPIN EXCITATIONS IN La 2 CuO 4 : CONSISTENT DESCRIPTION BY INCLUSION OF RING EXCHANGE

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. SPIN EXCITATIONS IN La2CuO4 : CONSISTENT DESCRIPTION BY INCLUSION OF RING EXCHANGE A.A.Katanina,b and A.P.Kampfa aInstitut für Physik, Universität Augsburg, Augsburg, Germany bInstitute of Metal Physics, Ekaterinburg, Russia

  2. Magnetic structure of La2CuO4 Heisenberg model j i Ring-exchange term l k j i • Appears in next-to-leading order in t/U expansion of Hubbard model • First introduced in connection with 3He(see, e.g., M.Roger et al, Rev.Mod.Phys 55 1 (1983))

  3. La2CuO4 Experimental spin-wave dispersion at T=10K (R.Coldea et al, Phys. Rev. Lett. 86, 5377 (2001))

  4. The Heisenberg model with ring exchange • Previously estimated values of parameters [1]: • J=146 meV; J´=J´´=0.02J; J<10-3J, J[]/J=0.41 • The derivation of effective spin model from three-band Hubbard model [2] led to estimate J[]/J=0.11 • [1] R.Coldea et al, Phys. Rev. Lett. 86, 5377 (2001) • [2] E. Müller-Hartmann and A. Reischl,cond-mat/0105392.

  5. Calculational steps • The Dyson-Maleev representation for spin operators • Calculation of renormalized spin-wave spectrum The factors {} are the renormalization factors • Solution of the self-consistent equations

  6. La2CuO4

  7. The results of fitting of experimental data • Parameters of the modelJ = 151.9 meV, J = J = 0.025J, J[] = 0.24J • Groud-state magnetization • Spin stiffness and the perpendicular susceptibilitys = 23.8 meV, c = 206meV,  = 4.8·10-5 K-1 • Earlier estimate from fitting the spin-spin correlation length (T) at T>TN is s = 23.9 meV • Renormalization factorsZc = 0.96, Z = 0.63, Z = 0.68 • Interlayer coupling J /J = 1.0·10-3 • The Neel temperature TN = 328 K  TNexp = 325 K

  8. Conclusions • The exchange parameters of La2CuO4 are determined with account of quantum fluctuations from the best fit to magnon spectrum • The values of exchange parameters are in goodagreement with other experimental data on La2CuO4.

More Related