31 October 2017 to 1 November 2017
IT4Innovations
Europe/Prague timezone

Calculating ultrafast laser-induced magnetization dynamics

31 Oct 2017, 17:00
20m
atrium (IT4Innovations)

atrium

IT4Innovations

Studentská 1B 708 33 Ostrava - Poruba
Users contributions Plenary talks 2

Speaker

Dr Karel Carva (Department of Condensed Matter Physics, Charles University)

Description

Since the first demonstration of femtosecond laser-induced demagnetization in 1996 [1], optical manipulation of magnetization has developed into a vibrant area of research that has explosively grown over the last decade. The most interesting one of discoveries is the demonstration of all-optical magnetization reversal and opto-magnetic recording with femtosecond laser pulses. All-optical magnetization switching (AOS) is emerging as a novel magnetic recording technology, its potential has been fully recognized by the magnetic recording industry, which enlisted AOS process on its roadmap towards ultra-high magnetic recording densities beyond 1 Tb/in^{2}. One of the critical problems in this field is related to the character of the transiently demagnetized state. Recently an insight into this problem has been provided by novel optical methods based on high harmonics generation [2]. Measurements of time-, energy-, and angle-resolved T-MOKE magnetic asymmetry spectra at M-edges have been compared to ab initio predictions for different deviations from the magnetic ground state, which allows us to draw conclusions about the importance of transversal magnetic excitations in the ultrafast laser-induced demagnetization [3]. An interesting magnetization dynamics has been observed in systems with 2 ferrimagnetically ordered sublattices: a complete reversal of magnetization in GdFeCo alloy. Most magnetic momentum in the system originates from Gd 4f states deep below the Fermi level, which prevents direct access to it by the laser. We calculate intraatomic exchange between Gd 4f and 5d orbitals [4] to allow mapping the problem to an effective orbital-resolved Heisenberg Hamiltonian. A subsequent simulation based on the LLG equation has reproduced the switching behavior and shown that the exchange coupling is sufficient to revert the large moment of Gd 4f shell on a ps time scale [5]. [1] E. Beaurepaire, J.-C. Merle, A. Daunois J.-Y. Bigot, Phys. Rev. Lett. 76, 4250 (1996). [2] Fan, T., et al., Proceedings of the National Academy of Sciences 112, pp. 14206–14211 (2015) [3] E. Turgut et al., Phys. Rev. B 94, 220408(R) (2016). [4] B. Frietsch et al., Nat. Commun. 6, 8262 (2015). [5] S. Wienholdt, D. Hinzke, K. Carva and others, Phys. Rev. B 88, 020406(R) (2013).

Primary authors

Dr Dominik Legut (IT4I) Dr Karel Carva (Department of Condensed Matter Physics, Charles University) Prof. Peter Oppeneer (Department of Physics and Astronomy, Uppsala University)

Presentation materials