presentation mini-simphosium

19
Ritwik Mondal Department of Physics and Astronomy Relativistic theory in magnetisation dynamics Ritwik Mondal, Marco Berritta, Peter M. Oppeneer

Upload: ritwik-mondal

Post on 19-Mar-2017

62 views

Category:

Science


0 download

TRANSCRIPT

Page 1: Presentation mini-simphosium

Ritwik Mondal Department of Physics and Astronomy

Relativistic theory in magnetisation dynamics

Ritwik Mondal, Marco Berritta, Peter M. Oppeneer

Page 2: Presentation mini-simphosium

Ritwik Mondal Department of Physics and Astronomy

Ultrafast demagnetisation

E. Beaurepaire et al. PRL 76, 4250 (1996) C. Stamm et al. Nat. Mater. 6, 740 (2007)

Page 3: Presentation mini-simphosium

Ritwik Mondal Department of Physics and Astronomy

Relativistic mechanism?

Page 4: Presentation mini-simphosium

Ritwik Mondal Department of Physics and Astronomy

What is needed?

• Proper relativistic formalism • Inclusion of exchange effect • Different relativistic light-spin interactions • ab initio expressions for the parameters which describe the system dynamics

• ab initio calculations

Page 5: Presentation mini-simphosium

Ritwik Mondal Department of Physics and Astronomy

Outline

•Relativistic Hamiltonian formulation •Foldy-Wouthuysen transformation

•Landau-Lifshitz-Gilbert equation •Gilbert damping parameter

•ac harmonic field •time-dependent general magnetic field

•LLG to LL equation of motion

•Conclusions

Page 6: Presentation mini-simphosium

Ritwik Mondal Department of Physics and Astronomy

Dirac-Kohn-Sham Hamiltonian

• Dirac Hamiltonian for electrons in a (ferro)magnetic materials, excited by laser pulse:

• four component Hamiltonian • fully relativistic • non-relativistic limit is important for description of low-energy systems

• two-component system: large components and small components

• Foldy-Wouthyusen transformation

Page 7: Presentation mini-simphosium

Ritwik Mondal Department of Physics and Astronomy

Foldy-Wouthuysen transformation

• unitary transformation • find an unitary matrix: • time-dependent FW transformation

• only keeping even terms • The large component upto :

Mondal et al. Phys. Rev. B 91, 174415 (2015)

Page 8: Presentation mini-simphosium

Ritwik Mondal Department of Physics and Astronomy

Spin-orbit coupling Hamiltonian

• gauge invariant • hermitian • two types of spin-orbit coupling: (1) with the ionic potential -

intrinsic SOC, (2) with the field from laser - extrinsic SOC • intrinsic SOC time-independent electric field • extrinsic SOC time-dependent electric field

Page 9: Presentation mini-simphosium

Ritwik Mondal Department of Physics and Astronomy

Fast magnetisation dynamics

Landau-Lifshitz-Gilbert equation

Page 10: Presentation mini-simphosium

Ritwik Mondal Department of Physics and Astronomy

LLG equation of motion

• Is it possible to derive from a fundamental Dirac equation?

• What is the expression for Gilbert damping parameter?

• How the relativistic effects play a role? • Can we have a Gilbert damping parameter which is ab initio calculable?

Page 11: Presentation mini-simphosium

Ritwik Mondal Department of Physics and Astronomy

Definitions

• wavelength of the incident light, = 800 nm • thickness of the sample, = 20 nm (multilayered system) • • within Coulomb gauge ( ), uniform/slowly varying

magnetic field:

• spherically symmetric potential: • spin angular momentum:

Page 12: Presentation mini-simphosium

Ritwik Mondal Department of Physics and Astronomy

Extrinsic SOC

• Is it hermitian? • in the component form:

• but the full Hamiltonian is hermitian • Magnetisation dynamics definition:

Mondal, Berritta, Oppeneer Phys. Rev. B 94, 144419 (2016)

Hickey and Moodera Phys. Rev. Lett. 102, 137601 (2009)

Page 13: Presentation mini-simphosium

Ritwik Mondal Department of Physics and Astronomy

Magnetisation dynamics

• Zeeman-like non relativistic field-spin interactions are responsible for precession.

• intrinsic SOC contributes to the relativistic counterpart in precession.

• extrinsic SOC dynamics:

• relation between magnetisation and magnetic flux:

• for a time-dependent magnetic field: • for an ac harmonic field: differential magnetic susceptibility

Page 14: Presentation mini-simphosium

Ritwik Mondal Department of Physics and Astronomy

ac harmonic field• for an ac harmonic field:

• damping tensor :

• electronic part (interband):

• damping tensor can be expressed as: a isotropic Gilbert (scalar) + Anisotropic Ising-like (tensor) + anti-symmetric Dzyaloshinskii-Moriya-like (vector) contributions.

Mondal, Berritta, Oppeneer Phys. Rev. B 94, 144419 (2016)

Page 15: Presentation mini-simphosium

Ritwik Mondal Department of Physics and Astronomy

General time-dependent field• for a general time-dependent field

• damping parameters:

• New torque: field derivative torque in LLG equation!

time (t)

f(t) Derivative

time (t)

Page 16: Presentation mini-simphosium

Ritwik Mondal Department of Physics and Astronomy

LLG to LL equations• for harmonic field:

• DM-like contributions act as renormalisation factor to LL equation.

• Take and : we are back to the original LL equation.

• for a general time-dependent magnetic field

Page 17: Presentation mini-simphosium

Ritwik Mondal Department of Physics and Astronomy

Conclusions• New expression for Gilbert damping parameter - very suitable

for ab initio calculations! • Gilbert damping parameter for an ac harmonic field is a

tensor that depends on susceptibility and . • Gilbert damping parameter for a general time-dependent

field depends only on . • Gilbert damping tensor contains an isotropic (scalar), an

anisotropic Ising-like (tensor) and a chiral Dzyaloshinskii-Moriya like contribution.

• For a Gilbert damping tensor the transformation of LLG to LL equation is non-trivial.

• Dzyaloshinskii-Moriya like contribution serves as a renormalisation factor in LL equation.

Page 18: Presentation mini-simphosium

Ritwik Mondal Department of Physics and Astronomy

Acknowledgements• Pablo Maldonado • Alex Aperis • Karel Carva • Boris A. Ivanov

Page 19: Presentation mini-simphosium

Ritwik Mondal Department of Physics and Astronomy

Different Hamiltonians