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Study of Planar Metallic Magnonic Crystals by Brillouin Light Scattering (CAT#: STEM-ST-0155-YJL)

Introduction

Similarly to photons in photonic crystals, the spectrum of spin excitations in materials with periodically modulated properties shows bands of allowed magnonic states, alternating with forbidden band gaps. This constitutes a new class of artificial crystals, now known as magnonic crystals (MCs), in which collective spin excitations rather than light are used to transmit and process information. Since the wavelengths of these excitations are shorter than those of light in the gigahertz range, MCs offer better prospects for miniaturization at these frequencies with the advantage that frequency position and width of the band gap are tunable by the applied magnetic field. A MC can be formed starting from uncoupled resonators and making them coupled by some interaction, such as dipolar or exchange magnetic coupling.




Principle

From a quantum point of view, Brillouin scattering is an interaction of light photons with acoustic or vibrational quanta (phonons), with magnetic spin waves (magnons), or with other low frequency quasiparticles interacting with light. The interaction consists of an inelastic scattering process in which a phonon or magnon is either created (Stokes process) or annihilated (anti-Stokes process). The energy of the scattered light is slightly changed, that is decreased for a Stokes process and increased for an anti-Stokes process. This shift, known as the Brillouin shift, is equal to the energy of the interacting phonon and magnon and thus Brillouin scattering can be used to measure phonon and magnon energies.

Applications

Brillouin scattering is used to determine acoustic velocities and elastic properties of a number of crystalline solids, glasses, and liquids.

Procedure

1. Sample preparation
2. Measurement by scattering detection instrument
3. Data analysis

Materials

Brillouin scattering measurement system (Brillouin spectrometer)