The dynamics and thermal equilibrium of spin waves (magnons) in a quantum ferromagnet as well as the macroscopic magnetisation are investigated. Thermal noise due to an interaction with lattice phonons and the effects of spatial correlations in the noise are considered. We first present a Markovian master equation approach with analytical solutions for any homogeneous spatial correlation function of the noise. We find that spatially correlated noise increases the decay rate of magnons with low wave vectors to their thermal equilibrium, which also leads to a faster decay of the ferromagnet's magnetisation to its steady-state value. For long correlation lengths and higher temperature we find that additionally there is a component of the magnetisation which decays very slowly, due to a reduced decay rate of fast magnons. This effect could be useful for fast and noise-protected quantum or classical information transfer and magnonics. We further compare ferromagnetic and antiferromagnetic behaviour in noisy environments and find qualitatively similar behaviour in Ohmic but fundamentally different behaviour in super-Ohmic environments. different dynamics to uncorrelated noise, even in the Markovian regime. In ion traps for example the occurrence of decoherene-free subspaces has inspired quantum computation solutions [18,19]. In the field of quantum metrology a re-instatement of the superior Heisenberg precision scaling has been proven possible in the presence of spatial noise correlations [20]. In spin chains and light-harvesting complexes spatial noise correlations have shown to enable robust transport through protected states [21][22][23]. These results pose the question how correlated noise affects the dynamics of magnons and macroscopic quantities in a quantum ferromagnet This paper is structured as follows: in section 2 we introduce the spin-wave Hamiltonian, in section 3 we discuss its interaction with a thermal environment, in section 4 we derive and solve a master equation for magnons, in section 5 we discuss the macroscopic magnetisation, in section 6 we point out relevant differences between ferro-and antiferromagnetic behaviour and reach our conclusions in section 7.
Spin-wave HamiltonianWe begin by introducing the key concepts and the Heisenberg model Hamiltonian for spins in real space with nearest-neighbour interaction. We then show how this Hamiltonian maps via the Holstein-Primakoff transform with a spin-wave approximation to a bosonic system. Subsequent transformation into k-space via Fourier lattice transform of the operators diagonalises the Hamiltonian and yields the dispersion relation of the system. This is the Hamiltonian describing 'magnons', the elementary collective magnetic excitations.We start with a Heisenberg model for the spins in the quantum ferromagnet with only nearest-neighbour interaction and a uniform magnetic field B in the negative z-direction: Figure 1. Ferromagnetic spins (symbolised by arrows) interact with a noise environment of lattice phonons (symbolised by dots). Close spin...