Closed mkmk0324 closed 1 month ago
@mkmk0324 I think equations of this form is not possible with linear spin wave theory as implemented in SpinW - because we have to write the Hamiltonian in terms of the boson operators and we can only include terms which are quadratic in sites i and j in these operators. The reason that the (Si.Sj)^2 term works is because it involves only the on-diagonal terms which mostly yields quadratic terms or terms which are of the form (ai.ai^dagger)(aj.aj^dagger) which are just constants - there are also some quartic and higher order cross-terms (ai.aj.ai.aj etc) which end up being ignored in the linear approximation. In your case, I think the off-diagonal terms will only involve terms higher order in the boson operators which we cannot express in linear spin wave theory.
If you need to use these Hamiltonian terms I think you have to use a different code such as Sunny which uses a generalisation of spin wave theory as its formulism, or an RPA code such as McPhase.
Thank you for your answer. I see that the category of SpinW only has quadratic formulas with diagonal terms. Thank you again for your very clear answer. I will study Sunny and Mcphase as well.
In #95 and #152 you explain how to write interactions using the biquadratic form, is it possible to extend the input to a more general form?
i.e.,
Is it possible to add a 4th order term of the form?