Fig. 5 | Nature Communications

Fig. 5

From: Correlation of the Dzyaloshinskii–Moriya interaction with Heisenberg exchange and orbital asphericity

Fig. 5

Correlation of DMI with \({\boldsymbol{m}}_{\mathbf{o}}^ \bot /{\boldsymbol{m}}_{\mathbf{o}}^\parallel\) and m D , and theoretical calculations based on the tight binding model and DFT. a Normalized \({\boldsymbol{m}}_{\mathrm{o}}^ \bot /{\boldsymbol{m}}_{\mathbf{o}}^\parallel\) and mD vs D. Values of \({\boldsymbol{m}}_{\mathrm{o}}^ \bot /{\boldsymbol{m}}_{\mathbf{o}}^\parallel\) and mD for all temperatures are normalized by the values measured at 300 K. b Calculated \({\boldsymbol{m}}_{\mathrm{o}}^ \bot\), \({\boldsymbol{m}}_{\mathbf{o}}^\parallel\) and EDMI values based on the tight-binding model as a function of temperature. Inset shows \(f_{{\mathrm{SD}}}^ \bot\)/\(f_{{\mathrm{SD}}}^\parallel\) as a function of temperature. c Physical parameters such as total D (Dtot), \({\boldsymbol{m}}_{\mathrm{o}}^ \bot /{\boldsymbol{m}}_{\mathbf{o}}^\parallel\), mD and ms obtained by DFT calculation. Strength and sign of Dtot are calculated around their magnetic ground state using the combination of the relativistic effect spin–orbit coupling with the spin spirals. A positive sign of Dtot indicates a left-rotational sense or left chirality

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