Fig. 4: Inverse spin Hall detection of propagating magnons in the device with different d.
From: Handedness manipulation of propagating antiferromagnetic magnons
a \(\Delta {V}_{{ISHE}}\) spectra under the tilted magnetic field \({\theta }_{H}\) = 30° at 13.0 GHz for the devices with different \(d\). The red lines represent the fitting results using the symmetric Lorentzian function, and the values of peak amplitude \({\left(\Delta {V}_{{{{\rm{ISHE}}}}}\right)}_{{{{\rm{peak}}}}}\) are extracted. b Distance dependence of \({\left(\Delta {V}_{{{{\rm{ISHE}}}}}\right)}_{{{{\rm{peak}}}}}\). The edge of the antenna corresponds to \(d\) = 0, and the values of \({\left(\Delta {V}_{{{{\rm{ISHE}}}}}\right)}_{{{{\rm{peak}}}}}\) are normalized at \(d\) = 0.0. The red line represents the fit of the exponential decay function.
