Correction to: Scientific Reports https://doi.org/10.1038/s41598-023-35670-y, published online 30 June 2023

The original version of this Article contained errors.

Equation 4 was incorrectly given as:

$$\begin{array}{c}{S}_{h}^{+}\left(\omega \right){|}_{\omega ={\omega }_{\lambda }}=\sqrt{\frac{{k}_{b}{T}_{\lambda }{\omega }_{\lambda }}{{Q}_{\lambda }{M}_{\lambda }}}\left(\frac{1}{{\omega }_{\lambda }^{2}{h}_{0}\xi }\right).\end{array}$$

The correct Equation 4 appears below.

$${S}_{h}^{+}\left(\omega \right){|}_{\omega ={\omega }_{\lambda }}=\sqrt{\frac{4{k}_{b}{T}_{\lambda }{\omega }_{\lambda }}{{Q}_{\lambda }{M}_{\lambda }}}\left(\frac{1}{{\omega }_{\lambda }^{2}{h}_{0}\xi }\right).$$

In addition, in the Sensitivity to HFGWs section,

“Based on the discussions presented in Aggarwal et al8, and using the C3,0,0 mode as an example, MAGE would be sensitive to a 0.004 \({M}_{\cdot }\) black hole merger, where \({M}_{\cdot }\) denotes the solar mass.”

now reads:

“Based on the discussions presented in Aggarwal et al8, and using the C3,0,0 mode as an example, MAGE would be sensitive to a 0.0004 \({M}_{\odot }\), where \({M}_{\odot }\) is the solar mass.”

The original Article has been corrected.