Table 2.

Fisher-estimated constraints on the EdGB gravity model from GW151226-like and GW170608-like signals. The lower part shows the case when all the parameters are unconstrained, while the upper part takes into account the prior information that |$\chi_1$| and |$\chi_2$| must necessarily be smaller than unity. The measurement accuracy of the symmetric mass ratio and the correlation coefficient between |$\eta$| and |$\sqrt{\alpha_{\rm EdGB}}$| are also shown.

signal|$\sqrt{\alpha_{\rm EdGB}}$| [km]|$\Delta\eta/\eta$||$c_{\eta,\sqrt{\alpha_{\rm EdGB}}}$|
 with spin prior  
GW151226-like3.35361%|$-$|0.708
GW170608-like2.96120%|$-$|0.245
 without spin prior  
GW151226-like5.8011600%0.968
GW170608-like5.237110%0.957
signal|$\sqrt{\alpha_{\rm EdGB}}$| [km]|$\Delta\eta/\eta$||$c_{\eta,\sqrt{\alpha_{\rm EdGB}}}$|
 with spin prior  
GW151226-like3.35361%|$-$|0.708
GW170608-like2.96120%|$-$|0.245
 without spin prior  
GW151226-like5.8011600%0.968
GW170608-like5.237110%0.957
Table 2.

Fisher-estimated constraints on the EdGB gravity model from GW151226-like and GW170608-like signals. The lower part shows the case when all the parameters are unconstrained, while the upper part takes into account the prior information that |$\chi_1$| and |$\chi_2$| must necessarily be smaller than unity. The measurement accuracy of the symmetric mass ratio and the correlation coefficient between |$\eta$| and |$\sqrt{\alpha_{\rm EdGB}}$| are also shown.

signal|$\sqrt{\alpha_{\rm EdGB}}$| [km]|$\Delta\eta/\eta$||$c_{\eta,\sqrt{\alpha_{\rm EdGB}}}$|
 with spin prior  
GW151226-like3.35361%|$-$|0.708
GW170608-like2.96120%|$-$|0.245
 without spin prior  
GW151226-like5.8011600%0.968
GW170608-like5.237110%0.957
signal|$\sqrt{\alpha_{\rm EdGB}}$| [km]|$\Delta\eta/\eta$||$c_{\eta,\sqrt{\alpha_{\rm EdGB}}}$|
 with spin prior  
GW151226-like3.35361%|$-$|0.708
GW170608-like2.96120%|$-$|0.245
 without spin prior  
GW151226-like5.8011600%0.968
GW170608-like5.237110%0.957
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