Table A1.

Model parameters for the cstat analysis. The redshifts for each galaxy are as given in Table 2. |$kT$| is the temperature of the apec model component; Z is the abundance relative to solar abundance. Where |$\mathrm{CFrac}$| was fitted as 1, there is no upper error, so only a lower bounds on the error is given. The errors represent the 90 per cent confidence intervals using |$\chi ^2$|⁠.

Target|$N_\text{H}^{\prime }$||$kT$|Z|$\mathrm{ Norm}$||$\mathrm{CFrac}$||$N_\text{H}$||$\dot{M}$||$\dot{M}_\text{u}$|
|$10^{22}$| cm|$-$|2(keV)(⁠|$Z_{\odot }$|⁠)|$10^{-4}$||$10^{22}$| cm|$-$|2(⁠|$\mathrm{ M}_\odot$| yr|$-$|1)(⁠|$\mathrm{ M}_\odot$| yr|$-$|1)
NGC 13160.0199|$1.00^{+0.05}_{-0.12}$||$0.21^{+0.03}_{-0.04}$|7.8e−3|$0.90^{+0.06}_{-0.01}$|3.8|$4.4^{+3.1}_{-2.2}$||$0.52 \pm 0.04$|
NGC 13320.0214|$0.67^{+0.04}_{-0.05}$||$0.11^{+0.03}_{-0.02}$|2.4|$1_{-0.04}$|4.7|$7.9^{+2.8}_{-0.4}$||$0.27^{+0.06}_{-0.05}$|
NGC 14040.0138|$0.69 \pm 0.01$||$0.21\pm 0.01$|20|$0.97^{+0.02}_{-0.03}$|2.2|$8.0\pm 0.3$||$0.62\pm 0.14$|
NGC 45520.0266|$0.70\pm 0.02$||$0.072^{+0.007}_{-0.006}$|7.3|$0.97^{+0.03}_{-0.15}$|4.6|$0.72^{+0.6}_{-0.1}$||$0.036^{+0.004}_{-0.006}$|
NGC 46360.0182|$0.76\pm 0.02$||$0.26\pm 0.02$|33|$1_{-0.24}$|0.33|$0.91^{0.23}_{-0.22}$||$0.32^{+0.06}_{-0.05}$|
NGC 46490.0202|$0.91\pm 0.01$||$0.32\pm 0.02$|23|$1_{-0.01}$|9.9|$4.0^{+1.5}_{-1.9}$|negligible
IC 14590.009 67|$0.73^{+0.16}_{0.07}$||$0.09^{+0.03}_{-0.02}$|1.6|$0.91^{+0.06}_{-0.39}$|6.2|$3.2^{+2.9}_{-2.5}$||$0.33^{+0.05}_{-0.06}$|
Target|$N_\text{H}^{\prime }$||$kT$|Z|$\mathrm{ Norm}$||$\mathrm{CFrac}$||$N_\text{H}$||$\dot{M}$||$\dot{M}_\text{u}$|
|$10^{22}$| cm|$-$|2(keV)(⁠|$Z_{\odot }$|⁠)|$10^{-4}$||$10^{22}$| cm|$-$|2(⁠|$\mathrm{ M}_\odot$| yr|$-$|1)(⁠|$\mathrm{ M}_\odot$| yr|$-$|1)
NGC 13160.0199|$1.00^{+0.05}_{-0.12}$||$0.21^{+0.03}_{-0.04}$|7.8e−3|$0.90^{+0.06}_{-0.01}$|3.8|$4.4^{+3.1}_{-2.2}$||$0.52 \pm 0.04$|
NGC 13320.0214|$0.67^{+0.04}_{-0.05}$||$0.11^{+0.03}_{-0.02}$|2.4|$1_{-0.04}$|4.7|$7.9^{+2.8}_{-0.4}$||$0.27^{+0.06}_{-0.05}$|
NGC 14040.0138|$0.69 \pm 0.01$||$0.21\pm 0.01$|20|$0.97^{+0.02}_{-0.03}$|2.2|$8.0\pm 0.3$||$0.62\pm 0.14$|
NGC 45520.0266|$0.70\pm 0.02$||$0.072^{+0.007}_{-0.006}$|7.3|$0.97^{+0.03}_{-0.15}$|4.6|$0.72^{+0.6}_{-0.1}$||$0.036^{+0.004}_{-0.006}$|
NGC 46360.0182|$0.76\pm 0.02$||$0.26\pm 0.02$|33|$1_{-0.24}$|0.33|$0.91^{0.23}_{-0.22}$||$0.32^{+0.06}_{-0.05}$|
NGC 46490.0202|$0.91\pm 0.01$||$0.32\pm 0.02$|23|$1_{-0.01}$|9.9|$4.0^{+1.5}_{-1.9}$|negligible
IC 14590.009 67|$0.73^{+0.16}_{0.07}$||$0.09^{+0.03}_{-0.02}$|1.6|$0.91^{+0.06}_{-0.39}$|6.2|$3.2^{+2.9}_{-2.5}$||$0.33^{+0.05}_{-0.06}$|
Table A1.

Model parameters for the cstat analysis. The redshifts for each galaxy are as given in Table 2. |$kT$| is the temperature of the apec model component; Z is the abundance relative to solar abundance. Where |$\mathrm{CFrac}$| was fitted as 1, there is no upper error, so only a lower bounds on the error is given. The errors represent the 90 per cent confidence intervals using |$\chi ^2$|⁠.

Target|$N_\text{H}^{\prime }$||$kT$|Z|$\mathrm{ Norm}$||$\mathrm{CFrac}$||$N_\text{H}$||$\dot{M}$||$\dot{M}_\text{u}$|
|$10^{22}$| cm|$-$|2(keV)(⁠|$Z_{\odot }$|⁠)|$10^{-4}$||$10^{22}$| cm|$-$|2(⁠|$\mathrm{ M}_\odot$| yr|$-$|1)(⁠|$\mathrm{ M}_\odot$| yr|$-$|1)
NGC 13160.0199|$1.00^{+0.05}_{-0.12}$||$0.21^{+0.03}_{-0.04}$|7.8e−3|$0.90^{+0.06}_{-0.01}$|3.8|$4.4^{+3.1}_{-2.2}$||$0.52 \pm 0.04$|
NGC 13320.0214|$0.67^{+0.04}_{-0.05}$||$0.11^{+0.03}_{-0.02}$|2.4|$1_{-0.04}$|4.7|$7.9^{+2.8}_{-0.4}$||$0.27^{+0.06}_{-0.05}$|
NGC 14040.0138|$0.69 \pm 0.01$||$0.21\pm 0.01$|20|$0.97^{+0.02}_{-0.03}$|2.2|$8.0\pm 0.3$||$0.62\pm 0.14$|
NGC 45520.0266|$0.70\pm 0.02$||$0.072^{+0.007}_{-0.006}$|7.3|$0.97^{+0.03}_{-0.15}$|4.6|$0.72^{+0.6}_{-0.1}$||$0.036^{+0.004}_{-0.006}$|
NGC 46360.0182|$0.76\pm 0.02$||$0.26\pm 0.02$|33|$1_{-0.24}$|0.33|$0.91^{0.23}_{-0.22}$||$0.32^{+0.06}_{-0.05}$|
NGC 46490.0202|$0.91\pm 0.01$||$0.32\pm 0.02$|23|$1_{-0.01}$|9.9|$4.0^{+1.5}_{-1.9}$|negligible
IC 14590.009 67|$0.73^{+0.16}_{0.07}$||$0.09^{+0.03}_{-0.02}$|1.6|$0.91^{+0.06}_{-0.39}$|6.2|$3.2^{+2.9}_{-2.5}$||$0.33^{+0.05}_{-0.06}$|
Target|$N_\text{H}^{\prime }$||$kT$|Z|$\mathrm{ Norm}$||$\mathrm{CFrac}$||$N_\text{H}$||$\dot{M}$||$\dot{M}_\text{u}$|
|$10^{22}$| cm|$-$|2(keV)(⁠|$Z_{\odot }$|⁠)|$10^{-4}$||$10^{22}$| cm|$-$|2(⁠|$\mathrm{ M}_\odot$| yr|$-$|1)(⁠|$\mathrm{ M}_\odot$| yr|$-$|1)
NGC 13160.0199|$1.00^{+0.05}_{-0.12}$||$0.21^{+0.03}_{-0.04}$|7.8e−3|$0.90^{+0.06}_{-0.01}$|3.8|$4.4^{+3.1}_{-2.2}$||$0.52 \pm 0.04$|
NGC 13320.0214|$0.67^{+0.04}_{-0.05}$||$0.11^{+0.03}_{-0.02}$|2.4|$1_{-0.04}$|4.7|$7.9^{+2.8}_{-0.4}$||$0.27^{+0.06}_{-0.05}$|
NGC 14040.0138|$0.69 \pm 0.01$||$0.21\pm 0.01$|20|$0.97^{+0.02}_{-0.03}$|2.2|$8.0\pm 0.3$||$0.62\pm 0.14$|
NGC 45520.0266|$0.70\pm 0.02$||$0.072^{+0.007}_{-0.006}$|7.3|$0.97^{+0.03}_{-0.15}$|4.6|$0.72^{+0.6}_{-0.1}$||$0.036^{+0.004}_{-0.006}$|
NGC 46360.0182|$0.76\pm 0.02$||$0.26\pm 0.02$|33|$1_{-0.24}$|0.33|$0.91^{0.23}_{-0.22}$||$0.32^{+0.06}_{-0.05}$|
NGC 46490.0202|$0.91\pm 0.01$||$0.32\pm 0.02$|23|$1_{-0.01}$|9.9|$4.0^{+1.5}_{-1.9}$|negligible
IC 14590.009 67|$0.73^{+0.16}_{0.07}$||$0.09^{+0.03}_{-0.02}$|1.6|$0.91^{+0.06}_{-0.39}$|6.2|$3.2^{+2.9}_{-2.5}$||$0.33^{+0.05}_{-0.06}$|
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