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Table A.4.

Time-integrated flare flux (erg per square centimetre) in HST-COS FUV.

Temporal flux evolution AU Mic F1 AU Mic F2 AU Mic F3 AU Mic F4 2MASS...168 F1 Karmn...+035 F1 2MASS...036 F1 2MASS...441 F1
Mendoza model 1.2787×10−9 7.0657×10−10 3.2834×10−10 1.8946×10−10 8.8510×10−11 7.1278×10−10 1.5559×10−9 6.3635×10−11
Davenport model 1.2769×10−9 7.1558×10−10 3.2823×10−10 1.9141×10−10 8.9296×10−11 7.2030×10−10 1.6056×10−9 6.5371×10−11
Feinstein model 6.3695×10−10 4.2002×10−10 2.2379×10−10 2.1785×10−10 8.1210×10−11 4.0197×10−10 7.3248×10−10 6.0898×10−11
Inverse H model 1.2908×10−9 6.4422×10−10 3.1229×10−10 2.2236×10−10 8.6776×10−11 5.4157×10−10 1.6026×10−9 7.2716×10−11
Inverse HCIII model 1.4917×10−9 7.1842×10−10 3.5056×10−10 2.7133×10−10 9.2140×10−11 5.3430×10−10 1.4785×10−9 7.2198×10−11
‘Fiducial flare’ model 2.5810×10−9 8.4980×10−10 5.0288×10−10 3.5072×10−10 - - - -
Observed 1.2793×10−9 6.7371×10−10 3.2174×10−10 1.9310×10−10 8.5826×10−11 5.9483×10−10 1.4291×10−9 6.8553×10−11

Notes. The time-integrated flare flux is calculated across FUV-A and FUV-B segments consistent with detector gaps specific to the observation (see Appendix A.4) in all temporally spectrally resolved models, including ‘fiducial flare’. 2MASS...168, Karmn...+035, 2MASS...036 and 2MASS...441 stand for 2MASS J01521830-5950168, Karmn J07446+0352MASS, J02365171-5203036 and 2MASS J22025453-6440441, respectively.

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