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Table 1.

Parameters of the group I models.

Group I

Initial cool loop Initial hot loop Heating



Name TiCL niCL P0 Name TiHL niHL L H0 Amax σev sev − Lmid iCL → fHL
m1 4.4 10.1 0.1 N/a N/a N/a 0.5 0.023 0.2 1.0 0 No
m2 4.5 10.0 N/a N/a N/a 1.0 2.0 No
m3 4.6 9.8 m22 5.7 9.2 2.0 4.0 Yes
m4 4.8 9.5 m23 5.8 9.3 3.0 6.0 Yes
m5 4.9 9.4 m24 5.9 9.3 4.0 8.0 Yes
m6 4.9 9.3 m25 5.9 9.3 5.0 10.0 Yes
m7 5.0 9.3 m26 5.9 9.3 5.5 11.0 Yes

Notes. Initial parameters of the group I models, with an increasing length L in the central part of the loop. The initial electron temperatures (logK) and densities (logcm−3) at the apex are respectively indicated for an initial cool (TiCL, niCL) and hot (TiHL, niHL) loops in equilibrium. For the cool loop in equilibrium, the pressure at the top of the vertical chromospheric legs is given by P0 (dyne cm−2). H0 (erg cm−3 s−1) is the uniform and constant term of the atmospheric heating H. The impulsive heating has an maximal amplitude Amax (erg cm−3 s−1), a spatial standard deviation σev (Mm), and a central position sev (Mm). The latter is given with respect to the center of the loop L mid = L c + L 2 $ L_{\mathrm{mid}} = L_{\mathrm{c}} + \frac{L}{2} $ (Mm). The column “iCL → fHL” indicates whether the initial cool loop has evolved into a final hot loop (marked as fHL) following the impulsive heating. Constant terms over a column are indicated by blanks, and N/a means that no hot loop in equilibrium could be built with the given parameters.

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