All Tables

Table 1: Atomic parameters of the observed lines. $\lambda _0$ denotes the laboratory wavelength, $\chi _{\rm l}$ the excitation potential of the lower energy level, and $\log gf$ the logarithm of the oscillator strength times the multiplicity of the level. The parameters $\alpha$ and $\sigma$ (in units of the Bohr radius, a₀) are used to calculate the line broadening by collisions with neutral hydrogen, atoms, while $g_{\rm l}$ , $g_{\rm u}$ , and $\bar g$ are the calculated Landé factors of the lower and upper levels, and the effective value, respectively.
Table 2: Differences between COG values of RF-predicted and calculated path length distributions. Values are presented for cases of waves excited by p-modes with inclinations, $\psi$ , of 0 $^\circ$ , 40 $^\circ$ , 50 $^\circ$ , and 60 $^\circ$ from the vertical. Note that in the case of vertical propagation ( $\psi =0$ $^\circ$ ) there is no distiction between ingressing or egressing forms of fast-mode waves, hence only one value is provided. When sampling a low plasma- $\beta$ environment the Alfvén and slow-mode waves are field aligned, remaining invariant to changes in the originating p-mode inclination: values are not provided for these two wave modes in the flux-tube reference frame due to their large magnitude and obvious incorrectness.