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Table 4:

a) SERTS/EIS observation (Keenan et al. 2000; Brown et al. 2008) for a solar active region along with predictions (for the line emissivity $\epsilon $ and intensity I, based upon the observed line flux at 258.37 Å) at $T_{\rm e}=10^{6.1}$ K and $n_{\rm e}=1.6$ $\times $ 109 cm-3. The ``-'' tag in the $\lambda $-columns denotes those wavelengths corrected by experimental energies.
${\rm\lambda_{obs}}$ Flux $\lambda^a$ ${\epsilon^a}$ $I_{\rm SERTS}^{a}$ $\lambda^b$ ${\epsilon^b}$ $I_{\rm SERTS}^{b}$ Transition
Å ${\rm SERTS^{\dag }}$ ${\rm EIS^{\dag }}$ Å ${\rm phot.~cm^3~s^{-1}}$   Å ${\rm phot.~cm^3~s^{-1}}$   Upper Low
253.81 3.28(1.02)c 86.8 -253.788 $2.273(-10){\rm ^d}$ 1.15 -253.787 2.762(-10) 1.18 ${\rm 2s 2p^2}$ ${\rm ^2P_{3/2}}$ ${\rm\to ~2s^2 2p}$ ${\rm ^2P_{1/2}}$
256.32 25.26(5.06) 462.5 -256.366 4.858(-10) 2.46 -256.384 6.036(-10) 2.57 ${\rm 2s 2p^2}$ ${\rm ^2P_{1/2}}$ ${\rm\to ~2s^2 2p}$ ${\rm ^2P_{1/2}}$
258.37 6.08(1.35) 452.3 -258.371 1.203(-09) 6.08 -258.371 1.427(-09) 6.08 ${\rm 2s 2p^2}$ ${\rm ^2P_{3/2}}$ ${\rm\to ~2s^2 2p}$ ${\rm ^2P_{3/2}}$
261.05 2.28(0.57) 17.1 -261.044 4.424(-10) 2.24 -261.063 4.909(-10) 2.09 ${\rm 2s 2p^2}$ ${\rm ^2P_{1/2}}$ ${\rm\to ~2s^2 2p}$ ${\rm ^2P_{3/2}}$
271.99 2.22(0.56) 152.3 -272.006 3.466(-10) 1.75 -271.983 4.378(-10) 1.87 ${\rm 2s 2p^2}$ ${\rm ^2S_{1/2}}$ ${\rm\to ~2s^2 2p}$ ${\rm ^2P_{1/2}}$
277.27 1.97(0.54) 116.5 -277.278 2.891(-10) 1.46 -277.254 3.665(-10) 1.56 ${\rm 2s 2p^2}$ ${\rm ^2S_{1/2}}$ ${\rm\to ~2s^2 2p}$ ${\rm ^2P_{3/2}}$
347.41 4.55(1.27) ... -347.409 7.764(-10) 3.92 -347.403 1.011(-09) 4.31 ${\rm 2s 2p^2}$ ${\rm ^2D_{3/2}}$ ${\rm\to ~2s^2 2p}$ ${\rm ^2P_{1/2}}$
356.03 4.84(0.56) ... -356.030 7.786(-10) 3.94 -356.011 1.090(-09) 4.64 ${\rm 2s 2p^2}$ ${\rm ^2D_{5/2}}$ ${\rm\to ~2s^2 2p}$ ${\rm ^2P_{3/2}}$
      -356.055 1.137(-10) 0.57 -356.050 1.483(-10) 0.63 ${\rm 2s 2p^2}$ ${\rm ^2D_{3/2}}$ ${\rm\to ~2s^2 2p}$ ${\rm ^2P_{3/2}}$

$\dag $ Units = 1012photons cm-2 s-1 sr-1; a,b,c,d the same definition as in Table 3a.

 

Table 4: b) Line intensity ratios relative to that of 258.37 Å for the SERTS/EIS observation. The caption and footnotes are the same as in Table 4a.
${\rm\lambda_{obs}}$ Ratio $\lambda^a$ $I/I_{\rm ref}^{a}$ $\lambda^b$ $I/I_{\rm ref}^{b}$ Transition
Å ${\rm SERTS^{\dag }}$ ${\rm EIS^{\dag }}$ Å   Å   Upper Low
253.81 0.54(0.21) 0.19 -253.788 0.19 -253.787 0.19 ${\rm 2s 2p^2}$ ${\rm ^2P_{3/2}}$ ${\rm\to ~2s^2 2p}$ ${\rm ^2P_{1/2}}$
256.32 4.15(1.24) 1.02 -256.366 0.40 -256.384 0.42 ${\rm 2s 2p^2}$ ${\rm ^2P_{1/2}}$ ${\rm\to ~2s^2 2p}$ ${\rm ^2P_{1/2}}$
258.37 1.00(0.31) 1.00 -258.371 1.00 -258.371 1.00 ${\rm 2s 2p^2}$ ${\rm ^2P_{3/2}}$ ${\rm\to ~2s^2 2p}$ ${\rm ^2P_{3/2}}$
261.05 0.38(0.13) 0.04 -261.044 0.37 -261.063 0.34 ${\rm 2s 2p^2}$ ${\rm ^2P_{1/2}}$ ${\rm\to ~2s^2 2p}$ ${\rm ^2P_{3/2}}$
271.99 0.37(0.12) 0.34 -272.006 0.29 -271.983 0.31 ${\rm 2s 2p^2}$ ${\rm ^2S_{1/2}}$ ${\rm\to ~2s^2 2p}$ ${\rm ^2P_{1/2}}$
277.27 0.32(0.11) 0.26 -277.278 0.24 -277.254 0.26 ${\rm 2s 2p^2}$ ${\rm ^2S_{1/2}}$ ${\rm\to ~2s^2 2p}$ ${\rm ^2P_{3/2}}$
347.41 0.75(0.27) ... -347.409 0.65 -347.403 0.71 ${\rm 2s 2p^2}$ ${\rm ^2D_{3/2}}$ ${\rm\to ~2s^2 2p}$ ${\rm ^2P_{1/2}}$
356.03 0.80(0.20) ... -356.030 0.65 -356.011 0.76 ${\rm 2s 2p^2}$ ${\rm ^2D_{5/2}}$ ${\rm\to ~2s^2 2p}$ ${\rm ^2P_{3/2}}$
      -356.055 0.09 -356.050 0.10 ${\rm 2s 2p^2}$ ${\rm ^2D_{3/2}}$ ${\rm\to ~2s^2 2p}$ ${\rm ^2P_{3/2}}$

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