Table 1: Atomic parameters of the spectral lines used for every element. Column 1: wavelength (in Å); Col. 2: excitation energy of the lower energy level in the transition (in eV); Col. 3: oscillator strengths based on an inverse solar analysis.
$\lambda$ $\chi_{l}$ $\log{gf}$ $\lambda$ $\chi_{l}$ $\log{gf}$

Si I; $\log \epsilon_{\circ} = 7.55$ A =14 Cr I; $\log \epsilon_{\circ} = 5.67$ A = 24

5665.56 4.92 -1.980 5304.18 3.46 -0.680

5690.43 4.93 -1.790 5312.86 3.45 -0.580

5701.10 4.93 -2.020 5318.77 3.44 -0.710

5772.14 5.08 -1.620 5480.51 3.50 -0.830

5793.09 4.93 -1.910 5574.39 4.45 -0.480

5948.55 5.08 -1.110 5783.07 3.32 -0.400

6125.02 5.61 -1.520 5783.87 3.32 -0.150

6142.49 5.62 -1.480 5787.92 3.32 -0.110

6145.02 5.61 -1.400 Mn I; $\log \epsilon_{\circ} = 5.39$ A= 25

6155.15 5.62 -0.750 4265.92 2.94 -0.440

6721.86 5.86 -1.090 4470.13 2.94 -0.550

Ca I; $\log \epsilon_{\circ} = 6.36$ A = 20 4502.13 2.92 -0.490

5512.98 2.93 -0.440 5399.47 3.85 -0.0969

5581.97 2.52 -0.650 5413.68 3.85 -0.470

5590.12 2.52 -0.710 5432.54 0.00 -3.620

5867.56 2.93 -1.590 6440.93 3.77 -1.250

6161.29 2.52 -1.220 Co I; $\log \epsilon_{\circ} = 4.92$ A = 27

6166.44 2.52 -1.120 5301.04 1.71 -1.930

6169.05 2.52 -0.730 5325.27 4.02 -0.120

6169.56 2.52 -0.440 5342.70 4.02 0.574

6449.82 2.52 -0.630 5483.36 1.71 -1.220

6455.60 2.52 -1.370 5647.23 2.28 -1.580

Sc II; $\log \epsilon_{\circ} = 3.10$ A = 21 6093.15 1.74 -2.340

5239.82 1.45 -0.760 6455.00 3.63 -0.280

5318.36 1.36 -1.700 Ni I; $\log \epsilon_{\circ} = 6.25$ A = 28

5526.82 1.77 0.150 5578.72 1.68 -2.650

6245.62 1.51 -1.040 5587.86 1.93 -2.380

6300.69 1.51 -1.960 5682.20 4.10 -0.390

6320.84 1.50 -1.840 5694.99 4.09 -0.600

6604.60 1.36 -1.160 5805.22 4.17 -0.580

Ti I; $\log \epsilon_{\circ} = 4.99$ A = 22 5847.00 1.68 -3.410

5471.20 1.44 -1.550 6086.28 4.26 -0.440

5474.23 1.46 -1.360 6111.07 4.09 -0.800

5490.15 1.46 -0.980 6128.98 1.68 -3.370

5866.46 1.07 -0.840 6130.14 4.26 -0.950

6091.18 2.27 -0.460 Na I; $\log \epsilon_{\circ} = 6.33$ A = 11

6126.22 1.07 -0.410 5688.22 2.104 -0.625

6258.11 1.44 -0.440 6154.23 2.102 -1.607

6261.11 1.43 -0.490 6160.75 2.104 -1.316

6303.76 1.44 -1.600 Mg I; $\log \epsilon_{\circ} = 7.58$ A= 12

6312.24 1.46 -1.580 5711.09 4.346 -1.706

V I; $\log \epsilon_{\circ} = 4.00$ A = 23 6318.72 5.108 -1.996

5668.37 1.08 -1.00 6319.24 5.108 -2.179

5670.85 1.08 -0.460 8712.69 5.932 -1.204

5727.05 1.08 -0.000 8736.02 5.946 -0.224

5727.66 1.05 -0.890 Al I; $\log \epsilon_{\circ} = 6.47$ A =13

5737.07 1.06 -0.770 6696.03 3.143 -1.570

6090.21 1.08 -0.150 6698.67 3.143 -1.879

6216.35 0.28 -0.900 7835.31 4.022 -0.728

6285.16 0.28 -1.650 7836.13 4.022 -0.559

6452.31 1.19 -0.820 8772.87 4.022 -0.425

8773.91 4.022 -0.212

**Table 1:** Atomic parameters of the spectral lines used for every element. Column 1: wavelength (in Å); Col. 2: excitation energy of the lower energy level in the transition (in eV); Col. 3: oscillator strengths based on an inverse solar analysis.
$\lambda$	$\chi_{l}$	$\log{gf}$		$\lambda$	$\chi_{l}$	$\log{gf}$
Si I; $\log \epsilon_{\circ} = 7.55$ A =14		Cr I; $\log \epsilon_{\circ} = 5.67$ A = 24
5665.56	4.92	-1.980		5304.18	3.46	-0.680
5690.43	4.93	-1.790		5312.86	3.45	-0.580
5701.10	4.93	-2.020		5318.77	3.44	-0.710
5772.14	5.08	-1.620		5480.51	3.50	-0.830
5793.09	4.93	-1.910		5574.39	4.45	-0.480
5948.55	5.08	-1.110		5783.07	3.32	-0.400
6125.02	5.61	-1.520		5783.87	3.32	-0.150
6142.49	5.62	-1.480		5787.92	3.32	-0.110
6145.02	5.61	-1.400		Mn I; $\log \epsilon_{\circ} = 5.39$ A= 25
6155.15	5.62	-0.750		4265.92	2.94	-0.440
6721.86	5.86	-1.090		4470.13	2.94	-0.550
Ca I; $\log \epsilon_{\circ} = 6.36$ A = 20		4502.13	2.92	-0.490
5512.98	2.93	-0.440		5399.47	3.85	-0.0969
5581.97	2.52	-0.650		5413.68	3.85	-0.470
5590.12	2.52	-0.710		5432.54	0.00	-3.620
5867.56	2.93	-1.590		6440.93	3.77	-1.250
6161.29	2.52	-1.220		Co I; $\log \epsilon_{\circ} = 4.92$ A = 27
6166.44	2.52	-1.120		5301.04	1.71	-1.930
6169.05	2.52	-0.730		5325.27	4.02	-0.120
6169.56	2.52	-0.440		5342.70	4.02	0.574
6449.82	2.52	-0.630		5483.36	1.71	-1.220
6455.60	2.52	-1.370		5647.23	2.28	-1.580
Sc II; $\log \epsilon_{\circ} = 3.10$ A = 21		6093.15	1.74	-2.340
5239.82	1.45	-0.760		6455.00	3.63	-0.280
5318.36	1.36	-1.700		Ni I; $\log \epsilon_{\circ} = 6.25$ A = 28
5526.82	1.77	0.150		5578.72	1.68	-2.650
6245.62	1.51	-1.040		5587.86	1.93	-2.380
6300.69	1.51	-1.960		5682.20	4.10	-0.390
6320.84	1.50	-1.840		5694.99	4.09	-0.600
6604.60	1.36	-1.160		5805.22	4.17	-0.580
Ti I; $\log \epsilon_{\circ} = 4.99$ A = 22		5847.00	1.68	-3.410
5471.20	1.44	-1.550		6086.28	4.26	-0.440
5474.23	1.46	-1.360		6111.07	4.09	-0.800
5490.15	1.46	-0.980		6128.98	1.68	-3.370
5866.46	1.07	-0.840		6130.14	4.26	-0.950
6091.18	2.27	-0.460		Na I; $\log \epsilon_{\circ} = 6.33$ A = 11
6126.22	1.07	-0.410		5688.22	2.104	-0.625
6258.11	1.44	-0.440		6154.23	2.102	-1.607
6261.11	1.43	-0.490		6160.75	2.104	-1.316
6303.76	1.44	-1.600		Mg I; $\log \epsilon_{\circ} = 7.58$ A= 12
6312.24	1.46	-1.580		5711.09	4.346	-1.706
V I; $\log \epsilon_{\circ} = 4.00$ A = 23		6318.72	5.108	-1.996
5668.37	1.08	-1.00		6319.24	5.108	-2.179
5670.85	1.08	-0.460		8712.69	5.932	-1.204
5727.05	1.08	-0.000		8736.02	5.946	-0.224
5727.66	1.05	-0.890		Al I; $\log \epsilon_{\circ} = 6.47$ A =13
5737.07	1.06	-0.770		6696.03	3.143	-1.570
6090.21	1.08	-0.150		6698.67	3.143	-1.879
6216.35	0.28	-0.900		7835.31	4.022	-0.728
6285.16	0.28	-1.650		7836.13	4.022	-0.559
6452.31	1.19	-0.820		8772.87	4.022	-0.425
		8773.91	4.022	-0.212

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