Table 2: Comparison of our theoretical results for Stark broadening of Ge I lines with experimental results. With $W_{\rm m}$ are denoted experimental full widths at half maximum in [Å] and with $W_{\rm e}$ and $W_{\rm GeII}$ our theoretical values for Stark widths due to electron- and Ge II-impacts, respectively. Accuracy is denoted as in Konjevic et al. (1984) and Konjevic & Wiese (1990), C means that error bars are within $\pm$ 50% and D⁺ that they are larger than $\pm$ 50%. Under Ref., 1 is for Musiol et al. (1988) and 2. for Jones & Miller (1974).
Transition $\lambda$ (Å) T(K) $N_{\rm e}$ $W_{\rm m}$ $W_{\rm e}$ $W_{\rm GeII}$ Acc. Ref.

10¹⁷ cm^-3 (Å) (Å) (Å)

4p² ³P-5s³P⁰ 2754.59 12 450 0.57 0.0509 0.0502 0.00644 C 1

2709.62 12 450 0.57 0.0434 0.0490 0.00628 C 1

2651.57 12 450 0.57 0.0358 0.0466 0.00596 C 1

2651.17 12 450 0.57 0.0427 0.0517 0.00662 C 1

2592.53 12 450 0.57 0.0452 0.0494 0.00633 C 1

4p² ¹S-5s³P⁰ 4685.83 11 000 1 0.35 0.248 0.0339 C 2

4p² ¹D-5s³P⁰ 3124.82 12 450 0.57 0.0628 0.0715 0.00928 C 1

4p² ¹D-5s¹P⁰ 3039.07 12 450 0.57 0.0622 0.0721 0.00924 C 1

4p² ¹S-5s¹P⁰ 4226.56 11 000 1 3.18 0.239 0.0318 C 2

12 450 0.57 0.0815 0.139 0.0185 D⁺ 1

**Table 2:** Comparison of our theoretical results for Stark broadening of Ge I lines with experimental results. With $W_{\rm m}$ are denoted experimental full widths at half maximum in [Å] and with $W_{\rm e}$ and $W_{\rm GeII}$ our theoretical values for Stark widths due to electron- and Ge II-impacts, respectively. Accuracy is denoted as in Konjevic et al. (1984) and Konjevic & Wiese (1990), C means that error bars are within $\pm$ 50% and D⁺ that they are larger than $\pm$ 50%. Under Ref., 1 is for Musiol et al. (1988) and 2. for Jones & Miller (1974).
Transition	$\lambda$ (Å)	T(K)	$N_{\rm e}$	$W_{\rm m}$	$W_{\rm e}$	$W_{\rm GeII}$	Acc.	Ref.
			10¹⁷ cm^-3	(Å)	(Å)	(Å)
4p² ³P-5s³P⁰	2754.59	12 450	0.57	0.0509	0.0502	0.00644	C	1
	2709.62	12 450	0.57	0.0434	0.0490	0.00628	C	1
	2651.57	12 450	0.57	0.0358	0.0466	0.00596	C	1
	2651.17	12 450	0.57	0.0427	0.0517	0.00662	C	1
	2592.53	12 450	0.57	0.0452	0.0494	0.00633	C	1
4p² ¹S-5s³P⁰	4685.83	11 000	1	0.35	0.248	0.0339	C	2
4p² ¹D-5s³P⁰	3124.82	12 450	0.57	0.0628	0.0715	0.00928	C	1
4p² ¹D-5s¹P⁰	3039.07	12 450	0.57	0.0622	0.0721	0.00924	C	1
4p² ¹S-5s¹P⁰	4226.56	11 000	1	3.18	0.239	0.0318	C	2
		12 450	0.57	0.0815	0.139	0.0185	D⁺	1

Source LaTeX | All tables | In the text