Contents

• The nature of ultraviolet spectra of AG Pegasi and other symbiotic stars: locations, origins, and excitation mechanisms of emission lines
• 1 Introduction
• 2 Data
• 3 Excitation and origin of AG Peg emission lines
• 4 Nature of the emission lines in symbiotic stars
• 5 Summary
• References
• 6 Online Material

A&A 451, 157-175 (2006)
DOI: 10.1051/0004-6361:20053396

The nature of ultraviolet spectra of AG Pegasi and other symbiotic stars: locations, origins, and excitation mechanisms of emission lines

M. Eriksson^1,2 - S. Johansson² - G. M. Wahlgren²

1 - University College of Kalmar, 391 82 Kalmar, Sweden
2 - Atomic Astrophysics, Lund Observatory, Lund University, Box 43, 221 00 Lund, Sweden

Received 10 May 2005 / Accepted 4 December 2005

Abstract
A detailed study of ultraviolet spectra of the symbiotic star AG Peg has been undertaken to derive the atomic excitation mechanisms and origin of formation for the lines common in symbiotic systems. More than 600 emission lines are observed in spectra from ${\it IUE}$, ${\it HST}$ and ${\it FUSE}$ of which 585 are identified. Population mechanisms and origin of formation are given for a majority of those lines. Based on the understanding of the AG Peg spectra ${\it IUE}$ data of 19 additional symbiotic stars are investigated and differences and similarities of their spectra are discussed. Fe II fluorescence lines pumped by strong emission lines between 1000 and 2000 Å are observed in 13 of these systems. Some of the symbiotic systems belonging to the subclass symbiotic novae have more than 100 Fe II fluorescence lines in the ultraviolet wavelength region. Forbidden lines are detected for 13 of the stars, mostly from highly-ionized spectra such as Ar V, Ne V and Mg V. Further, [Mg VI] and [Mg VII] lines are observed in a symbiotic star (AG Dra) for the first time. Five of the symbiotic stars have broad white-dwarf wind profiles ( ${\it FWHM} > 400$ km s^-1) for a few lines in their spectra. The stars with no such broad lines can be divided into two similarly sized groups, one where all lines have FWHM less than 70 km s^-1 and the other where one, a few or all of the broad ( ${\it FWHM} > 400$ km s^-1) lines of AG Peg have an enhanced broad wing (110-140 km s^-1).

Key words: atomic processes - line: formation - stars: binaries: symbiotic - ultraviolet: stars

1 Introduction

From numerous recordings with the ${\it IUE}$ satellite during 1978 to 1995 symbiotic stars are today known to be interacting binaries consisting of a white dwarf and a red giant with orbital periods of typically a few years. Symbiotic stars have composite spectra, an M-star continuum dominating at red and infrared wavelengths, a nebula continuum at ultraviolet and optical wavelengths, a rising continuum toward the far ultraviolet from the presence of a hot component and numerous strong emission lines throughout the spectrum indicating large plasma regions within the systems.

AG Peg is a symbiotic system consisting of a white dwarf and a red giant orbiting each other with a period of $812.3\pm6.3$ days (Kenyon et al. 1993). The luminosity of the white dwarf decreased by a factor of $\sim$4 during 1984-1997 (Kenyon et al. 2001). This decline can be understood as a decrease of its radius by a factor of $\sim$2 under constant temperature (Altamore & Cassatella 1997; Mürset & Nussbaumer 1994) or as an increase in the temperature of the white dwarf Schmutz 1996, which would imply a even larger decrease of its radius.

Between the two stars there is a region where the fast wind ( $v=~\sim\!900$ km s^-1) (Nussbaumer et al. 1995) from the white dwarf collides with the slow wind ( $v=~\sim\!60$ km s^-1) (Eriksson et al. 2004) from the red giant (Mürset et al. 1995). More recent and detailed ideas are discussed with respect to the wind structure concerning shock fronts from the wind collision region (Contini 2003) and the possibility of bipolar outflow (Yoo et al. 2002).

AG Peg belongs to a small subclass of symbiotic stars called symbiotic novae that have undergone nova events when the luminosity has increased by three to four magnitudes. Ultraviolet region line lists are available for two symbiotic novae, RR Tel (Penston et al. 1983) and V1016 Cyg (Nussbaumer & Schild 1981). Both of these systems have spectra dominated by allowed transitions from one to three times ionized elements, but also forbidden lines from more highly ionized elements have an impact on the spectrum. V1016 Cyg erupted in 1964 and RR Tel in 1944, while AG Peg erupted at least 150 years ago. An interesting open question is whether the decline of the UV flux in AG Peg during the 1980s is a natural evolutionary stage of symbiotic novae and whether, subsequently, RR Tel and V1016 Cyg will undergo a similar spectrum evolution in the future. A time analysis of the AG Peg spectrum can therefore give insights into what happens at the end of nova eruptions in symbiotic stars.

During the last 25 years the emission lines in AG Peg have been used for various diagnostics to measure parameters such as electron density (Keyes & Plavec 1980; Penston & Allen 1985) and temperature (Kenyon & Webbink 1984; Altamore & Cassatella 1997). By careful analysis of the spectra it is possible to categorize the emission lines in terms of population processes and line profiles. It is important to understand the origins of the emission lines as well as the processes that populate the corresponding upper levels when using them in any analysis. Here we explain the appearance of most of the emission lines formed at UV wavelengths in AG Peg. The main goal is to obtain an enhanced understanding of the emission lines, which would be helpful for anyone who wants to use emission lines as a diagnostic tool for symbiotic stars or related novae-like environments. Furthermore, the spectral investigation gives insight into how the UV spectum has evolved during the period 1978-1995.

Symbiotic stars are categorized in terms of stellar (S) and dusty (D) types based on their appearence at IR wavelengths (Allen 1982). The S-types have typical orbital periods of a few years and the cooler component consists of a solar-mass star on the red giant branch, while the D-types have orbital periods mostly in excess of 20 years and the cool component in those systems is typically a Mira. The small subset of D' type symbiotic stars has a cool star of spectral type G or K rather than M (Belczynski et al. 2000). The hot components are dominantly white dwarfs in both the S and D type systems. However, a few exceptions have the hot component as an accreation disk around a main sequence star (Kenyon & Garcia 1986).

Beyond the shared basic properties defining the group, the characteristics of symbiotic stars differ significantly. Besides the nova-like outbursts exhibited by the symbiotic novae, other phenomena observed in symbiotic stars are white-dwarf winds (Nussbaumer et al. 1995), recurrent-novae eruptions (Belczynski & Mikalojewska 1998), jets (Burgarella et al. 1992) and wind collision regions (Mürset et al. 1997).

By applying the understanding of the AG Peg spectrum at UV wavelengths to a set of 19 symbiotic stars we aim to detect differences and similarities among them. A detailed study of the lines showing broad white-dwarf wind lines in AG Peg is done to see how common such winds are in symbiotic systems. Fe II lines caused by photo-exitation by accidental resonance (PAR) are investigated to see whether this phenomenon is unique to a few symbiotic stars (Eriksson et al. 2003; Hartman & Johansson 2000) or more common among such systems. Also, forbidden lines of highly-ionized ions are analyzed to compare the ionization degree of low-density regions in symbiotic stars.

 

 

Table 1: Spectra used for AG Peg.

Instrument	Coverage (Å)	Spectum identification
IUE (LWR)	1900-3350	02591, 06389, 07504
		09672, 09310, 10579
IUE (LWP)	1900-3350	09698, 16684, 19235
		21635, 24149, 24285
		25565, 25995, 28122
		30936
IUE (SWP)	1150-1980	02326, 02334, 06335
		06809, 08760, 10454
		13957, 15651, 29862
		29863, 37420, 37477
		40149, 43006, 43007
		46149, 47715, 50707
		54749, 55055
HST (GHRS)	1222-1258	z27e0206t
	1354-1389	z27e0207n
	1383-1418	z27e0208t
	1468-1503	z27e0209t
	1532-1567	z27e020at
	1623-1657	z27e020bn
	1696-1737	z27e020dt
FUSE (LWRS)	920-1190	Q1110101
FUSE (MDRS)	920-1190	Q1110103

Figure 1: The dots represent the noise level for each of the different orders in the longest exposed IUE spectra, LWP25995 and SWP47715. The lines represent the noise level in the ${\it HST}$ and ${\it FUSE}$ spectra used in this work. The y-axis gives the value of the logarithm of the noise level measured in erg cm-2 s-1 Å-1. The noise level is defined as twice the standard deviation of the pixel intensity from the mean intensity, measured in wavelength regions not affected by spectral lines.

2 Data

The present study utilizes ultraviolet spectral data obtained from three different satellite observatories, spanning over nearly 25 years. The data were extracted from the Multimission Archive at STScI (MAST) in reduced format and are listed in Table 1. The extensive temporal coverage (1978-1995) of the International Ultraviolet Explorer IUE data for AG Peg allows us to follow spectrum developments during these years. The same data were exploited by Eriksson et al. (2004) to study wind affected line profiles for this star. Figure 1 prestents the noise levels for each spectral order for the longest exposures of the IUE high resolution observations. The figure thus provides a guide to the weakest detectable features and possible explanation for the relative strength of observed features. The resolution of ${\it IUE}$ spectra depends on several parameters, such as the dispersion angle, the reduction routine used and the wavelength being considered. No instrumental profile is deconvolved from the FWHM given in tables in this paper. Imhoff 1984 measured widths of platinum lines, with the FWHM being between 16 and 30 km s^-1. Therefore, the widths of lines narrower than 40 km s^-1 in our tables should be treated with caution.

The data recorded by the Goddard High Resolution Spectrograph (GHRS) onboard the Hubble Space Telescope (HST) during 1994 overlap in wavelength with the IUE data but were recorded at a later epoch and for only limited wavelength intervals. The greater sensitivity of the GHRS detectors makes it possible to measure intensities to a greater accuracy than can be done from the IUE spectra.

Two spectra of AG Peg have been recorded by the Far Ultraviolet Spectroscopic Explorer (FUSE) satellite, one in July 2001 and one in June 2003. The inclusion of FUSE spectra in our analysis increases the wavelength range for the detection of emission lines. However, since those spectra were obtained several years after the IUE and HST data we must be careful when incorporating these data sets into the analysis. The spectrum of AG Peg underwent obvious changes during the lifetime of the IUE (Eriksson et al. 2004) and we might expect that its development would continue in the sense that certain spectral lines would increase or decrease in intensity and width. Without contemporaneous observations in other wavelength regions, emission line intensities from the FUSE data cannot be rigorously correlated with the line intensities at longer wavelengths.

For the symbiotic stars other than AG Peg presented in this analysis only ${\it IUE}$ data are used. Since some of the Fe II lines as well as some of the forbidden lines are quite weak, one SWP and one LWP spectrum, observed with large aperture and with long exposure time, were selected for each system. The emission lines associated with the white-dwarf wind in AG Peg were easily saturated in the ${\it IUE}$ spectrum, which is why an extra SWP spectrum was retrieved from the MAST archive for some of the symbiotic systems. Table 2 lists the data used for the selected objects.

   

Table 2: IUE spectra used for the selected symbiotic stars.

Object	LWP/LWRa	SWPa	SWPb
Z And	LWP06225	26177	26938
EG And	LWP25855	56021	46879
R Aqr	LWP21998	31102	40265
T CrB	LWP01536	28490
BF Cyg	LWP15253	35843	58386
CH Cyg	LWP08631	28011
CI Cyg	LWR10427	18602	50760
AG Dra	LWP24400	15656	55373
RW Hya	LWR10227	13601
SY Mus	LWR10829	14236	16383
AX Per	LWP19332	21443	06807
RX Pup	LWR10831	31285	16597
HM Sge	LWP12921	40081
RR Tel	LWR16187	20246	18371
KX Tra	LWP17871	38742
PU Vul	LWP26780	37190	49265
V1016 Cyg	LWP04961	29830	24657
V1329 Cyg	LWP13121	24663	05615
HBV475	LWP08277	30853

^a Spectrum with long exposure times used to detect
  weak Fe II fluorescence lines and forbidden lines.
^b Spectrum with short exposure times used when allowed
  lines are saturated in longer exposed spectra.

3 Excitation and origin of AG Peg emission lines

The spectral lines can be divided into different categories depending upon their widths and profiles. However, lines that look similar in one spectrum can show a different appearance in later spectra. This means that the time history of a spectral line is also important. Some narrow lines are selectively populated by radiative line excitation and they are classified as fluorescence lines, whereas others originate from excited levels populated by collisions or recombination. We have categorized the spectral lines by their overall appearance in the following way:

1.

Broad emission lines ( ${\it FWHM} > 500$ km s^-1) in spectra until 1981 that later evolve into narrower ( ${\it FWHM }< 80$ km s^-1) emission lines.

2.

Emission lines caused by fluorescence.

3.

Narrow emission lines from levels excited by collisions.

4.

Narrow emission lines from levels populated by recombination.

5.

Narrow emission lines from levels with an uncertain population mechanism.

6.

Interstellar absorption lines

7.

Stellar absorption lines.

The lines showing a broad structure originate from ions of higher ionization stages, and they are partially or completely formed in the wind of the white dwarf before 1980 (Eriksson et al. 2004). During 1980-1985 the broad contribution from the white-dwarf wind to these lines vanished as a result of the reduced bolometric luminosity (a factor of 2-3) of the white dwarf. Narrow "nebular'' lines replaced these broad wind lines in later spectra. Unfortunately, no ${\it IUE}$ spectra of AG Peg were recorded during the years 1982 to 1985, when most of the line profiles must have undergone a rapid change. The narrow lines are most probably formed at further distance from the white dwarf, like in the extended parts of the red giant, such as its wind or upper atmosphere, or in the surrounding nebula. These lines involve mostly permitted lines and intercombination lines, but there are also a few forbidden lines originating from metastable states with lifetimes on the order of seconds. Most of the absorption lines are believed to be formed in the outer parts of the surrounding nebula (Penston & Allen 1985). In Table 3 we present for each element the number of identified lines observed in the UV spectrum of AG Peg.

   

Table 3: The distribution of emission lines for AG Peg, according to population processes.

Spec.	Processa				Tot		Spec.	Processa				Tot
	fl.	rec.	col.	unk				fl.	rec.	col.	unk
H I		1			1		[Ne V]			3		3
He I		8			8		Mg II			2	7	9
He II		14			14		Mg IV		7			7
C II			5	3	8		[Mg V]			3		3
C III		8		3	11		Al II]			1		1
C III]			2		2		Al III			2		2
C IV			2		2		Si I				5	5
N I	1			4	5		Si II			3	5	8
N I]			4		4		Si II]			2		2
N III		5		4	9		Si III				4	4
N III]			5		5		Si III]			1		1
N IV		1			1		Si IV			2	5	7
N IV]			2		2		P II			3	1	4
N V			2		2		P II]			1		1
O I			2		2		P III			2		2
O I]				2	2		P IV				1	1
O III	16	6			22		P IV]			1		1
O III]	1	1	3	2	7		S I	1		5		6
[O III]			1		1		S I]			1		1
O IV		3		2	5		S II]			1		1
O IV]		5			5		S IV]			5		5
O V		3		1	4		S V				1	1
O V]				1	1		S V]				1	1
O VI			2		2		[Ar V]			1		1
Ne III		8			8		Fe II*	226	3	85	32	346
Ne III]		2			2		Fe III	3			11	14
[Ne III]			1		1		Fe V		4			4
[Ne IV]			4		4		[Fe VI]			2		2
Ne V]			2		2		Co II*	5			6	11

$\parbox{12cm}{ $^{*}$\space Spin-forbidden transitions are also incl... ...\space fl = fluorescence; rec = recombination; col = collision; unk = unknown.}$

   

Table 4: The broad emission lines in AG Peg spectra.

			Before 1986				After 1986
Line	IPa		FWHMb	Intc			FWHMb	Intc
He II $\lambda$3203	24.6		800	394A			40	550B
He II $\lambda$2733			770	235A			61	326B
He II $\lambda$2511			790	215A			40	243B
He II $\lambda$2385			800	207A			48	300C
He II $\lambda$2307			740	143A			40	235C
He II $\lambda$1640			770	7370D			66	22 040E
C IV $\lambda$1550	47.9		tcp	tcp			45	24 420E
C IV $\lambda$1548			tcp	tcp			37	44 470E
N IV $\lambda$1718	47.5		680	1443D			<145	214F
N IV] $\lambda$1486			tcp	tcp			32	14 200E
N V $\lambda$1242	77.5		800	4168D			56	12 570E
N V $\lambda$1238			430	3529D			70	19 560E
O V $\lambda$2781	77.4		820	54A			38	29C
O V $\lambda$1371			860	424G			<83	473F
Ne III $\lambda$2678	41.0		480	128A			37	28C
Si IV $\lambda$1402	33.5		tcp	tcp			36	2439E
Si IV $\lambda$1393			tcp	tcp			37	3796E
S V $\lambda$1502	45.1		820	358G
S V] $\lambda$1199			770	480G			40	1066C
unid $\lambda$1266			550	858G
unid $\lambda$1260			700	1556G
unid $\lambda$1253			790	1469G

^a The ionization potential in eV of the next lower ion. ^b Given in km s^-1. ^c Peak intensity in units of 10^-14 erg cm^-2 s^-1 Å^-1. The indices on the measured intensities stand for: ^A As measured in LWR05596, ^B LWP28122, ^C LWP25995, ^D SWP02326, ^E SWP55055, ^F SWP47715, ^G SWP02334. tcp = Two component profile as the spectral line has a narrow emission component superimposed on the broad white dwarf wind profile.

3.1 Broad wind lines

In IUE spectra recorded before 1986 there are 22 emission lines with a FWHM larger than 600 km s^-1 (Table 4). These lines originate from abundant elements in higher ionization stages than for the narrow lines, and they are presumably formed in the hot white-dwarf wind. An analysis of some of these lines has yielded that the terminal velocity of the white-dwarf wind is $\sim$900 km s^-1 (Vogel & Nussbaumer 1994). A few of the lines are ground-state transitions (resonance lines) and show P Cygni structure while others are LS-allowed transitions having an excited lower level. In a few cases the transitions are spin-forbidden (intercombination lines). After 1986, when the broad wind lines were replaced by narrow emission (Fig. 2), it is notable that the six lines with highest peak intensity in the ${\it IUE}$ spectra (He II $\lambda$1640, C IV  $\lambda\lambda$1548, 1550, N IV] $\lambda$1486, N V $\lambda\lambda$1238, 1242) had broad line profiles in earlier spectra.

He⁺ has a low ionization energy compared to the other emitting ions detected in the white-dwarf wind, which is why the He II lines can be considered as recombination lines. The He II lines with wavelengths in the range of ${\it IUE}$ are Balmer $\alpha$, Balmer $\beta$, and the whole Paschen series except Pa$\alpha$. He II Balmer $\beta$ is close in wavelength to H Ly$\alpha$ and therefore totally absorbed. The He II lines detected in ${\it IUE}$ spectra of AG Peg are He II Balmer $\alpha$ and 13 consecutive Pashen lines starting with Pa$\beta$ and reaching upper levels with quantum numbers n=5-17. Only the second to the sixth lines can be detected from the noise before 1986 when the lines were broad.

Figure 2: The development of He II Balmer $\alpha$. The spectrum to the left (SWP02326) was recorded in 1978 and the spectrum to the right (SWP40148) was recorded in 1990. The large change in profile width is related to the change in origin for He II emission between those dates. In 1978 most of the He II emission originated from the white-dwarf wind while in 1990 the emission instead came from the heated part of the extended red-giant atmosphere.

For a few of the white-dwarf lines (C IV $\lambda\lambda$1548, 1558, N IV]1486, Si IV $\lambda$1402, Si IV $\lambda$1393) the development into narrow "nebular'' lines had already started in 1978, and the structure in the line profile, as shown in Fig. 3, is caused by the narrow line superimposed on the broad line. That the contribution of narrow emission lines occurred earlier for the ions of lower ionisation potential gives an idea into why the emission lines changed origin. As the white dwarf emerged at the end of the nova-like outburst the wind became less dense and more transparent for UV photons. The line intensities from the white-dwarf wind would then decrease at the same time that the material in the extended part of the red-giant atmosphere facing the white dwarf would be subjected to more of the white-dwarf UV radiation. The heated part of the red giant atmosphere became hotter and more ionised, resulting in the strong, narrow-emission lines. In recent ${\it FUSE}$ observations of AG Peg it is clear that the O VI resonance doublet still has contributions from the white-dwarf wind (Fig. 8). Since the ionisation energy of O VI is 114 eV its presence would be expected with a temperature increase in the white-dwarf wind, contrary to what is given by Zanstra determinations (Altamore & Cassatella 1997).

The O III Bowen lines were also broader than the nebular lines in early ${\it IUE}$ spectra. Like the white-dwarf lines discussed earlier the O III Bowen lines also evolved into narrower lines during the 1980s. The reason that they are not included in Table 4 is that they have less than half of the FWHM of the other broad line profiles and are formed in a different way (fluorescence). The Bowen lines are discussed in Sect. 3.3.

Figure 3: The IUE spectrum (SWP02334) of AG Peg, recorded in 1978, illustrates the difference in the profiles between lines from ions of ionisation energy near 40 eV and those of higher ionisation energy (around 70 eV). The N IV] $\lambda$1486 had a contribution from a "nebular line'' already in 1978 while all flux in the N V resonance doublet came from the white-dwarf wind.

3.2 The "nebular'' lines

A majority of the emission lines observed in IUE spectra of AG Peg have a FWHM between 10 and 50 km s^-1 and have had the same line profile although changed in intensity between 1978 and 1995. There is a wide range in ionisation energy for the narrow lines, from singly-ionised elements to more highly-ionised species such as Mg V, S IV and Fe V. Most of the emission lines correspond to LS-allowed transitions or intercombination lines but there are also a few parity-forbidden lines such as [Mg V] $\lambda$2928.

3.2.1 Narrow fluorescence lines

The process of photo-excitation by accidental resonance (PAR) can account for as many as 218 of the 585 identified lines in ${\it IUE}$ spectra of AG Peg. The Fe II levels y⁴H_11/2 and w²D_3/2 are known to be pumped by C IV $\lambda$1548 in at least eight symbiotic systems (Johansson 1983; Eriksson et al. 2001). The levels (⁵D)5p ⁶F_9/2 and (³F)4p ⁴G_9/2 are known to be pumped by H Ly$\alpha$ in the symbiotic star RR Tel (Johansson & Jordan 1984; Hartman & Johansson 2000) and they are involved in laser action in gas condensations of $\eta$ Car (Johansson & Letokhov 2004). In an analysis of AG Peg (Eriksson et al. 2003) 29 Fe II levels were shown to be populated by the PAR mechanism, and in the present work 11 newly identified pumped channels lead to a total of 40 presumably pumped Fe II levels, of which 22 are confirmed by three or more fluorescence lines (Table 5).

   

Table 5: Pumped Fe II channels confirmed by 3 or more fluorescence lines.

Pumping Line	Fe II channel	$\delta$ $\lambda^{a}$ (Å)	No.b
Si III] $\lambda$1892.03	a4P3/2-x4F5/2	0.15	6
Si III] $\lambda$1892.03	a4D7/2-z4G9/2	0.05	14
N IV $\lambda$1718.55	a6D3/2-z4G5/2	-0.45	6
O III] $\lambda$1666.15	a6D7/2-y4P5/2	0.03	4
O III] $\lambda$1660.81	a4F9/2-z2G9/2	0.03	5
He II $\lambda$1640.07	a4F3/2-y4G5/2	0.08	4
C IV $\lambda$1548.19	a4F9/2-y4H11/2	0.01	13
C IV $\lambda$1548.19	a4F7/2-y2D5/2	0.51	7
C IV $\lambda$1548.19	a4P1/2-w2D3/2	0.22	13
N IV] $\lambda$1486.50	a4G5/2-u4F3/2	-0.03	7
O IV] $\lambda$1401.16	a6D5/2-(3D)4p 4P3/2	-0.12	4
N V $\lambda$1242.78	a4F5/2-v2G7/2	-0.04	3
N V $\lambda$1238.80	a4P5/2-(4P)4s4p 4P5/2	-0.22	5
H I $\lambda$1215.67	a4D5/2-(b3P)4p 4S3/2	0.31	4
H I $\lambda$1215.67	a4D5/2-(5D)5p 4D5/2	0.18	6
H I $\lambda$1215.67	a4D1/2-(5D)5p 4D3/2	0.85	5
He II $\lambda$1084.94	a6D9/2-x4H7/2	0.96	4
He II $\lambda$1084.94	a6D9/2-x4H9/2	0.64	3
He II $\lambda$1084.94	a6D9/2-x4H11/2	0.05	3
He II $\lambda$1084.94	a6D9/2-u2G9/2	-0.01	3
He II $\lambda$1025.27	a4D1/2-(4F)4s4p 6F3/2	-0.17	5
He II $\lambda$933.45	a4F5/2-(3H)5p 4G7/2	-0.07	6

^a $\lambda_{\rm lab}$(pumped Fe II channel) - $\lambda_{\rm lab}$(pumping line).
^b Number of observed Fe II fluorescence lines from the pumped level.

Most of the spectral lines that pump (selectively excite) Fe II are formed in the white-dwarf wind. Since the profiles of those lines change as their origin evolves from being dominated by the white-dwarf wind to the heated part of the red-giant atmosphere (or wind) the emission from the pumped Fe II levels also changes after 1986. Fe II channels that are separated by more than 40 km s^{- 1} from their pumping line cannot be pumped by the narrow emission lines and therefore those lines disappeared after 1986 (Fig. 4). However, the Fe II fluorescence lines excited in channels that are close in wavelength to their pumping lines can be pumped by the narrow "nebular'' emission lines and they do appear in the spectrum throughout the lifetime of IUE. There are four lines from highly- ionised elements (Si III] $\lambda$1892, O III]  $\lambda\lambda$1660, 1666 and O IV] $\lambda$1401), which are not white-dwarf wind lines but still responsible for PAR processes in Fe II. These lines have in common that they are narrower than the other pumping lines, even compared to the FWHM after 1986, and that they, along with the corresponding fluorescence lines, did not change during the years 1978-1995.

In AG Peg H Ly$\alpha$ activates numerous Fe II channels resulting in fluorescence lines from both primary and secondary decays of the pumped levels. Lines from the (⁵D)5s levels (i.e. the e⁶D and e⁴D terms) are seen in the AG Peg spectrum. Those lines are also seen in RR Tel, where they are explained as secondary decay from H Ly$\alpha$ pumped (⁵D)5p levels (Hartman & Johansson 2000), and we conclude that the same explanation is valid for AG Peg. A consequence of the density decrease in the white-dwarf wind is that it becomes less dominant (less extended in the binary system) as well as less opaque so that the H II region can grow and more H Ly$\alpha$ radiation can reach the Fe⁺ ions. This leads to an increase of the intensity of the H Ly$\alpha$ pumped Fe II fluorescence lines (Fig. 5). It is interesting to note that the velocity shift is the same for the Fe II fluorescence lines but differs from the velocity shift of the lines from collisionally excited Fe II levels.

Figure 4: The total intensity of all Fe II lines from the upper level y2D5/2, which is pumped by the C IV $\lambda$1548.187 line through the channel a4F7/2-y2D5/2 at 1548.697 Å. When the broad foot of the C IV resonance lines vanished the activity in this channel stopped.

Figure 5: The strength of the $\lambda$2508.34 Fe II line representing the channel a4D7/2-(b3F) 4p 4G9/2 pumped by H Ly$\alpha$. As the temperature increased the H II region around the white dwarf became larger, which allowed more H Ly$\alpha$ to reach the Fe II regions.

We observe lines from Fe II levels that are not selectively photo-excited by strong lines. The population of these levels can in general be explained by collisional or recombination excitation (see later sections). However, we also observe emission lines from 21 Fe II levels of medium excitation energy ( ${\it EP}\approx 7$-8 eV), for which neither of the excitation mechanisms mentioned above is plausible. Absorption lines of Fe II at short wavelengths are observed, and they give an explanation to the population of seven of those 21 levels (Fig. 6). These are levels belonging to the LS terms y⁴D, z²F and x⁶P (except for y⁴D_1/2 and x⁶P_3/2), and they are photo-excited by continuum radiation from the white dwarf through the channels a⁴F-y⁴D, a⁴P-z²F and a⁶D-x⁶P. Only the strongest transitions between these terms are observed as absorption lines in AG Peg, probably due to the low continuum level.

Figure 6: Grotrian diagram of Fe II showing the levels involved in continuum fluorescence. The dotted lines are the pumped channels while the solid lines represent decay channels observed in AG Peg.

   

Table 6: Pumped channels in ions other than Fe II.

Pumping line	Pumped element	Pumped transition	$\lambda^{a}$ (Å)
O IV] $\lambda$1401.16	S I	3p4 3P2-(4S)5s 3S1	1401.51
N V $\lambda$1242.78	N I	2p3 2D5/2-(1D)3s 2D5/2	1243.18
N V $\lambda$1242.78	Co II	4s a5F3-4s4p y5P3	1242.49
H I $\lambda$1215.67	Co II	3d8 a3P2-(4F)5p 5D3	1213.26
H I $\lambda$1215.67	Fe III	3d6 5D4-(6S)4p 7P3	1214.57
H I $\lambda$1215.67	Fe III	3d6 5D4-(6S)4p 7P4	1213.45
continuumb	Co II	3d8 3F4-4p v3D3	1187.42

^a Wavelength of the pumped channel.
^b Absorption at 1187 Å is observed, which explains the presence
of emission from the Co II v³D₃ level.

The strong emission line $\lambda$1411.94 in AG Peg is identified as the 2p^{3 2}P_3/2-2p²3s ²D_5/2 transition of N I but no emission is detected from the 2p²3s ²D_3/2 level. We suggest that the level 2p²3s ²D_5/2 is selectively populated by being pumped by N V $\lambda$1242 in the absorption channel 2p^{3 2}D_5/2-2p²3s ²D_5/2. A similar case is $\lambda$1409.34, which is identified as a transition from the S I level (⁴S)5s ³S₁ having a high excitation energy (8.85 eV). We suggest the S I level is pumped by O IV] $\lambda$1401. Furthermore, two pumped channels in Co II and two in Fe III have been detected in the ${\it IUE}$ spectrum of AG Peg (Table 8).

3.2.2 Parity forbidden lines

Radiative transitions between levels of the same parity must be formed by magnetic dipole (M1) or electric quadrupole (E2) interaction, which means many orders of magnitude smaller transition probabilities than electric dipole (E1) transitions including a parity change. Observations of M1 and E2 radiation from an astrophysical plasma require that the density of the plasma is low enough so the radiative lifetime of the metastable state is smaller than the time scale for deexcitation by collisional quenching. Hence, the lines from the parity forbidden transitions originate from low density regions, such as from a nebula surrounding the system. In the IUE spectra of AG Peg, 14 parity-forbidden emission lines have been identified, originating from highly-ionised elements such as Ne V and Fe VI (Table 7). The ionisation energies are very high for the ions emitting M1 and E2 radiation, which implies that all parity-forbidden radiation originates from a thin plasma, heated and ionized by the UV radiation from the white dwarf. There is a difference among the forbidden lines in IUE spectra before and after 1986. Before 1986 only six of the 14 observed parity-forbidden lines were present, and they originated from the ions O²⁺, Ne²⁺ and Ne³⁺. No forbidden lines from higher ionisation stages were observed. After 1986 the forbidden emission from O²⁺ ([O III] $\lambda$2321.66) vanished and the emission from Ne²⁺ ([Ne III] $\lambda$1814.63) became weaker, while eight new emission lines from Ar⁴⁺, Ne⁴⁺, Mg⁴⁺ and Fe⁵⁺ appeared in the IUE spectrum.

   

Table 7: Parity forbidden lines observed in AG Peg.

Spectrum	Ionization	$\lambda_{\rm lab}$ (vac).	Shifta	Width	Transition	Aij	Noteb
	(eV)	(Å)	(km s-1)	(km s-1)		(s-1)
[Fe VI]	75.01	1957.28	bl	bl	3d3 2G7/2-3d3 2D15/2	0.91	$\uparrow$
		1944.30	17	20	3d3 2G7/2-3d3 2D13/2	12	$\uparrow$
[Mg V]	109.25	2928.0	bl	bl	2p4 3P1-2p4 1D2	0.55	$\uparrow$
		2783.50	bl	bl	2p4 3P2-2p4 1D2	1.90	$\uparrow$
		1324.45	45	20	2p4 3P1-2p4 1S0	23	$\uparrow$
[Ne V]	97.08	2975.66	152	51	2p2 1D2-2p2 1S0	2.60	$\uparrow$
		1575.18	124	84	2p2 3P1-2p2 1S0	4.20	$\uparrow$
[Ar V]	59.81	2692.02	41	40	3p2 3P1-3p2 1S0	6.80	$\uparrow$
[Ne IV]	63.46	2425.23	-6	18	2p3 4S3/2-2p3 2D5/2	0.00018	$\leftrightarrow$
		2422.60	-7	17	2p3 4S3/2-2p3 2D3/2	0.0053	$\leftrightarrow$
		1601.67	bl	bl	2p3 4S3/2-2p3 2P1/2	0.53	$\leftrightarrow$
		1601.50	bl	bl	2p3 4S3/2-2p3 2P3/2	1.33	$\leftrightarrow$
[Ne III]	40.96	1814.63	21	40	2p4 3P1-2p4 1S0	2.20	$\leftrightarrow$
[O III]	35.12	2321.66	49	25	2p2 3P1-2p2 1S0	0.22	$\downarrow$

^a $\frac{\lambda_{\rm lab} - \lambda_{\rm obs}}{\lambda_{\rm lab}} \cdot 3 \times 10^{5}$; ^b $\downarrow$ = Only observed before 1986, $\leftrightarrow$ = observed throughout 1978 to 1995, $\uparrow$ = only observed after 1986,
bl = blend.

3.2.3 Population by recombination or collisions

Emission lines from a particular ion can originate from different regions in the symbiotic system. Still, after discarding the emission lines that originated from the white-dwarf wind before 1986 as well as all fluorescence lines and parity-forbidden lines, the remaining emission lines from a specific ion have about the same velocity shifts. The widths of these remaining emission lines did not change during 1978-1995, but the relative shift between different ions was variable. In Table 3 all ions observed in AG Peg are listed with the number of corresponding emission lines that are formed by collision or recombination, excluding the white-dwarf wind emission lines. We will now give suggestions for how and where some of those lines are formed.

A) The helium 2s ³S₁- np ³P₂ series

Four emission lines from the He I 2s ³S₁-np ³P₂ series (n=5-8) are identified in the RR Tel spectrum Penston et al. 1983. In the IUE spectra of AG Peg recorded before 1986 there are no traces of He I emission. The broad He II emission lines from the white-dwarf wind before 1986 are presumably formed by recombination. Because of the high temperature and strong UV flux in the white-dwarf wind there is no neutral helium there. However, after 1986 seven He I emission lines of the series 2s ³S₁-np ³P₂ ( $5 \leq n \leq 11$) are present in the spectrum as "nebular'' lines with a mean FWHM of 35 km s^-1. The explanation of the He I emission is probably linked to the change of the He II lines from broad wind profiles to "narrow'' lines having an average FWHM of 49 km s^-1 (see Sect. 3.1). Kenyon et al. (1993) suggest that the presence of He I is caused by heating of the red-giant atmosphere by radiation from He⁺ ions in a region around the white dwarf. If He II in the white-dwarf wind is responsible for He I emission from the red-giant atmosphere, then the absence of He I lines before 1986 is a problem. Another suggestion is that when the white-dwarf wind became less dense during the transition period it was not able to produce broad He II emission enough to be observed by ${\it IUE}$, but at the same time more continuum radiation from the white dwarf reached the red-giant atmosphere, ionising helium to both He⁺ and He²⁺ (Fig. 7). This implies that after 1986 both the He I and He II emission lines are formed in the red-giant atmosphere facing the white dwarf.

Figure 7: Suggestion of the origin of broad He emission ( left) and narrow He emission ( right) before and after 1986 (see text).

B) The ns ²S-np ²P transitions in alkali-like spectra

It is only possible to detect the 2s ²S-2p ²P doublet transition for three species, C IV, N V, and O VI, within the wavelength regions covered by ${\it IUE}$ and ${\it FUSE}$. Atomic lithium and the ions Be⁺ and B²⁺ are too rare to be observed and for the three-electron systems heavier than oxygen the 2s-2p transition lies shortward of 900 Å. Two of the three observable doublets, C IV  $\lambda\lambda$1548.19, 1550.77 and N V $\lambda\lambda$1238.80, 1242.78 are observed as broad ($\sim$800 km s^-1) emission lines that evolve into narrow emission ($\sim$40 km s^-1) during the 1980s as discussed in Sect. 3.1. The O VI $\lambda$1031.92, 1037.614 resonance doublet is outside the range of ${\it IUE}$, but is observed with ${\it FUSE}$ (Fig. 8). Since ${\it FUSE}$ was launched in 1999 there have been no data on the O VI resonance doublet in AG Peg prior to the dramatic change of profile of the N V and C IV resonance doublets. However, at the base of the O VI resonance lines there are wings (FWHM $\sim$ 800 km s^-1, based on Gaussian fit of the line wings in the Q1110101 spectra) indicating that the O VI doublet evolved in the same way as the C IV and N V doublets. The peak intensity of the nebular components appears to have increased from 2001 (Q1110101) to the 2003 FUSE observation (Q1110103) while the intensity of the broad underlying wind-profile decreased slightly. This could mean that the same transfer of origin of the C IV resonance doublet at the end of 1970s to the beginning of the 1980s and the N V resonance doublet during the 1980s and beginning of 1990s (Eriksson et al. 2004) is now taking place for the O VI resonance doublet.

For the iso-electronic sequence of spectra involving 11 electrons the 3s ²S-3p ²P doublets are reachable with ${\it IUE}$ for three different elements (Mg II $\lambda\lambda$2796.35, 2803.53, Al III  $\lambda\lambda$1854.72, 1862.79 and Si IV $\lambda\lambda$1393.76, 1402.77), and one with ${\it FUSE}$ (P V $\lambda\lambda$1117.98, 1128.01). The P V resonance doublet is not detected in the FUSE data probably because of a low abundance of phosphorus in the red-giant atmosphere. Energetically it would be possible since the O VI resonance doublet is observed, and the ionisation potential of O V (113.9 eV) is higher than for P IV (51.4 eV). The Si IV resonance lines evolved in the same manner as the C IV and N V resonance lines and are discussed in Sect. 3.1. The Mg II resonance doublet (Fig. 8) is known to be common in the chromospheres of red-giant stars (Kondo et al. 1976) and is probably emitted all around the red giant atmosphere. Both the Mg II and Al III resonance doublets consist of narrow emission lines throughout 1978 to 1995 and have probably never been formed in the white-dwarf wind because of the low ionisation temperature required.

Figure 8: The ns 2S-np 2P doublets observed in AG Peg. The figures represent the profile of the resonance doublets after the transition period in the middle of the 1980s. The resonance doublets corresponding to n = 3 (Si IV, Al III, Mg II) and C IV almost completely consist of narrow components, while the N V and O VI resonance doublets still have detectable contributions from the broad white-dwarf wind profile.

C) The ns^{2 1}S-nsnp ³P transitions in alkaline-earth-like spectra

The spin-forbidden ns^{2 1}S-nsnp ³P transition includes two possible intercombination lines: ¹S₀-³P₁, which is often strong in emission in hot nebular spectra, and ¹S₀-³P₂. Since $\Delta J = 2$ for the latter line, it can only occur via a magnetic quadrupole transition, which has a very small transition probability. Similar to the observational restrictions for the 2s ²S-2p ²P transitions discussed in the previous subsection, the 2s^{2 1}S-2p ³P transitions can only be observed for C III], N IV] and O V]. The C III] $\lambda$1908.73 (¹S₀-³P₁) emission line is observed as strong ( $I \sim3.5 \times 10^{-11}$ erg cm^-2 s^-1 Å^-1) and narrow ( ${\it FWHM} \sim 35$ km s^-1) in all of the IUE observations. This is probably due to the ionization energy of C III, which is too low for C²⁺ ions to survive in the white-dwarf wind, but the ionisation potential of C II is not too high for C²⁺ to be produced in the heated part of the red-giant atmosphere. At the detection limit in the longest exposed spectra at 1906.67 Å there is a weak feature ( $I \sim 30 \times 10^{-13}$ erg cm^-2 s^-1 Å^-1), which can possibly be identified as the E2 (¹S₀-³P₂) transition of C III] blended with Mg IV.

The N IV] $\lambda$1486.50 (¹S₀-³P₁) emission line is a broad wind line before 1986 and is observed as a narrow emission line after 1986 as discussed in Sect. 3.1. Interestingly, the [N IV] M2 transition at 1483.32 Å is present throughout the ${\it IUE}$ observations but has a FWHM around 150 km s^-1, which is very different from the FWHM of N IV] $\lambda$1486.50 both before and after 1986. Since O V has a higher ionisation energy than N IV one would also expect the O V] $\lambda$1218.34 emission line to have evolved from a broad wind profile to a narrow nebular line. However, its relative closeness to H Ly$\alpha$ at 1215.67 Å causes absorption by the neutral hydrogen in the surrounding nebula and the O V] $\lambda$1218.34 line is absent before 1986. When the temperature of the white dwarf increased the H II region expanded further out into the surrounding nebula, making it more transparent for the O V] $\lambda$1218.34 emission, which after 1986 is observed as a strong emission line.

In the Mg I iso-electronic sequence of 12-electron ions the transition 3s^{2 1}S₀-3s3p ³P₁ is observed in four elements (Al II], Si III], P IV] and S V]). The S V] $\lambda$1199.04 feature evolved from a broad wind profile to a narrow nebular line during the 1980s, while Al II] $\lambda$2669.95, Si III] $\lambda$1892.03, and P IV] $\lambda$1467.43 are observed as narrow (FWHM $\sim$ 30 km s^-1) throughout the time interval 1978 to 1995. The intensity ratio I(¹S₀-³P₁)/I(¹S₀-³P₂) has been used in C III and N IV as a diagnostic tool to obtain electron densities in AG Peg Nussbaumer & Schild 1979,Nussbaumer & Schild 1981. The same transitions can be used for O V, Al II, Si III, P IV and S V to derive complementary information about the plasma. Understanding the origin of the ¹S-³P lines is therefore of great importance.

Figure 9: The intercombination multiplet 2s22p 2P-2s2p2 4P in N III] and O IV] spectra. The fine-structure component 3/2-5/2 is over-exposed in the N III] plot. The region of the N III] multiplet has not been observed by HST (GHRS) at high resolution. The dynamic range of ${\it IUE}$ was not sufficient to record spectra where the weakest N III] components are observable at the same time that N III] 3/2-5/2 is not over-exposed.

D) The excited (sp)^k 2<k<8 configurations

The more ionised an element is the more sensitive the average energy of a configuration is to the principal quantum number, n. Excited states in highly-ionized spectra, for which all electrons have the same n as the ground configuration, are therefore at relatively low excitation energies. As an example the LS term 2s2p^{2 4}P of C II is at $\sim$5.3 eV, while the LS term 2s2p3p ⁴P is at an energy of ($\sim$23.1 eV), i.e. more than a factor of four higher. Because of the low energy required for exciting the (sp)^k configurations they can be populated through collisions. Allowed emission lines from (sp)^k, 2<k<8, dominate the contribution from C II, N III, O IV, Si II, P II, P III, S II and S IV and they are also present in C III, N IV and O V. An intercombination transition, ns²np ²P-nsnp^{2 4}P, is specially strong in N III, O IV and S IV (Fig. 9), and is also present in the Si II spectrum. The metastable nsnp^{2 4}P is the lowest excited term in systems with five and 13 electrons and it can therefore only decay to the ground state, which explains why the corresponding multiplets are so strong. Those multiplets can be used for electron density diagnostics (Nussbaumer & Storey 1982; Nussbaumer & Storey 1979).

E) Emission lines from neutral atoms heavier than helium

Emission lines from NI, OI and SI are observed in the ultraviolet spectrum of AG Peg. Most of the emission lines from neutral elements are from allowed transitions to levels within the ground configuration, except for the ground state (Fig. 9). That the emitting gas is optically thick for transitions to the ground state indicates that the region of neutral elements is of relatively high density and low temperature (<3000 K). All of the four observed oxygen lines and five of the six observed sulphur lines correspond to transitions from np³(⁴S)n's ⁵S or ³S to the ground term np^{4 3}P. That the ³P-⁵S intercombination lines of S I $\lambda$1900.29 and O I $\lambda\lambda$1355.60, 1358.51 are observed is interesting since their transition probabilities are $\sim$10⁴ times smaller than for the ³P-³S transitions. This limits the electron density of the emitting region, presumably the outermost part of the surrounding nebula or the part of the red giant obscured from the white-dwarf emission.

Figure 10: The O I multiplet 2p4 3P-2p3(4S)3s 3S. The component 3P2-3S1to the ground level is in absorption while the other two fine-structure components are in emission.

F) Recombination to third, fourth and fifth ionization states

The population of some levels, from which emission is observed in AG Peg, cannot be understood by collisions or any pumping mechanisms. These include levels with very high excitation energy having no known decay channels that coincide with strong UV emission lines of other elements, and exotic configurations (doubly-excited and/or involving f-electrons) rarely populated in astrophysical plasmas. If an ion is emitting lines from doubly-excited levels or levels close to the ionization energy, recombination is the most plausible explanation. Based on this reasoning we suggest recombination as the excitation mechanism for some lines. The previous discussion of the strong 2s ²S-2p ²P transitions reveals a large abundance of C IV, N V and O VI in a hot region of AG Peg, implying that recombination to C III, N IV and O V is reasonable. Both C III and O V lines have been observed from levels rarely populated by collisions and are most certainly populated by recombination (such as 4f ³F₄ in C III and 5f ³F₄ in O V). Although the N V $\lambda\lambda$1238.80, 1242.78 doublet is almost as strong as the C IV resonance doublet none of the observed N IV lines originate from levels that require recombination excitation. However, the N IV] $\lambda$1486.50 emission line is one of the strongest lines in the ${\it IUE}$ wavelength range, indicating high presence of N³⁺ ions and the N III spectrum shows a few lines, such as N III $\lambda$1387.38, with upper level 4d ²D_3/2 presumably populated by recombination. Also, recombination lines of the third spectra, C III, N III and O III, were present throughout 1978-1995 and are formed in the extended red-giant atmosphere at a distance from the white dwarf sufficient to provide a temperature that gives a mixture of two and three times ionised elements.

The O V recombination lines first appeared after 1986. Before 1986, O⁵⁺ ions probably only existed in the white-dwarf wind, but after the transition period in the middle of 1980s O⁵⁺ ions were produced in the red-giant atmosphere by photo-ionisation, which explains the appearance of O V recombination lines. Four emission lines between 1669-1699 Å are identified as Mg IV lines corresponding to the multiplet (³P)3s ⁴P-(³P)3p ⁴D. These lines are the only observed Mg IV lines in the spectra of AG Peg, and the (³P)3p ⁴D term has an excitation energy of $\sim$75 eV. The population of these levels is likely to be due to recombination of Mg V 2p^{4 3}P in less dense parts of the surrounding nebula since only parity forbidden lines from Mg V are observed.

   

Table 8: The relative line strengths of the Fe II multiplet a⁶D-z⁶D.

Transition	$\lambda_{\rm vac}$(lab) (Å)	gAa	Ib
9/2-9/2	2600.17	2.39	0c
9/2-7/2	2586.65	0.37	0c
7/2-9/2	2626.45	0.75	1.23
7/2-7/2	2612.65	1.00	1.00
7/2-5/2	2599.15	0.32	0.39
5/2-7/2	2632.11	0.87	bl
5/2-5/2	2618.40	0.30	0.92
5/2-3/2	2607.87	0.45	0.61
3/2-5/2	2631.83	0.70	bl
3/2-3/2	2621.19	0.02	0.72
3/2-1/2	2614.61	0.37	0.47
1/2-3/2	2629.08	0.43	0.53
1/2-1/2	2622.45	0.12	0.52

^a The gA values from Schnabel et al. (2004) are scaled in such a way that gA for the a⁶D_7/2-z⁶D_7/2 transition is equal to 1.00.
^b The observed intensity relative to I(a⁶D_7/2-z⁶D_7/2) = 1.00.
^c Both transitions to the ground level a⁶D_9/2 are observed in absorption.

G) The Fe II (⁵D)4p levels

The lowest excited odd-parity levels in Fe II belong to the subconfiguration (⁵D)4p, which is built on the lowest parent term ⁵D of Fe III. This subconfiguration contains six LS terms (⁴P, ⁴D ⁴F, ⁶P, ⁶D and ⁶F) and accounts for 25 fine-structure levels. Transitions from (⁵D)4p are observed in the ultraviolet region to levels within the terms (⁵D)4s ⁶D, (⁵D)4s ⁴D, 3d^{7 4}F and 3d⁷ a⁴P forming strong Fe II multiplets. Since transitions from all the 25 levels are observed, collisional excitation is the most likely population process. However, the decay of the (⁵D)5s levels, populated by the cascading decay of the H Ly$\alpha$ pumped (⁵D)5p levels (see Sect. 3.2.1), causes deviations in the thermal population of (⁵D)4p. Thus, the observed line strengths within the (⁵D)4s-(⁵D)4p and 3d⁷-(⁵D)4p multiplets are different from what is expected from their gA-values, as measured by Schnabel et al. (2004) (Table 8). Also of importance is that the transition to the ground level (⁵D)4s ⁶D_9/2 is in absorption, which indicates that the optical depths also will influence the relative line strengths.

Figure 11: Figure demonstrating our idea of the excitation mechanism in Fe III and Fe II responsible for the observed octet transitions in Fe II. The presumed recombination channels are presented as dotted lines, the pumped channel as a double lines and the decay channels as solid lines. Only the levels involved in the process are plotted in this Grotrian diagram.

Figure 12: The three O III 2p3p 3S-2p3d 3P transitions in spectrum lwp25995. Whit the dynamical range of IUE it is not sufficient to observe the 3S1-3P0 transition without having the 3S1-3P2 transition saturated because of the large difference of intensity.

H) The octet levels in Fe II

Three emission lines ( $\lambda\lambda$1926.07, 1915.62 and 1887.83) have been identified as originating from the z⁸P term in Fe II, which has no spin-allowed decay channels. These three lines require an explanation since the Fe II octet transitions are very rare in stellar spectra. In fact, they have only been observed in the spectrum of the sun Johansson 1977.

If Fe III is to recombine to any octet level of Fe II by electron capture the metastable septet level (⁶S)4s ⁷S₃ of Fe III has to be populated. The PAR mechanism in Fe III results in population of the (⁶S)4p ⁷P levels. Furthermore, by the observed Fe III fluorescence lines at 1955.27, 1914.06 and 1895.46 Å corresponding to (⁶S)4s ⁷S-(⁶S)4p ⁷P transitions the metastable Fe III (⁶S)4s ⁷S₃ level is known to be populated. In Fig. 11 our suggestion of the process leading to the Fe II octet transitions is shown.

3.3 The O III Bowen lines

The first known PAR process was the pumping of O III through the channel 2p^{2 3}P₂-2p3d ³P₂ at 303.80 Å by He II Ly$\alpha$ at 303.78 Å Bowen 1934,1935. In the spectra of AG Peg emission lines corresponding to 2p3p ³S-2p3d ³P and 2p3p ³D-2p3d ³P transitions are observed, which concludes that the Bowen mechanism is active in the system. The possibility of allowed primary decays from 2p3d ³P to 2p3p ³P, which form emission lines around 3430 Å, is outside the ${\it IUE}$ range. However, all six possible emission lines corresponding to the secondary decays 2p3s ³P-2p3p ³P are observed and hence, the 2p3p ³P-2p3d ³P is certainly active. Also, two emission lines, O III $\lambda$3341.73, 3300.34 are observed as secondary decays from 2p3s ³P-2p3p ³S transitions.

It is not only the ³P₂ level that is populated by PAR in AG Peg, the two other fine structure levels, ³P₁ and ³P₀, are also populated through channels within 2p^{2 3}P-2p3d ³P between 303.41 Å and 303.80 Å (Eriksson et al. 2005). From the three emission lines corresponding to 2p3p ³S-2p3d ³P (Fig. 12) the relative population rate of the fine structure levels in 2p3d ³P can be estimated. The theoretical relative LS intensities for the transitions (³S₁-³P₂:³S₁-³P₁:³S₁-³P₀) are 100:60:20 and the observed relative intensities, which can not be measured exactly because of saturation of the strongest line, are 100: < 20: < 3. The population rate of ³P₁ and ³P₀ is less than for ³P₂ by a factor of at least 3 and 7, respectively.

When the observed Balmer $\alpha$ and Pashen lines of He II became narrower by a factor of $\sim$20 during the middle of the 1980s the He II Ly$\alpha$ pumped O III lines also changed in appearance. In spectra recorded in 1981 and earlier the FWHM of the Bowen lines was $\sim$120 km s^-1, which was a factor of $\sim$6 smaller than that of the white-dwarf wind lines but more than a factor of 3 broader than the emission lines from the nebula and the red-giant atmosphere. The FWHM of the O III Bowen lines then decreased and was $\sim$45 km s^-1 in the early 1990s. The widths of the emission lines associated with the white-dwarf wind in early ${\it IUE}$ spectra decreased more rapidly during the 1980s, and the Bowen lines were actually among the broadest UV emission lines in spectra of AG Peg in the early 1990s. After 1986 the net flux of the O III Bowen lines increased by $\sim$50%. This could mean that after the He II region changed location from the white-dwarf wind to the heated part of the red-giant atmosphere more He II emission was able to reach the O²⁺ ions.

3.4 A line list for AG Peg

All emission features observed in this work are listed in Table 13. Lines longward of 1980 Å were observed with ${\it IUE}$ (${\it LWP}$), the lines between 1170 and 1980 Å with ${\it IUE}$ (${\it SWP}$) and the lines below 1170 were observed with ${\it FUSE}$ ( ${\it LWRS}$ and ${\it MDRS}$). In order to make comparison of line strengths useful for lines within the wavelength range of each instrument all peak intensities and FWHM are tabulated as measured in the same spectra, LWP25995 for 1980-3350 Å, SWP47715 for 1170-1980 Å and Q1110101 for lines below 1170 Å, which we call the reference spectra. A few emission features are present in spectra other than the reference spectra. These features are marked with "oth'' in the first column in the table and no information about intensity or FWHM are given in Table 14. The reference spectra were selected as such since they have the lowest noise level, which has the disadvantage that the strongest lines are saturated and no information about peak intensity or FWHM can be given in Table 13. The saturated lines are marked by "oe'' in the second column. In Cols. 4-7 the identifications of the observed lines are presented. For the unidentified lines those columns are left blank. Features that are considered to be blended with unknown features are marked with the superscript "bl'' on the measured intensity in the second column. In Col. 8 we have noted the subsection to which the reader can refer for our suggestion of the process responsible for the formation of the feature. For the wavelength intervals covered by the ${\it HST}$ (GHRS) observations Col. 9 presents the intensities.

In Table 14 all of the emission lines absent in the reference spectra are given with the observed wavelengths (Col. 1), peak intensities (Col. 2) and widths (Col. 3). The identifications are given in Cols. 4-7 as in Table 13. Column 9 lists the spectra from which the lines were measured.

Table 15 lists all of the lines that were over-exposed in the reference spectra and is constructed in the same manner as Table 14.

Table 16 is a list of the absorption lines in AG Peg. The first column gives the observed wavelength. If the wavelength is superscripted with a; the line is measured in LWP09698, b; SWP15651 and c; SWP10454, while all other lines are measured in the reference spectra. The superscript "*'' means that the line is not measured in this work but that its presence is revealed by profile fitting of the N V and C IV resonance lines (Eriksson et al. 2004). The equivalent widths of the lines are given in Col. 2 and the identifications in Cols. 3-6. In Col. 7, IS stands for interstellar line and bl for line blended by unknown contributors.

4 Nature of the emission lines in symbiotic stars

4.1 White-dwarf wind lines

A question one might ask is whether the broad wind features associated with some of the lines between 1000 and 2000 Å in AG Peg (before 1986) are unique to this star or if they are common among the symbiotic stars. To answer this question the lines showing broad wind profiles in AG Peg were analyzed for the symbiotic stars listed in Table 2. It turned out that the widths of over 400 km s^-1 observed in AG Peg before 1986 are rare but not unique among these other systems, as it was observed for four of the nineteen selected symbiotic systems (PU Vul, T CrB, CH Cyg and EG And).

PU Vul is one of the symbiotic stars classified as symbiotic novae Vogel & Nussbaumer 1992, just like AG Peg. The Si IV $\lambda$1393 line shows a P Cygni profile with terminal velocity of 750 km s^-1, which is similar to the white-dwarf wind velocity of AG Peg (Eriksson et al. 2004). We suggest, therefore, that the broad lines in PU Vul can be explained by a fast wind from the white dwarf triggered by the slow nova outburst. EG And is known to have a fast ($\sim$500 km s^-1) wind from the white dwarf (Vogel 1993), which can explain the broad profiles underlying the narrower nebular lines in its spectrum. Interestingly, in 1995 the C IV $\lambda$1548 line displayed a P Cygni profile associated with a terminal velocity of only 114 km s^-1. We have not been able to explain this absorption component but modeling of the same line in AG Peg has revealed an absorption component. This is the collision region of the white dwarf and red giant winds associated with a terminal velocity of half the white dwarf wind velocity. This should be noticed since EG And also has a region where the winds from the two stars collide (Tomov 1995). More surprising are the broad lines in T CrB and CH Cyg, since the white dwarf in these systems is known to be accreting matter from the red-giant wind (Iijima 1982; Kenyon & Garcia 1986), and therefore no white-dwarf wind is expected. The argument of matter falling into the disk surrounding the white dwarf is further strengthened here as inverted P Cygni profiles are observed in the lines C IV $\lambda$1548 (both systems) and He II $\lambda$1640 (only in T CrB). Even if we cannot explain how the lines are broadened to over 700 km s^-1 the reason can be the infall of matter on the disk surrounding the white dwarf.

The 15 symbiotic systems with no trace of lines having FWHM greater than 400 km s^-1 can be divided into two distinct categories with respect to the lines showing broad wind profiles in AG Peg. For eight of the stars all of those lines have FWHM between 40 and 70 km s^-1, which is normal for most of the lines observed by ${\it IUE}$ in spectra of symbiotic stars. Such lines are called nebular lines and their origin being the red giant upper atmosphere irradiated by the white dwarf. For the remaining seven systems some of those emission lines have a FWHM between 110 and 140 km s^-1. Common to these latter systems is that they all have underwent outbursts which could lead to an outflow of matter from the white dwarf. In Table 9 the widths of five lines associated with the white-dwarf wind in a few of the symbiotic systems is given for 20 symbiotic systems.

   

Table 9: The nature of lines having white dwarf wind profile in AG Peg in symbiotic stars.

Object	He II $\lambda$1640	C IV $\lambda$1548	N IV $\lambda$1486	N V $\lambda$1238	Si IV $\lambda$1393	Comment
EG And	(tcp)	52 (s, pc)	36		34	B
CH Cyg	42 (s)	730 (pc*)		321	str	B
T CrB	573 (pc*)	821 (pc*)	320	788		B
PU Vul		166			982 (pc)	B
V1329 Cyg	159	226				b
Z And	113	64	67	114	69	N*
RX Pup	68	128 (s)	118	111	112	N*
HBV475	142	130				N*
R Aqr		112			110	N*
HM Sge	137	111	130	131	110	N*
AG Dra	110	58	41	70 (pc)	56	N*
RW Hya	64	56	55			N
SY Mus	66	67	36	58	39	N
BF Cyg	38	65 (s, pc)	65		69	N
CI Cyg	68	44	53	55	50	N
V1016 Cyg	65	65	51	52	64	N
RR Tel	70	68	39	51	43	N
AX Per	64	52	46	58	58	N
KX Tra	69	50	36	58	54	N
AG Pega	770	(tcp, pc)	(tcp)	800	(tcp)	B
AG Pegb	66	45		56	36	N

N) All five lines have FWHM less than 70 km s^-1.
N*) One, a few or all of the five lines have a FWHM between 120 and 150 km s^-1, which is significantly broader than for the majority of lines in their spectra.
b) Two of the five lines are observable in IUE spectra of V1329 Cyg, the widths of those lines are broader than for the stars denoted N* but narrower than 400 km s^-1.
B) Very broad lines (FWHM > 400 km s^-1) are observed as single lines or as narrow lines superimposed on broad sockets (str).
pc) P cygni profile.
pc*) Inverted P cygni profile.
tcp = Two component profile as the spectral line has a narrow emission component superimposed on the broad white dwarf wind profile.

4.2 Fe II fluorescence

From Sect. 3.2.1 it was clear that the Fe⁺ ions in AG Peg are subjected to radiation from both a high-temperature region and a cool region emitting H Ly$\alpha$. Also, in RR Tel Fe II fluorescence lines are observed, pumped both by lines from highly-ionized ions and by H Ly$\alpha$(Hartman & Johansson 2000). A study of fluorescence lines in symbiotic stars (Eriksson et al. 2004) indicated that the Fe II regions in stars associated with slow nova eruptions were pumped by both H Ly$\alpha$ and high-ionization lines resulting in numerous (>10) actively pumped Fe II channels. Other symbiotic stars (with no indication of slow nova eruptions) showed fewer fluorescence lines and no H Ly$\alpha$ pumping. A special case is those objects known to have an accreting hot component, whose spectra showed no Fe II fluorescence.

In the present study ultraviolet Fe II fluorescence lines have been searched for in the symbiotic stars listed in Table 2. The presence of the Fe II lines $\lambda\lambda$2507.55, 2509.10 in emission serves as an indication of H Ly$\alpha$ pumping, while lines from the C IV pumped Fe II levels (see Table 5) serve as indicators of an Fe II region subjected to radiation from a high-ionization region. Absence of fluorescence lines in IUE data of a symbiotic star is not a sufficient reason to conclude that there is no pumping of Fe II. The lower limit of the peak intensity, for a line to be detected with the ${\it IUE}$, is around $3 \times 10^{-13}$ erg cm^-2 s^-1. However, in systems where the (⁵D)4s-(⁵D)4p resonance transitions but still no Fe II fluorescence lines are observed fluorescence can be ruled out or assumed to play a negligible role. Therefore, a search for Fe II lines corresponding to the a⁶D-z⁶D and a⁶D-z⁶P multiplets, which normally form the strongest Fe II lines in the IUE wavelength domain, has been carried out. The results of this search are presented in Table 10.

Among the twenty symbiotic systems considered in this study six belong to the subgroup of symbiotic slow novae: AG Peg, HM Sge, PU Vul, RR Tel, PU Vul, V1016 Cyg and V1329 Cyg. Except for HM Sge, both H Ly$\alpha$ and C IV $\lambda$1548 pumping of Fe II occurs in these systems, as observed by Eriksson et al. (2004). Emission lines in HM Sge are, in general, one magnitude fainter than in other symbiotic novae and even the Fe II resonance lines cannot be observed in the IUE spectra. This anomaly for HM Sge could indicate that it has no significant Fe II region or that the S/N ratio of ${\it IUE}$ is not high enough to see the Fe II emission.

Three of the symbiotic systems (CH Cyg, CI Cyg and T CrB) are known to have accreting disks around their hot components. As pointed out by Eriksson et al. (2004) no Fe II fluorescence can be detected in those systems. However, the Fe II resonance lines are observed in CH Cyg, which implies that there might be a Fe II region but no fluorescence in symbiotic systems involving accretion onto the hot component.

It becomes more problematic when considering the results of the 11 "normal'' symbiotic stars, which do not belong to the subgroup symbiotic novae or show any sign of a disk. Four of those systems, BF Cyg, HBV475, AG Dra and KX Tra, have no detectable Fe II emission lines in the ${\it IUE}$ spectra, and they are in a way similar to the symbiotic nova HM Sge as regards Fe II. The systems RW Hya and R Aqr show Fe II fluorescence lines from levels pumped by high-ionization lines only. However, ${\it IUE}$ spectra of the systems EG And, SY Mus, Z And and RX Pup have Fe II lines from both C IV $\lambda$1548 and H Ly$\alpha$ pumped levels. Even if neither is designated as a symbiotic nova, recurrent outbursts have been observed for Z And (Tomov et al. 2003) and RX Pup (Mikolajewska et al. 1999). This could mean that the dynamics and structure of a symbiotic system change during the outbursts (both for recurrent and slow novae) so that emission from both highly-ionized regions and H I regions can reach the Fe⁺ ions. Then the group of symbiotic stars having numerous fluorescence lines (Eriksson et al. 2004) would be expanded to include all symbiotic stars associated with outbursts and not only symbiotic novae. A complication to this simple idea is that outbursts also have been observed in the symbiotic stars CI Cyg and AG Dra (Belczynski et al. 2000), which do not have numerous fluorescence lines. Since CI Cyg is, as discussed in the previous paragraph, a disk-system for which no Fe II fluorescence has been observed and AG Dra is known to be metal deficient, the lack of Fe II emission lines in these two systems is no surprise. Two normal symbiotic stars seem to fall outside the established groups: SY Mus, which emits Fe II fluorescence from both H Ly$\alpha$ and C IV $\lambda$1548 pumped levels, and AX Per, which is the only symbiotic star known to emit Fe II lines only from H Ly$\alpha$ pumped levels.

 

 

Table 10: Fe II emission in symbiotic stars.

	C IV	H Ly$\alpha$	(5D)4s-(5D)4p
Object	pumped	pumped	collisionally excited
AG Peg	yes	yes	yes
SY Mus	yes	yes	yes
Z And	yes	yes	yes
RX Pup	yes	yes	yes
V1016 Cyg	yes	yes	yes
RR Tel	yes	yes	yes
V1329 Cyg	yes	yes	no
PU Vul	yes	yes	no
EG And	yes	yes	no
CH Cyg	no	yes	yes
RW Hya	yes	no	no
AX Per	no	yes	no
R Aqr	no	no	yes
CI Cyg	no	no	no
HBV475	no	no	no
T CrB	no	no	no
HM Sge	no	no	no
AG Dra	no	no	no
BF Cyg	no	no	no
KX Tra	no	no	no

4.3 Forbidden lines

Forbidden lines indicate low density regions in astrophysical sources. In AG Peg, this low density region must be very hot since the forbidden lines belong to highly ionized atoms. As a check whether such a region with high temperature and low density is common in symbiotic stars a search was conducted for forbidden lines in the ${\it IUE}$ spectra of the other symbiotic stars. As indicators of lower temperature in the low density regions forbidden lines of N II, O I, O II and O III were selected. Forbidden lines of third to fifth spectra of the noble gases, as well as [Mg V] (observed in AG Peg) serve as indicators of high temperature. Also, the presence of [Mg VI] and [Mg VII] lines would imply an even higher temperature in the low density region than for AG Peg. A list of the forbidden lines searched for in the IUE spectra of all 20 selected symbiotic stars is given in Table 11.

Forbidden lines are detected in ${\it IUE}$ spectra for 14 of the 20 selected symbiotic stars (see Table 11). [Mg V] is seen in the spectra of eight of the symbiotic stars, and is the most frequently observed among the forbidden lines. There are four systems showing forbidden lines from magnesium: EG And, RW Hya, CH Cyg and R Aqr. EG And has forbidden lines from [O II], [Ar III] and [Ne III], RW Hya from [O III] and [Ar III], CH Cyg from [O III] and [Ar III] and R Aqr from [O II] and [O III] and [Ar III]. The absence of [Ar V] and [Ne V] in these four systems indicates that the temperature in the low density region is too low for the formation of Mg⁴⁺. The system AG Dra has only forbidden lines from [Mg VI] and [Mg VII]. The relative locations of the forbidden line regions within the symbiotic stars, and thereby the radiation field they are subjected to are poorly known. Therefore, a more detailed analysis of the forbidden line regions are not possible at this point. Assuming local thermal equilibrium, the forbidden lines observed can be explained by one region of one dominant temperature in 6 of the 14 systems showing forbidden lines (see Table 11).

   

Table 11: Forbidden lines searched for in 20 symbiotic stars.

$\lambda_{\rm vac}$ (Å)	Spectra	Config.a	Transition	Aij (s-1)	Nob.
3110.08	[Ar III]	3p4	3P1-1S0	4.02	3
3071.44	[N II]	2p2	3P2-1S0	1.4 $\times$ 10-4	3
3063.72	[N II]	2p2	3P1-1S0	0.032	1
3006.10	[Ar III]	3p4	3P2-1S0	0.043	1
2993.64	[Mg V]	2p4	3P0-1D2	6.7 $\times$ 10-5	2
2975.66	[Ne V]	2p2	1D2-1S0	2.60	2
2973.15	[O I]	2p4	3P1-1S0	0.075	1
2959.23	[O I]	2p4	3P2-1S0	2.4 $\times$ 10-4	1
2928.87	[Mg V]	2p4	3P1-1D2	0.55	8
2868.99	[Ar IV]	3p3	4S3/2-2P1/2	0.97	3
2854.48	[Ar IV]	3p3	4S3/2-2P3/2	2.55	4
2786.82	[Ar V]	3p2	3P2-1S0	0.081	0
2783.50	[Mg V]	2p4	3P2-1D2	1.90	8
2692.02	[Ar V]	3p2	3P1-1S0	6.80	4
2629.92	[Mg VII]	2p2	3P2-1D2	3.39	1
2509.98	[Mg VII]	2p2	3P1-1D2	1.30	1
2471.09	[O II]	2p3	4S3/2-2P3/2	0.052	6
2470.97	[O II]	2p3	4S3/2-2P1/2	0.021	6
2442.12	[Mg VII]	2p2	3P1-1D2	1.3 $\times$ 10-4	0
2425.15	[Ne IV]	2p3	4S3/2-2D5/2	4.1 $\times$ 10-4	3
2422.51	[Ne IV]	2p3	4S3/2-2D3/2	5.3 $\times$ 10-3	4
2418.20	[Mg V]	2p4	1D1-1S0	4.20	2
2332.11	[O III]	2p2	3P2-1S0	6.3 $\times$ 10-4	1
2321.66	[O III]	2p2	3P1-1S0	0.22	5
1814.63	[Ne III]	2p4	3P1-1S0	2.20	3
1806.49	[Mg VI]	2p3	4S3/2-2D5/2	3.2 $\times$ 10-3	2
1805.94	[Mg VI]	2p3	4S3/2-2D3/2	0.12	2
1793.70	[Ne III]	2p4	3P2-1S0	5.1 $\times$ 10-3	0
1601.67	[Ne IV]	3p3	4S3/2-2P1/2	0.53	4
1601.50	[Ne IV]	3p3	4S3/2-2P3/2	1.33	4
1592.27	[Ne V]	2p2	3P2-1S0	6.8 $\times$ 10-3	0
1574.77	[Ne V]	2p2	3P1-1S0	4.20	2

^a All forbidden lines in this table have the ground configuration for both upper and lower level.
^b The number of symbiotic stars where the lines were observed.

   

Table 12: Forbidden spectra in symbiotic stars.

Object	Spectra	comm.
Z And	O I, N II, Mg V
EG And	O II, Ne III, Ar III	*
R Aqr	O II+III, Ar III	*
T CrB
BF Cyg
CH Cyg	O II, Ar III
CI Cyg
AG Dra	Mg VI+VII	*
RW Hya	O III, Ar IV	*
SY Mus	Ar V, Mg V
AG Peg	O III, Ne III+IV+V, Ar V, Mg V
AX Per
RX Pup
HM Sge	O II, Ar IV, Ne IV, Mg V
RR Tel	N II, O II+III, Ar III+IV+V, Ne III+IV+V, Mg V+VI
KX Tra	Mg V+VI	*
PU Vul
V1016 Cyg	N II, O II+III, Ar IV, Ne IV, Mg V
V1329 Cyg
HBV475	Mg V	*

* All forbidden lines in the system can be explaind by a low density region
  in local thermal equilibrium and of one dominant temperature.

5 Summary

The ultraviolet spectrum of AG Peg is indeed complex. In terms of number of lines the emission spectrum is dominated by nebular lines. Overall, the lines reflect a variety of physical processes and locations. A few emission lines are associated with the red-giant chromosphere such as Mg II $\lambda\lambda$2803.53, 2796.35 which are the strongest lines between 2000 and 3000 Å. They have a self-absorbed structure, which is typical for resonance lines. In large contrast to the red giant chromospheric lines, the AG Peg spectrum also contains parity-forbidden lines from highly-ionized ions like Ne³⁺ and Mg⁵⁺. These forbidden lines originate in the thin outer nebula. As an indication of the complexity of the system, intercombination and allowed lines from highly ionized ions are also observed. Most of these lines, such as Si III] $\lambda$1892.03, are excited by collisions while a few lines like O V $\lambda$1506.76 are excited by recombination. These lines are formed in the heated part of the extended red-giant atmosphere. A large number of the lines in the AG Peg spectrum are fluorescence lines, for which location of formation is not well understood. Superimposed on the spectra of nebular lines are a few broad wind lines. These lines are from highly-ionized elements and those that decay to the ground level display a P Cygni profile, showing that they are formed in the white-dwarf wind. A segment of the line-list for AG Peg can be seen in Table 13.

 

 

Table 13: A sample of the AG Peg line list.

$\lambda_{\rm obs}$ (Å)	Ia	Wb	$\lambda_{\rm id}$ (Å)	Spec.	Lower level	Upper level	Secc	Excf
2837.13	652	43	2837.14	O III	2p3p 3D3	2p3d 3P2	3	fl
			7.10	O IV	2s2p(3P)3s 4P5/2	2s2p(3P)3p 4S3/2	unk
2836.43	46	24	2836.55	Fe II	4s b2P3/2	4p z4G5/2	2.1	fl
2833.91	50	56	2834.20	Fe II	4s a4D7/2	4p z6P5/2	2.3G	col
			3.92	Fe II	4p z6P5/2	5s e6D5/2	2.1	fl
2832.28	46	26	2832.40	Fe II	4s b2P3/2	4p z2D5/2		unk
Oth			2831.76	Fe II	4s b2G7/2	4p x4G5/2	2.1	fl
2829.82	59	34	2829.91	He I	2s 3S1	6p 3P2	2.3A	rec

During the 1980s the spectrum of AG Peg changed remarkably. Before 1986 six forbidden lines were observable in IUE spectra: [O III] $\lambda$2321.66, [Ne III] $\lambda$1814.63 and four [Ne IV] lines. After 1986 the [O III] line has disappeared while six new lines from four times ionized ions (Ar⁴⁺, Ne⁴⁺ and Mg⁴⁺) and two lines from Fe⁵⁺ are observed. An explanation for the change among the parity forbidden lines can be a temperature increase in the region emitting those lines. All of the 22 emission lines observed by IUE with ${\it FWHM} > 400$ km s^-1 before 1986 (the white-dwarf wind lines) partially or completely disappeared after 1986 and were replaced by narrow nebular lines. The transformation of the broad wind lines occurred first for the lines of lower ionization energies and later for lines of higher ionization energies. A continuous temperature increase in the white-dwarf wind during the 1980s would explain the order in which the white-dwarf wind lines disappeared, but the temperature of the white dwarf was according to Zanstra determinations constant during the same period (Altamore & Cassatella 1997). However, a temperature increase of the wind does not mean that the temperature of the white dwarf surface increased. Eriksson et al. (2004) showed that the opacity in the white-dwarf wind for two of the wind emission lines decreased, which means that more radiation from the white dwarf reaches further into the wind. A shell in the white-dwarf wind emitting, for example, C³⁺ emission moves outward in the white-dwarf wind until all C³⁺ ions in the wind are ionized to C⁴⁺.

A few of the lines which possessed wind profiles in the spectra before 1986 are shown to be pumping Fe II channels and are thereby the cause of many of the observed Fe II fluorescence lines. When the broad wind profiles disappeared in the 1980s, only the Fe II fluorescence lines corresponding to the closest coincidances remained while the other Fe II fluorescence lines vaniched.

Observations by ${\it FUSE}$ reveal that the O VI $\lambda$1031, 1037 doublet still showed a broad wind profile in 2001. The evolution of the fluorescence lines followed that of their pumping lines. As the broad wind lines vanished so did the fluorescence lines associated with channels too far apart in wavelength from the replacing nebular lines while the fluorescence lines with very close wavelength coincidences remained in the spectrum. Fe II fluorescence lines pumped by H Ly$\alpha$ became stronger during the 1980s, indicating growth of the H II region in the system.

Many of the emission lines in spectra of AG Peg have been and surely will continue to be used for various diagnostics. When establishing diagnostics, such as for determining temperatures or densities, it is crucial to understand the nature of the lines employed.

White-dwarf winds in symbiotic stars seem to be quite rare, since broad wind profiles only could be detected in five of the 20 symbiotic systems. In the beginning we suspected that such a wind was linked to the slow nova eruption that has occurred in some of these systems. This idea must be re-considered since only two, PU Vul and AG Peg, of the five systems having broad wind profiles belong to the subclass of symbiotic novae. For seven of the other 15 symbiotic stars the FWHM of the lines show wind profiles in AG Peg are between 110-140 km s^-1, while the FWHM of the same lines in the other eight symbiotic stars were 40-70 km s^-1.

Except for the total lack of Fe II emission lines in the IUE spectrum of HM Sge, Fe II fluorescence lines pumped by both H Ly$\alpha$ and C IV $\lambda$1548 were observed in the symbiotic novae. Even if Fe II fluorescence lines were observed in most symbiotic stars only four of the 14 symbiotic systems with no slow nova eruption known had Fe II pumped by both H Ly$\alpha$ and C IV. Three systems in our selection have suggested accretion disks around the hot component. The spectra of these three systems showed no signs of Fe II fluorescence. During slow nova eruptions the cool H I region and a region hot enough to create ions like C³⁺ simultaneously are in the line of sight with the large region with Fe⁺ ions, while this rarely is the case for symbiotic systems under "normal'' conditions.

Acknowledgements

All of the data presented in this paper were obtained from the Multimission Archive at the Space Telescope Science Institute (MAST). STScI is operated by the Association of Universities for Research in Astronomy, Inc., under NASA contract NAS5-26555. Support for MAST for non-HST data is provided by the NASA Office of Space Science via grant NAG-7584 and by other grants and contracts. We are grateful to the anonymous referee for a careful reading of the manuscript.

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6 Online Material

   

Table 13F: All emission lines observed in AG Peg.

$\lambda_{\rm obs}$ (Å)	Ia	wb	$\lambda_{\rm id}$ (Å)	spec.	Lower level	Upper level	Secc	Excf	$I_{\rm ghrs}^{d}$	$w_{\rm ghrs}^{e}$
3341.62	996	40	3341.73	O III	2p3s 3P2	2p3p 3S1	3	fl
3311.70	171	21	3311.97	Fe II	4s2 c4D5/2	(5D)5p 4D5/2	2.1	fl
Oth			3300.34	O III	2p3s 3P0	2p3p 3S1	3	fl
3299.10	292	17
3297.84	168	18	3297.72	He I	1s2s 1S1	1s8p 1P1	2.3A	rec
3296.86	136	20	3296.77	Fe II	4s a4D3/2	4p z6D3/2	2.3G	col
3255.69	205	38
3249.08	225	39
3245.18	126	18	3245.44	Fe II	3d7 d2D3/2	4p w2D3/2	2.1	fl
3244.66	121	20	3244.66	Fe II	4s c2G9/2	4p z2F7/2		fl
3203.97	991	61	3204.02	He II	n=3	n=5	1	rec
3163.86	97		3164.01	Fe II	3d7 a4P5/2	4p z4F5/2	2.3G	col
3162.72	91	23	3162.89	Fe II	3d7 a4P3/2	4p z4F3/2	2.3G	col
3157.15	71	42
3154.96	133		3155.12	Fe II	4s b2G9/2	4p z2G9/2	2.1	fl
3136.1	160	91
3133.64	oe		3133.70	O III	2p3p 3S1	2p3d 3P2	3	fl
3122.43	628	45	3122.54	O III	2p3p 3S1	2p3d 3P1	3	fl
3117.23	112	36
3116.47	82	38	3116.58	O III	2p3p 3S1	2p3d 3P0	3	fl
3079.41	55	25	3079.57	Fe II	4p z4P5/2	5s e4D7/2	2.1	fl
3072.44	50	21	3072.49	O IV	3s 2S1/2	3p 2P1/2		rec
3072.05	44	19	3072.02	Fe II	4p z4P1/2	5s e4D3/2	2.1	fl
3064.23	75		3064.32	O IV	3s 2S1/2	3p 2P3/2		rec
3060.09	131		3060.17	O III	2p3s 3P2	2p3p 3P1	3	fl
Oth			3049.88	Fe II	4p z4P3/2	5s e4D3/2	2.1	fl
3047.98	oe		3047.99	O III	2p3s 3P2	2p3p 3P2	3	fl
3043.81	90	32
3040.62	32		3040.67	Fe II	4s2 c4D3/2	4p u4F3/2	2.1	fl
3036.23	53		3036.30	O III	2p3s 3P1	2p3p 3P1	3	fl
3034.26	32		3034.33	Fe II	4p z4P3/2	5s e4D1/2	2.1	fl
3030.6	35bl		3030.57	Fe II	4s c2G9/2	4p y4H11/2	2.1	fl
3025.74	78
3025.36	94		3025.42	O III	2p3s 3P0	2p3p 3P1	3	fl
3024.26	217	50	3024.31	O III	2p3s 3P1	2p3p 3P2	3	fl
3003.36	128bl	32	3003.52	Fe II	3d7 a4P3/2	4p z4P5/2	2.3G	col
2989.89	45	29	2989.94	Fe II	4p z4F5/2	5s e6D5/2	2.1	fl
2988.36	66	35
2986.38	66		2986.51	Fe II	4p z4F7/2	5s e6D7/2	2.1	fl
			6.42	Fe II	3d7 a4P1/2	4p z4P3/2	2.3G	col
2985.63	163		2985.96	Fe II	4s2 d4P5/2	(5D)5p 4P5/2	2.1	fl
			5.70	Fe II	3d7 a4P5/2	4p z4P5/2	2.3G	col
2984.54	149	48	2984.65	O III	2p3s 1P1	2p3p 1D2	2.3F	rec
2980.1	108		2980.22	Fe II	4s a4D1/2	4p z6F3/2	2.3G	col
			0.19	Fe II	4s2 d4P3/2	(5D)5p 4D3/2	2.1	fl
2979.87	220		2979.95	Fe II	4s c2F5/2	4p w2D3/2	2.1	fl
2977.23	39		2977.26	Fe II	4s a2I13/2	4p y4H11/2	2.1	fl
2976.71	46		2976.81	Fe II	4s a4D1/2	4p z6F1/2	2.3G	col
2974.15	103	51	2975.66	[Ne V]	2p2 1D2	2p2 1S0	2.2	col
2971.23	97	30	2971.38	Fe II	4s a4D3/2	4p z6F5/2	2.3G	col
2970.66	26		2970.80	Fe II	4s b2G7/2	4p z2F5/2		fl
2965.6	64		2965.90	Fe II	3d7 a4P3/2	4p z4P3/2	2.3G	col
			5.53	Fe II	4s a4D3/2	4p z6F3/2	2.3G	col
			5.49	Fe II	3d7 a4P1/2	4p z4P1/2	2.3G	col
2962.05	41		2962.14	Fe II	4s a4D3/2	4p z6F1/2	2.3G	col
2960.47	61	38	2960.56	O III	2p3p 1P1	2p3d 1D2	2.3F	rec
2954.55	130	23	2954.64	Fe II	4s a4D5/2	4p z6F7/2	2.3G	col
2949.95	62bl	32	2950.04	Fe II	4s b2G7/2	4p z2F7/2		fl
2948.40	86	28	2948.52	Fe II	3d7 a4P5/2	4p z4P3/2	2.3G	col
2945.9	113		2946.13	Fe II	4s a4D5/2	4p z6F5/2	2.3G	col
			5.97	He I	2s 3S1	5p 3P2	2.3A	rec
2945.17	74	26	2945.26	Fe II	3d7 a4P3/2	4p z4P1/2	2.3G	col
2940.23	51bl	37	2940.37	Fe II	4s a4D5/2	4p z6F3/2	2.3G	col
2937.23	184	36	2937.37	Mg II	3p 2P3/2	4s 2S1/2		unk
2935.02	43	29
2933.70	34	29
2931.74	99	30
2929.33	259		2929.49	Mg II	3p 2P1/2	4s 2S1/2		unk
2927.29	208		2926.44	Fe II	4s a4D7/2	4p z6F9/2	2.3G	col
			8.0	[Mg V]	2p4 3P1	2p4 1D2	2.2	col
2918.19	27		2918.32	Fe II	4s a4D5/2	4p z6P7/2	2.3G	col
2916.91	58	16	2917.01	Fe II	4s a4D7/2	4p z6F7/2	2.3G	col
2908.57	34		2908.71	Fe II	4s a4D7/2	4p z6F5/2	2.3G	col
2903.17	59	33
2895.86	51	23
2895.52	31	13	2895.63	Fe II	4s b4H9/2	4p z4H11/2	2.1	fl
2893.57	59	23	2893.68	Fe II	4s a4D3/2	4p z6P5/2	2.3G	col
2892.29	30
2891.84	50
2890.40	48bl	33	2890.53	Fe II	4p z4F3/2	5s e4D5/2	2.1	fl
2888.81	139	24	2888.94	Fe II	4s b2P3/2	4p y4P5/2	2.1	fl
2886.89	39	20	2887.08	Fe II	4s b2H11/2	4p z4G9/2	2.1	fl
2885.46	78	23	2885.61	Fe II	4p z4D5/2	5s e4D7/2	2.1	fl
2884.53	55bl	36	2884.56	Fe II	4s b2H11/2	4p z4H13/2		unk
2883.13	19bl		2883.04	Fe II	4p z4F7/2	5s e4D7/2	2.1	fl
2882.36	80	20
2881.60	42bl		2881.60	Fe II	4s a4D7/2	4p z6P7/2	2.3G	col
2876.08	100	26	2876.19	Fe II	4s a2F7/2	4p z2G9/2	2.1	fl
2869.66	75		2869.72	Fe II	4s a4D5/2	4p z6P5/2	2.3G	col
2865.89	52bl	69	2866.30	Fe II	4p z4F3/2	5s e4D3/2	2.1	fl
2865.13	51	36
2859.40	46bl		2859.47	Fe II	4p z4D1/2	5s e4D3/2	2.1	fl
2857.64	166	35	2857.75	Fe II	4p z4D7/2	5s e4D7/2	2.1	fl
2856.92	94	43	2857.22	Fe II	4p z6P5/2	5s e6D7/2	2.1	fl
			6.99	Fe II	4s a4G9/2	4p z4G9/2	2.1	fl
2852.53	120		2852.56	Fe II	4p z4F3/2	5s e4D1/2	2.1	fl
2850.45	44	22	2850.44	Fe II	4s a4G9/2	4p z4H11/2		unk
2849.11	57		2849.16	Fe II	4p z4F5/2	5s e4D3/2	2.1	fl
2848.81	44		2848.94	Fe II	4p z4D5/2	5s e4D5/2	2.1	fl
			8.61	Fe II	4p z6P3/2	5s e6D3/2	2.1	fl
2846.23	152	39	2846.43	Fe II	4p z4F7/2	5s e4D5/2	2.1	fl
			6.26	Fe II	4p z4D3/2	5s e4D3/2	2.1	fl
			6.22	Fe II	4s b4D5/2	4p x4F5/2	2.1	fl
2844.21	67	44	2844.31	Fe II	4s b4D3/2	4p x4F5/2	2.1	fl
			4.15	Fe II	4s b2H9/2	4p z4I9/2		unk
2841.34	51bl		2841.49	Fe II	4s b2P1/2	4p z2D3/2		unk
2840.26	241	24	2840.35	Fe II	4p z4F9/2	5s e4D7/2	2.1	fl
2838.91	49	22	2839.05	Fe II	4p z6P3/2	5s e6D1/2	2.1	fl
2837.13	652	43	2837.14	O III	2p3p 3D3	2p3d 3P2	3	fl
			7.10	O IV	2s2p(3P)3s 4P5/2	2s2p(3P)3p 4S3/2	unk
2836.43	46	24	2836.55	Fe II	4s b2P3/2	4p z4G5/2	2.1	fl
2833.91	50	56	2834.20	Fe II	4s a4D7/2	4p z6P5/2	2.3G	col
			3.92	Fe II	4p z6P5/2	5s e6D5/2	2.1	fl
2832.28	46	26	2832.40	Fe II	4s b2P3/2	4p z2D5/2		unk
Oth			2831.76	Fe II	4s b2G7/2	4p x4G5/2	2.1	fl
2829.82	59	34	2829.91	He I	2s 3S1	6p 3P2	2.3A	rec
2829.38	57	24	2829.46	Fe II	4s b2H11/2	4p z4I9/2		unk
2828.17	57	30	2828.26	Fe II	4s b2H11/2	4p z4I13/2		unk
2826.53	64bl	52	2826.58	Fe II	4s a4G11/2	4p z4G9/2	2.1	fl
2824.06	30		2824.16	Fe II	4s a4G11/2	4p z4H13/2		unk
2820.08	48	27	2820.17	Fe II	4s a4G11/2	4p z4H11/2		unk
2819.43	62		2819.53	O III	2p3p 3D2	2p3d 3P2	3	fl
2817.70	53	26	2817.92	Fe II	4p z6P5/2	5s e6D3/2	2.1	fl
oth
2810.49	134	46	2810.61	Fe II	4p z6P7/2	5s e6D7/2	2.1	fl
			0.49	O III	2p3p 3D2	2p3d 3P1	3	fl
2808.62	31		2808.73	O III	2p3p 3D1	2p3d 3P2	3	fl
2807.94	48bl		2808.00	Fe II	4s b4D5/2	4p y2D5/2	2.1	fl
2806.04	31		2806.15	Fe II	4s b4D3/2	4p y2D5/2	2.1	fl
2803.5	oe		2803.53	Mg II	3s 2S1/2	3p 2P1/2	2.3B	col
2799.60	34bl		2799.76	O III	2p3p 3D1	2p3d 3P1	3	fl
2798.72	283	29	2798.82	Mg II	3p 2P3/2	3d 2D5/2		unk
2796.3	oe		2796.35	Mg II	3s 2S1/2	3p 2P3/2	2.3B	col
2794.88	15		2794.96	O III	2p3p 3D1	2p3d 3P0	3	fl
2791.49	193	36	2791.60	Mg II	3p 2P1/2	3d 2D3/2		unk
2785.98	41		2786.12	Ne III	2p3(2D)3s 3D2	2p3(2D)3p 3D2	3.2F	rec
			6.01	Fe II	4p z6F11/2	5s e6D9/2	2.1	fl
			5.85	Fe II	3d7 a4F3/2	4p z6D3/2	2.3G	col
2783.91	363	113	2784.51	Fe II	4s b2H11/2	4p z2G9/2	2.1	fl
			3.50	[Mg V]	2p4 3P2	2p4 1D2	2.2	col
2781.68	29		2781.83	O V	2s3s 3S1	2s3p 3P2	1	rec
2780.02	44	31
2778.80	72
2778.45	53bl		2778.47	Ne III	2p3(2D)3s 3D3	2p3(2D)3p 3D3	3.2F	rec
2777.62	83	21	2777.73	Fe II	4p z6F7/2	5s e6D7/2	2.1	fl
2776.08	96	21	2776.16	Fe II	3d7 a4F5/2	4p z6D5/2	2.3G	col
2775.47	88	23	2775.55	Fe II	3d7 a4F7/2	4p z6D9/2	2.3G	col
2773.45	43	16	2773.55	Fe II	4s a4D5/2	4p z4D7/2	2.3G	col
2771.89	631	28	2772.00	Fe II	4s b2G9/2	4p y4H11/2	2.1	fl
2770.00	104	76	2770.17	Fe II	4s a4G11/2	4p z4I13/2		unk
			9.97	Fe II	4s a4G7/2	4p z2G9/2	2.1	fl
2768.21	90	30	2768.33	Fe II	4p z6F9/2	5s e6D7/2	2.1	fl
			8.23	Fe II	4p z6F3/2	5s e6D5/2	2.1	fl
2764.40	65	49	2764.62	He I	2s 3S1	7p 3P2	2.3A	rec
2762.59	41		2762.63	Fe II	4s a4D1/2	4p z4D3/2	2.3G	col
2760.01	69bl	35	2760.15	Fe II	3d7 a4F7/2	4p z6D7/2	2.3G	col
2756.44	153	29	2756.55	Fe II	4s a4D7/2	4p z4F9/2	2.3G	col
2755.60	57	33	2755.70	Fe II	4p z6F7/2	5s e6D5/2	2.1	fl
2753.96	56bl	42	2754.10	Fe II	4s b2H9/2	4p z2I11/2		unk
2752.66	39bl	57	2752.96	Fe II	4p z6F3/2	5s e6D3/2	2.1	fl
2751.77	29	23	2751.94	Fe II	4s b2P3/2	4p z2D3/2		unk
2751.36	32	16
2750.75	45	16
2750.07	137	47	2750.30	Fe II	4s a4D1/2	4p z4D1/2	2.3G	col
			0.13	Fe II	4s a4D5/2	4p z4F7/2	2.3G	col
			9.99	Fe II	4s a4D3/2	4p z4D3/2	2.3G	col
2747.74	118	24	2747.79	Fe II	4s a4D5/2	4p z4D5/2	2.3G	col
2747.22	123	22	2747.30	Fe II	4s a4D3/2	4p z4F5/2	2.3G	col
2745.03	39	13	2745.08	Fe II	3d7 a4F7/2	4p z6D5/2	2.3G	col
2743.94	93	42	2794.04	Fe II	4p z6F3/2	5s e6D1/2	2.1	fl
			4.01	Fe II	4s a4D1/2	4p z4F3/2	2.3G	col
2742.09	100	16	2742.21	Fe II	4s a2F5/2	4p y4G5/2	2.1	fl
2740.27	141	33	2740.36	Fe II	4s a4D7/2	4p z4D7/2	2.3G	col
2737.71	41	21	2737.78	Fe II	4s a4D3/2	4p z4D1/2	2.3G	col
2734.09	oe		2734.10	He II	n=3	n=6	1	rec
2733.15	111	31	2733.26	Fe II	3d7 a4F9/2	4p z6D9/2	2.3G	col
2731.45	116	33	2731.54	Fe II	4s a4D3/2	4p z4F3/2	2.3G	col
2728.11	126	35	2728.35	Fe II	4s a4D5/2	4p z4D3/2	2.3G	col
			8.19	Fe II	4s a4G11/2	4p z2G9/2	2.1	fl
2725.60	103	21	2725.69	Fe II	4s a4D5/2	4p z4F5/2	2.3G	col
2723.92	38	24	2724.00	He I	2s 3S1	8p 3P2	2.3A	rec
2723.39	48	17	2723.43	Fe II	4s2 d4P3/2	(4P)4sp 4P5/2	2.1	fl
2722.77	43	17	2722.94	Fe II	4p z6P3/2	5s e4D1/2	2.1	fl
2719.33	68	71	2719.42	Fe II	4s a2F7/2	4p y4G5/2	2.1	fl
			9.42	Fe II	4s2 b4G5/2	(5D)5p 4D3/2	2.1	fl
			9.16	Fe II	4s c2P1/2	(b3P)4p 4P1/2	2.1	fl
2717.11	51	71	2717.34	Fe II	4s2 d4P5/2	(4P)4sp 4P5/2	2.1	fl
			7.02	Fe II	4s a2F5/2	4p z2F5/2		fl
2715.13	102	24	2715.22	Fe II	4s a4D7/2	4p z4D5/2	2.3G	col
2712.58	94	19
2709.90	49	46	2710.18	Fe II	4s a4D5/2	4p z4F3/2	2.3G	col
			9.86	Fe II	4s b2P3/2	4p y4D5/2		fl
2707.36	64	48	2707.37	Fe II	4s b2D5/2	4p y2P3/2		unk
			7.14	Fe II	4p z6P5/2	5s e4D3/2	2.1	fl
2704.77	36	21	2704.79	Fe II	4s a2F7/2	4p z2F7/2		fl
2698.14	48	33
2696.77	30	39	2696.92	He I	2s 3S1	9p 3P2	2.3A	rec
			6.91	N III	4s 2S1/2	5p 2P3/2	2.3F	rec
2693.54	70	28	2693.63	Fe II	4s a4D7/2	4p z4F5/2	2.3G	col
2691.65	101	40	2692.02	[Ar V]	3p2 3P1	3p2 1S0	2.2	col
2689.93	54bl	36	2690.01	Fe II	4s b2P3/2	4p y4D3/2		fl
2687.18	37bl		2687.27	Fe II	4s d2F7/2	4s4p x4H9/2	2.1	fl
2686.85	26	21	2686.95	O III	2s2p2(4P)3s 5P3	2s2p2(4P)3p 5S2	2.3F	rec
2683.24	86	19	2683.30	Fe II	4s d2F3/2	4p u2G9/2	2.1	fl
2681.56	50	34
2679.50	43	34	2679.44	Ne III	2p3(4S)3s 3S1	2p3(4S)3p 3P1	1	rec
2678.67	28		2678.70	Ne III	2p3(4S)3s 3S1	2p3(4S)3p 3P2	1	rec
2677.73	102	34	2677.93	He I	2s 3S1	10p 3P2	2.3A	rec
2675.20	90	21	2675.38	O III	2s2p2(4P)3s 5P2	2s2p2(4P)3p 5S2	2.3F	rec
2669.85	436	29	2669.95	Al II]	3s2 1S0	3p 3P1	2.3C	col
2667.35	56	24
2666.69	50	29
2664.89	46bl		2664.99	Fe II	4s b2H9/2	4p y4G11/2		unk
2664.01	76bl		2664.06	He I	2s 3S1	11p 3P2	2.3A	rec
2650.16	76	19	2650.26	Fe II	4s d2F5/2	4p u2G7/2	2.1	fl
Oth			2644.55	Fe II	4s2 b4G5/2	4p x4H7/2	2.1	fl
2639.03	85	52	2639.32	Fe II	4s2 b4G7/2	4p u2G9/2	2.1	fl
			9.01	Fe II	4s2 b4G9/2	4p x4H11/2	2.1	fl
2631.94	174	75	2632.11	Fe II	4s a6D5/2	4p z6D7/2	2.3G	col
			1.83	Fe II	4s a6D3/2	4p z6D5/2	2.3G	col
			1.80	Fe II	4s b4F7/2	4p z4G9/2	2.1	fl
2630.69	43	15	2630.86	Fe II	4s b4F3/2	4p z4G5/2	2.1	fl
2628.99	92	30	2629.08	Fe II	4s a6D1/2	4p z6D3/2	2.3G	col
2626.35	212	29	2626.45	Fe II	4s a6D7/2	4p z6D9/2	2.3G	col
2622.41	90	22	2622.45	Fe II	4s a6D1/2	4p z6D1/2	2.3G	col
2621.11	125	34	2621.19	Fe II	4s a6D3/2	4p z6D3/2	2.3G	col
2619.82	134bl	56	2619.86	Fe II	4s b4F9/2	4p z4G9/2	2.1	fl
2618.30	160bl	46	2618.40	Fe II	4s a6D5/2	4p z6D5/2	2.3G	col
2617.62	228	26
2614.60	82bl	69	2614.61	Fe II	4s a6D3/2	4p z6D1/2	2.3G	col
2612.56	173	29	2612.65	Fe II	4s a6D7/2	4p z6D7/2	2.3G	col
2611.83	80	34	2611.85	Fe II	4s a4D3/2	4p z4P5/2	2.3G	col
2610.79	54	22	2610.81	Ne III	2p3(2D)3s 3D3	2p3(2D)3p 3F4	3.2F	rec
2607.76	105	29	2607.87	Fe II	4s a6D5/2	4p z6D3/2	2.3G	col
2607.13	87	20
2605.68	208	25	2605.82	Fe II	4s c2F5/2	4p v2G7/2	2.1	fl
2599.05	68bl	50	2599.15	Fe II	4s a6D7/2	4p z6D5/2	2.3G	col
2596.34	470	27
2592.28	72bl	35	2592.32	Fe II	4s a4D5/2	4p z4P5/2	2.3G	col
2591.21	67bl	39	2591.33	Fe II	4s b4P3/2	4p y4P5/2	2.1	fl
2588.68	44	79	2588.95	O III]	2p3p 1P1	2p3d 3P1	3	fl
			8.72	Fe II	4s c2G7/2	4p x2H9/2	2.1	fl
Oth			2583.36	Fe II	4s a4D3/2	4p z4P3/2	2.3G	col
Oth			2581.94	Fe II	4p z2D5/2	5s f4F5/2	2.1	fl
2567.13	63	33	2567.26	O III]	2p3s 3P2	2p3p 1D2	2.3F	unk
2564.68	105	28	2564.80	Co II	4s b3F3	4p z3F4		unk
2564.23	42bl		2564.25	Fe II	4s a4D5/2	4p z4P3/2	2.3G	col
2563.17	90	20	2563.30	Fe II	4s a4D7/2	4p z4P5/2	2.3G	col
2558.00	58	70	2558.27	Fe II	4s b4F9/2	4p y4D7/2		fl
			7.92	Fe II	4s b4F3/2	4p z2D3/2		unk
			7.85	Fe II	4s a4H7/2	4p z4G9/2	2.1	fl
2550.49	102	20	2550.54	Fe II	4s a2F7/2	4p x4F5/2	2.1	fl
Oth			2549.69	Fe II	4s a2I11/2	4p x2H9/2	2.1	fl
2549.26	111	25	2549.36	Fe II	4s a4H9/2	4p z4G9/2	2.1	fl
2542.50	126	20	2542.60	Fe II	4s a4H7/2	4p z4G5/2	2.1	fl
			2.58	Si III	3p 1P1	3p2 1D2		unk
2539.40	122	20	2539.56	Fe II	4s a4H11/2	4p z4G9/2	2.1	fl
Oth			2539.35	Fe II	4s a2F5/2	4p y2D5/2	2.1	fl
2538.03	76	31	2538.13	Fe II	3d7 a4F5/2	4p z6F7/2	2.3G	col
			7.90	Fe II	4p z6D9/2	5s e6D9/2	2.1	fl
2537.43	64	30	2537.61	Fe II	4s a4H11/2	4p z4H13/2		unk
			7.57	Fe II	4s a4H9/2	4p z4H9/2		unk
2534.49	241	26
2531.75	89	27	2531.85	Fe II	3d7 a4F5/2	4p z6F5/2	2.3G	col
2530.94	111	24
Oth
Oth			2527.06	Fe II	4s b4P5/2	4p y4P5/2	2.1	fl
2526.60	133	15	2526.68	Fe II	4p z6D7/2	5s e6D7/2	2.1	fl
2525.87	48bl	38	2526.15	Fe II	4s a4H13/2	4p z4H13/2		unk
2524.87	120	20	2524.87	Si I	3p2 3P1	3p4s 3P0	2.3E	unk
2519.70	77	33	2519.96	Si I	3p2 3P1	3p4s 3P1	2.3E	unk
			9.86	Fe II	3d7 a4F7/2	4p z6F9/2	2.3G	col
			9.81	Fe II	4s a2F7/2	4p y2D5/2	2.1	fl
2516.79	133	38	2516.87	Si I	3p2 3P2	3p4s 3P2	2.3E	unk
			6.75	Fe II	3d7 a2D3/2	4p z4G5/2	2.1	fl
2513.96	101bl	36	2513.91	Fe II	4p z6D9/2	5s e6D7/2	2.1	fl
2512.57	73bl		2512.81	C II	2s2p2 2P3/2	2p3 2D5/2	2.3D	unk
2511.89	529	61	2511.96	He II	n=3	n=7	1	rec
2509.77	32bl		2509.88	C II	2s2p2 2P3/2	2p3 2D3/2	2.3D	unk
2509.02	843	23	2509.10	Fe II	4s c4F7/2	(3F)4p 4G9/2	2.1	fl
2507.46	336		2507.65	Si I	3p2 3P1	3p4s 3P2	2.3E	unk
			2507.55	Fe II	4s b4F7/2	(5D)5p 6F9/2	2.1	fl
2507.13	192bl		2507.19	Fe II	4s c4F9/2	(3F)4p 4G9/2	2.1	fl
2506.70	62	23	2506.85	Fe II	4s a4G9/2	4p x4G9/2		unk
2505.94	56	30	2505.97	Fe II	3d7 a4F7/2	4p z6F5/2	2.3G	col
2498.55	134	16	2498.57	Fe II	4s a4G5/2	4p x4G5/2		unk
2493.94	106	49	2494.05	Fe II	3d7 a4F9/2	4p z6F11/2	2.3G	col
			4.02	Fe II	4s a4H13/2	4p z4I15/2		unk
			3.98	Fe II	4s a4G7/2	4p x4G5/2		unk
			3.94	Fe II	4s a4H11/2	4p z4I13/2		unk
2493.02	675	34	2493.10	Fe II	4s b2H9/2	4p y4H11/2	2.1	fl
2484.91	143bl	35	2484.95	Fe II	3d7 a4F9/2	4p z6F9/2	2.3G	col
2484.39	80	28	2484.47	Fe II	4s c2G7/2	4p w2H9/2		unk
2483.74	73	21
2482.98	579	29	2483.08	Fe II	4s c2D3/2	4p w2D3/2	2.1	fl
2481.70	628	23	2481.80	Fe II	4s b2H11/2	4p y4H11/2	2.1	fl
2479.90	366	23	2479.98	Fe II	4s c2D5/2	4p w2D3/2	2.1	fl
2476.96	50	25	2477.01	Fe II	4s a4H7/2	4p z2G9/2	2.1	fl
2474.06	61bl	39	2474.20	Fe II	4s c4P5/2	(b3P)4p 4S3/2	2.1	fl
2473.53	101bl	34	2473.66	Fe II	4s c4P5/2	(5D)5p 4D5/2	2.1	fl
2471.06	119	16	2471.15	Fe II	3d7 a2H11/2	4p z4G9/2	2.1	fl
2470.23	57bl	47	2470.26	Fe II	4s b4D7/2	(3D)4p 4P5/2		unk
Oth			2464.76	Fe II	4s a4G9/2	4p x4F7/2	2.1	fl
2459.65	87		2459.72	Fe II	4s b4D5/2	(3D)4p 4P3/2	2.1	fl
2459.46	721	28	2459.53	Fe II	4s a4G9/2	4p y4H11/2	2.1	fl
2458.23	121	26	2458.30	Fe II	4s b4D3/2	(3D)4p 4P3/2	2.1	fl
2457.68	111	29	2457.71	Fe II	4s c4P5/2	(5D)5p 4P5/2	2.1	fl
Oth			2455.71	O III	2p3s 1P1	2p3p 1S0	2.3F	rec
2448.43	140	23	2448.50	Fe II	4s a2I11/2	4p w2H9/2		unk
Oth			2437.94	Fe II	4s a4G7/2	4p y2D5/2	2.1	fl
2436.89	582	21	2436.96	Fe II	4s a4G11/2	4p y4H11/2	2.1	fl
Oth			2435.69	Fe II	4s b4F3/2	4p y4G5/2	2.1	fl
			5.66	Ne III	2p3(2D)3s 1D2	2p3(2D)3p 3P2	2.3F	rec
Oth			2429.98	Ne III	2p3(2D)3s 1D2	2p3(2D)3p 3P1	2.3F	rec
2427.85	64bl	32	2427.93	Fe II	3d7 a2H11/2	4p z4I13/2		unk
Oth			2426.42	Fe II	4s b2P3/2	4p y2D5/2	2.1	fl
Oth			2425.23	[Ne IV]	2p3 4S3/2	2p3 2D5/2	2.2	col
Oth			2422.60	[Ne IV]	2p3 4S3/2	2p3 2D3/2	2.2	col
2417.36	159	19
Oth			2413.67	Ne III	2p3(4S)3p 3P1	2p3(4S)3d 3D2	2.3F	rec
			3.47	Ne III	2p3(4S)3p 3P2	2p3(4S)3d 3D3	2.3F	rec
2411.36	84	40	2411.25	Fe II	4s a6D3/2	4p z6F5/2	2.3G	col
2407.85	220	17	2407.96	Fe II	4s c4P1/2	(3P)4p 4S3/2	2.1	fl
2399.87	166	16	2399.97	Fe II	4s a6D5/2	4p z6F5/2	2.3G	col
			2399.96	Fe II	3d7 a4F3/2	4p z4D5/2	2.3G	col
2396.28	172	20	2396.36	Fe II	4s a6D7/2	4p z6F9/2	2.3G	col
2395.47	94	38	2395.62	Fe II	3d7 a2H11/2	4p z2G9/2	2.1	fl
2392.19	134	28	2392.21	Fe II	3d7 a4F7/2	4p z4F9/2	2.3G	col
2389.34	73		2389.36	Fe II	4s a6D7/2	4p z6F7/2	2.3G	col
2386.08	332	49	2386.13	He II	n=3	n=8	1	rec
2383.96	90	24	2383.97	Fe II	3d7 a4F5/2	4p z4D5/2	2.3G	col
2379.91	68bl	62	2380.00	Fe II	3d7 a4F7/2	4p z4D7/2	2.3G	col
2362.18	130	28	2362.24	Co II	4s a5F1	4p z5D2		unk
2360.66	96	15	2360.68	Fe II	4s b2D3/2	4p w2D3/2	2.1	fl
2359.66	131bl	27	2359.83	Fe II	4s a6D3/2	4p z6P5/2	2.3G	col
2350.86	137	29	2350.89	Si II]	3p 2P3/2	3p2 4P1/2	2.3D	col
2348.93	116	24	2349.02	Fe II	4s a6D5/2	4p z6P5/2	2.3G	col
2347.98	224	56	2348.12	Co II	4s a5F2	4p z5D2		unk
			7.92	Fe II	3d7 d2D15/2	(b3P)4p 4S3/2	2.1	fl
2344.94	188	24	2345.00	Fe II	4s a6D1/2	4p z6P3/2	2.3G	col
2335.15	410	19	2335.12	Si II]	3p 2P1/2	3p2 4P1/2	2.3D	col
2333.49	109bl	33	2333.52	Fe II	4s a6D7/2	4p z6P5/2	2.3G	col
2326.77	463	25	2326.84	Co II	4s a5F3	4p z5D2		unk
2326.04	173	27
Oth			2321.66	[O III]	2p2 3P1	2p2 1S0	2.2	col
Oth			2316.46	Co II	4s c3F4	4p v3D3	2.1	fl
2315.57	141	25	2315.58	Fe II	4s c4F5/2	4p u4F3/2	2.1	fl
2311.97	282	25	2312.00	Fe II	4s c4F3/2	4p u4F3/2	2.1	fl
2306.85	355	49	2306.91	He II	n=3	n=9	1	rec
2297.49	512	25	2297.58	C III	2s2p 1P1	2p2 1D2		unk
2281.60	128	22	2281.73	Fe II	4s b4F9/2	4p y4H11/2	2.1	fl
2280.55	248	22	2280.62	Fe II	4s a6D7/2	4p z4F9/2	2.3G	col
Oth			2253.83	Fe II	4s a6D7/2	4p z4F7/2	2.3G	col
2253.34	388	29	2253.34	He II	n=3	n=10	1	rec
2228.01	270	20	2228.07	Fe II	4s a4H9/2	4p y4H11/2	2.1	fl
2220.51	487	28	2220.59	Fe II	4s a4H11/2	4p y4H11/2	2.1	fl
2215.31	150	39	2215.36	He II	n=3	n=11	1	rec
Oth			2211.81	Fe II	4s a4H13/2	4p y4H11/2	2.1	fl
2187.30	251	46	2187.29	He II	n=3	n=12	1	rec
Oth
2168.04	296	19	2168.11	Fe II	3d7 a2H11/2	4p y4H11/2	2.1	fl
2165.93	180		2165.93	He II	n=3	n=13	1	rec
Oth
Oth			2149.28	He II	n=3	n=14	1	rec
2142.43	237	25	2142.46	Fe II	4s b2F5/2	4p w2D3/2	2.1	fl
Oth			2136.03	He II	n=3	n=15	1	rec
Oth
Oth			2125.31	He II	n=3	n=16	1	rec
Oth			2122.12	Fe II	4s b4D3/2	4p w2D3/2	2.1	fl
Oth			2038.11	Fe II	4s c2P3/2	(4P)4sp 2S1/2	2.1	fl
Oth			2003.85	Fe II	4s c2P1/2	(4P)4sp 2S1/2	2.1	fl
Oth
1979.04	43	29
1978.60	43	24
1978.29	71	17	1978.51	Fe II	4s2 b4G9/2	(2I)4sp 4H11/2	2.1	fl
1975.36	129bl	35	1975.55	Fe II	3d7 a2G9/2	4p y4H11/2	2.1	fl
Oth			1975.07	Fe II	3d7 a2G7/2	4p y2D5/2	2.1	fl
1974.53	29bl	33	1974.83	Fe II	4s2 d4P3/2	(4F)4sp 6D5/2	2.1	fl
Oth			1973.78	Fe II	4s2 b4G9/2	(2I)4sp 4H9/2	2.1	fl
1973.32	18	20
Oth			1972.16	Fe II	4s2 b4G11/2	(2I)4sp 4H9/2	2.1	fl
1971.49	25bl	33	1971.63	Fe II	4s2 d4P5/2	(4F)4sp 6D5/2	2.1	fl
1970.83	15	20	1971.03	Fe II	3d7 a2D3/2	(3D)4p 4P3/2	2.1	fl
1970.58	17	17
1970.02	24	18	1970.36	Fe II	3d7 a4P3/2	4p z2F5/2		fl
1965.73	136	29	1965.92	Fe II	4s a2F5/2	4p w2D3/2	2.1	fl
1963.99	30	20
Oth			1957.28	[Fe VI]	3d3 2G7/2	3d3 2D15/2	2.2	col
Oth
Oth
Oth
1947.41	46	14	1947.64	Fe II	4s d2G9/2	(3H)5p 4G7/2	2.1	fl
1946.77	20		1947.00	Fe II	4s c4P5/2	(4D)4sp 4P3/2	2.1	fl
1944.19	20	20	1944.30	[Fe VI]	3d3 2G7/2	3d3 2D13/2	2.2	col
1943.33	19	17	1943.48	Fe III	(4G)4s 5G2	(4G)4p 5H3		unk
1941.86	26	20	1942.00	Fe II	3d7 b2F5/2	4p v2G7/2	2.1	fl
			1.90	Fe II	4s c2P3/2	(4F)4sp 6F3/2	2.1	fl
1940.55	20	22	1940.70	Fe II	4s d2F5/2	(4F)4sp 6F3/2	2.1	fl
1938.51	57bl	46	1938.77	Fe II	4s c2P3/2	(4D)4sp 2P3/2		unk
1934.30
1928.58	63	33
1928.01	38	26	1928.09	Fe III	(4G)4s 5G6	(4G)4p 5H5		unk
1926.07	57	23	1926.24	Fe II	4s a6D7/2	4sp z8P5/2	2.3H	rec
Oth
1922.91	123	80	1923.34	C III	2s3d 3D1	2s4f 3F2	2.3F	rec
			3.16	C III	2s3d 3D2	2s4f 3F3	2.3F	rec
			2.96	C III	2s3d 3D3	2s4f 3F4	2.3F	rec
			2.79	Fe III	(4G)4s 5G5	(4G)4p 5H6		unk
Oth
1919.96	19	30	1920.02	O III	2p3p 1D2	2p4s 1P1	2.3F	rec
Oth
1915.62	28	17	1915.79	Fe II	4s a6D7/2	4sp z8P7/2	2.3H	rec
1913.89	207	33	1914.06	Fe III	(6S)4s 7S3	(6S)4p 7P3	2.1	fl
1912.72	22	27
1911.66	16	16	1911.72	Fe II	4s2 b4G7/2	(4F)4sp 6F5/2	2.1	fl
1911.37	30	16	1911.44	Fe II	4s2 b4G5/2	(4F)4sp 6F5/2	2.1	fl
1910.34	25bl	53	1910.77	Fe II	4s c2P1/2	(4F)4sp 6F3/2	2.1	fl
Oth			1909.91	Fe II	4s b4P5/2	4p y2P3/2		unk
1908.57	oe		1908.73	C III]	2s2 1S0	2s2p 3P1	2.3C	col
1907.03	41bl	31	1907.24	Fe II	4s a4G5/2	4p w2D3/2	2.1	fl
1906.67	19	30	1906.72	Mg IV	(3P)3s 4P3/2	(3P)3p 4P1/2	2.3F	rec
			6.68	C III]	2s2 1S0	2s2p 3P2	2.3C	col
1905.58	22		1905.68	Fe II	4s c2D5/2	(5D)5p 4D5/2	2.1	fl
1900.15	58	27	1900.29	S I]	3p4 3P2	4s 5S2	2.3E	col
1897.32	27	24	1897.55	Fe II	4s b2P3/2	4p w2D3/2	2.1	fl
			7.48	Fe II	4s a4D5/2	4p z2D5/2		unk
1895.31	87	35	1895.46	Fe III	(6S)4s 7S3	(6S)4p 7P4	2.1	fl
Oth			1894.29	C III	2s3p 1P1	2s4s 1S0	2.3F	rec
Oth			1893.89	Mg IV	(3P)3s 4P5/2	(3P)3p 4P5/2	2.3F	rec
1891.90	oe		1892.03	Si III]	3s2 1S0	3p 3P1	2.3C	col
1890.49	88	40	1890.66	Fe III	(4G)4s 5G6	(4G)4p 5F5		unk
1889.34	26	25	1889.45	Fe III	(4G)4s 5G3	(4P)4p 5D2		unk
1888.40	26	25	1888.52	P IV	3s3p 1P1	3p2 1D2		unk
1887.83	29	21	1888.01	Fe II	4s a6D9/2	4sp z8P9/2	2.3H	rec
1887.28	38bl		1887.45	Fe III	(4G)4s 5G3	(4G)4p 5F3		unk
1887.05	29bl		1887.20	Fe III	(4G)4s 5G4	(4G)4p 5F3		unk
1886.57	44	22	1886.76	Fe III	(4G)4s 5G5	(4G)4p 5F4		unk
1884.94	110	56	1885.22	N III	3d 2D5/2	4f 2F7/2	2.3F	rec
			5.09	Fe II	3d7 a4P5/2	4p x4F5/2	2.1	fl
			5.06	N III	3d 2D3/2	4f 2F5/2	2.3F	rec
1883.95	60	21	1884.12	Fe II	4s2 d4P3/2	(3F)5p 4D5/2	2.1	fl
Oth			1883.72	Fe II	4s a4D7/2	4p z4G5/2	2.1	fl
1882.02	35	24
Oth			1881.89	Fe II	4s a4D7/2	4p z2D5/2		unk
Oth			1881.25	Fe II	3d7 a2P1/2	(3D)4p 4P3/2	2.1	fl
1879.16	97	21
Oth
Oth			1877.02	Fe II	4s a4G5/2	4sp x6P7/2	2.1	fl
1874.82	32bl		1874.97	Fe II	4s a4D5/2	4p y4D7/2		fl
1874.55	33bl		1874.58	Mg IV	(3P)3s 4P5/2	(3P)3p 4P3/2	2.3F	rec
1872.44	99	48	1872.64	Fe II	4s2 b4G9/2	(2F)4sp 4G9/2	2.1	fl
			1872.57	Fe II	4s a2S1/2	(3P)4p 4S3/2	2.1	fl
1870.93	19	29	1871.08	Fe II	4s a4D3/2	4p z2D3/2		unk
1869.51	92	56	1869.82	Fe III	(4G)4s 5G3	(4G)4p 5F2		unk
			9.55	Fe II	4s2 b4G11/2	(2F)4sp 4G11/2	2.1	fl
1862.59	248	45	1862.81	Fe II	3d7 a2P3/2	(3D)4p 4P3/2	2.1	fl
			2.79	Al III	3s 2S1/2	3p 2P1/2	2.3B	col
1856.63	48	23
1854.53	338	55	1854.72	Al III	3s 2S1/2	3p 2P3/2	2.3B	col
Oth			1853.73	Co II	4s2 a5D2	(4F)5p 5D3	2.1	fl
1851.65	35	26
1851.33	30	18	1851.53	Fe II	4s a4D3/2	4p y4D5/2		fl
Oth
Oth			1850.20	Fe III	(4F)4s 5F4	(4F)4p 5D4		unk
Oth			1849.40	Fe III	(4F)4s 5F5	(4F)4p 5D4		unk
1847.32	37	21	1847.48	Fe II	4s a4D7/2	4p z2G9/2	2.1	fl
1843.10	47	21	1843.26	Fe II	4s2 b4G11/2	(4G)4sp 4G11/2	2.1	fl
1840.04	37	38	1840.25	Co II	4s2 a5D4	(4F)5p 5D4		unk
			0.06	Fe II	4s2 b4G7/2	(4G)4sp 4G5/2	2.1	fl
			0.00	Fe II	4s2 b4G7/2	(4G)4sp 4G7/2	2.1	fl
1839.63	54	41	1839.80	Fe II	4s2 b4G5/2	(4G)4sp 4G5/2	2.1	fl
			9.74	Fe II	4s2 b4G5/2	(4G)4sp 4G7/2	2.1	fl
1839.21	25	21	1839.27	Co II	4s2 a5D3	(4F)4p 5D3	2.1	fl
Oth			1836.72	N I]	2p3 2P3/2	3s 4P1/2	2.3E	col
			6.71	N I]	2p3 2P1/2	3s 4P1/2	2.3E	col
Oth			1835.57	N I]	2p3 2P1/2	3s 4P3/2	2.3E	col
Oth			1834.01	N I]	2p3 2P1/2	3s 4P3/2	2.3E	col
1831.80	171	25	1836.98	Fe II	4s2 b4G7/2	(4G)4sp 4H9/2	2.1	fl
1831.50	35bl		1831.66	Fe II	4s2 b4G9/2	(4G)4sp 4H9/2	2.1	fl
1829.85	34	26	1829.95	Fe V	(4P)4s 5P1	(4F)4p 5F2	2.3F	rec
1826.10	48	38	1826.25	S I	3p4 g3P0	4s 3S1	2.3E	col
1823.39	118	18
1820.18	28bl		1820.34	S I	3p4 g3P1	4s 3S1	2.3E	col
1817.22	191	31	1817.45	Si II	3p 2P3/2	3p2 2D3/2	2.3D	col
1816.75	962	31	1816.93	Si II	3p 2P3/2	3p2 2D5/2	2.3D	col
Oth			1814.63	[Ne III]	2p4 3P1	2p4 1S0	2.2	col
Oth
1810.15	30	20	1810.23	P II]	2p2 1S0	2s2p3 3P1	2.3D	col
Oth
1808.20	71	48
1807.76	92	27	1808.01	Si II	3p 2P1/2	3p2 2D3/2	2.3D	col
1807.07	26	15	1807.31	S I	3p4 g3P2	4s 3S1	2.3E	col
1805.44	46	32	1805.67	N III	3p 2P3/2	4s 2S1/2	2.3F	rec
1803.54	77	22	1803.82	S II]	3p3 2P1/2	3p4 4P1/2	2.3D	col
Oth			1795.57	Fe II	4s2 b4G7/2	(3H)5p 4G7/2	2.1	fl
			5.33	Fe II	4s2 b4G5/2	(3H)5p 4G7/2	2.1	fl
			5.27	Fe II	4s2 b4G9/2	(3H)5p 4G7/2	2.1	fl
Oth			1788.00	Fe II	4s2 a6S5/2	4sp x6P3/2	2.1	fl
1786.58	67	40	1786.82	Si II	3d 2D3/2	3p3 2D3/2	2.3D	unk
			6.75	Fe II	4s2 a6S5/2	4sp x6P5/2		fl
1785.12	108bl	55	1785.27	Fe II	4s2 a6S5/2	4sp x6P7/2	2.1	fl
Oth			1783.98	Fe II	4s b4D7/2	4sp y6F7/2	2.1	fl
Oth
1781.45	47	24	1781.51	Fe II	4s a4D7/2	4p y4G5/2	2.1	fl
1780.87	74bl	45	1780.95	Fe II	4s b4D5/2	4sp y6F7/2	2.1	fl
1779.65	51		1779.82	Fe II	4s c4P5/2	(4F)4sp 6F3/2	2.1	fl
1768.15	264	17
Oth			1760.82	C II	2s2p2 2D3/2	3p 2P1/2		col
Oth			1760.47	C II	2s2p2 2D3/2	3p 2P3/2		col
			0.40	C II	2s2p2 2D5/2	3p 2P3/2		col
Oth			1757.74	Fe II	4s c4P3/2	(4F)4sp 6F3/2	2.1	fl
1753.80	1482	19	1754.00	N III]	2p 2P3/2	2s2p2 4P1/2	2.3D	col
1753.32	79	36	1753.47	Mg II	3p 2P3/2	5s 2S1/2		unk
1752.03	515bl	41	1752.16	N III]	2p 2P3/2	2s2p2 4P3/2	2.3D	col
Oth			1751.66	N III	2s2p2 2P3/2	2p3 2D5/2	2.3D	unk
Oth			1750.66	Mg II	3p 2P1/2	5s 2S1/2		unk
1749.49	oe		1749.67	N III]	2p 2P3/2	2s2p2 4P5/2	2.3D	col
1748.51	960	24	1748.64	N III]	2p 2P1/2	2s2p2 4P1/2	2.3D	col
Oth			1747.85	N III	2s2p2 2P1/2	2p3 2D3/2	2.3D	unk
1746.61	64bl	45	1746.82	N III]	2p 2P1/2	2s2p2 4P3/2	2.3D	col
1745.08	136	36	1745.25	N I	2p3 2P3/2	3s 2P1/2	2.3E	unk
1742.60	39	34	1742.73	N I	2p3 2P3/2	3s 2P3/2	2.3E	unk
1737.40	63	50	1737.62	Mg II	3p 2P3/2	4d 2D5/2		unk
			7.33	Co II	4s a3D3	4sp y5P3	2.1	fl
1728.79	157bl	33	1728.85	Fe II	4s a4D3/2	4p x4F5/2	2.1	fl	37	34
1727.17	53	31	1727.38	Si IV	3d 2D3/2	4p 2P1/2		unk
Oth			1725.98	Fe II	3d7 a2D3/2	4sp x6P3/2		fl
1725.13	86	104	1725.36	Fe II	4s b2D5/2	(4P)4sp 4P5/2	2.1	fl
			5.02	Fe II	3d7 a2D25/2	4p w2D3/2	2.1	fl
			4.96	Fe II	3d7 a4F7/2	4p y4P5/2	2.1	fl
1722.41	94	56	1722.56	Si IV	3d 2D3/2	4p 2P3/2		unk
			2.53	Si IV	3d 2D5/2	4p 2P3/2		unk
Oth			1721.68	C II	2s2p2 2P3/2	2p3 2P3/2	2.3D	col
1720.96	39bl	40	1721.01	C II	2s2p2 2P1/2	2p3 2P1/2	2.3D	col
1720.64	33	19	1720.85	Ne V]	2p2 1D2	2s2p3 5S2	2.3D	col
1718.34	214	145	1718.55	N IV	2p 1P1	2p2 1D2	1	rec	107	145
			8.10	Fe II	3d7 a4F5/2	4p z4G5/2	2.1	fl
Oth			1713.00	Fe II	3d7 a4F7/2	4p z4G9/2	2.1	fl
Oth			1706.83	Fe II	4s c2G7/2	4sp x4H7/2	2.1	fl
1698.63	50	12	1698.78	Mg IV	(3P)3s 4P3/2	(3P)3p 4D5/2	2.3F	rec
1696.47	153bl	34	1696.79	Fe II	3d7 a4F9/2	4p z4G9/2	2.1	fl
1682.79	45	32	1683.00	Mg IV	(3P)3s 4P5/2	(3P)3p 4D7/2	2.3F	rec
1682.30	114	27	1682.37	Fe II	4p z4P1/2	(3F)4d 4P3/2	2.1	fl
1679.95	42	30	1679.96	Mg IV	(3P)3s 4P3/2	(3P)3p 4D3/2	2.3F	rec
1677.67	115	18	1677.84	Fe II	3d7 a2P1/2	4p w2D3/2	2.1	fl
1675.48	63	29	1675.71	Fe II	4p z4P3/2	(3F)4d 4P3/2	2.1	fl
1671.35	53	25	1671.42	Fe II	4p z4P5/2	(3F)4d 4P5/2	2.1	fl
1669.47	68	23	1669.57	Mg IV	(3P)3s 4P3/2	(3P)3p 4D1/2	2.3F	rec
1666.81	158	18	1666.69	S I	3p4 1D2	(2D)4s 1D2	2.3E	unk
1666.01	oe		1666.15	O III]	2p2 3P2	2s2p3 5S2	2.3D	col
1665.14	131	31
1660.61	oe		1660.81	O III]	2p2 3P1	2s2p3 5S2	2.3D	col
1640.07	oe		1640.35	He II	n=2	n=3	1	rec	8700	82
1625.45	97bl	35	1625.58	Fe II	4s b2F5/2	4p u4F3/2	2.1	fl
1613.83	63	39	1613.94	Fe II	4s b4D1/2	4p u4F3/2	2.1	fl
			3.84	Fe II	4s b4D3/2	4p u4F3/2	2.1	fl
1601.51	60	45	1601.67	[Ne IV]	2p3 4S3/2	2p3 2P1/2	2.2	col
			1.50	[Ne IV]	2p3 4S3/2	2p3 2P3/2	2.2	col
1601.18	71
1599.85	55	23	1600.01	Fe II	3d7 a2H9/2	4p v2G7/2	2.1	fl
1589.91	79	26
Oth			1588.29	Fe II	3d7 a4F3/2	4p x4G5/2	2.1	fl
1579.06	90	36
1577.84	125bl	49	1577.88	C III	2s3d 3D1	2p3d 3F2	2.3F	rec
1577.13	129	23	1577.30	C III	2s3d 3D2	2p3d 3F3	2.3F	rec
1576.37	153bl	48	1576.48	C III	2s3d 3D3	2p3d 3F4	2.3F	rec
1574.53	258	84	1575.18	[Ne V]	2p2 3P1	2p2 1S0	2.2	col
1565.72	118	35
1560.02	242	27	1560.25	Fe II	3d7 a4F7/2	4p x4F5/2	2.1	fl
1553.32	225	33							137	21
1550.65	oe		1550.77	C IV	2s 2S1/2	2p 2P1/2	1	col	7570	48
1548.11	oe		1548.19	C IV	2s 2S1/2	2p 2P3/2	1	col	11650	46
Oth			1538.63	Fe II	4s a4G5/2	(5D)5p 4D3/2	2.1	fl
1538.13	98	27	1538.16	Fe II	3d7 a4P5/2	4p w2D3/2	2.1	fl
1537.10	324	37	1537.37	Fe II	4s c2F5/2	(3H)5p 4G7/2	2.1	fl	129	25
			7.03	Fe II	4s c2F7/2	(3H)5p 4G7/2	2.1	fl
Oth			1534.05	O V	2p3p 1P1	2s4p 1P1	2.3F	rec
1533.25	390	35	1533.43	Si II	3p 2P3/2	4s 2S1/2		unk
Oth
1515.01	44	30	1515.23	Fe II	4s b2H11/2	4sp x4H11/2	2.1	fl
1514.20	135	30	1514.38	Fe II	4s a4G5/2	4sp x4H7/2	2.1	fl
1512.55	235	32	1512.69	Fe II	4s a4G7/2	4sp x4H7/2	2.1	fl
1506.75	144	52	1506.76	O V	2s4d 3D3	2s5f 3F4	2.3F	rec
1502.55	79	26	1502.69	Fe II	4s a4G5/2	4p u2G7/2	2.1	fl
Oth			1501.76	S V	3s3p 1P1	3p2 1D2	1	unk
1492.10	144bl	32	1492.26	Co II	4s a5P2	4sp y5P3	2.1	fl	125	24
1488.36	139	32	1438.38	Si I	3p2 1S0	3s3p3 1P1	2.3E	unk
1486.42	oe		1486.50	N IV]	2s2 1S0	2p 3P1	1	col	8290	38
1483.26	139	160	1483.32	[N IV]	2s2 1S0	2p 3P2	2.3C	col	73	301
1471.93	95	26	1471.94	Fe II	4p z6D5/2	(3F)4d 4P5/2	2.1	fl
Oth
1467.25	134	33	1467.43	P IV]	3s2 1S0	3p 3P1	2.3C	col
1464.68	84	29
1459.73	98	31
Oth			1457.76	Fe II	4s2 a6S5/2	(4D)4sp 6F3/2	2.1	fl
1445.59	82bl	62	1445.69	Fe II	4s a2S1/2	(4F)4sp 6F3/2	2.1	fl
1423.71	433	32	1423.79	S IV]	3p 2P3/2	3p2 4P1/2	2.3D	col
1422.37	137	25	1422.53	Fe II	4s b4D3/2	4p u4F3/2	2.1	fl
1416.77	582	40	1416.98	S IV]	3p 2P3/2	3p2 4P3/2	2.3D	col	235	36
1413.57	130	23	1413.70	Fe II	4s a4H11/2	4sp x4H11/2	2.1	fl	61	23
1411.77	1182	36	1411.94	N I	2p3 2P3/2	3s 2D5/2	2.1	fl	301	49
1409.15	106	92	1409.34	S I	3p4 3P1	(4S)5s 3S1	2.1	fl	60	51
			9.33	Co II	3d8 a3P2	4p v3D3		unk
1407.24	1630	51	1407.38	O IV]	2p 2P3/2	2s2p2 4P1/2	2.3D	col	854	42
1406.54	67	41
1405.90	1214	36	1406.08	S IV]	3p 2P3/2	3p2 4P5/2	2.3D	col	384	38
1404.65	oe		1404.80	O IV]	2p 2P3/2	2s2p2 4P3/2	2.3D	col	1350	41
			4.77	S IV]	3p 2P1/2	3p2 4P1/2	2.3D	col
1402.65	oe		1402.77	Si IV	3s 2S1/2	3p 2P1/2	1	col	579	49
1401.04	oe		1401.16	O IV]	2p 2P3/2	2s2p2 4P5/2	2.3D	col	3870	41
1399.61	1723	47	1399.78	O IV]	2p 2P1/2	2s2p2 4P1/2	2.3D	col	1030	41
1397.96	58		1398.13	S IV]	3p 2P1/2	3p2 4P3/2	2.3D	col
1397.08	385	34	1397.23	O IV]	2p 2P1/2	2s2p2 4P3/2	2.3D	col	185	56
1393.67	oe		1393.76	Si IV	3s 2S1/2	3p 2P3/2	1	col	1080	54
Oth			1393.21	Fe II	3d7 a2H11/2	4sp x4H9/2	2.1	fl
1387.10	214	80	1387.38	N III	3p 2P3/2	4d 2D5/2	2.3F	rec
			7.26	N III	2s2p2 2S1/2	2p3 2D3/2	2.3D	unk
1385.64	129	35	1385.78	Fe II	3d7 a2P1/2	(5D)5p 4D3/2	2.1	fl
1383.41	117	22	1383.54	Fe II	3d7 a2P3/2	(5D)5p 4D5/2	2.1	fl
1381.08	193	30	1381.22	Fe II	4s b4P3/2	(4P)4sp 4P5/2	2.1	fl
1376.26	67		1376.34	Fe V	(4F)4s 5F5	(4F)4p 5F5	2.3F	rec
1375.56	164	33	1375.75	Fe II	3d7 a2P3/2	(5D)5p 4D3/2	2.1	fl	110	24
1373.44	69	22	1373.59	Fe V	(4F)4s 5F4	(4F)4p 5F4	2.3F	rec
1372.93	209	28
1371.18	473	83	1371.30	O V	2s2p 1P1	2p2 1D2	1	unk	214	126
			0.94	Fe V	(4F)4s 5F1	(4F)4p 5F2	2.3F	rec
1367.80	89	22
1362.60	161	22	1362.78	Fe II	4s b4P5/2	(4P)4sp 4P5/2	2.1	fl
1360.05	184	40	1360.30	O III]	2s2p3 1P1	2p4 3P1	2.3D	unk
1358.35	298	31	1358.51	O III]	2s2p3 1P1	2p4 3P0	2.3D	unk	107	24
			1358.51	O I]	2p4 3P1	3s 5S2	2.3E	unk
1355.43	406	31	1355.60	O I]	2p4 3P2	3s 5S2	2.3E	unk	121	24
1345.54	99	31
1344.80	115	45	1344.85	P III	3p 2P3/2	3p2 2D3/2	2.3D	col
1344.29	85		1344.33	P III	3p 2P3/2	3p2 2D5/2	2.3D	col
1343.41	253	34	1343.51	O IV	2s2p2 2P3/2	2p3 2D5/2	2.3D	unk
1338.47	85	38	1338.62	O IV	2s2p2 2P1/2	2p3 2D3/2	2.3D	unk
1336.71	119	63
1335.55	315	25	1335.71	C II	2p 2P3/2	2s2p2 2D5/2	2.3D	col
1324.25	115	20	1324.45	[Mg V]	2p4 3P1	2p4 1S0	2.2	col
1323.15	63	20
Oth			1312.49	Fe II	4s b4D7/2	(2F)4sp 4G9/2	2.1	fl
1310.92	58	27	1310.95	N I	2p3 2P1/2	3d 2D3/2	2.3E	unk
1310.47	60	46	1310.70	P II	3p2 3P2	3p3 3P2	2.3D	col
			0.54	N I	2p3 2P3/2	3d 2D5/2	2.3E	unk
Oth			1310.15	Fe II	3d7 a2G9/2	4p u2G9/2	2.1	fl
1309.69	74bl		1309.87	P II	3p2 3P2	3p3 3P1	2.3D	col
1308.63	41		1308.71	C III	2p2 1S0	2s3p 1P1	2.3F	rec
1305.90	2566	46	1306.03	O I	2p4 3P0	3s 3S1	2.3E	col
1304.73	2345	46	1304.86	O I	2p4 3P1	3s 3S1	2.3E	col
1301.86	83	16	1301.87	P II	3p2 3P0	3p3 3P1	2.3D	col
1301.03	96bl		1301.15	Si III	3p 3P1	3p2 3P0	2.3D	unk
Oth			1300.86	O III]	2p2 1S0	2s2p3 3D1	2.3D	col
Oth			1298.89	Si III	3p 3P1	3p2 3P1	2.3D	unk
Oth			1296.73	Si III	3p 3P0	3p2 3P1	2.3D	unk
Oth							1
Oth							1
Oth							1
1252.48	149	26
1250.01	197	108	1250.43	Si II	3p2 2D5/2	3p3 2D5/2	2.3D	unk
			0.09	Si II	3p2 2D3/2	3p3 2D3/2	2.3D	unk
1248.20	130bl	50	1248.43	Si II	3p2 4P3/2	3p3 4S3/2	2.3D	unk
1247.25	236	29	1247.38	C III	2s2p 1P1	2p2 1S0		unk
1242.73	oe		1242.78	N V	2s 2S1/2	2p 2P1/2	1	col	6080	67
1238.74	oe		1238.80	N V	2s 2S1/2	2p 2P3/2	1	col	9990	67
1227.70	283	73
1218.26	2237	71	1218.34	O V]	2s2 1S0	2p 3P1	2.3F	unk
1215.65	936	106	1215.67	H I	n=1	n=2		rec
1199.04	1066	40	1199.13	S V]	3s2 1S0	3p 3P1	1	unk
1184.43	180	28	1184.51	N III	2s2p2 2P3/2	2p3 2P3/2	2.3D	unk
Oth			1174.93	C III	2s2p 3P1	2p2 3P2		unk
1151.04	65		1151.15	Fe II	4s a6D5/2	4s4p y6F7/2	2.1	fl
1147.27	71		1147.41	Fe II	4s a6D7/2	4s4p y6F7/2	2.1	fl
1145.38	1014	58	1145.58	Ne V]	2p2 3P2	2s2p3 5S2	2.3D	col
1141.22	94
1136.38	492	60	1136.49	Ne V]	2p2 3P1	2s2p3 5S2	2.3D	col
1128.21	96	90	1128.35	Si IV	3p 2P3/2	3d 2D5/2		unk
			8.33	Si IV	3p 2P3/2	3d 2D3/2		unk
1124	115pc	700
1084.7	1940	63	1084.9	He II	n=2	n=5	2.3F	rec
1067.62	227
1037.62	4140	116	1037.61	O VI	2s 2S1/2	2p 2P1/2	1	col
1031.92	7970	120	1031.92	O VI	2s 2S1/2	2p 2P3/2	1	col
974	359pc	700
967	212pc	700
958.51	351

^a Peak intensity measured in 10¹³ erg cm^-2 s^-1 Å^-1.
^b Gaussian widths measured in km s^-1.
^c Reference to the section in the paper the mechanism responsible for the line is discussed.
^d Intensity measured with GHRS.
^e width measured with GHRS.
^f Excitation mechanism, fl=fluorescence, rec=recombination, col=collision and unk=unknown excitation mechanism

   

Table 14: Intensities of emission lines not detectable with LWP25995 or SWP47715.

$\lambda_{\rm obs}$	Ia	wb	$\lambda_{\rm id}$	spec.	Lower level	Upper level	spectra
3300.29	234	45	3300.34	O III	2p3s 3P0	2p3p 3S1	LWP19253
3049.78	58	18	3049.88	Fe II	4p z4P3/2	5s e4D3/2	LWP25565
2831.45	57	22	2831.76	Fe II	4s b2G7/2	4p x4G5/2	LWR06398
2817.11	52	20					LWP19253
2644.61	76	32	2644.55	Fe II	4s2 b4G5/2	4p x4H7/2	LWP09698
2583.28	144	17	2583.36	Fe II	4s a4D3/2	4p z4P3/2	LWP09698
2581.81	79	20	2581.94	Fe II	4p z2D5/2	5s f4F5/2	LWP25565
2549.69	61		2549.69	Fe II	4s a2I11/2	4p x2H9/2	LWP09698
2539.19	91		2539.35	Fe II	4s a2F5/2	4p y2D5/2	LWR06389
2528.28	89	23					LWR09130
2527.02	32		2527.06	Fe II	4s b4P5/2	4p y4P5/2	LWR09130
2464.62	62	30	2464.76	Fe II	4s a4G9/2	4p x4F7/2	LWR06398
2455.53	47		2455.71	O III	2p3s 1P1	2p3p 1S0	LWP09698
2437.89	142	28	2437.94	Fe II	4s a4G7/2	4p y2D5/2	LWP09698
2435.70	159	47	2435.69	Fe II	4s b4F3/2	4p y4G5/2	LWP09698
			5.66	Ne III]	2p3(2D)3s 1D2	2p3(2D)3p 3P2
2429.94	61	16	2429.98	Ne III]	2p3(2D)3s 1D2	2p3(2D)3p 3P1	LWP09698
2426.32	79	16	2426.42	Fe II	4s b2P3/2	4p y2D5/2	LWR09130
2425.28	64	19	2425.23	[Ne IV]	2p3 4S3/2	2p3 2D5/2	LWP09698
2422.66	108	16	2422.60	[Ne IV]	2p3 4S3/2	2p3 2D3/2	LWP09698
2413.64	85		2413.67	Ne III	2p3(4S)3p 3P1	2p3(4S)3d 3D2	LWP09698
			3.47	Ne III	2p3(4S)3p 3P2	2p3(4S)3d 3D3
2321.28	48	25	2321.66	[O III]	2p2 3P1	2p2 1S0	LWR09130
2316.42	53	26	2316.46	Co II	4s c3F4	4p v3D3	LWR09130
2253.78	187	37	2253.83	Fe II	4s a6D7/2	4p z4F7/2	LWR09130
2211.72	221	23	2211.81	Fe II	4s a4H13/2	4p y4H11/2	LWP25565
2179.99	619	29					LWP25565
2152.70	230	29					LWR06389
2149.26	195	45	2149.28	He II	n=3	n=13	LWP09698
2136.06	158	35	2136.03	He II	n=3	n=14	LWP09698
2127.87	241	24					LWR06389
2125.30	113		2125.31	He II	n=3	n=15	LWR06389
2121.96	62		2122.12	Fe II	4s b4D3/2	4p w2D3/2	LWR09130
2092.38	235	19					LWR06389
2037.98	299	19	2038.11	Fe II	4s c2P3/2	(4P)4sp 2S1/2	LWR06389
2003.72	242	39	2003.85	Fe II	4s c2P1/2	(4P)4sp 2S1/2	LWR06389
2001.77	195	28					LWR06389
1974.85	32	15	1975.07	Fe II	3d7 a2G7/2	4p y2D5/2	SWP15651
1973.58	25	20	1973.78	Fe II	4s2 b4G9/2	(2I)4sp 4H9/2	SWP37477
1971.98	45	21	1972.16	Fe II	4s2 b4G11/2	(2I)4sp 4H9/2	SWP15651
1957.05	36	44	1957.28	[Fe VI]	3d3 2G7/2	3d3 2D15/2	SWP43007
1956.35	77	28					SWP43007
1951.69	34	23					SWP43007
1950.85	65	28					SWP43007
1925.70	137	25					SWP02334
1921.14	58	20					SWP15651
1919.00	30	30					SWP15651
1909.74	89	17	1909.91	Fe II	4s b4P5/2	4p y2P3/2	SWP15651
1894.16	40	17	1894.29	C III	2s3p 1P1	2s4s 1S0	SWP15651
1893.83	61	36	1893.89	Mg IV	(3P)3s 4P5/2	(3P)3p 4P5/2	SWP15651
1883.71	31	19	1883.72	Fe II	4s a4D7/2	4p z4G5/2	SWP37477
1881.75	24		1881.89	Fe II	4s a4D7/2	4p z2D5/2	SWP29862
1880.99	28	19	1881.25	Fe II	3d7 a2P1/2	(3D)4p 4P3/2	SWP15651
1877.66	146	53					SWP15651
1876.94	93	16	1877.02	Fe II	4s a4G5/2	4sp x6P7/2	SWP02334
1853.52	53	31	1853.73	Co II	4s2 a5D2	(4F)4p 5D3	SWP15651
1850.50	136	26					SWP43007
1850.06	53	91	1850.20	Fe III	(4F)4s 5F4	(4F)4p 5D4	SWP43007
1849.15	38	24	1849.40	Fe III	(4F)4s 5F5	(4F)4p 5D4	SWP43007
1836.52	22	34	1836.72	N I	2p3 2P3/2	3s 4P1/2	SWP40149
			6.71	N I	2p3 2P1/2	3s 4P1/2
1835.37	27	21	1835.57	N I	2p3 2P3/2	3s 4P3/2	SWP40149
1833.83	29	20	1834.01	N I	2p3 2P1/2	3s 4P3/2	SWP40149
1814.50	51	40	1814.63	[Ne III]	2p4 3P1	2p4 1S0	SWP15651
1813.85	41	18					SWP43007
1809.84	101	22					SWP43007
1795.30	94	52	1795.57	Fe II	4s2 b4G7/2	(3H)5p 4G7/2	SWP15651
			5.33	Fe II	4s2 b4G5/2	(3H)5p 4G7/2
			5.27	Fe II	4s2 b4G9/2	(3H)5p 4G7/2
1787.79	49	22	1788.00	Fe II	4s2 a6S5/2	4sp x6P3/2	SWP37477
1783.88	99	44	1783.98	Fe II	4s b4D7/2	4sp y6F7/2	SWP10454
1782.64	42	49					SWP43007
1760.78	40	32	1760.82	C II	2s2p2 2D3/2	3p 2P1/2	SWP29862
1760.26	103	49	1760.47	C II	2s2p2 2D3/2	3p 2P3/2	SWP29862
			0.40	C II	2s2p2 2D5/2	3p 2P3/2
1757.61	46	22	1757.74	Fe II	4s c4P3/2	(4F)4sp 6F3/2	SWP43007
1751.45	47	33	1751.66	N III	2s2p2 2P3/2	2p3 2D5/2	SWP15651
1750.46	65	41	1750.66	Mg II	3p 2P1/2	5s 2S1/2	SWP40149
1747.64	36		1747.85	N III	2s2p2 2P1/2	2p3 2D3/2	SWP15651
1725.78	141	17	1725.98	Fe II	3d7 a2D3/2	4sp x6P3/2	SWP15651
1721.46	102	23	1721.68	C II	2s2p2 2P3/2	2p3 2P3/2	SWP10454
1712.99	56	18	1713.00	Fe II	3d7 a4F7/2	4p z4G9/2	SWP43007
1706.78	164	19	1706.83	Fe II	4s c2G7/2	4sp x4H7/2	SWP15651
1588.07	167	21	1588.29	Fe II	3d7 a4F3/2	4p x4G5/2	SWP06355
1538.59	152	18	1538.63	Fe II	4s a4G5/2	(5D)5p 4D3/2	SWP29862
1533.8	170		1534.05	O V	2p3p 1P1	2s4p 1P1	SWP29862
1531.0	232	127					SWP29862
1502.0	429	937	1501.76	S V	3s3p 1P1	3p2 1D2	SWP02334
1468.88	103	49					SWP29862
1457.53	163	23	1457.76	Fe II	4s2 a6S5/2	(4D)4sp 6F3/2	SWP15651
1392.99	195	24	1393.21	Fe II	3d7 a2H11/2	4sp x4H9/2	SWP02334
1312.41	94	16	1312.49	Fe II	4s b4D7/2	(2F)4sp 4G9/2	SWP29862
1310.01	184	27	1310.15	Fe II	3d7 a2G9/2	4p u2G9/2	SWP06355
1300.75	145	16	1300.86	O III]	2p2 1S0	2s2p3 3D1	SWP15651
1298.78	120	30	1298.89	Si III	3p 3P1	3p2 3P1	SWP29862
1296.58	90	19	1296.73	Si III	3p 3P0	3p2 3P1	SWP29862
1265.98	858	554					SWP02334
1260.40	1556	699					SWP02334
1253.26	1469	789					SWP02334
1174.86	399	41	1174.93	C III	2s2p 3P1	2p2 3P2	SWP15651

^a Peak intensity measured in 10¹³ erg cm^-2 s^-1 Å^-1.
^b Gaussian widths measured in km s^-1.

   

Table 15: Emission lines saturated in LWP25995 or SWP47715.

$\lambda_{\rm obs}$	Ia	wb	$\lambda_{\rm id}$	spec.	Lower level	Upper level	spectra
3133.62	3204	49	3133.70	O III	2p3p 3S1	2p3d 3P2	LWP21635
3047.86	805	34	3047.99	O III	2p3s 3P2	2p3p 3P2	LWP30936
2803.5	717		2803.53	Mg II	3s 2S1/2	3p 2P1/2	LWP21635
2796.3	828		2796.35	Mg II	3s 2S1/2	3p 2P3/2	LWP21635
2734.00	596	54	2734.10	He II	n=3	n=5	LWP19253
1908.65	3389	36	1908.73	C III	2s2 1S0	2s2p 3P1	SWP55055
1891.96	5239	29	1892.03	Si III	3s2 1S0	3p 3P1	SWP55055
1749.55	2077	36	1749.67	N III	2p 2P3/2	2s2p2 4P5/2	SWP55055
1666.06	8540	38	1666.15	O III]	2p2 3P2	2s2p3 5S2	SWP55055
1660.70	3540	34	1660.81	O III]	2p2 3P1	2s2p3 5S2	SWP55055
1640.28	22040	60	1640.35	He II	n=2	n=3	SWP55055
1550.79	24420	45	1550.77	C IV	2s 2S1/2	2p 2P1/2	SWP55055
1548.21	44470	37	1548.19	C IV	2s 2S1/2	2p 2P3/2	SWP55055
1486.42	14200	32	1486.50	N IV	2s2 1S0	2p 3P1	SWP55055
1404.74	2389	26	1404.80	O IV]	2p 2P3/2	2s2p2 4P3/2	SWP55055
			4.77	S IV	3p 2P1/2	3p2 4P1/2
1402.78	2439	36	1402.77	Si IV	3s 2S1/2	3p 2P1/2	SWP55055
1401.07	7500	43	1401.16	O IV]	2p 2P3/2	2s2p2 4P5/2	SWP55055
1393.75	3796	37	1393.76	Si IV	3s 2S1/2	3p 2P3/2	SWP55055
1242.78	12570	56	1242.78	N V	2s 2S1/2	2p 2P1/2	SWP55055
1238.79	19560	70	1238.80	N V	2s 2S1/2	2p 2P3/2	SWP55055

^a Peak intensity measured in 10¹³ erg cm^-2 s^-1 Å^-1.
^b Gaussian widths measured in km s^-1.

   

Table 16: Aborption lines in AG Peg.

$\lambda_{\rm obs}$	ekvi	$\lambda_{\rm id}$	spec.	Lower level	Upper level	shift	rem
2852.92	0.21	2852.96	Mg I	3s2 1S0	3s3p 1P1	IS
2606.49a	0.26	2606.46	Mn II	4s a7S3	4p z7P2
2600.13	0.20	2600.17	Fe II	4s a6D9/2	4p z6D9/2
2594.51	0.17	2594.50	Mn II	4s a7S3	4p z7P3
2586.68	0.37	2585.65	Fe II	4s a6D9/2	4p z6D7/2
2576.88	0.14	2576.87	Mn II	4s a7S3	4p z7P4
2514.83	0.21	2515.07	Si I	2p2 3P0	2p3s 3P1
2382.75	0.26	2382.77	Fe II	4s a6D9/2	4p z6F11/2
2374.55	0.20	2374.46	Fe II	4s a6D9/2	4p z6F9/2
1969.90b	0.15	1970.36	Fe II	3d7 a4P3/2	4p z2F5/2
1913.26	0.15	1913.25	Fe I	4s2 a5D3	(2D)4p 3D2
1859.44	0.18
1838.34b	0.21
1801.49	0.15
1788.61	0.21
1737.82	0.13
1719.41b	0.23	1720.03	Fe II	3d7 a4P1/2	(3D)4p 4P3/2
1670.76	0.37	1670.99	Fe II	3d7 a4F3/2	4p y4D3/2
		0.79	Al II	2s2 1S0	3p 1P1
		0.79	Fe II	3d7 a4F5/2	4p y4D5/2
		0.75	Fe II	3d7 a4F9/2	4p y4D7/2
1658.97	0.12	1659.48	Fe II	3d7 a4F7/2	4p y4D5/2
1656.82	0.21	1657.07	Fe II	3d7 a4F3/2	4p x4D3/2
		6.93	C I	2p2 3P0	2p3s 3P1	IS
1642.33	0.11	1642.37	Fe II	4s a6D9/2	4p z4H11/2
1608.34	0.31	1608.45	Fe II	4s a6D9/2	4sp y6P7/2
1558.97	0.23	1559.09	Fe II	3d7 a4F9/2	4p x4F9/2
1558.51	0.14	1558.54	Fe II	3d7 a4F5/2	4p y2D5/2
1548.56*	0.04	1548.70	Fe II	3d7 a4F7/2	4p y2D5/2
1548.27*	0.02	1548.41	Fe II	3d7 a4P1/2	4p w2D3/2
1548.06*	0.02	1548.20	Fe II	3d7 a4F9/2	4p y4H11/2
1526.64	0.16	1526.71	Si II	3p 2P1/2	4s 2S1/2
1470.35c	0.10
1470.08c	0.15
1401.50	0.06	1401.51	S I	3p4 3P2	(4S)5s 3S1
1334.40	0.22	1334.53	C II	2p 2P1/2	2s2p2 2D3/2	IS
1328.71	0.15	1328.83	C I	2p2 3P0	2s2p3 3P1	IS
1304.35	0.07	1304.49	P II	3p2 3P1	3p3 3P0
1304.19	0.09	1304.37	Si II	3p 2P1/2	3p2 2S1/2
1302.12	0.10	1302.12	O I	2p4 3P2	3s 3S1	IS
1277.14	0.21	1277.28	C I	2p2 3P1	2p3d 3D2	IS
		7.25	C I	2p2 3P0	2p3d 3D1	IS
1260.35	0.16	1260.53	Fe II	4s a6D9/2	4sp x6P7/2
		1260.42	Si II	3p 2P1/2	3d 2D3/2
1259.41	0.23	1259.52	S II	3p3 4S3/2	3p4 4P5/2
1253.70	0.21	1253.81	S II	3p3 4S3/2	3p4 4P3/2
1250.47	0.24	1250.58	S II	3p3 4S3/2	3p4 4P1/2
1242.63*	0.03	1242.74	Fe II	3d7 a4F5/2	4p v2G7/2
1206.39	0.10	1206.50	Si III	3s2 1S0	3p 1P1
1200.64b	0.14	1200.71	N I	2p3 4S3/2	3s 4P5/2	IS
1200.16b	0.18	1200.23	N I	2p3 4S3/2	3s 4P3/2	IS
1199.48b	0.13	1199.55	N I	2p3 4S3/2	3s 4P1/2	IS
1193.19	0.11	1193.29	Si II	3p 2P1/2	3p2 2P1/2
1190.29b	0.14	1190.42	Si II	3p 2P1/2	3p2 2P3/2
1187.42	0.05	1187.42	Co II	3d8 a3F4	4p v3D3
1134.96	0.18	1134.97	N I	2p3 4S3/2	2p4 4P5/2	IS
1134.28	0.45	1134.42	N I	2p3 4S3/2	2p4 4P3/2	IS
		4.17	N I	2p3 4S3/2	2p4 4P1/2	IS
1122.42	0.98
1110.10	0.19	1110.28	Fe II	4s a6D9/2	(5D)5p 6F9/2
1108.45	0.66	1108.51	Fe II	3d7 a4F3/2	4p u4F3/2	bl
1094.06	0.28	1094.08	Fe II	3d7 a4F7/2	(4D)4s4p 6D5/2
1092.37	0.44
1078.97	0.31
1077.34	0.58
1064.63	0.25
1063.11	0.59	1063.18	Fe II	4s a6D9/2	(4D)4s4p 6D9/2	bl
1051.15	0.38
1049.50	0.59
1040.31	0.13
1039.17	0.15	1039.23	O I	2p4 3P2	2p3 (4S)4s 3S1	IS
1038.62	0.11
1038.09	0.15
1014.33	0.14
1012.90	0.40
1009.76	0.15
1008.53	0.28
974.06	0.10	974.07	O I	2p4 3P2	(2D)3s 1D2	IS
973.22	0.10	973.23	O I	2p4 3P1	(4S)4d 3D2

ⁱ Equivalent width measured in Å.