The population of planetary nebulae and H ii regions in M81.

The population of planetary nebulae and H ii regions in M81.

A study of radial metallicity gradients and chemical evolution.
Key Words.:
Galaxies: abundances, evolution - Galaxies, individual: M81 - Planetary nebulae - H ii regions

Abstract

Context:M81 is an ideal laboratory to investigate the galactic chemical and dynamical evolution through the study of its young and old stellar populations.

Aims:We analyze the chemical abundances of planetary nebulae and H ii regions in the M81 disk for insight on galactic evolution, and compare it with that of other galaxies, including the Milky Way.

Methods:We acquired Hectospec/MMT spectra of 39 PNe and 20 H ii regions, with 33 spectra viable for temperature and abundance analysis. Our PN observations represent the first PN spectra in M81 ever published, while several H ii region spectra have been published before, although without a direct electron temperature determination. We determine elemental abundances of helium, nitrogen, oxygen, neon, sulfur, and argon in PNe and H ii regions, and determine their averages and radial gradients.

Results:The average O/H ratio of PNe compared to that of the H ii regions indicates a general oxygen enrichment in M81 in the last 10 Gyr. The PN metallicity gradient in the disk of M81 is =-0.0550.02. Neon and sulfur in PNe have a radial distribution similar to that of oxygen, with similar gradient slopes. If we combine our H ii sample with the one in the literature we find a possible mild evolution of the gradient slope, with results consistent with gradient steepening with time. Additional spectroscopy is needed to confirm this trend. There are no Type I PNe in our M81 sample, consistently with the observation of only the brightest bins of the PNLF, the galaxy metallicity, and the evolution of post-AGB shells.

Conclusions:Both the young and the old populations of M81 disclose shallow but detectable negative radial metallicity gradient, which could be slightly steeper for the young population, thus not excluding a mild gradients steepening with the time since galaxy formation. During its evolution M81 has been producing oxygen; its total oxygen enrichment exceeds that of other nearby galaxies.

1 Introduction

The study of chemical evolution of galaxies hinges on the confrontation between sets of evolutionary chemical models and arrays of observational data. Comparison of models with reliable abundance determinations are needed to understand the framework of galaxy evolution, and to test star formation history, stellar nucleosynthesis, and the mechanisms of galaxy assembly and formation.

Galactic metallicity gradients, and especially their time evolution, are important probes of galaxy formation and evolution. Observationally, most studied galaxies display a radial metallicity gradient with a negative slope, indicative of higher metallicity toward the inner galaxy. Time variation of gradient slopes in galaxies is hard to come by, given the lack of reliable time-tagging metallicity probes. From the viewpoint of theory, different models predict opposite time evolution of the metallicity gradient, showing the sensitivity of this physical parameter to the adopted parameterization of the processes (e.g., Magrini et al. 2007). A key factor to forwarding our knowledge in this field is the acquisition of high quality spectra to obtain abundances for a variety of probes, in a wide selection of different galaxies, including our own, to cover as much as possible the parameter space of initial masses, metallicities, and galaxy type.

The planetary nebula (PN) abundances of elements that are invariant during the evolution of low- and intermediate-mass stars (the so-called -elements) probe the environment at the epoch of the formation of the PN progenitors. Oxygen, neon, sulfur, and argon are, for the most part, manufactured in high mass stars (M8 M), thus their concentration in PNe across galactic disks probe the metallicity gradient in remote epochs. The metallicity gradients of PNe, compared to gradients of young stellar populations (such as those given by H ii regions) allow the study of the chemical evolution of galaxies. Galactic metallicity gradients are measured in terms of log (X/H)/ dex kpc, where X/H is the abundance of element X with respect to hydrogen and R is the galactocentric distance.

Planetary nebula gradients in the Milky Way indicate that the metallicity decreases inside out by 0.01 to 0.07 dex kpc (e. g., Maciel & Quireza 1999, Henry et al. 2004, Stanghellini et al. 2006, Perinotto & Morbidelli 2006). The most recent of these studies seem to agree that the PN metallicity gradients are rather flat, i.e., their slope is not steeper than -0.02 dex kpc, and only slightly shallower than that derived from H ii regions, implying that the Galactic metallicity gradient does not vary very much within the time frame of Galactic evolution. The metallicity gradients based on Galactic PNe are hindered by the uncertainties in PN distances, by the interstellar absorption in the direction of the Galactic center, and by the paucity of PN observations in the direction of the Galactic anti-center. These factors, together with the interest of studying metallicity gradients of other spiral galaxies of different morphological types and belonging to different groups, prompt us to investigate the PN (and H ii region) metallicity gradients in the M81 disk.

M81 is the largest member of the nearest interacting group of galaxies at a distance of 3.630.34 Mpc (Freedman et al. (2001)). Its two brightest companions, M82 and NGC 3077, are located within a projected distance of 60 kpc. The disturbed nature of the system is evident from the observations in the 21 cm emission line of H i, showing extended tidal streams and debris between the galaxies (Gottesman & Weliachew (1975); Yun et al. (1994)). The simulation of Yun ((1999)) explains many of these tidal features as being the result of close encounters between M81 and each of its neighbors 200-300 Myr ago. The most prominent debris (e.g., Sabbi et al. 2008, Weisz et al. (2008)) are considered tidal dwarf galaxies, new stellar systems that formed in gas stripped from interacting galaxies.

The -element abundances of PNe and H ii regions in M81 have remained elusive, with the exception of 17 H ii regions (Garnett & Shields 1987, GS87). With the PNe (Jacoby et al. 1989, Magrini et al. 2001) and H ii regions (Lin et al. 2003) locations, and their de-projected (PA=157 and inclination=59, Kong et al. 2000) galactocentric distances available we are in the position to push forward a determination of abundance gradients from PNe and H ii regions in the M81 disk. The location of M81 within its group will allow us to study the effect of galaxy interactions and mergers in the evolution of a galaxy and of its abundance gradient.

In order to sample the M81 disk to the necessary S/N for abundance analysis we need spectroscopy with a 6-8m class telescope. MMT/Hectospec medium-resolution spectroscopy offers the unique opportunity to study both the PNe and the H ii  region populations with the same setup, during the same night, and adopting the same analysis techniques, thus avoiding most biases that commonly affect the comparison of chemical abundances in population of different ages (e.g. Fe/H from old RGB stars is difficult to compare with O/H from the present time H ii  regions). We present here the results from the study of a sample of bright PNe in M81, with the goal of obtaining the metallicity and explore their gradients within the M81 disk. Their properties as a group are discussed, and compared with those of H ii  regions from both our MMT observations and from the literature. The combined properties of M81 PNe and H ii  regions are also compared with their homologs in other nearby galaxies and in the Milky Way.

In 2 we describe the observation and analysis techniques, and give the measured fluxes and calculated abundances. 3 includes the analysis of the derived abundances and the determination of the metallicity gradients, 4 presents the discussion of our results, and the conclusions are in 5.

2 The MMT observations: data reduction and analysis

2.1 Observations

We obtained the spectra of PNe and H ii  regions in M81 with the MMT Hectospec fiber-fed spectrograph (Fabricant et al. 2005). The spectrograph was equipped with an Atmospheric Dispersion Corrector and it was used with a single setup: 270 mm grating at a dispersion of 1.2 Å pixel. The resulting total spectral coverage ranged from approximately 3600 Å to 9100 Å, thus including the basic emission-lines necessary for the determination of physical and chemical properties.

The PNe were selected among those observed with the INT through with [O iii], H, and Stromgren Y filters (Magrini et al. 2001), which allowed us to cover the whole field of M81, and to identify a large number of disk PNe at large galactocentric distances. An earlier survey by Jacoby et al. (1989) was limited to the M81 bulge. It is worth noting that the INT images allow us to have accurate positions (0.5″) and finding charts for the selected PNe and H ii regions, a crucial information given the crowding of the inner and spiral arm fields of M81.

The first target selection was performed by scaling the PN brightness in [O iii]  with those of M33 PNe, whose medium-resolution spectra have been observed by us using the identical technique (Magrini et al., 2009, 2010, hereafter M09, M10). We also endeavored to have PN targets at several galactocentric distances, in order to characterize the PN metallicity gradient. The instrument deploys 300 fibers over a 1 degree diameter field of view and the fiber diameter is 1.5″ . The projected size of M81 on the sky is smaller than the whole field of view of MTT/Hectospec, and we took advantage of this by placing some of the fibers in the outermost periphery of M81, where some H ii  regions and few PNe, both belonging to the outer disk and to the intra-group population, have been identified. In addition, since the available catalog of H ii  regions by Lin et al. (2003) is based on H  photometry, our INT [O iii]  observations have been useful to select [O iii]-bright H ii regions essential for chemical abundance determination. As stated by Magrini et al. (2001), we expect the misclassification of H ii regions into PNe and vice-versa to be lower than3 of the whole sample.

The observations were carried out in queue mode in four runs during the months of November and December 2008. Each of the observing runs consisted of 3 to 5 exposures of 1800s each, for a total of 16 exposures (or 8 hours of observation). We used the same fiber setup during all observing runs, and thus PNe and HII regions were observed within the same conditions, including the same exposure time. Priority was given to PNe when placing the fibers, since a set of H ii region spectra already exists in the literature (GS87). A large number of fibers were devoted to sky measurements, to ensure that sky spectra were obtained in several positions around each target.

Cosmic rays were removed with the appropriate hectospec.hcosmic routine in the hectospec analysis package. Cosmic rays are detected via subtraction of multiple images, flagging the high or low pixels. The flagged pixels are interpolated over, and the resultant images are combined by average. This method avoids problems with clipping that other programs suffer from. In order to perform the sky subtraction we first inspected the sky spectra and eliminated those with unusual signals. Then we averaged the six spectra closer (in fiber location) to the targets, scaled the result to match the object spectrum, and subtracted.

The spectral calibration was achieved with the standard star Hilt600 (Massey et al. (1988)), observed during the first night. This star was chosen by its excellent spectral coverage compared to the spectra of the PNe. It is worth noting that our analysis does not hinge on flux calibration, rather spectral calibration and flux ratios, thus this approach is sufficient to the science goals. Other stars were observed during the run nights, but the excellent spectral coverage of Hilt600 makes it the ideal choice for this type of calibration. Variations in sky conditions are taken into account since sky subtraction was performed before flux calibration.

In Table 1 we give the IDs, equatorial coordinates, and equivalent [O iii]  magnitude of the planetary nebulae and H ii regions observed with MMT medium-resolution spectroscopy. All PN IDs are from Magrini et al. (2001), except for PN4 and PN5, which are identified PNe with unpublished positions (Magrini, private communication). There are 39 PNe and 20 H ii regions whose spectra have been acquired and analyzed. With the exception of PN 49m and PN 79m, whose spectral lines are below the detection limit, we detect at least the major spectral lines in each target.

Id. m
(1) (2) (3) (4)
PN 3m 9:54:26.54 69:10:30.5 24.41
PN 4 9:54:47.50 69:35:42.0 24.15
PN 4m 9:54:27.66 69:13:55.0 24.45
PN 5 9:54:53.80 69:08:01.0 23.87
PN 6m 9:54:36.70 69:17:00.5 24.39
PN 7m 9:54:38.52 69:10:36.8 24.53
PN 8m 9:54:45.50 69:08:06.6 24.06
PN 9m 9:54:46.52 69:05:39.0 23.66
PN 11m 9:54:53.15 69:13:32.2 24.51
PN 14m 9:54:09.28 69:11:31.0 24.75
PN 15m 9:55:01.01 69:12:04.3 24.45
PN 17m 9:55:10.09 69:02:37.1 24.24
PN 28m 9:55:13.62 69:07:10.3 23.91
PN 29m 9:55:14.78 68:55:30.0 23.56
PN 32m 9:55:15.70 69:08:39.8 24.23
PN 33m 9:55:15.96 69:13:31.7 24.30
PN 38m 9:55:19.47 68:54:45.7 24.39
PN 41m 9:55:02.58 69:06:26.3 23.77
PN 45m 9:55:21.81 69:07:50.6 23.86
PN 49m 9:55:23.38 69:02:50.9 23.66
PN 63m 9:55:28.25 69:01:26.5 24.26
PN 70m 9:55:30.62 69:07:56.3 23.66
PN 79m 9:55:34.58 69:09:00.9 24.49
PN 93m 9:55:39.07 69:05:42.1 23.48
PN 117m 9:55:50.11 68:59:48.4 24.04
PN 121m 9:55:51.46 69:05:14.9 23.56
PN 127m 9:55:52.93 69:10:52.1 24.60
PN 128m 9:55:53.02 69:06:15.2 24.19
PN 136m 9:55:06.11 68:57:18.5 24.60
PN 137m 9:55:07.29 69:12:10.4 24.47
PN 147m 9:56:20.74 68:58:26.8 24.41
PN 149m 9:56:27.09 69:05:26.4 23.66
PN 153m 9:56:28.70 69:00:32.8 23.56
PN 157m 9:56:31.99 69:03:31.3 24.09
PN 158m 9:56:32.84 69:03:58.8 24.23
PN 160m 9:56:04.48 69:06:36.0 24.31
PN 166m 9:56:08.41 69:08:37.8 24.49
PN 167m 9:56:08.54 69:03:56.0 24.53
PN 169m 9:56:09.87 68:59:56.0 24.39
ii 4 9:54:34.67 69:05:52.2
ii 5 9:54:36.1 69:06:30.5
ii 31 9:54:43.62 69:03:29.9
ii  42 9:54:47.66 69:02:18.7
ii 72 9:54:52.93 69:08:51.8
ii 78 9:54:53.84 69:01:08.8
ii 79 9:54:54.28 69:10:56.4
ii 81 9:54:54.53 69:09:30.5
ii 121 9:55:02.87 69:04:49.3
ii 123 9:55:03.64 69:10:54.6
ii 133 9:55:04.98 69:09:53.6
ii 201 9:55:22.82 69:09:52.9
ii 213 9:55:26.01 69:11:58.9
ii 228 9:55:32.66 69:11:55.4
ii 233 9:55:34.59 69:08:31.1
ii 249 9:55:37.61 69:12:03.6
ii 262 9:55:41.42 69:11:12.2
ii 282 9:55:46.50 68:59:24.6
ii 325 9:55:58.48 69:09:9.9
ii 328 9:55:59.29 68:59:37.6
ii 348 9:56:03.23 69:07:38.3
ii 352 9:56:03.79 69:09:37.8
ii 384 9:56:08.33 69:05:14.8
ii 403 9:56:11.78 69:07:44
Table 1: Observing log

In Table 2, available online in its completeness, we give for each target the ion and wavelength (columns 1 and 2) of the observed emission line, then the relative observed flux (column 3), its uncertainty (column 4), and the line intensity (column 5) obtained with the extinction correction given as a header for each target. All fluxes and intensities are normalized for F=100 and I=100. Both PNe and H ii regions are listed in Table 2. Target names are given for each target at the head of the corresponding flux list. The emission-line fluxes were measured with the package SPLOT of IRAF1. Errors in the fluxes were calculated taking into account the statistical error in the measurement of the fluxes, as well as systematic errors of the flux calibrations, background determination, and sky subtraction. Observations of same objects during different runs were stacked together and the resulting spectra have been used for the analysis.

Ion (Å)
(1) (2) (3) (4) (5)
PN 3m, c=0.5020.027
[O ii] 3727 373.9 58.6 517.3
H 4340 50.0 3.5 58.0
H 4861 100.0 4.5 100.0
[O iii] 4959 35.4 3.8 34.4
[O iii] 5007 104.2 5.2 99.9
[N ii] 5755 1.3 0.3 1.1
He i 5876 9.1 0.3 7.2
[N ii] 6548 59.8 3.5 42.2
H 6563 412.0 6.9 290.1
[N ii] 6584 142.5 4.5 100.0
[S ii] 6717 60.3 3.8 41.4
[S ii] 6731 44.3 3.4 30.4
Table 2: Observed Fluxes and Line Intensities

We derived c(H)  from the H/H flux ratios, as described in M09, and used the Galactic extinction curve by Mathis (1990) to correct the observed flux for interstellar extinction. In a few PNe the derived intensity of the H line is more than 30 off the theoretical prediction (I=0.466 for T=10,000 K, case B, Oserbrock & Ferland 2006). The reason for this offset could be an uncertain c(H). The average c(H) calculated for our PNe is 0.70.3, a reasonable value if we consider the average c(H) of Galactic PNe (from Cahn et al. 1992, c(H)=0.95) and the relative metallicities of the Galaxy to M81. We will recall these outliers later in the discussion and indicate them with different symbols in the Figures.

To our knowledge, this is the first attempt in the literature to detect PN emission line fluxes in M81 thus we cannot extend our discussion to comparison with previous work. The spectral quality is excellent. In Figure 1 we show a few examples of our M81 PN spectra, where the plasma and abundance diagnostic lines are well evident, and the S/N obtained with our observations makes us confident on the data quality.

Several H ii regions have been already observed by GS87, where the Authors refer to the catalog by Hodge & Kennicutt (1983) for coordinates. Since the latter are given in image coordinates rather than Galactic coordinates, it has been hard to eliminate from our sample of H ii regions those that have been already analyzed by GS87 or comparing targets from the two sets. But by comparing the position visually, we did not find any obvious overlap between the two samples, thus cannot compare the results.

Figure 1: Sample of medium-resolution spectra of M81 PNe.

2.2 Plasma diagnostics

We perform plasma diagnostics by using the 5-level atom model included in the nebular analysis package in IRAF/STSDAS (Shaw & Dufour 1994), consistently with our work in M33 (M09, M10). To calculate densities we use the doublet of the sulfur lines [S ii]6716,6731, while for the electron temperatures we use the ratios [O iii]4363/(5007 +4959), [N ii]5755/(6548 + 6584), and [S iii]6312/(9059 + 9532). In some cases, even if the sulfur lines are available, their ratio is outside the diagnostic ranges for density calculation (e.g., Stanghellini & Kaler 1989), and we assumed a density of 10cm. We calculate the medium- and low-excitation temperatures respectively from the [O iii] and [S iii], and from the [N ii] line ratios, respectively (see also Osterbrock & Ferland 2006,5.2).

2.3 Abundance analysis

Of the 39 PNe with emission line spectra, [O iii] and [N ii] temperature diagnostics are available respectively for 10 and 12 PNe, with only 3 PNe in common. In the analysis of the M33 PNe (M09) we were able to infer the electron temperature for targets whose plasma diagnostics were not available by using the correlation between the electron temperature and the He ii line intensity. In the case of M81 none of the PNe show the He ii emission; as a consequence, abundance analysis was possible only for the 19 PNe where electron temperature was diagnosed directly. There are also 14 H ii regions whose temperature analysis was based on auroral lines, and their plasma and abundance analysis was performed in a similar way than for the PNe. Electron temperature diagnostics for more than one excitation state was available for 5 of the 14 regions.

The plasma diagnostics are given in Table 3, available online, together with the ionic abundances of the PNe and H ii regions. Column (1) gives the diagnostics, and column (2) the value as determined from our analysis. The targets are listed sequentially, as in Table 1, and the first line for each target gives the target name.

(1) (2)
Name PN 3m
[N ii] 8893
N[S ii] 100
He i/H 0.051
He/H 0.051
[O ii]/H 3.320
[O iii]/H 5.440
ICF(O) 1.0
O/H 3.864
12+log(O/H) 8.587
[N ii]/H 2.916
ICF(N) 1.164
N/H 3.394
12+log(N/H) 7.531
[S ii]/H 2.250
ICF(S) 1.001
S/H 7.066
12+log(S/H) 6.849
Table 3: Plasma Analysis and Abundances

The abundance analysis of the PNe and the H ii regions was performed following the prescription given by M09, M10; abundances of all elements except helium where calculated with the ionization correction factors (ICFs) given in Kingsburgh & Barlow (1994) for the case were only optical lines are detected. Where both T[O III] and T[N II] were available we used T[O III] to derive the abundances of medium and high excitation ions, and T[N II] for the low excitation ones. In several H ii regions the temperature from the auroral line of [SIII] were also available, corresponding to transition of intermediate excitation. If only one of the electron temperature diagnostics was available we use that temperature to derive abundances for all ions. Helium abundances were calculated with the formulation of Benjamin et al. (1999) in two density regimes, and taking into account Clegg’s (1987) collisional populations, as in M09. The sulfur abundances for our PNe are mostly based on [S ii] lines, thus highly unreliable. We used the interpolation to the Galactic PN data by Kingsburgh & Barlow to infer [S iii]/[S ii] from the [O iii]/[O ii] ratios, where possible, and obtained an estimate of [S iii], which is observed only in three PNe. In order to check whether the sulfur correction is sensible, in Figure 2 we plot log versus log for the Kingsburgh & Barlow sample. On the same plot we locate our M81 PNe with measured [S iii]. The solid line, representing , has the correct slope for both the Galactic and M81 data, but it overcorrect slightly for [S iii]. Since the [S iii] lines we observe in M81 are quite faint, the relation by Kingsburgh & Barlow (1994) seems reasonable.

Figure 2: The log(S/log(S) versus log(O/log(O) correlation (solid line), based on the Galactic PNe from Kingsburgh & Barlow (1994, open circles). Our targets are shown with filled circles.

The formal errors in the ionic and total abundances were computed taking into account the uncertainties in (i) the observed fluxes, (ii) the electron temperatures and densities, and (iii) c(H). We performed complete formal error propagation for a subsample of target, representing a spread of flux error and magnitudes, and realized that the errors in the electron temperature completely dominate the errors in the ionic abundances for all elements except helium. In particular, the flux uncertainty of the weaker of the diagnostic lines in the electron temperatures, 5755 for T[N II] and 4363 for T[O III], determine the errors in the abundances. In Table 4 we give the error analysis for the PN subsample, including the ones with the minimum and maximum flux errors; column (1) gives the PN name, column (2) gives the relative flux error for the weaker line in the temperature diagnostics (in PN 9m we could calculate both T[N II] and T[O III], thus we give the two errors), columns (3) and (4) give the relative errors in T[N II] and T[O III] respectively, and finally columns (5) through (7) give the abundance errors, in dex. We derived the errors for all other targets by interpolation of the F-A(X) curves. In the case of the helium abundances we run the error analysis by using the formulae by Benjamin et al. (1999), and found that the factor determining the uncertainties is the relative error on the helium flux lines. The abundances, their uncertainties, together with the galactocentric distances (see 3.1) are given in Table 5.

It is worth noting that another source of error that we could not estimate explicitly is intrinsic to the ICF method. The uncertainties due to the ICF are very moderate for oxygen, but can be quite large for the other atoms, especially sulfur, thus these abundance uncertainties should be considered as formal errors, but might underestimate the real uncertainties. Another source of abundance uncertainties is the use of a single electron temperature for both low- and high-ionization ions. This regards the 16 PNe and 9 H ii regions where only one choice of the electron temperature was available. We have analyzed the sample of targets where two electron temperatures were available, and found that the average difference between electron temperatures of the order of 20. We tested that the resulting atomic abundance uncertainties are lower than those due to flux errors on the auroral lines.

The sets where we have oxygen and neon in common is limited to 6 PNe and 7 H ii regions. There is a clear correlation between these two -elements in both sets, with correlation coefficients R=0.7 and 0.9 respectively for PNe and H ii regions. This high correlation is expected, since both elements are produced in the Type II SN environment. The large uncertainties in the sulfur abundances make the comparison between oxygen and sulfur less meaningful, although the two sets have higher overlap than the previously described pair (16 PNe and 14 H ii regions in common), the correlation coefficient is only 0.4 and 0.3 for the two sets.

Figure 3: log (N/O) vs. He/H; broken lines show He/H=.125 and log(N/O)=-0.3. Type I PNe would be located in the upper-right quadrant.

Figure 3 shows the log(N/O) vs. helium plot, to classify Type I PNe. These are the nitrogen and helium-enriched PNe, whose progenitors have likely undergo the third dredge-up and hot bottom-burning, and thus are likely to have higher progenitor masses (Peimbert & Torres-Peimbert 1983, Marigo 2001). The top right portion of the plot, where He/H0.125 and log(N/O)-0.3, is the locus of Type I PNe as determined for the Milky Way by Perinotto et al. (2004). Since the metallicity of M81 is similar to that of the Milky Way, we can use the same diagnostic plot for M81 PNe. Clearly, there are no Type I PNe among those observed by us in M81. In the next section we discuss the population of the observed PNe and its implications for gradients and evolutionary studies, and show that indeed we do not expect an observed population of Type I PNe among our targets.

In Table 5, at the bottom of each set of targets, we give the average abundances, relative to hydrogen (linear for helium, and in logarithmic format for the other elements. Uncertainties represent ranges of abundances). The average oxygen abundance of M81 PNe (2.832.0110) is lower that what has been inferred for the Galactic disk PNe (4.492.28 for Type II PNe, Stanghellini & Haywood 2010) and about 1.6 higher than the average oxygen abundance of Type II I PNe in M33 (M09).

The H ii regions observed by us span a small fraction of the galaxy radius (5.8 to 9.8 kpc from galaxy center). The average O/H value for these regions, (3.421.78)10, should be compared to the oxygen abundance of PNe in the same radial range, which is (1.961.27)10, showing a 0.25 dex oxygen enrichment in this area of the galaxy. The comparison between PNe and H ii region average abundances of other elements is very limited, since the sets have 2 or 3 objects in common in the 5.8-9.8 kpc region.

2.4 The population of M81 PNe.

The PNe whose medium-resolution spectra are presented here are selected form the bright end of the planetary nebula luminosity function (PNLF) of the M81 disk. They have two peculiarities, as a group: first, we do not detect the He ii 4686 emission lines in any of them; this is a signature of moderately low central star temperature (less than 100,000 K). Second, none of the PNe whose abundance analysis was performed (i.e., whose electron temperature has been measured from the emission lines) is of Type I, thus they must be the progeny of stars with turnoff masses (M) in the1-2 M range.

The properties of the M81 PN sample are important to define their nature when we compare the population of M81 PNe to those of other galaxies. M81 has similar metallicity to that of the Milky Way (Davidge 2009). In M81, as in most external galaxies, the observed PN population belong to the brightest few magnitude bins. The nature of the brightest PNe varies notably with the metallicity of the host galaxy. In their runaway evolution from the AGB, the PN central stars (CS) reach hot temperature while keeping very bright; later, both brightness and temperature decline. A PN is visible only when the CS temperature is high enough to ionize hydrogen, and the nebula is optically thin to the H radiation (e.g., Stanghellini & Renzini 2000). At relatively high metallicities such as those of M81 or the Galaxy, the brightest PNe are not those with the hottest CSs (e.g., Villaver et al. 2002). In fact, the post-AGB shells with very hot CSs are statistically still enshrouded in dust at early phases or their evolution, thus still thick to the H radiation. A lower metallicity implies a shorter thinning time (Käufl et al. 1993). Plenty of Type I PNe have been observed within the bright end of the PNLF of low metallicity galaxies such as M33, the LMC, and the SMC; this is not the case in M81, where the high metallicity prevents massive progenitor PNe (i.e., the Type I) to populate the bright end of the PNLF.

To illustrate this point, in Figure 4 we show the luminosity function (PNLF) of Galactic PNe in the H-equivalent absolute magnitude. The H fluxes are from Cahn et al. (1992), and the PN distances from Stanghellini et al. 2008 (see also Stanghellini & Haywood 2010). The solid histogram represents the homogeneous Galactic sample of 331 PNe where both distance and H flux are known, and where spectroscopy has been performed and a lower limit or a detection of the He ii 4686 line has been acquired. The shaded histogram is the subsample of Galactic PNe with I/I 5. It is clear that at least 80-90 of the bright Galactic PNe do not show the He ii lines, in qualitative agreement with not finding this emission line in the M81 PN sample.

Figure 4: The Galactic PNLF in the light of H for a homogeneous sample of PN (unshaded histogram) and for a subsample of PNe with no He ii emission lines (shaded histogram, see text). Data are from Cahn et al. 1992, Stanghellini & Haywood 2010.

In order to quantify the expectation of detecting the He ii emission line in a given PN population of a certain metallicity we use Käufl et al.’s (1993) models to derive PN opacity, where the non-evolving term of the opacity,, scales directly with the dust-to-gas ratio (see their Eq. 10). We also express this ratio as expected at different metallicities, M/M(O/H)/(O/H) (Draine 2009), where the right hand side term refers to the ratio of the oxygen vs. hydrogen abundance in a given galaxy compared to that of the Milky Way. To obtain the ratio for M81 scaled to that of the Galaxy we use the H ii region oxygen abundances in M81 (4.9910) and in the Galaxy (5.25, Deharveng et al. 2000) to find , thus for a given type of M81 PN the thinning time would be similar to that of the Galactic homologous. We conclude that the lack of He ii-emitting PNe in M81 is totally expected, given the Galactic PNLF for both He ii–emitting and non-emitting PNe (Figure 4).

It is interesting to compare the PN population of M81 with that of M33 as well. Magrini et al. (2010) obtained an average oxygen abundance of O/H=2.04for H ii regions in the M33 disk, corresponding to a dust-to-mass ratio of410, or, less than half that of M81. By running the Käufl et al.’s models for M33 we obtain (Balmer line) thinning times1.5 times shorter than in M81 or the Galaxy, which can account for the relatively higher frequency of He ii-emitting, bright PNe that where observed in M33 by M09.

We know that the brightest PNe in a given population excludes the progeny of the massive AGB stars, i.e., those with M M (Stanghellini & Renzini 2000). The sample of M81 PNe under study here thus does not include the progeny of the more massive AGB stars. This agrees very well with the observational fact that we do not observe any Type I PNe in our M81 sample.

3 Radial metallicity gradients in M81

3.1 The planetary nebula gradients

The metallicity gradient of a disk galaxy is generally intended as the metallicity variation between the galactic center and the periphery, measured radially. These gradients are essential constraints for the chemical evolution models, and, depending on the probe, can constrain the galactic composition at different times in evolution. Planetary nebulae with low-mass progenitors, such as non-Type I PNe, probe the early stages of disk metallicity. We could derive the metallicity gradients in M81 from oxygen abundances, thus probing the -element evolution through the galactic disk. We estimate the distances of our target PNe from the center of M81 by using a rotation angle of 157 and an inclination of 59. The error in the target coordinates is very low, and the major source of error in the distance calculation is the uncertainty in the galaxy inclination, which we take as in Connolly et al. (1972), , and we propagate to estimate the galactocentric distance uncertainties.

Figure 5: Oxygen abundances vs. galactocentric distances for M81 targets. Top panel: the observed sample of PNe, with formal error bars and least square fit represented by solid line. Open symbols represent those PNe whose extinction constant might be overestimated. Middle panel: The H ii region sample from MMT spectra (open squares) superimposed to the PN population of the top panel. Bottom panel: The H ii regions from GS87 (filled squares) superimposed to the MMT H ii regions of the middle panel (open squares). The line represents the least square fit for the combined sample, as given in Table 6.

In Table 6, columns (3) and (4), we give the metallicity gradients calculated for oxygen, neon, and sulfur. Slopes are in dex kpc, while intercepts are in dex, with the usual notation of A(X)=log(X/H)+12. In Figure 5 (top panel) we show the oxygen gradient from the M81 PNe, where the line represent the linear fit. Only PNe are plotted in this top panel, with filled symbols representing the general PN population, and the open symbols indicating those PNe whose extinction correction from the H/H ratio does not well reproduce the line intensity expected for the H emission line. These open data points might thus have larger uncertainties than inferred from the formal error analysis.

We perform the fits with the routine fitexy (see Numerical Recipes, Press et al. 1992) and obtain =-0.0550.02 dex kpc. Should we exclude the open symbols in the fit we would obtain a very similar result (=-0.0530.02 dex kpc).

In Figure 6 we show the metallicity gradients for sulfur (top) and neon (bottom), where the PNe are plotted with filled symbols. The solid lines represent the fits obtained with the fitexy routines that consider the formal errors both in abundances and distances (see Table 6). Fits obtained with the least square method are very similar.

3.2 ii regions in the A(X)–R plots

The bottom panel of Figure 5 shows the H ii region analysis of oxygen abundances from this paper (open symbols) and from GS87 (filled symbols). Formal errorbars have been applied to the data obtained in this paper, while in the case of the GS87 sample we assume a 0.05 relative uncertainty in the distances, and a 0.25 dex uncertainty in the oxygen abundances. It is worth noting that we have recalculated the galactocentric distances for the GS87 targets by assuming the same distance to M81 than we use thorough this paper (d=3.63 Mpc) for homogeneity, although this does not affect the resulting gradient significantly. The composite data sample has been fitted including the distance and abundances uncertainties with the fitexy routine, to give a gradient (=-0.0930.02 dex kpc) not too dissimilar, yet steeper, from that of PNe. A direct least square fit would give a slightly milder gradient (=-0.07 dex kpc). It is worth noting that both the average O/H abundance in H ii regions and the intercept of the linear metallicity gradient are consistently higher that the respective values for PNe, as shown in Table 6, with PNe under abundant with respect to H ii  regions by almost a factor of 2, on average. This is well seen in the middle panel of Figure 5, where PNe and H ii regions from MMT observations are plotted together.

Figure 6: Sulfur (top panel) and neon (bottom panel) abundances from MMT observations vs. galactocentric distances for M81 PNe (filled circles) and H ii regions (open squares). The lines represent the linear fits to the PNe as discussed in the text.

In Figure 6 we show the sulfur (top) and neon (bottom) abundances in H ii regions versus their galactocentric distances (open symbols), plotted together with the PN data (filled symbols). Since the H ii regions observed with the MMT span a small fraction of the galaxy radius, metallicity gradients derived form these species would not be very meaningful. Within the distance ranges populated by our H ii region data we find=1.1, and =0.9. Any further comparison is not sensible given the limited data at hand, and we prefer to postpone a complete discussion of the sulfur and neon abundances in PNe as compared to the H ii regions of M81 when more H ii  region spectral data with diagnostic lines relative to these atoms will be available.

X N log(X/H)/R A(X)
(1) (2) (3) (4)
O 19 -0.0550.02 8.720.18
Ne 6 -0.0470.03 8.180.27
S 16 -0.0690.01 7.270.10
X N log(X/H)/R A(X)
O 31 -0.0930.02 9.370.24
Table 6: Metallicity Gradients

4 Discussion

4.1 Galaxy evolution through oxygen abundances

The O/H abundances are among the most reliable in emission-line targets when only optical spectra are available. In the case of M81, PNe and H ii  regions provide a meaningful comparison between young and old stellar objects, since the techniques of data acquisition, analysis, and abundance calculation are the same for both classes of objects. In particular, for several H ii  regions presented here, those observed with the MMT, the actual data acquisition is identical that that of the PNe, thus the comparison among data set is even more compelling.

It is worth emphasizing that the H ii region gradient is not based exclusively on our MMT data, which cover a limited radial range, but also on the results by GS87. The spectroscopic observations of GS87 did not allow a direct measurement of the electron temperature. They derived  by applying an indirect calibration made through the photoionization models by Pagel et al. ((1979)). The errors on the electron temperature are estimated of the order of 1200 K, mainly due to the scatter of the measurements on which Pagel et al. ((1979)) based their calibrations. We have estimated, using the IRAF ionic task, that an uncertainty of 1200 K in  translates in 0.2 dex in the ionic abundances. Thus, the chemical abundances of GS87 result less accurate than ours, and may introduce biases in the determination of the gradient. We conservatively have assumed uncertainties of 0.25 dex for the oxygen abundances from GS87.

As shown in Figure 5, the radial oxygen gradient slope of H ii regions is mildly steeper than that of PNe, with differences compatible with the slope uncertainties. Since there are no Type I PNe in our sample it is sensible to assume that the PN progenitor (turnoff) masses are smaller than 2 M, implying a population older than t 1 Gyr (Maraston 1998). The lower limit for PN progenitor mass is around 1 M, corresponding to a galactic age of t 10 Gyr.

In Figure 7 we plot the slope of the oxygen radial gradients in M81 (squares) for PNe and H ii  regions, against the mean age of the population considered. H ii  regions are placed at t=0, while PN ages are inferred from the presumed mass of progenitors (see Stanghellini & Haywood 2010 for a detailed discussion of the different PN types). The horizontal error bar for PNe indicates the age range of the population, while all vertical error bars indicate the uncertainties in the slopes. It appears that the slope of the M81 metallicity gradient did not vary very much during the past 10 Gyr. A flattening with time, as predicted by many chemical evolution models, is not supported by our observations. On the contrary, a constant slope, or a mild steepening of gradient slopes with time is inferred.

Figure 7: The slope of the oxygen gradients, in dex kpc, versus the age of the stellar population considered, for the Galaxy (filled circles, adapted from Stanghellini & Haywood 2010), M33 (starred symbols, adapted from M09 and M10) and M81 (squares, this paper). The zero-age populations represent the slopes of the gradients estimated though H ii  region oxygen abundances, while all other points are slopes of PN gradients, see text. Error-bars in the x direction represent the approximate age span of the populations, and in the y direction are the estimated metallicity uncertainties. The zero-age data point for M81 is uncertain, as it is based on the combination of of the H ii regions observed with the MMT and the GS87 sample

While uncertainties in the actual slopes are high, it is worth comparing the results of M81 with what found in M33 PNe and H ii  regions (M09 and M10, starred symbols), and the Milky Way (PNe from Stanghellini & Haywood 2010, H ii  regions from Deharveng et al. 2000, filled circles). The metallicity gradients are generally steeper in M81 than in either the Milky Way and M33, but in all three galaxies we observe mild flattening with the age of the population, going from steeper for H ii  regions to flatter for non-Type I PNe. It is worth noting that in the Galaxy the PN types I, II, and III were independently selected to calculate the oxygen radial gradients, while in M33 we were able to distinguish between Type I and non-Type I.

Since the gradient slopes seem to flatten with the age of the population considered, there is an indication that the gradients themselves are steepening with the galaxy age in all the three galaxies considered. It is a mild steepening, and with large uncertainties, but it is consistently found in all three galaxies, so it is worth exploring it.

Let us recall that the slope of the H ii gradient in M33 excluded the central kpc, as explained by M10. If we were including H ii  regions in the central kpc we would obtain nearly no gradient evolution between H ii  regions and Type I PNe in M33. There is thus some evolution of the oxygen gradients with time, where the slopes vary by 1 to dex per radial kpc in 10 Gyr. Stanghellini & Haywood (2010) offer the hypothesis that portions of the Milky Way at different radial distances might have evolved at different rates. The model by Schönrich & Binney (2009) illustrates this type of evolution, which could hold as well for the other spiral galaxies and for M81.

In Figure 8 we show the global oxygen evolution in different galaxies, where average oxygen abundances in H ii regions are plotted against the same quantities in non-Type I PNe. In the case of the disk galaxies, both populations cover a reasonable radial range and are representative of the whole disks. The SMC and LMC oxygen abundance are from Leisy & Dennefeld (2006), and the H ii  regions in the Magellanic Clouds are from Dennefeld (1989). The samples of PNe and H ii  regions considered in the Galaxy and M33 are as described earlier in this section. M81 PN and H ii regions abundances are from this paper, both selected consistently within the galactocentric distance domain where both sets of targets coexist. The error-bars in the lower right of the plot represent conservative data ranges for the galaxies considered here. The solar point is from Asplund et al. (2005). In this plot M81 stands out as the galaxy with most chemical enrichment in the group considered. M33, as found by M10, shows almost no enrichment, and the other galaxies show either low enrichment (the Galaxy and the LMC) or slight depletion of oxygen in the SMC, where the cause could be extremely efficient ON cycle at very low metallicity (Karakas & Lattanzio 2007). The average enrichment of M81 is 0.25 dex.

Figure 8: Difference between average oxygen abundance of H ii  regions and non-type I PNe vs. zero-age average oxygen abundance for M81 (square, this paper), compared to that of M33 (starred symbol, M09 and M10), the Magellanic Clouds (LMC: triangle, SMC: diamond; Garnett 1999, M09), and the Milky Way (filled circle, Stanghellini & Haywood 2010, Peimbert 1999). The solar value represented is from Asplund et al. (2005). The M81 datum is derived from PN and H ii regions in the 5.8-9.8 kpc range, and does not include the GS87 data.The M81 galaxy shows considerable metal enrichment.

The M81 galaxy disk shows indication of chemical enrichment through oxygen abundances. It also shows generally steeper metallicity gradients than both M33 and the Galaxy. The non-type I PNe gradients in M81 is - 0.055 dex kpc, while homologous slopes are - 0.03 and - 0.02 dex kpc respectively in M33 and the Galaxy, indicating that whatever process produces the metallicity gradients in spiral galaxies, it is more efficient in M81 and the overall galaxy metallicity is not a factor. Similarly for H ii  regions, the M81 gradient slope is - 0.09 dex kpc, to be compared with - 0.044 and -0.04 dex kpc for M33 and the Milky Way respectively. Indication of steeper gradients, and sizable chemical evolution, are thus the defining characteristics of M81 compared with other spirals. The oxygen enrichment indicates that this galaxy has suffered outflow to a lesser extent than the comparison galaxies, and steeper oxygen gradients are compatible with this explanation.

M81 MW
Morphological type Sa Sbc
Total mass [M] 2.310(a) 1.8-3.710 (b)
Gas mass [M] 2.910(c) 410 (d)
Luminosity [L] 1.910 (a)
Total SFR [Myr] 0.4-0.8 (e) 0.35 (f)
Max V [km s] 260 (g) 200 (h)

(a) Appleton et al. ((1981)); (b) Hodge & Miller ((1992)); (c) Karachentsev & Kashibadze ((2006)); (d) van der Kruit ((1990)); (e) Gordon et al. ((2004)); (f) Walterbos & Braun (1994); (g) Rohlfs & Krertschmann ((1980)); (h) MD05.

Table 7: Properties of M81 and the Galaxy

4.2 The chemical evolution of M81: comparison with the Milky Way

It is evident from the above analysis that the metallicity gradient slopes in the galaxies examined do not depend on the average galactic metallicity: M33 is metal poor (its metallicity is similar to that of the LMC, Leisy & Dennefeld 2006) and M81 is closer in metal contents to the Galaxy. Since M81 is also closer to the Galaxy in stellar mass content (see Table 7 for a direct comparison of the main properties of these two galaxies), it makes sense to compare these two galaxies directly, to explore the relations of the metallicity gradients to the characteristics of the galaxy disks and to their evolution. The observations of PNe tell us that the gradient of M81 is steeper than that of our Galaxy in old stellar populations; the trend seems to persist in the young stellar population, but this needs further confirmation.

From a theoretical point of view, there are two main reasons that could influence the gradient slopes, (1) the rotational velocity of the galaxy and (2) the different situation of these two galaxies within their environment.

Mollá & Diaz (2005) noted that metallicity gradients depend on the rotational velocity of the galaxy (thus presumably on its total mass), and on its morphological type: more massive galaxies tend to evolve faster and have flatter gradients than lower mass galaxies; for a given rotation velocity, gradients are steeper for late type than for early type galaxies. Both effects would imply a steeper gradient for the Galaxy than for M81, contrary to the observations. Some other factor must be at play.

It is likely that the situation of M81 within its group of galaxies influences its metallicity gradient. The tidal H i features near M81 are consistent with a large-scale redistribution of gas in this galaxy. M81 is the only massive galaxy of its group, surrounded by several small galaxies. The interaction of M81 with the dwarf galaxies of its group probably steepens the gradient of the major member due to the effect of stripping gas from the external regions of the major companion, while interaction of galaxies with more or less the same mass would redistribute the gas in both galaxies, and thus flatten the gradient.

The chemical evolution models of Valle et al. (2005) consider the effects of gas stripping due to galaxy encounters on the star formation rate and the evolution of the metallicity. They found that, for a stripping occurring 1-3 Gyr after the formation of the galaxy and removing 97 of the gas, the region affected by the gas removal has a SFR almost a factor of 10 lower than in the model without stripping and the relative metallicity is then reduced by about 40. The metallicity reduction is not strongly dependent on the time and duration of the stripping episode, but is quite sensitive to the relative amount of gas removed from the region. This effect should be more pronounced in the outer than the inner galactic regions, due to the proximity of the interacting galaxies, and it might explain why M81 has steeper metallicity gradients than the Galaxy. Unfortunately, the models by Valle et al. (2005) are limited to a single radial region, thus this conclusion is of qualitative nature. A radially-resolved chemical evolution modeling taking into account the effects of stripping would be necessary to determine the effect of tidal interaction on the gradient, and also to compare with other results.

5 Conclusions

Hectospec/MMT spectroscopy of a sizable sample of PN and H ii regions in the nearby M81 galaxy has proven very efficient to find chemistry of the young and old stellar populations, and to pin point the radial metallicity gradients. We were able to detect the diagnostic lines for plasma and abundance analysis in 19 PNe and 14 H ii regions. Their analysis indicates that the galaxy is clearly chemically enriched, with =1.8, from MMT spectra where PNe and H ii regions were simultaneously acquired. We also found that there is a noticeable PN metallicity gradient in oxygen, with =-0.055 dex kpc, and that neon and sulfur gradient slopes are within 15 of the oxygen one. The MMT sample of H ii regions have limited galactocentric distribution, thus they are insufficient probes of the metallicity gradient. The gradient slope from the combined MMT and GS87 H ii region samples is steeper (-0.093 dex kpc) than that of the PNe, possibly indicating an evolution of the radial metallicity gradients with time: older stellar population show shallower gradients, thus gradients are steepening with the time since galaxy formation. These results have been compared to their homologous for the Milky Way and M33, where similar (yet less marked) gradient steepening is inferred. We plan to increase the size of the H ii region sample, and to extend their gradient study to other atoms such as neon and sulfur in the near future, for a more complete comparison with the PNe, with the goal of obtaining firmer observational constraints for the chemical evolutionary models.

Acknowledgements.
We warmly thank D. Fabricant for making Hectospec available to the community, and the Hectospec instrument team and MMT staff for their expert help in preparing and carrying out the Hectospec observing runs. We thank N. Caldwell, D. Ming, and their team for the help during the data reduction. L.S. acknowledges the hospitality of the Observatoire de Paris and the Osservatorio Astrofisico di Arcetri for their hospitality during different stages of this project.
PN F T[N II] T[O III] A(O) A(N) A(S)
dex dex dex
(1) (2) (3) (4) (5) (6) (7)
PN 5 16 6 0.09 0.06 0.06
PN3 m 23 8 0.17 0.11 0.10
PN9 m 27,5 9 2 0.21 0.13 0.12
PN158 m 48 23 0.29 0.20 0.19
Table 4: Temperatures and Abundances Uncertainties
Name R [kpc] He/H A(N) A(O) A(Ne) A(S) A(Ar)
(1) (2) (3) (4) (5) (6) (7)
PN 3m 10.490.177 0.0510.002 7.530.11 8.590.17 6.85 0.10
PN 5 6.2760.094 7.410.06 8.170.09 6.850.06 6.370.06
PN 9m 7.3440.156 0.1010.002 7.490.13 8.540.21 7.670.12 6.510.12 5.760.12
PN 15m 9.0060.007 8.180.16
PN 17m 4.8580.261 0.1380.015 7.590.13 8.590.21 6.870.12
PN 29m 12.140.415 0.1090.017 7.130.05 8.24 0.06 7.710.05 6.410.05
PN 33m 10.860.110 7.070.18 7.940.28 6.430.18
PN 38m 12.540.385 0.1220.061 8.110.22 6.080.13
PN 41m 4.6770.110 0.1790.063 7.200.18 8.110.28 6.780.18
PN 45m 4.3260.018 0.0780.006 7.840.06 8.890.09 6.950.06
PN 63m 3.5160.117 0.0890.002 7.740.14 8.620.22 6.860.13
PN 70m 4.7850.084 0.1270.005 7.670.18 8.730.28 6.970.18
PN 93m 2.8050.109 0.0680.003 7.790.05 8.510.05 8.060.05 7.100.05
PN 121m 4.1190.218 0.1840.014 7.66 0.3 8.81 0.50 6.98 0.30
PN 128m 5.3390.265 7.830.18 8.270.28 7.160.18
PN 149m 10.140.547 0.1450.018 7.600.04 8.130.04 7.620.04 6.480.04 5.840.04
PN 153m 8.3810.277 0.1470.007 7.400.13 8.310.21 8.040.12 6.780.12
PN 157m 9.7590.493 0.2010.023 8.070.04
PN 158m 10.150.525 0.1660.078 7.37 0.20 7.940.29 7.400.19 6.910.19
Average 0.1270.045 7.58 8.45 7.81 6.86 6.08
HII 4 9.0760.396 0.0790.034 7.150.33 8.58 0.50 7.920.34 6.450.33 6.110.33
HII 5 8.6960.342 0.0720.021 8.060.07 8.870.04 6.630.03 5.870.03
HII 31 8.6480.455 0.0790.026 7.600.32 8.60 0.50 6.870.32 6.010.32
HII 72 6.7730.070 0.0860.011 7.870.13 8.820.22 8.280.13 6.790.13 6.050.13
HII 79 8.16 00.006 0.0770.020 7.300.29 8.260.45 7.620.29 6.630.29 5.880.29
HII 81 7.0270.031 0.1040.037 7.410.32 8.40 0.50 7.730.32 6.590.32 5.890.32
HII 123 7.7620.002 0.0840.007 7.400.10 8.430.18 7.680.10 6.760.10 6.300.10
HII 133 6.7210.001 0.0910.159 7.900.05 8.670.04 8.190.05 6.700.05 6.040.05
HII 201 6.7500.070 0.1070.032 7.630.13 8.260.22 7.730.13 6.550.13 5.970.13
HII 228 9.8490.211 0.0520.021 7.410.04 8.350.04 6.790.04 5.920.04
HII 233 5.7970.138 0.0860.043 7.860.25 8.50 0.38 6.540.25
HII 262 9.7160.280 0.0730.017 7.330.07 8.320.09 6.730.07 6.060.07
HII 325 9.2610.403 0.0810.042 7.230.37 8.18 0.60 6.420.37 5.960.37
HII 403 9.6530.493 0.0690.016 7.460.13 8.570.22 6.870.13 6.210.13
Average 0.0820.013 7.63 8.54 7.95 6.69 6.04
Table 5: Galactocentric distances and elemental abundances

Footnotes

  1. IRAF is distributed by the National Optical Astronomy Observatory, which is operated by the Association of Universities for Research in Astronomy (AURA) under cooperative agreement with the National Science Foundation

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