A spatially resolved study of ionized regions in galaxies at different ...
A spatially resolved study of ionized regions in galaxies at different ... A spatially resolved study of ionized regions in galaxies at different ...
106 4 • Long-slit spectrophotometry of multiple knots of Hii galaxies intermediate and high redshifts seems to have properties similar to that of Hii galaxies we know in the Local Universe. This type of objects is thought to be more frequent in a younger Universe and they are possible building blocks for the largest galaxies that we can detect at low redshifts (Kauffmann et al., 1993). If interactions among dwarf irregular galaxies was a basic mechanism of galaxy formation in the past, it is important to study the cases taking place in the nearby Universe now and the links between dwarf interactions and the star formation history of BCDs. Moreover, it is important to know the true distribution functions of the properties of these objects, among which the chemical abundances are of the greatest relevance. Hägele et al. (2006) and Hägele et al. (2008) performed a detailed analysis of a sample of 10 Hii galaxies in the Local Universe, deriving precise elemental abundances from high signal-to-noise spectra. Their spectral range included from the UV [Oii] λλ 3727,29 Å doublet, to the near IR [Siii] λλ 9069,9532 Å lines. This allowed the derivation of the different line temperatures: T e ([Oii]), T e ([Sii]), T e ([Oiii]), T e ([Siii]), T e ([Nii]), needed in order to study the temperature and ionization structure of each Hii galaxy considered as a multizone ionized region. From this sample, some of these objects presented several bright knots. We selected one galaxy, J1657 (we follow the ID used in that work), at a redshift of 0.038 (161.2 Mpc, from Mould et al., 2000), whose knots have enough signal-to-noise to perform a precise analysis similar to the one done for the main knot and in which the slit covers their lineal spatial distribution. To complete this study, we observed another Hii galaxy which presents a similar morphology. Although IIZw71 is catalogued as a BCD galaxy it is, in fact, characterised by several very luminous Hα knots distributed along a ring that is rotating around the host galaxy. It has been catalogued as a probable polar-ring galaxy (B17) in the Polar-Ring Catalogue (Whitmore et al., 1990). Polar ring galaxies (PRGs) are systems with two kinematically separated components. The central component (the host galaxy) is usually a lenticular galaxy or occasionally an elliptical galaxy. The other component, the polar ring, follows an approximately circumpolar orbit around the host and it is characterised by the presence of stars, molecular gas ,and dust, inside another larger ring composed of neutral hydrogen. Thus, this ring becomes an appropriate place for star formation. It is thought that these objects are formed as a consequence of the interaction between galaxies with a small impact parameter (Bournaud and Combes, 2003). In the case of IIZw71, there are proofs from interferometric observations of interaction with IIZw70, another BCD. In fact, although clearly separated on optical images, both galaxies share a common HI envelope with a gaseous bridge or streamer connecting both structures (see Figure 3 of Cox et al., 2001). This points to an ongoing interaction between the two galaxies. Therefore this system becomes an ideal scenario for studying the effects of interactions in the formation and evolution of BCDs in the Local Universe. A distance of 18.1 Mpc to the system is adopted by Cox et al. (2001), taking a
4.2. Observations and reduction 107 value of H o = 75 Km s −1 Mpc −1 . This implies a linear scale of 90 pc/arcsec on the sky. It is important to realize that the combination of accurate spectrophotometry and wide spectral coverage cannot be achieved using single-arm spectrographs where, in order to reach the necessary spectral resolution, the wavelength range must be split into several independent observations. In those cases, the quality of the spectrophotometry is at best doubtful mainly because the different spectral ranges are not observed simultaneously. This problem applies to both objects and calibrators. Furthermore, one can never be sure of observing exactly the same region of the nebula in each spectral range. To avoid all these problems, the use of double-arm spectrographs is required. In this chapter we present simultaneous blue and red observations of the galaxy J1657 observed with the double arm TWIN spectrograph at the 3.5m telescope of the Calar Alto Observatory at the Complejo Astronómico Hispano Alemán (CAHA). Similarly, in a single long-slit exposition, we have observed the main bursts of star formation along the direction of the polar ring of IIZw71 with the ISIS double-beam spectrograph mounted on the 4.2m William Herschel Telescope (WHT). The analysis of the obtained spectra were used to make a comparative analysis of the different bursts of star formation. In the next section we describe the long-slit spectroscopic observations of the two objects. In section 4.3, we present the results of our study, including the determination of physical properties, such as electron density and reddening in the observed knots, and of chemical abundances. In section 4.4 we discuss our results, including a study of the kinematics of the polar ring, the determination of metallicity, the reddening, the stellar properties by means of fitting synthesis stellar populations and the star formation rates in the individual knots. 4.2 Observations and reduction 4.2.1 CAHA observations Blue and red spectra were obtained simultaneously using the double beam Cassegrain Twin Spectrograph (TWIN) mounted on the 3.5m telescope of the Calar Alto Observatory at the Complejo Astronómico Hispano Alemán (CAHA), Spain. This galaxy was part of a four night observing run in 2006 June and they were acquired under excellent seeing and photometric conditions. Site#22b and Site#20b, 2000 × 800 px 15 µm, detectors were attached to the blue and red arms of the spectrograph, respectively. The T12 grating was used in the blue covering the wavelength range 3400-5700 Å (centered at λ c = 4550 Å), giving a spectral dispersion of 1.09 Å pixel −1 (R ≃ 4170). On the red arm, the T11 grating was mounted providing a spectral range from 5800 to 10400 Å (λ c = 8100 Å) and a spectral dispersion of 2.42 Å pixel −1 (R ≃ 3350). The pixel size for this set-up configuration is 0.56 arcsec for both spectral ranges. The slit width was ∼1.2 arcsec, which, combined with the spectral dispersions, yielded spectral resolutions of about 3.2 and 7.0 Å FWHM in the blue and the red
- Page 76 and 77: 56 3 • IFS of a GEHR in NGC 6946
- Page 78 and 79: 58 3 • IFS of a GEHR in NGC 6946
- Page 80 and 81: 60 3 • IFS of a GEHR in NGC 6946
- Page 82 and 83: 62 3 • IFS of a GEHR in NGC 6946
- Page 84 and 85: 64 3 • IFS of a GEHR in NGC 6946
- Page 86 and 87: 66 3 • IFS of a GEHR in NGC 6946
- Page 88 and 89: 68 3 • IFS of a GEHR in NGC 6946
- Page 90 and 91: 70 3 • IFS of a GEHR in NGC 6946
- Page 92 and 93: 72 3 • IFS of a GEHR in NGC 6946
- Page 94 and 95: 74 3 • IFS of a GEHR in NGC 6946
- Page 96 and 97: 76 3 • IFS of a GEHR in NGC 6946
- Page 98 and 99: 78 3 • IFS of a GEHR in NGC 6946
- Page 100 and 101: 80 3 • IFS of a GEHR in NGC 6946
- Page 102 and 103: 82 3 • IFS of a GEHR in NGC 6946
- Page 104 and 105: β[H 84 3 • IFS of a GEHR in NGC
- Page 106 and 107: 86 3 • IFS of a GEHR in NGC 6946
- Page 108 and 109: 88 3 • IFS of a GEHR in NGC 6946
- Page 110 and 111: 90 3 • IFS of a GEHR in NGC 6946
- Page 112 and 113: 92 3 • IFS of a GEHR in NGC 6946
- Page 114 and 115: 94 3 • IFS of a GEHR in NGC 6946
- Page 116 and 117: 96 3 • IFS of a GEHR in NGC 6946
- Page 118 and 119: 98 3 • IFS of a GEHR in NGC 6946
- Page 120 and 121: 100 3 • IFS of a GEHR in NGC 6946
- Page 122 and 123: 102 3 • IFS of a GEHR in NGC 6946
- Page 124 and 125: 104 3 • IFS of a GEHR in NGC 6946
- Page 128 and 129: 108 4 • Long-slit spectrophotomet
- Page 130 and 131: 110 4 • Long-slit spectrophotomet
- Page 132 and 133: 112 4 • Long-slit spectrophotomet
- Page 134 and 135: 114 4 • Long-slit spectrophotomet
- Page 136 and 137: Hδ 116 4 • Long-slit spectrophot
- Page 138 and 139: 118 4 • Long-slit spectrophotomet
- Page 140 and 141: 120 4 • Long-slit spectrophotomet
- Page 142 and 143: 122 4 • Long-slit spectrophotomet
- Page 144 and 145: Table 4.4 continued SDSS J1657 Knot
- Page 146 and 147: 126 4 • Long-slit spectrophotomet
- Page 148 and 149: 128 4 • Long-slit spectrophotomet
- Page 150 and 151: 130 4 • Long-slit spectrophotomet
- Page 152 and 153: 132 4 • Long-slit spectrophotomet
- Page 154 and 155: 134 4 • Long-slit spectrophotomet
- Page 156 and 157: 136 4 • Long-slit spectrophotomet
- Page 158 and 159: 138 4 • Long-slit spectrophotomet
- Page 160 and 161: 140 4 • Long-slit spectrophotomet
- Page 162 and 163: 142 4 • Long-slit spectrophotomet
- Page 164 and 165: 144 4 • Long-slit spectrophotomet
- Page 166 and 167: 146 4 • Long-slit spectrophotomet
- Page 168 and 169: 148 4 • Long-slit spectrophotomet
- Page 170 and 171: 150 Conclusions and future work has
- Page 172 and 173: 152 Conclusions and future work oth
- Page 174 and 175: 154 Conclusions and future work The
106 4 • Long-slit spectrophotometry <strong>of</strong> multiple knots <strong>of</strong> Hii <strong>galaxies</strong><br />
<strong>in</strong>termedi<strong>at</strong>e and high redshifts seems to have properties similar to th<strong>at</strong> <strong>of</strong> Hii <strong>galaxies</strong> we<br />
know <strong>in</strong> the Local Universe. This type <strong>of</strong> objects is thought to be more frequent <strong>in</strong> a younger<br />
Universe and they are possible build<strong>in</strong>g blocks for the largest <strong>galaxies</strong> th<strong>at</strong> we can detect<br />
<strong>at</strong> low redshifts (Kauffmann et al., 1993). If <strong>in</strong>teractions among dwarf irregular <strong>galaxies</strong><br />
was a basic mechanism <strong>of</strong> galaxy form<strong>at</strong>ion <strong>in</strong> the past, it is important to <strong>study</strong> the cases<br />
tak<strong>in</strong>g place <strong>in</strong> the nearby Universe now and the l<strong>in</strong>ks between dwarf <strong>in</strong>teractions and the<br />
star form<strong>at</strong>ion history <strong>of</strong> BCDs. Moreover, it is important to know the true distribution<br />
functions <strong>of</strong> the properties <strong>of</strong> these objects, among which the chemical abundances are <strong>of</strong><br />
the gre<strong>at</strong>est relevance.<br />
Hägele et al. (2006) and Hägele et al. (2008) performed a detailed analysis <strong>of</strong> a sample<br />
<strong>of</strong> 10 Hii <strong>galaxies</strong> <strong>in</strong> the Local Universe, deriv<strong>in</strong>g precise elemental abundances from high<br />
signal-to-noise spectra. Their spectral range <strong>in</strong>cluded from the UV [Oii] λλ 3727,29 Å doublet,<br />
to the near IR [Siii] λλ 9069,9532 Å l<strong>in</strong>es. This allowed the deriv<strong>at</strong>ion <strong>of</strong> the <strong>different</strong> l<strong>in</strong>e<br />
temper<strong>at</strong>ures: T e ([Oii]), T e ([Sii]), T e ([Oiii]), T e ([Siii]), T e ([Nii]), needed <strong>in</strong> order to <strong>study</strong><br />
the temper<strong>at</strong>ure and ioniz<strong>at</strong>ion structure <strong>of</strong> each Hii galaxy considered as a multizone<br />
<strong>ionized</strong> region.<br />
From this sample, some <strong>of</strong> these objects presented several bright knots. We selected one<br />
galaxy, J1657 (we follow the ID used <strong>in</strong> th<strong>at</strong> work), <strong>at</strong> a redshift <strong>of</strong> 0.038 (161.2 Mpc, from<br />
Mould et al., 2000), whose knots have enough signal-to-noise to perform a precise analysis<br />
similar to the one done for the ma<strong>in</strong> knot and <strong>in</strong> which the slit covers their l<strong>in</strong>eal sp<strong>at</strong>ial<br />
distribution.<br />
To complete this <strong>study</strong>, we observed another Hii galaxy which presents a similar morphology.<br />
Although IIZw71 is c<strong>at</strong>alogued as a BCD galaxy it is, <strong>in</strong> fact, characterised by several<br />
very lum<strong>in</strong>ous Hα knots distributed along a r<strong>in</strong>g th<strong>at</strong> is rot<strong>at</strong><strong>in</strong>g around the host galaxy.<br />
It has been c<strong>at</strong>alogued as a probable polar-r<strong>in</strong>g galaxy (B17) <strong>in</strong> the Polar-R<strong>in</strong>g C<strong>at</strong>alogue<br />
(Whitmore et al., 1990). Polar r<strong>in</strong>g <strong>galaxies</strong> (PRGs) are systems with two k<strong>in</strong>em<strong>at</strong>ically separ<strong>at</strong>ed<br />
components. The central component (the host galaxy) is usually a lenticular galaxy<br />
or occasionally an elliptical galaxy. The other component, the polar r<strong>in</strong>g, follows an approxim<strong>at</strong>ely<br />
circumpolar orbit around the host and it is characterised by the presence <strong>of</strong> stars,<br />
molecular gas ,and dust, <strong>in</strong>side another larger r<strong>in</strong>g composed <strong>of</strong> neutral hydrogen. Thus, this<br />
r<strong>in</strong>g becomes an appropri<strong>at</strong>e place for star form<strong>at</strong>ion. It is thought th<strong>at</strong> these objects are<br />
formed as a consequence <strong>of</strong> the <strong>in</strong>teraction between <strong>galaxies</strong> with a small impact parameter<br />
(Bournaud and Combes, 2003). In the case <strong>of</strong> IIZw71, there are pro<strong>of</strong>s from <strong>in</strong>terferometric<br />
observ<strong>at</strong>ions <strong>of</strong> <strong>in</strong>teraction with IIZw70, another BCD. In fact, although clearly separ<strong>at</strong>ed on<br />
optical images, both <strong>galaxies</strong> share a common HI envelope with a gaseous bridge or streamer<br />
connect<strong>in</strong>g both structures (see Figure 3 <strong>of</strong> Cox et al., 2001). This po<strong>in</strong>ts to an ongo<strong>in</strong>g<br />
<strong>in</strong>teraction between the two <strong>galaxies</strong>. Therefore this system becomes an ideal scenario for<br />
<strong>study</strong><strong>in</strong>g the effects <strong>of</strong> <strong>in</strong>teractions <strong>in</strong> the form<strong>at</strong>ion and evolution <strong>of</strong> BCDs <strong>in</strong> the Local<br />
Universe. A distance <strong>of</strong> 18.1 Mpc to the system is adopted by Cox et al. (2001), tak<strong>in</strong>g a