H. Salo
University of Oulu
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Featured researches published by H. Salo.
Monthly Notices of the Royal Astronomical Society | 2014
Jarkko Laine; Eija Laurikainen; H. Salo; Sébastien Comerón; Ronald J. Buta; D. Zaritsky; E. Athanassoula; Albert Bosma; J–C. Muñoz–Mateos; Dimitri A. Gadotti; Joannah L. Hinz; S. Erroz–Ferrer; A. Gil de Paz; Taehyun Kim; K. Menéndez–Delmestre; Trisha Mizusawa; Michael W. Regan; Mark Seibert; Kartik Sheth
We study the surface brightness profiles of disc galaxies in the 3.6 mu m images from the Spitzer Survey of Stellar Structure in Galaxies (S(4)G) and K-s-band images from the Near-Infrared S0-Sa galaxy Survey (NIRS0S). We particularly connect properties of single exponential (type I), downbending double exponential (type II), and upbending double exponential (type III) disc profile types, to structural components of galaxies by using detailed morphological classifications, and size measurements of rings and lenses. We also study how the local environment of the galaxies affects the profile types by calculating parameters describing the environmental density and the tidal interaction strength. We find that in majority of type II profiles the break radius is connected with structural components such as rings, lenses, and spirals. The exponential disc sections of all three profile types, when considered separately, follow the disc scaling relations. However, the outer discs of type II, and the inner discs of type III, are similar in scalelength to the single exponential discs. Although the different profile types have similar mean environmental parameters, the scalelengths of the type III profiles show a positive correlation with the tidal interaction strength.
Monthly Notices of the Royal Astronomical Society | 2015
E. Athanassoula; Eija Laurikainen; H. Salo; Albert Bosma
Barred galaxies have very interesting morphological features. Here we examine the barlens, a lens-like component whose extent along the bar major axis is shorter than that of the bar and whose outline is oval or circular. We show that such a component can also be found in a number of N-body plus SPH simulations. We analyse its properties by converting simulation snapshots into images, which we then analyse in the same way as images of observed galaxies. We make extensive comparisons with galaxies from the NIRS0S (Near Infrared S0 Survey) and the S
Monthly Notices of the Royal Astronomical Society | 2015
M. K. Seidel; J. Falcón-Barroso; Inma Martinez-Valpuesta; Simón Díaz-García; Eija Laurikainen; H. Salo; Johan H. Knapen
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Astronomy and Astrophysics | 2015
M. Herrera-Endoqui; Simón Díaz-García; Eija Laurikainen; H. Salo
G (Spitzer Stellar Structure Survey of Galaxies) samples and find very good agreement. These comparisons include morphology, radial projected density profiles, shapes, sizes and fluxes. We observe the barlens component in our simulations from different viewing angles. This reveals that {it barlenses are the vertically thick part of the bar seen face-on, i.e. that a barlens seen edge-on is a boxy/peanut/X bulge}. This finding makes it possible to follow barlens dynamics in terms of already studied families of periodic orbits. Some barlenses, notably those with near-circular projected isodensity curves, can be mistaken for classical bulges in morphological studies and classifications. This can introduce severe errors in modelling of individual galaxies, since the dynamics of classical bulges is very different from that of peanuts, and a bias in statistical morphological studies, leading to overestimates of the true frequency and mass of classical bulges. Thus, properly accounting for the barlens component will show that the fraction of disc galaxies lacking a classical bulge can be much larger than so far believed. Finally, based on the shape of the isodensity curves, we propose a rule of thumb for measuring the barlens extent along the bar major axis of galaxies sufficiently far from edge-on for the peanut not to be visible.
Astronomy and Astrophysics | 2017
Eija Laurikainen; H. Salo
We present the BaLROG (Bars in Low Redshift Optical Galaxies) sample of 16 morphologically distinct barred spirals to characterise observationally the influence of bars on nearby galaxies. Each galaxy is a mosaic of several pointings observed with the IFU spectrograph SAURON leading to a tenfold sharper spatial resolution (~100 pc) compared to ongoing IFU surveys. In this paper we focus on the kinematic properties. We calculate the bar strength Qb from classical torque analysis using 3.6 {mu}m Spitzer (S4G) images, but also develop a new method based solely on the kinematics. A correlation between the two measurements is found and backed up by N-body simulations, verifying the measurement of Qb . We find that bar strengths from ionised gas kinematics are ~2.5 larger than those measured from stellar kinematics and that stronger bars have enhanced influence on inner kinematic features. We detect that stellar angular momentum dips at 0.2
Astronomy and Astrophysics | 2015
Sébastien Comerón; H. Salo; Joachim Janz; Eija Laurikainen; P. Yoachim
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Astronomy and Astrophysics | 2016
Sébastien Comerón; H. Salo; R. F. Peletier; J. Mentz
0.1 bar lengths and half of our sample exhibits an anti-correlation of h3 - stellar velocity (v/{sigma}) in these central parts. An increased flattening of the stellar {sigma} gradient with increasing bar strength supports the notion of bar-induced orbit mixing. These measurements set important constraints on the spatial scales, namely an increasing influence in the central regions (0.1-0.5 bar lengths), revealed by kinematic signatures due to bar-driven secular evolution in present day galaxies.
Astronomy and Astrophysics | 2017
M. Herrera-Endoqui; H. Salo; Eija Laurikainen; Johan H. Knapen
Context. A catalogue of the features for the complete Spitzer Survey of Stellar Structure in Galaxies (S4G), including 2352 nearby galaxies, is presented. The measurements are made using 3.6 μm images, largely tracing the old stellar population; at this wavelength the effects of dust are also minimal. The measured features are the sizes, ellipticities, and orientations of bars, rings, ringlenses, and lenses. Measured in a similar manner are also barlenses (lens-like structures embedded in the bars), which are not lenses in the usual sense, being rather the more face-on counterparts of the boxy/peanut structures in the edge-on view. In addition, pitch angles of spiral arm segments are measured for those galaxies where they can be reliably traced. More than one pitch angle may appear for a single galaxy. All measurements are made in a human-supervised manner so that attention is paid to each galaxy. Aims. We create a catalogue of morphological features in the complete S4G. Methods. We used isophotal analysis, unsharp masking, and fitting ellipses to measured structures. Results. We find that the sizes of the inner rings and lenses normalized to barlength correlate with the galaxy mass: the normalized sizes increase toward the less massive galaxies; it has been suggested that this is related to the larger dark matter content in the bar region in these systems. Bars in the low mass galaxies are also less concentrated, likely to be connected to the mass cut-off in the appearance of the nuclear rings and lenses. We also show observational evidence that barlenses indeed form part of the bar, and that a large fraction of the inner lenses in the non-barred galaxies could be former barlenses in which the thin outer bar component has dissolved.
Astronomy and Astrophysics | 2018
Eija Laurikainen; H. Salo; Jarkko Laine; Joachim Janz
Morphological characteristics of the vertically thick inner bar components are studied. At high galaxy inclinations they manifest as Boxy/Peanut/X-shape features, and near to face-on view as barlenses. Using the Spitzer Survey of Stellar Structure in Galaxies (S4G) and the Near-IR S0 galaxy Survey (NIRS0S), we compared the properties of 88 X-shape features, 85 barlenses, and the photometric bulges of 41 non-barred galaxies. Sizes and minor-to-major axis ratios (b/a) of these structures are compared, and interpreted by means of synthetic images using N-body simulation models. Barlenses and their parent galaxies are also divided into different sub-groups. The synthetic images are analyzed in a similar manner as the observations. This is the first time that the observed properties of barlenses and X-shape features are compared, over a large range of galaxy inclinations. Our analysis are consistent with the idea that barlenses and X-shape features are physically the same phenomenon. However, which of the two features is observed depends, not only on galaxy inclination, but also on its central flux concentration. The observed nearly round face-on barlens morphology is expected when at least a few percents of the disk mass is in a central component, within a region much smaller than the size of the barlens itself. We also discuss that the large range of stellar population ages obtained for the photometric bulges in the literature, are consistent with our interpretation.
Monthly Notices of the Royal Astronomical Society | 2011
Eija Laurikainen; H. Salo; Ronald J. Buta; Johan H. Knapen
The formation mechanisms of thick discs are under discussion. Thick discs might have formed either at high redshift on a short time-scale or might have been built slowly over time. They may have an internal or an external origin. Here we study in detail the kinematics and the stellar populations of the thick disc of ESO533-4. ESO533-4 is a nearby bulgeless galaxy. nWe present the first ever IFU study of an edge-on galaxy with enough depth to study the thick disc. We exposed ESO533-4 with VIMOS@VLT for 6.5hours. The FOV covered an axial extent 0.1-0.7r_25 (1-7kpc). We used pPXF and the MILES library to obtain velocity and stellar population maps. We compared our kinematic data with simple GADGET-2 models. nThe apparent rotational lag of the thick disc of ESO533-4 is compatible with that expected from the combinations of two effects: differential asymmetric drift and the projection effects arising from studying a disc a few degrees (2-3) away from edge-on. Thus, ESO533-4 contains little or no retrograde material. This is compatible with three formation scenarii: the secular heating of an initially thin disc, the formation of the thick disc at high redshift in a turbulent disc phase, and its creation in a major merger event. If happening in all galaxies, this last mechanism would cause retrograde thick discs in half of them. Retrograde discs have not been observed in the five massive disc galaxies (v_c>120km s^-1) for which thick disc kinematics are known. The populations of the thin and the thick discs are separated in the Age-log(Z/Z_Sun) plane. Thus, the thin and thick discs are made of two distinct stellar populations. Although the stellar population results are not conclusive due to the high dust extinction in ESO533-4, they do not favour a secular evolution origin for the thick disc. Hence, we suggest that the thick disc of ESO533-4 formed in a relatively short event (Abridged).