scholarly journals Multiwavelength Energy Distributions of Ultraluminous IRAS Galaxies

1994 ◽  
Vol 159 ◽  
pp. 332-332
Author(s):  
D. Rigopoulou ◽  
A. Lawrence

Ultraluminous IRAS Galaxies (ULG's) have luminosities comparable to quasars while their space density is much higher than that of active galaxies. Much debate has centered around the origin of the energy source for these objects, whether this is a burst of star formation or a hidden quasar. The sample studied here is the Sanders et al. (1988) sample, 10 objects with LFIR ≥ 1012L⊙. We discuss our new observations at X-ray and submm wavelengths together with other published data for some of the objects. Some useful ideas can be gained from comparisons of the shape of the spectral energy distributions (SED's) of the ultraluminous objects with other “archetype” objects such as typical starbursts i.e. M82 or type 2 AGN i.e. NGC1068.

2003 ◽  
Vol 590 (1) ◽  
pp. 128-148 ◽  
Author(s):  
Joanna K. Kuraszkiewicz ◽  
Belinda J. Wilkes ◽  
Eric ◽  
J. Hooper ◽  
Kim K. McLeod ◽  
...  

2019 ◽  
Vol 492 (2) ◽  
pp. 1887-1901 ◽  
Author(s):  
Xiaotong Guo ◽  
Qiusheng Gu ◽  
Nan Ding ◽  
E Contini ◽  
Yongyun Chen

ABSTRACT The physical parameters of galaxies and/or active galactic nucleus (AGNs) can be derived by fitting their multiband spectral energy distributions (SEDs). By using cigale code, we perform multiband SED fitting (from ultraviolet to infrared) for 791 X-ray sources (518 AGNs and 273 normal galaxies) in the 7 Ms Chandra Deep Field-south survey (CDFS). We consider the contributions from AGNs and adopt more accurate redshifts than published before. Therefore, more accurate star formation rates (SFRs) and stellar masses (M*) are derived. We classify the 518 AGNs into type-I and type-II based on their optical spectra and their SEDs. Moreover, six AGN candidates are selected from the 273 normal galaxies based on their SEDs. Our main results are as follows: (1) the host galaxies of AGNs have larger M* than normal galaxies, implying that AGNs prefer to host in massive galaxies; (2) the specific star formation rates (sSFRs) of AGN host galaxies are different from those of normal galaxies, suggesting that AGN feedback may play an important role in the star formation activity; (3) we find that the fraction of optically obscured AGNs in CDFS decreases with the increase of intrinsic X-ray luminosity, which is consistent with previous studies; and (4) the host galaxies of type-I AGNs tend to have lower M* than type-II AGNs, which may suggest that dust in the host galaxy may also contribute to the optical obscuration of AGNs.


2020 ◽  
Author(s):  
Κωνσταντίνος Κουρουμπατζάκης

Παρουσιάζουμε μια εκτεταμένη μελέτη δεικτών ρυθμού αστρογένεσης (ΡΑ) γαλαξιών και αστρικών πληθυσμών (ΑΠ), εστιάζοντας στην γραμμή εκπομπής υδρογόνου α (Ηα) και την σύγκριση του με άλλους δείκτες ΡΑ. Παρουσιάζουμε φωτομετρία στην φασματική γραμμή Ηα για το αντιπροσωπευτικό δείγμα γαλαξιών Star Formation Reference Survey (SFRS) του τοπικού Σύμπαντος. Διερευνούμε το αποτέλεσμα της διόρθωσης της απόσβεσης μέσω της μείωσης Balmer, της περίσσειας υπερύθρου (IR excess), και φασματικών κατανομών ενέργειας (spectral energy distributions, SED). Επίσης διερευνούμε το αποτέλεσμα της συνεισφοράς της εκπομπής των γραμμών του αζώτου [N II] στις μετρήσεις της λαμπρότητας της γραμμής Ηα μέσω απεικόνισης με φίλτρα μικρού φασματικού εύρους. Επίσης ποσοτικοποιούμε την συσχέτιση μεταξύ απόσβεσης και μεταλλικότητας των γαλαξιών. Για ένα δείγμα του SFRS με καλής ποιότητας δεδομένα ακτίνων Χ (Chandra) διερευνούμε σε υπό-γαλαξιακές κλίμακες την συσχέτιση μεταξύ της φωτεινότητας ακτίνων Χ (ΦΧ) από υψηλής μάζας δυαδικά συστήματα αστέρων ακτίνων Χ (HMXBs) και ΡΑ. Βρίσκουμε συμφωνία με υπάρχουσες μελέτες ΦΧ-ΡΑ για log ΡΑ μέχρι −3 M/yr και περίσσεια ΦΧ για ΑΠ με μικρότερους ΡΑ. Η περίσσεια αυτή πιθανότατα προκαλείται από ένα πληθυσμό δυαδικών συστημάτων αστέρων χαμηλής μάζας ακτίνων Χ (LMXBs). Οι ΡΑ μέσω Ηα έχουν την καλύτερη συσχέτιση με ΦΧ καθώς η εκπομπή Ηα προέρχεται απο ΑΠ με ηλικίες παραπλήσιες με τα HMXBs. Προκειμένου να μελετήσουμε την επίδραση της μεταλλικότητας στην συσχέτιση ΦΧ-ΡΑ παρουσιάζουμε μια συστηματική μελέτη των διαφοροποιήσεων της μεταλλικότητας και της ΦΧ εντός του δακτυλιοειδή γαλαξία NGC 922. Βρίσκουμε πως η μεταλλικότητα του δακτυλίου του NGC 922 είναι πολύ χαμηλότερη ([12 + log(O/H)]=8.2) σε σύγκριση με αυτή του πυρήνα. Βρίσκουμε πως υπάρχει μια αντισυσχέτιση μεταξύ της ΦΧ και της μεταλλικότητας στον γαλαξία NGC 922. Οι διάφορες υπογαλαξιακές περιοχές έχουν ΑΠ παραπλήσιας ηλικίας και έτσι η διαφορετική μεταλλικότητα των περιοχών αυτών είναι ο κύριος λόγος για αυτήν την αντισυσχέτιση.


2009 ◽  
Vol 400 (3) ◽  
pp. 1199-1207 ◽  
Author(s):  
D. Rigopoulou ◽  
V. Mainieri ◽  
O. Almaini ◽  
A. Alonso-Herrero ◽  
J.-S. Huang ◽  
...  

2020 ◽  
Vol 500 (3) ◽  
pp. 2859-2860
Author(s):  
A S G Robotham ◽  
S Bellstedt ◽  
C del P Lagos ◽  
J E Thorne ◽  
L J Davies ◽  
...  

2020 ◽  
Vol 644 ◽  
pp. A82
Author(s):  
O. Miettinen

Context. Infrared dark clouds (IRDCs) can be the birth sites of high-mass stars, and hence determining the physical properties of dense cores in IRDCs is useful to constrain the initial conditions and theoretical models of high-mass star formation. Aims. We aim to determine the physical properties of dense cores in the filamentary Seahorse IRDC G304.74+01.32. Methods. We used data from the Wide-field Infrared Survey Explorer (WISE), Infrared Astronomical Satellite (IRAS), and Herschel in conjuction with our previous 350 and 870 μm observations with the Submillimetre APEX Bolometer Camera (SABOCA) and Large APEX BOlometer CAmera, and constructed the far-IR to submillimetre spectral energy distributions (SEDs) of the cores. The SEDs were fitted using single or two-temperature modified blackbody emission curves to derive the dust temperatures, masses, and luminosities of the cores. Results. For the 12 analysed cores, which include two IR dark cores (no WISE counterpart), nine IR bright cores, and one H II region, the mean dust temperature of the cold (warm) component, the mass, luminosity, H2 number density, and surface density were derived to be 13.3 ± 1.4 K (47.0 ± 5.0 K), 113 ± 29 M⊙, 192 ± 94 L⊙, (4.3 ± 1.2) × 105 cm−3, and 0.77 ± 0.19 g cm−3, respectively. The H II region IRAS 13039-6108a was found to be the most luminous source in our sample ((1.1 ± 0.4) × 103 L⊙). All the cores were found to be gravitationally bound (i.e. the virial parameter αvir < 2). Two out of the nine analysed IR bright cores (22%) were found to follow an accretion luminosity track under the assumptions that the mass accretion rate is 10−5 M⊙ yr−1, the stellar mass is 10% of the parent core mass, and the radius of the central star is 5 R⊙. Most of the remaing ten cores were found to lie within 1 dex below this accretion luminosity track. Seven out of 12 of the analysed cores (58%) were found to lie above the mass-radius thresholds of high-mass star formation proposed in the literature. The surface densities of Σ > 0.4 g cm−3 derived for these seven cores also exceed the corresponding threshold for high-mass star formation. Five of the analysed cores (42%) show evidence of fragmentation into two components in the SABOCA 350 μm image. Conclusions. In addition to the H II region source IRAS 13039-6108a, some of the other cores in Seahorse also appear to be capable of giving birth to high-mass stars. The 22 μm dark core SMM 9 is likely to be the youngest source in our sample that has the potential to form a high-mass star (96 ± 23 M⊙ within a radius of ~0.1 pc). The dense core population in the Seahorse IRDC has comparable average properties to the cores in the well-studied Snake IRDC G11.11-0.12 (e.g. Tdust and L agree within a factor of ~1.8); furthermore, the Seahorse, which lies ~60 pc above the Galactic plane, appears to be a smaller (e.g. three times shorter in projection, ~100 times less massive) version of the Snake. The Seahorse core fragmentation mechanisms appear to be heterogenous, including cases of both thermal and non-thermal Jeans instability. High-resolution follow-up studies are required to address the fragmented cores’ genuine potential of forming high-mass stars.


2019 ◽  
Vol 15 (S341) ◽  
pp. 21-25
Author(s):  
M. J. I. Brown ◽  
K. J. Duncan ◽  
H. Landt ◽  
M. Kirk ◽  
C. Ricci ◽  
...  

AbstarctWe present ongoing work on the spectral energy distributions (SEDs) of active galactic nuclei (AGNs), derived from X-ray, ultraviolet, optical, infrared and radio photometry and spectroscopy. Our work is motivated by new wide-field imaging surveys that will identify vast numbers of AGNs, and by the need to benchmark AGN SED fitting codes. We have constructed 41 SEDs of individual AGNs and 80 additional SEDs that mimic Seyfert spectra. All of our SEDs span 0.09 to 30μm, while some extend into the X-ray and/or radio. We have tested the utility of the SEDs by using them to generate AGN photometric redshifts, and they outperform SEDs from the prior literature, including reduced redshift errors and flux density residuals.


Author(s):  
Yurika Yamada ◽  
Makoto Uemura ◽  
Ryosuke Itoh ◽  
Yasushi Fukazawa ◽  
Masanori Ohno ◽  
...  

Abstract We report on the variations of the physical parameters of the jet observed in the blazar Mrk 421, and discuss the origin of X-ray flares in the jet, based on analysis of several spectral energy distributions (SEDs). The SEDs are modeled using the one-zone synchrotron self-Compton model, its parameters determined using a Markov chain Monte Carlo method. The lack of data at TeV energies means many of the parameters cannot be uniquely determined and are correlated. These are studied in detail. We find that the optimal solution can be uniquely determined only when we apply a constraint to one of four parameters: the magnetic field (B), the Doppler factor, the size of the emitting region, and the normalization factor of the electron energy distribution. We used 31 sets of SEDs from 2009 to 2014 with optical–UV data observed with UVOT/Swift and the Kanata telescope, X-ray data with XRT/Swift, and γ-ray data with the Fermi Large Area Telescope. The result of our SED analysis suggests that, in the X-ray faint state, the emission occurs in a relatively small area (∼1016 cm) with a relatively strong magnetic field (B ∼ 10−1 G). The X-ray bright state shows a tendency opposite to that of the faint state, that is, a large emitting area (∼1018 cm), probably downstream of the jet, and a weak magnetic field (B ∼ 10−3 G). The high X-ray flux was due to an increase in the maximum energy of electrons. On the other hand, the presence of two kinds of emitting areas implies that the one-zone model is unsuitable for reproducing at least part of the observed SEDs.


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