H. Teräsranta
Helsinki University of Technology
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Featured researches published by H. Teräsranta.
The Astrophysical Journal | 1998
Ann E. Wehrle; E. Pian; Claudia M. Urry; L. Maraschi; I. M. McHardy; A. J. Lawson; G. Ghisellini; R. C. Hartman; Greg M. Madejski; F. Makino; Alan P. Marscher; S. J. Wagner; J. R. Webb; G. S. Aldering; Margo F. Aller; Hugh D. Aller; Dana E. Backman; T. J. Balonek; P. Boltwood; Jerry T. Bonnell; J. Caplinger; A. Celotti; W. Collmar; J. Dalton; A. Drucker; R. Falomo; C. E. Fichtel; Wolfram Freudling; Walter Kieran Gear; N. Gonzales
The blazar 3C 279, one of the brightest identified extragalactic objects in the γ-ray sky, underwent a large (factor of ~10 in amplitude) flare in γ-rays toward the end of a 3 week pointing by Compton Gamma Ray Observatory (CGRO), in 1996 January-February. The flare peak represents the highest γ-ray intensity ever recorded for this object. During the high state, extremely rapid γ-ray variability was seen, including an increase of a factor of 2.6 in ~8 hr, which strengthens the case for relativistic beaming. Coordinated multifrequency observations were carried out with Rossi X-Ray Timing Explorer (RXTE), Advanced Satellite for Cosmology and Astrophysics (ASCA; or, Astro-D), Roentgen Satellite (ROSAT), and International Ultraviolet Explorer (IUE) and from many ground-based observatories, covering most accessible wavelengths. The well-sampled, simultaneous RXTE light curve shows an outburst of lower amplitude (factor of 3) well correlated with the γ-ray flare without any lag larger than the temporal resolution of ~1 day. The optical-UV light curves, which are not well sampled during the high-energy flare, exhibit more modest variations (factor of ~2) and a lower degree of correlation. The flux at millimetric wavelengths was near a historical maximum during the γ-ray flare peak, and there is a suggestion of a correlated decay. We present simultaneous spectral energy distributions of 3C 279 prior to and near to the flare peak. The γ-rays vary by more than the square of the observed IR-optical flux change, which poses some problems for specific blazar emission models. The synchrotron self-Compton (SSC) model would require that the largest synchrotron variability occurred in the mostly unobserved submillimeter/far-infrared region. Alternatively, a large variation in the external photon field could occur over a timescale of a few days. This occurs naturally in the mirror model, wherein the flaring region in the jet photoionizes nearby broad emission line clouds, which, in turn, provide soft external photons that are Comptonized to γ-ray energies.
Nature | 2002
Alan P. Marscher; Svetiana G. Jorstad; Josá Luis Gómez; Margo F. Aller; H. Teräsranta; M. L. Lister; Alastair M. Stirling
Accretion of gas onto black holes is thought to power the relativistic jets of material ejected from active galactic nuclei (AGN) and the ‘microquasars’ located in our Galaxy. In microquasars, superluminal radio-emitting features appear and propagate along the jet shortly after sudden decreases in the X-ray fluxes. This establishes a direct observational link between the black hole and the jet: the X-ray dip is probably caused by the disappearance of a section of the inner accretion disk as it falls past the event horizon, while the remainder of the disk section is ejected into the jet, creating the appearance of a superluminal bright spot. No such connection has hitherto been established for AGN, because of insufficient multi-frequency data. Here we report the results of three years of monitoring the X-ray and radio emission of the galaxy 3C120. As has been observed for microquasars, we find that dips in the X-ray emission are followed by ejections of bright superluminal knots in the radio jet. The mean time between X-ray dips appears to scale roughly with the mass of the black hole, although there are at present only a few data points.
The Astrophysical Journal | 2005
M. Błazejowski; G. Blaylock; I. H. Bond; S. M. Bradbury; J. H. Buckley; D. A. Carter-Lewis; O. Celik; P. Cogan; W. Cui; M. K. Daniel; C. Duke; Abe D. Falcone; D. J. Fegan; S. J. Fegan; J. P. Finley; L. Fortson; S. Gammell; K. Gibbs; G. G. Gillanders; J. Grube; K. Gutierrez; J. Hall; D. Hanna; J. Holder; D. Horan; B. Humensky; G. E. Kenny; M. Kertzman; D. Kieda; J. Kildea
We report results from an intensive multiwavelength monitoring campaign on the TeV blazar Mrk 421 over the period of 2003-2004. The source was observed simultaneously at TeV energies with the Whipple 10 m telescope and at X-ray energies with the Rossi X-Ray Timing Explorer (RXTE) during each clear night within the Whipple observing windows. Supporting observations were also frequently carried out at optical and radio wavelengths to provide simultaneous or contemporaneous coverages. The large amount of simultaneous data has allowed us to examine the variability of Mrk 421 in detail, including cross-band correlation and broadband spectral variability, over a wide range of flux. The variabilities are generally correlated between the X-ray and gamma-ray bands, although the correlation appears to be fairly loose. The light curves show the presence of flares with varying amplitudes on a wide range of timescales at both X-ray and TeV energies. Of particular interest is the presence of TeV flares that have no coincident counterparts at longer wavelengths, because the phenomenon seems difficult to understand in the context of the proposed emission models for TeV blazars. We have also found that the TeV flux reached its peak days before the X-ray flux did during a giant flare (or outburst) in 2004 (with the peak flux reaching ~135 mcrab in X-rays, as seen by the RXTE ASM, and ~3 crab in gamma rays). Such a difference in the development of the flare presents a further challenge to both the leptonic and hadronic emission models. Mrk 421 varied much less at optical and radio wavelengths. Surprisingly, the normalized variability amplitude in the optical seems to be comparable to that in the radio, perhaps suggesting the presence of different populations of emitting electrons in the jet. The spectral energy distribution of Mrk 421 is seen to vary with flux, with the two characteristic peaks moving toward higher energies at higher fluxes. We have failed to fit the measured spectral energy distributions (SEDs) with a one-zone synchrotron self-Compton model; introducing additional zones greatly improves the fits. We have derived constraints on the physical properties of the X-ray/gamma-ray flaring regions from the observed variability (and SED) of the source. The implications of the results are discussed.
Astronomy and Astrophysics | 2003
C. M. Raiteri; Massimo Villata; G. Tosti; R. Nesci; E. Massaro; Margo F. Aller; Hugh D. Aller; H. Teräsranta; Omar M. Kurtanidze; M. G. Nikolashvili; M. A. Ibrahimov; I. E. Papadakis; T. P. Krichbaum; A. Kraus; A. Witzel; H. Ungerechts; U. Lisenfeld; U. Bach; G. Cimò; S. Ciprini; L. Fuhrmann; G. N. Kimeridze; L. Lanteri; M. Maesano; F. Montagni; G. Nucciarelli; Luisa Ostorero
Eight optical and four radio observatories have been intensively monitoring the BL Lac object 0716+714 in the last years: 4854 data points have been collected in the UBVRI bands since 1994, while radio light curves extend back to 1978. Many of these data, which all together constitute the widest optical and radio database available on this object, are presented here for the first time. Four major optical outbursts were observed at the beginning of 1995, in late 1997, at the end of 2000, and in fall 2001. In particular, an exceptional brightening of 2.3 mag in 9 days was detected in the R band just before the BeppoSAX pointing of October 30, 2000. A big radio outburst lasted from early 1998 to the end of 1999. The long-term trend shown by the optical light curves seems to vary with a characteristic time scale of about 3.3 years, while a longer period of 5.5–6 years seems to characterize the radio long-term variations. In general, optical colour indices are only weakly correlated with brightness; a clear spectral steepening trend was observed during at least one long-lasting dimming phase. Moreover, the optical spectrum became steeper after
The Astrophysical Journal | 2001
R. C. Hartman; M. Böttcher; G. Aldering; Hugh D. Aller; Margo F. Aller; Dana E. Backman; Thomas J. Balonek; D. L. Bertsch; S. D. Bloom; H. Bock; Paul Boltwood; Michael T. Carini; W. Collmar; G. de Francesco; Elizabeth Colleen Ferrara; Wolfram Freudling; Walter Kieran Gear; Patrick B. Hall; J. Heidt; Philip A. Hughes; Stanley D. Hunter; Shardha Jogee; W. N. Johnson; G. Kanbach; S. Katajainen; M. Kidger; Tsuneo Kii; M. Koskimies; A. Kraus; H. Kubo
\rm JD \sim 2\,451\,000
Astronomy and Astrophysics | 2001
C. M. Raiteri; M. Villata; Hugh D. Aller; Margo F. Aller; J. Heidt; Omar M. Kurtanidze; L. Lanteri; M. Maesano; E. Massaro; Franco Montagni; R. Nesci; Kim K. Nilsson; Maria G. Nikolashvili; P Nurmi; L Ostorero; Tapio Pursimo; R Rekola; A. Sillanpää; L. Takalo; H. Teräsranta; G. Tosti; T. J. Balonek; Markus Feldt; A Heines; C Heisler; J. Hu; M. Kidger; J. R Mattox; E. J McGrath; A. Pati
, the change occurring in the decaying phase of the late-1997 outburst. The radio flux behaviour at different frequencies is similar, but the flux variation amplitude decreases with increasing wavelength. The radio spectral index varies with brightness (harder when brighter), but the radio fluxes seem to be the sum of two different-spectrum contributions: a steady base level and a harder-spectrum variable component. Once the base level is removed, the radio variations appear as essentially achromatic, similarly to the optical behaviour. Flux variations at the higher radio frequencies lead the lower-frequency ones with week–month time scales. The behaviour of the optical and radio light curves is quite different, the broad radio outbursts not corresponding in time to the faster optical ones and the cross-correlation analysis indicating only weak correlation with long time lags. However, minor radio flux enhancements simultaneous with the major optical flares can be recognized, which may imply that the mechanism producing the strong flux increases in the optical band also marginally affects the radio one. On the contrary, the process responsible for the big radio outbursts does not seem to affect the optical emission.
The Astrophysical Journal | 2000
Esko Valtaoja; H. Teräsranta; M. Tornikoski; A. Sillanpää; M. F. Aller; Hugh D. Aller; Philip A. Hughes
Of the blazars detected by EGRET in GeV γ-rays, 3C 279 is not only the best observed by EGRET but also one of the best monitored at lower frequencies. We have assembled 11 spectra, from GHz radio through GeV γ-rays, from the time intervals of EGRET observations. Although some of the data have appeared in previous publications, most are new, including data taken during the high states in early 1999 and early 2000. All of the spectra show substantial γ-ray contribution to the total luminosity of the object; in a high state, the γ-ray luminosity dominates over that at all other frequencies by a factor of more than 10. There is no clear pattern of time correlation; different bands do not always rise and fall together, even in the optical, X-ray, and γ-ray bands. The spectra are modeled using a leptonic jet, with combined synchrotron self-Compton plus external Compton γ-ray production. Spectral variability of 3C 279 is consistent with variations of the bulk Lorentz factor of the jet, accompanied by changes in the spectral shape of the electron distribution. Our modeling results are consistent with the UV spectrum of 3C 279 being dominated by accretion disk radiation during times of low γ-ray intensity.
Astronomy and Astrophysics | 2006
M. Villata; C. M. Raiteri; Thomas J. Balonek; Margo F. Aller; S. G. Jorstad; O. M. Kurtanidze; Fabrizio Nicastro; K. Nilsson; Hugh D. Aller; Akira Arai; A. A. Arkharov; U. Bach; E. Benítez; A. Berdyugin; C. S. Buemi; M. Böttcher; D. Carosati; R. Casas; A. Caulet; W. P. Chen; P. S. Chiang; Yi Chou; S. Ciprini; J. M. Coloma; G. Di Rico; C. Díaz; N. V. Efimova; C. Forsyth; A. Frasca; L. Fuhrmann
The BL Lacertae object AO 0235+16 is well known for its extreme optical and radio variability. New optical and radio data have been collected in the last four years by a wide international collaboration, which conrm the intense activity of this source: on the long term, overall variations of 5 mag in the R band and up to a factor 18 in the radio fluxes were detected, while short-term variability up to 0:5 mag in a few hours and 1: 3m ag in one day was observed in the optical band. The optical data also include the results of the Whole Earth Blazar Telescope (WEBT) rst-light campaign organized in November 1997, involving a dozen optical observatories. The optical spectrum is observed to basically steepen when the source gets fainter. We have investigated the existence of typical variability time scales and of possible correlations between the optical and radio emissions by means of visual inspection and Discrete Correlation Function (DCF) analysis. On the long term, the autocorrelation function of the optical data shows a double-peaked maximum at 4100{4200 days (11:2{11:5 years), while a double-peaked maximum at 3900{4200 days (10:7{11:5 years) is visible in the radio autocorrelation functions. The existence of this similar characteristic time scale of variability in the two bands is by itself an indication of optical-radio correlation. A further analysis by means of Discrete Fourier Transform (DFT) technique and folded light curves reveals that the major radio outbursts repeat quasi-regularly with a periodicity of5:7 years, i.e. half the above time scale. This period is also in agreement with the occurrence of some of the major optical outbursts, but not all of them. Visual inspection and DCF analysis of the optical and radio light curves then reveal that in some cases optical outbursts seem to be simultaneous with radio ones, but in other cases they lead the radio events. Moreover, a deep inspection of the radio light curves suggests that in at least two occasions (the 1992{1993 and 1998 outbursts) flux variations at the higher frequencies may have led those at the lower ones.
The Astrophysical Journal | 2000
Tadayuki Takahashi; J. Kataoka; Greg M. Madejski; John Richard Mattox; Claudia M. Urry; S. J. Wagner; F. Aharonian; M. Catanese; L. Chiappetti; Paolo S. Coppi; B. Degrange; Giovanni Fossati; Hidetoshi Kubo; H. Krawczynski; F. Makino; Herman L. Marshall; L. Maraschi; F. Piron; Ronald A. Remillard; Fumio Takahara; Makoto Tashiro; H. Teräsranta; T. C. Weekes
The BL Lac-type active galaxy OJ 287 exhibits a 12 year periodicity with a double-peaked maxima in its optical flux variations. Several models sought to explain this periodicity, the first one firmly established in any active galactic nucleus (AGN), as a result of the orbital motion of a pair of supermassive black holes. In one class of models the orientation of the jets changes in a regular manner, and the optical flaring is due to a consequent increase in the Doppler boosting factor. In another class of models the optical flaring reflects a true increase in luminosity, either due to an enhanced accretion during the pericenter passage or due to a collision between the secondary black hole and the accretion disk of the primary black hole. However, these models have been based solely on the optical data. Here we consider the full radio flux density monitoring data between 8 and 90 GHz from the Michigan, Metsahovi, and Swedish-ESO Submillimeter Telescope AGN monitoring programs. We find that the radio flux density and polarization data, as well as the optical polarization data, indicate that the first of the two optical peaks is a thermal flare occurring in the vicinity of the black hole and the accretion disk, while the second one is a synchrotron flare originating in a shocked region down the jet. None of the proposed binary black hole models for OJ 287 offers satisfactory explanations for these observations. We suggest a new scenario, in which a secondary black hole penetrates the accretion disk of the primary during the pericenter passage, causing a thermal flare visible only in the optical regime. The pericenter passage enhances accretion into the primary black hole, leading to increased jet flow and formation of shocks down the jet. These become visible as standard radio and optical synchrotron flares roughly a year after the pericenter passage and are identified with the second optical peaks. In addition to explaining the radio and the optical data, our model eliminates the need for a strong precession of the binary and for an ultramassive (≥1010 M☉) primary black hole. If our interpretation is correct, the next periodic optical flare, a thermal one, should occur around 2006 September 25. Nonthermal, simultaneous optical and radio flares should follow about a year later.
Astrophysical Journal Supplement Series | 1999
Esko Valtaoja; A. Lähteenmäki; H. Teräsranta; Markku Lainela
Context. The radio quasar 3C 454.3 underwent an exceptional optical outburst lasting more than 1 year and culminating in spring 2005. The maximum brightness detected was