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Parsec-scale jet behavior of NRAO 190 after a γ-ray outburst in August 1994. / Yurchenko, A. V.; Marchenko-Jorstad, S. G.; Marscher, A. P.

In: Astronomy and Astrophysics, Vol. 358, No. 2, 2000, p. 428-432.

Research output: Contribution to journalArticlepeer-review

Harvard

Yurchenko, AV, Marchenko-Jorstad, SG & Marscher, AP 2000, 'Parsec-scale jet behavior of NRAO 190 after a γ-ray outburst in August 1994', Astronomy and Astrophysics, vol. 358, no. 2, pp. 428-432.

APA

Yurchenko, A. V., Marchenko-Jorstad, S. G., & Marscher, A. P. (2000). Parsec-scale jet behavior of NRAO 190 after a γ-ray outburst in August 1994. Astronomy and Astrophysics, 358(2), 428-432.

Vancouver

Yurchenko AV, Marchenko-Jorstad SG, Marscher AP. Parsec-scale jet behavior of NRAO 190 after a γ-ray outburst in August 1994. Astronomy and Astrophysics. 2000;358(2):428-432.

Author

Yurchenko, A. V. ; Marchenko-Jorstad, S. G. ; Marscher, A. P. / Parsec-scale jet behavior of NRAO 190 after a γ-ray outburst in August 1994. In: Astronomy and Astrophysics. 2000 ; Vol. 358, No. 2. pp. 428-432.

BibTeX

@article{6ef806194bd14cc59dc892a2dba6a5f6,
title = "Parsec-scale jet behavior of NRAO 190 after a γ-ray outburst in August 1994",
abstract = "We present the results of a three-year Very Long Baseline Array (VLBA) imaging campaign on the bright blazar NRAO 190 after it was identified as a source of a prominent γ-ray flare detected in August 1994 by the EGRET instrument on the Compton Gamma Ray Observatory (McGlynn et al. 1997). The source was observed at 22 GHz at 5 epochs and at 43 GHz once. As is typical for blazars, our results show a one-sided jet structure dominated by a bright, unresolved core with a prominent but gradually weakening knot moving down the jet with an apparent velocity of 8.5h-1c, (Ho = 100h km s-1 Mpc-1,qo = 0.5). The time of ejection of this knot can be extrapolated, to within the errors, to the epoch of the aforementioned γ-ray flare. We interpret our results in terms of the {"}standard{"} relativistic shocked jet model (Blandford & K{\"o}nigl 1979; Marscher & Gear 1985). The angular resolution of the VLBA, together with the results of Mets{\"a}hovi 22 GHz total flux monitoring, allow us to examine the brightness variations of separate source components. During the time of our monitoring, we observed the evolution of the source shortly after the peak of a major outburst and also during and after a lower amplitude flare. The first event created a strong, superluminally moving component, while the latter produced no significant changes in the jet structure. The characteristics of the jet were therefore different in the aftermath of each flare, possibly because the first disturbance generated rarefactions in its wake.",
keywords = "Galaxies: active, Galaxies: jets, Galaxies: quasars: individual: NRAO 190, Radiation mechanisms: non-thermal, Shock waves",
author = "Yurchenko, {A. V.} and Marchenko-Jorstad, {S. G.} and Marscher, {A. P.}",
year = "2000",
language = "English",
volume = "358",
pages = "428--432",
journal = "ASTRONOMY & ASTROPHYSICS",
issn = "0004-6361",
publisher = "EDP Sciences",
number = "2",

}

RIS

TY - JOUR

T1 - Parsec-scale jet behavior of NRAO 190 after a γ-ray outburst in August 1994

AU - Yurchenko, A. V.

AU - Marchenko-Jorstad, S. G.

AU - Marscher, A. P.

PY - 2000

Y1 - 2000

N2 - We present the results of a three-year Very Long Baseline Array (VLBA) imaging campaign on the bright blazar NRAO 190 after it was identified as a source of a prominent γ-ray flare detected in August 1994 by the EGRET instrument on the Compton Gamma Ray Observatory (McGlynn et al. 1997). The source was observed at 22 GHz at 5 epochs and at 43 GHz once. As is typical for blazars, our results show a one-sided jet structure dominated by a bright, unresolved core with a prominent but gradually weakening knot moving down the jet with an apparent velocity of 8.5h-1c, (Ho = 100h km s-1 Mpc-1,qo = 0.5). The time of ejection of this knot can be extrapolated, to within the errors, to the epoch of the aforementioned γ-ray flare. We interpret our results in terms of the "standard" relativistic shocked jet model (Blandford & Königl 1979; Marscher & Gear 1985). The angular resolution of the VLBA, together with the results of Metsähovi 22 GHz total flux monitoring, allow us to examine the brightness variations of separate source components. During the time of our monitoring, we observed the evolution of the source shortly after the peak of a major outburst and also during and after a lower amplitude flare. The first event created a strong, superluminally moving component, while the latter produced no significant changes in the jet structure. The characteristics of the jet were therefore different in the aftermath of each flare, possibly because the first disturbance generated rarefactions in its wake.

AB - We present the results of a three-year Very Long Baseline Array (VLBA) imaging campaign on the bright blazar NRAO 190 after it was identified as a source of a prominent γ-ray flare detected in August 1994 by the EGRET instrument on the Compton Gamma Ray Observatory (McGlynn et al. 1997). The source was observed at 22 GHz at 5 epochs and at 43 GHz once. As is typical for blazars, our results show a one-sided jet structure dominated by a bright, unresolved core with a prominent but gradually weakening knot moving down the jet with an apparent velocity of 8.5h-1c, (Ho = 100h km s-1 Mpc-1,qo = 0.5). The time of ejection of this knot can be extrapolated, to within the errors, to the epoch of the aforementioned γ-ray flare. We interpret our results in terms of the "standard" relativistic shocked jet model (Blandford & Königl 1979; Marscher & Gear 1985). The angular resolution of the VLBA, together with the results of Metsähovi 22 GHz total flux monitoring, allow us to examine the brightness variations of separate source components. During the time of our monitoring, we observed the evolution of the source shortly after the peak of a major outburst and also during and after a lower amplitude flare. The first event created a strong, superluminally moving component, while the latter produced no significant changes in the jet structure. The characteristics of the jet were therefore different in the aftermath of each flare, possibly because the first disturbance generated rarefactions in its wake.

KW - Galaxies: active

KW - Galaxies: jets

KW - Galaxies: quasars: individual: NRAO 190

KW - Radiation mechanisms: non-thermal

KW - Shock waves

UR - http://www.scopus.com/inward/record.url?scp=0041124382&partnerID=8YFLogxK

M3 - Article

AN - SCOPUS:0041124382

VL - 358

SP - 428

EP - 432

JO - ASTRONOMY & ASTROPHYSICS

JF - ASTRONOMY & ASTROPHYSICS

SN - 0004-6361

IS - 2

ER -

ID: 88370268