1. Multiwavelength observations of short time-scale variability in NGC 4151. II. Optical observations
- Author
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S. Kaspi, D. Maoz, H. Netzer, B. M. Peterson, T. Alexander, A. J. Barth, R. Bertram, F.-Z. Cheng, K. K. Chuvaev, R. A. Edelson, A. V. Filippenko, S. Hemar, L. C. Ho, O. Kovo, T. Matheson, R. W. Pogge, B.-C. Qian, S. M. Smith, R. M. Wagner, H. Wu, S.-J. Xue, and Z.-L. Zou
- Subjects
Physics ,010504 meteorology & atmospheric sciences ,Astrophysics::High Energy Astrophysical Phenomena ,Astrophysics (astro-ph) ,Flux ,Order (ring theory) ,FOS: Physical sciences ,Astronomy and Astrophysics ,Astrophysics ,Light curve ,01 natural sciences ,Galaxy ,Wavelength ,Amplitude ,Space and Planetary Science ,0103 physical sciences ,Continuum (set theory) ,Emission spectrum ,010303 astronomy & astrophysics ,Astrophysics::Galaxy Astrophysics ,0105 earth and related environmental sciences - Abstract
We present the results of an intensive ground-based spectrophotometric monitoring campaign of the Seyfert galaxy NGC~4151 for a period of over two months, with a typical temporal resolution of one day. Light curves for four optical continuum bands and the H$\alpha$ and H$\beta$ emission lines are given. During the monitoring period, the continuum at 6925~\AA\ varied by $\sim$17\% while the continuum at 4600~\AA\ varied by $\sim$35\%, with larger variations in the near UV. The wavelength dependence of the variation amplitude also extends into the far UV. The dependence in the 2700$-$7200~\AA\ range can be explained by the different relative starlight contributions at different wavelengths, but the large variability at 1275~\AA\ cannot be explained in this way. The continuum variability timescale is of order 13 days and is similar at all optical wavelength bands. No evidence for a time lag between the optical continuum and the UV continuum and emission lines was found. The H$\alpha$ emission line flux varied by about 12\% with a gradual rise throughout the campaign. Its cross correlation with the continuum light curve gives a lag of $0-2$ days. The variations in the H$\beta$ emission line flux are about 30\% and lag the continuum by 0$-$3 days. This is in contrast to past results where a time lag of 9$\pm$2 days was found for both emission lines. This may be due to a different variability timescale of the {\em{ionizing}} continuum, or to a real change in the BLR gas distribution in the 5.5 years interval between the two campaigns., Comment: 16 pages, LaTeX (including aas2pp4 and epsf), including 10 PostScript figures; To appear in the ApJ (October 20, 1996) Vol. 470
- Published
- 1996