Spectrophotometric Reverberation Mapping of Intermediate-mass Black Hole NGC 4395

Abstract Understanding the origins of massive black hole seeds and their coevolution with their host galaxy requires studying intermediate-mass black holes (IMBHs) and estimating their mass. However, measuring the masses of these IMBHs is challenging, due to the high-spatial-resolution requirement. Spectrophotometric reverberation monitoring is performed for a low-luminosity Seyfert 1 galaxy, NGC 4395, to measure the size of the broad-line region and black hole mass. The data were collected using the 1.3 m Devasthal fast optical telescope and 3.6 m Devasthal optical telescope at ARIES, Nainital, over two consecutive days in 2022 March. The analysis revealed strong emission lines in the spectra and light curves of the merged 5100 Å spectroscopic continuum flux ( f 5100 ) with the photometric continuum V band and H α , with fractional variabilities of 6.38% and 6.31% respectively. In comparison to several previous studies with lag estimation &lt;90 minutes, our calculated H α lag supersedes them by <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:msubsup> <mml:mrow> <mml:mn>125.0</mml:mn> </mml:mrow> <mml:mrow> <mml:mo>−</mml:mo> <mml:mn>6.1</mml:mn> </mml:mrow> <mml:mrow> <mml:mo>+</mml:mo> <mml:mn>6.2</mml:mn> </mml:mrow> </mml:msubsup> </mml:math> minutes, using the ICCF and JAVELIN methods. The velocity dispersion ( σ line ) of the broad-line clouds is measured to be <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:msubsup> <mml:mrow> <mml:mn>544.7</mml:mn> </mml:mrow> <mml:mrow> <mml:mo>−</mml:mo> <mml:mn>25.1</mml:mn> </mml:mrow> <mml:mrow> <mml:mo>+</mml:mo> <mml:mn>22.4</mml:mn> </mml:mrow> </mml:msubsup> </mml:math> km s −1 , yielding a black hole mass of ∼ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:msubsup> <mml:mrow> <mml:mn>2.2</mml:mn> </mml:mrow> <mml:mrow> <mml:mo>−</mml:mo> <mml:mn>0.2</mml:mn> </mml:mrow> <mml:mrow> <mml:mo>+</mml:mo> <mml:mn>0.2</mml:mn> </mml:mrow> </mml:msubsup> <mml:mo>×</mml:mo> <mml:msup> <mml:mrow> <mml:mn>10</mml:mn> </mml:mrow> <mml:mrow> <mml:mn>4</mml:mn> </mml:mrow> </mml:msup> <mml:msub> <mml:mrow> <mml:mi>M</mml:mi> </mml:mrow> <mml:mrow> <mml:mo>⊙</mml:mo> </mml:mrow> </mml:msub> </mml:math> and an Eddington ratio of 0.06.

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Publication Details

Journal
The Astrophysical Journal
Published
2024-11-01
DOI
https://doi.org/10.3847/1538-4357/ad7fe1
Citations
6
Primary Topic
Astrophysical Phenomena and Observations
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article
Field-Weighted Citation Impact
1.99
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article

Spectrophotometric Reverberation Mapping of Intermediate-mass Black Hole NGC 4395

Priyanka Jalan, Jong-Hak Woo, Amitesh Omar, Archana Gupta et al.
6 citations
The Astrophysical Journal
Astrophysical Phenomena and Observations
1.99
article

Spectrophotometric Reverberation Mapping of Intermediate-mass Black Hole NGC 4395

Priyanka Jalan, Jong-Hak Woo, Amitesh Omar, Archana Gupta, C. S. Stalin, Krishan Chand, Suvendu Rakshit, Amit Kumar Mandal, Hojin Cho, Shivangi Pandey, Jincen Jose
article en
6 citations

Abstract

Abstract Understanding the origins of massive black hole seeds and their coevolution with their host galaxy requires studying intermediate-mass black holes (IMBHs) and estimating their mass. However, measuring the masses of these IMBHs is challenging, due to the high-spatial-resolution requirement. Spectrophotometric reverberation monitoring is performed for a low-luminosity Seyfert 1 galaxy, NGC 4395, to measure the size of the broad-line region and black hole mass. The data were collected using the 1.3 m Devasthal fast optical telescope and 3.6 m Devasthal optical telescope at ARIES, Nainital, over two consecutive days in 2022 March. The analysis revealed strong emission lines in the spectra and light curves of the merged 5100 Å spectroscopic continuum flux ( f 5100 ) with the photometric continuum V band and H α , with fractional variabilities of 6.38% and 6.31% respectively. In comparison to several previous studies with lag estimation &lt;90 minutes, our calculated H α lag supersedes them by <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:msubsup> <mml:mrow> <mml:mn>125.0</mml:mn> </mml:mrow> <mml:mrow> <mml:mo>−</mml:mo> <mml:mn>6.1</mml:mn> </mml:mrow> <mml:mrow> <mml:mo>+</mml:mo> <mml:mn>6.2</mml:mn> </mml:mrow> </mml:msubsup> </mml:math> minutes, using the ICCF and JAVELIN methods. The velocity dispersion ( σ line ) of the broad-line clouds is measured to be <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:msubsup> <mml:mrow> <mml:mn>544.7</mml:mn> </mml:mrow> <mml:mrow> <mml:mo>−</mml:mo> <mml:mn>25.1</mml:mn> </mml:mrow> <mml:mrow> <mml:mo>+</mml:mo> <mml:mn>22.4</mml:mn> </mml:mrow> </mml:msubsup> </mml:math> km s −1 , yielding a black hole mass of ∼ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:msubsup> <mml:mrow> <mml:mn>2.2</mml:mn> </mml:mrow> <mml:mrow> <mml:mo>−</mml:mo> <mml:mn>0.2</mml:mn> </mml:mrow> <mml:mrow> <mml:mo>+</mml:mo> <mml:mn>0.2</mml:mn> </mml:mrow> </mml:msubsup> <mml:mo>×</mml:mo> <mml:msup> <mml:mrow> <mml:mn>10</mml:mn> </mml:mrow> <mml:mrow> <mml:mn>4</mml:mn> </mml:mrow> </mml:msup> <mml:msub> <mml:mrow> <mml:mi>M</mml:mi> </mml:mrow> <mml:mrow> <mml:mo>⊙</mml:mo> </mml:mrow> </mml:msub> </mml:math> and an Eddington ratio of 0.06.

The Astrophysical JournalVol. 976(1)
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Astrophysical Phenomena and Observations
1.99
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