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Covering factor in AGNs: Evolution versus selection
Aims. In every proposed unification scheme for active galactic nuclei (AGNs), an integral element is the presence of circumnuclear dust arranged in torus-like structures, partially obscuring the nuclear (accretion-associated) radiation. A crucial model parameter in this context is the covering facto...
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Published in: | Astronomy and astrophysics (Berlin) 2024-02, Vol.682, p.A120 |
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creator | Rałowski, Mateusz Hryniewicz, Krzysztof Pollo, Agnieszka Stawarz, Łukasz |
description | Aims.
In every proposed unification scheme for active galactic nuclei (AGNs), an integral element is the presence of circumnuclear dust arranged in torus-like structures, partially obscuring the nuclear (accretion-associated) radiation. A crucial model parameter in this context is the covering factor (CF), which can be defined as the ratio of the infrared luminosity of the dusty torus,
L
IR
, to the accretion disk bolometric luminosity,
L
agn
. Recent research has discussed the potential redshift evolution of the CF. Our study aims to determine whether this observed evolution is genuine or if selection effects significantly influence it.
Methods.
Based on cross-matched multiwavelength photometrical data from the five major surveys (SDSS, GALEX, UKIDSS, WISE,
Spitzer
), a sample of over 17 000 quasars was derived. The main parameters of quasars, such as black hole masses and the Eddington ratios, were calculated based on the spectroscopic data. The data were divided into two redshift bins: low-
z
quasars (redshift from 0.7 to 1.1) and high-
z
quasars (from 2.0 to 2.4). The associated smaller datasets with higher quality data were constructed from the WISE
W
3 and
W
4 detections with
S
/
N
> 5 and the
Spitzer
MIPS 24 μm photometry. The CF was determined by computing the ratio of integrated luminosities,
L
IR
and
L
agn
, using two methods: power-law fitting and the area between all photometric points. We explored different selection effects and their influence on CF estimates. Finally, statistical tests were employed to assess the hypothesis of CF evolution within the higher-quality datasets.
Results.
We identified an issue with the accuracy of the WISE
W
4 filter. Whenever feasible, it is recommended to utilize
Spitzer
MIPS 24 μm data. Luminosities obtained through direct integration of all photometric data points exhibit higher accuracy compared to values derived from a power-law approximation. The Efron & Petrosian test confirmed the presence of luminosity evolution with redshift for both
L
IR
and
L
agn
. The low-
z
and high-
z
samples both exhibit a similar correlation between
L
agn
and
L
IR
. The calculated median CF values are comparable within the errors: log CF
low-
z
= −0.18 ± 0.11 and log CF
high-
z
= −0.01 ± 0.13. Additionally, the
Spitzer
photometry dataset reinforces this consistency with log CF
low-
z
= −0.19 ± 0.11 and log CF
high-
z
= −0.18 ± 0.11.
Conclusions.
No discernible evolution of the CF was observed in the subsample of quasars wi |
doi_str_mv | 10.1051/0004-6361/202245487 |
format | article |
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In every proposed unification scheme for active galactic nuclei (AGNs), an integral element is the presence of circumnuclear dust arranged in torus-like structures, partially obscuring the nuclear (accretion-associated) radiation. A crucial model parameter in this context is the covering factor (CF), which can be defined as the ratio of the infrared luminosity of the dusty torus,
L
IR
, to the accretion disk bolometric luminosity,
L
agn
. Recent research has discussed the potential redshift evolution of the CF. Our study aims to determine whether this observed evolution is genuine or if selection effects significantly influence it.
Methods.
Based on cross-matched multiwavelength photometrical data from the five major surveys (SDSS, GALEX, UKIDSS, WISE,
Spitzer
), a sample of over 17 000 quasars was derived. The main parameters of quasars, such as black hole masses and the Eddington ratios, were calculated based on the spectroscopic data. The data were divided into two redshift bins: low-
z
quasars (redshift from 0.7 to 1.1) and high-
z
quasars (from 2.0 to 2.4). The associated smaller datasets with higher quality data were constructed from the WISE
W
3 and
W
4 detections with
S
/
N
> 5 and the
Spitzer
MIPS 24 μm photometry. The CF was determined by computing the ratio of integrated luminosities,
L
IR
and
L
agn
, using two methods: power-law fitting and the area between all photometric points. We explored different selection effects and their influence on CF estimates. Finally, statistical tests were employed to assess the hypothesis of CF evolution within the higher-quality datasets.
Results.
We identified an issue with the accuracy of the WISE
W
4 filter. Whenever feasible, it is recommended to utilize
Spitzer
MIPS 24 μm data. Luminosities obtained through direct integration of all photometric data points exhibit higher accuracy compared to values derived from a power-law approximation. The Efron & Petrosian test confirmed the presence of luminosity evolution with redshift for both
L
IR
and
L
agn
. The low-
z
and high-
z
samples both exhibit a similar correlation between
L
agn
and
L
IR
. The calculated median CF values are comparable within the errors: log CF
low-
z
= −0.18 ± 0.11 and log CF
high-
z
= −0.01 ± 0.13. Additionally, the
Spitzer
photometry dataset reinforces this consistency with log CF
low-
z
= −0.19 ± 0.11 and log CF
high-
z
= −0.18 ± 0.11.
Conclusions.
No discernible evolution of the CF was observed in the subsample of quasars with high supermassive black hole (SMBH) mass bin or high luminosities, as the CF values for low-
z
and high-
z
quasars have the same distributions. The relationship between
L
IR
and
L
agn
deviates slightly from the expected 1:1 scaling, suggesting a more intricate connection between CF and
L
agn
. However, no statistically significant dependence of CF on luminosities could be claimed across the entire dataset (merged redshifts). It is worth noting that the low-
z
/low-luminosity portion of the CF distribution is influenced by contamination, possibly due to polar dust, as suggested in the literature, while the high-
z
/high-luminosity segment is affected by observational biases.</description><identifier>ISSN: 0004-6361</identifier><identifier>EISSN: 1432-0746</identifier><identifier>DOI: 10.1051/0004-6361/202245487</identifier><language>eng</language><publisher>Heidelberg: EDP Sciences</publisher><subject>Accretion disks ; Accuracy ; Active galactic nuclei ; Cosmic dust ; Data points ; Datasets ; Evolution ; Luminosity ; Parameters ; Photometry ; Power law ; Quasars ; Red shift ; Statistical tests ; Supermassive black holes ; Toruses</subject><ispartof>Astronomy and astrophysics (Berlin), 2024-02, Vol.682, p.A120</ispartof><rights>2024. This work is licensed under https://creativecommons.org/licenses/by/4.0 (the “License”). Notwithstanding the ProQuest Terms and conditions, you may use this content in accordance with the terms of the License.</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c322t-ad92719654ec99e9a077f4a9a8cc2f2eca453b8ce51ee3db77dff4c3067f040d3</citedby><cites>FETCH-LOGICAL-c322t-ad92719654ec99e9a077f4a9a8cc2f2eca453b8ce51ee3db77dff4c3067f040d3</cites><orcidid>0000-0002-0297-3346</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,776,780,27903,27904</link.rule.ids></links><search><creatorcontrib>Rałowski, Mateusz</creatorcontrib><creatorcontrib>Hryniewicz, Krzysztof</creatorcontrib><creatorcontrib>Pollo, Agnieszka</creatorcontrib><creatorcontrib>Stawarz, Łukasz</creatorcontrib><title>Covering factor in AGNs: Evolution versus selection</title><title>Astronomy and astrophysics (Berlin)</title><description>Aims.
In every proposed unification scheme for active galactic nuclei (AGNs), an integral element is the presence of circumnuclear dust arranged in torus-like structures, partially obscuring the nuclear (accretion-associated) radiation. A crucial model parameter in this context is the covering factor (CF), which can be defined as the ratio of the infrared luminosity of the dusty torus,
L
IR
, to the accretion disk bolometric luminosity,
L
agn
. Recent research has discussed the potential redshift evolution of the CF. Our study aims to determine whether this observed evolution is genuine or if selection effects significantly influence it.
Methods.
Based on cross-matched multiwavelength photometrical data from the five major surveys (SDSS, GALEX, UKIDSS, WISE,
Spitzer
), a sample of over 17 000 quasars was derived. The main parameters of quasars, such as black hole masses and the Eddington ratios, were calculated based on the spectroscopic data. The data were divided into two redshift bins: low-
z
quasars (redshift from 0.7 to 1.1) and high-
z
quasars (from 2.0 to 2.4). The associated smaller datasets with higher quality data were constructed from the WISE
W
3 and
W
4 detections with
S
/
N
> 5 and the
Spitzer
MIPS 24 μm photometry. The CF was determined by computing the ratio of integrated luminosities,
L
IR
and
L
agn
, using two methods: power-law fitting and the area between all photometric points. We explored different selection effects and their influence on CF estimates. Finally, statistical tests were employed to assess the hypothesis of CF evolution within the higher-quality datasets.
Results.
We identified an issue with the accuracy of the WISE
W
4 filter. Whenever feasible, it is recommended to utilize
Spitzer
MIPS 24 μm data. Luminosities obtained through direct integration of all photometric data points exhibit higher accuracy compared to values derived from a power-law approximation. The Efron & Petrosian test confirmed the presence of luminosity evolution with redshift for both
L
IR
and
L
agn
. The low-
z
and high-
z
samples both exhibit a similar correlation between
L
agn
and
L
IR
. The calculated median CF values are comparable within the errors: log CF
low-
z
= −0.18 ± 0.11 and log CF
high-
z
= −0.01 ± 0.13. Additionally, the
Spitzer
photometry dataset reinforces this consistency with log CF
low-
z
= −0.19 ± 0.11 and log CF
high-
z
= −0.18 ± 0.11.
Conclusions.
No discernible evolution of the CF was observed in the subsample of quasars with high supermassive black hole (SMBH) mass bin or high luminosities, as the CF values for low-
z
and high-
z
quasars have the same distributions. The relationship between
L
IR
and
L
agn
deviates slightly from the expected 1:1 scaling, suggesting a more intricate connection between CF and
L
agn
. However, no statistically significant dependence of CF on luminosities could be claimed across the entire dataset (merged redshifts). It is worth noting that the low-
z
/low-luminosity portion of the CF distribution is influenced by contamination, possibly due to polar dust, as suggested in the literature, while the high-
z
/high-luminosity segment is affected by observational biases.</description><subject>Accretion disks</subject><subject>Accuracy</subject><subject>Active galactic nuclei</subject><subject>Cosmic dust</subject><subject>Data points</subject><subject>Datasets</subject><subject>Evolution</subject><subject>Luminosity</subject><subject>Parameters</subject><subject>Photometry</subject><subject>Power law</subject><subject>Quasars</subject><subject>Red shift</subject><subject>Statistical tests</subject><subject>Supermassive black holes</subject><subject>Toruses</subject><issn>0004-6361</issn><issn>1432-0746</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2024</creationdate><recordtype>article</recordtype><recordid>eNo9kFFLwzAUhYMoOKu_wJeAz3U3uWnT-DbKnMLQF30OWZpIR21m0g7897ZM9nS4h49zOYeQewaPDAq2BACRl1iyJQfORSEqeUEWTCDPQYrykizOxDW5SWk_nZxVuCBYh6OLbf9FvbFDiLTt6Wrzlp7o-hi6cWhDTycgjYkm1zk7G7fkypsuubt_zcjn8_qjfsm375vXerXNLXI-5KZRXDJVFsJZpZwyIKUXRpnKWu65s0YUuKusK5hz2OykbLwXFqGUHgQ0mJGHU-4hhp_RpUHvwxj76aXmilcopZwSMoInysaQUnReH2L7beKvZqDndfTcXc_d9Xkd_AOypFZ-</recordid><startdate>20240201</startdate><enddate>20240201</enddate><creator>Rałowski, Mateusz</creator><creator>Hryniewicz, Krzysztof</creator><creator>Pollo, Agnieszka</creator><creator>Stawarz, Łukasz</creator><general>EDP Sciences</general><scope>AAYXX</scope><scope>CITATION</scope><scope>8FD</scope><scope>H8D</scope><scope>L7M</scope><orcidid>https://orcid.org/0000-0002-0297-3346</orcidid></search><sort><creationdate>20240201</creationdate><title>Covering factor in AGNs: Evolution versus selection</title><author>Rałowski, Mateusz ; Hryniewicz, Krzysztof ; Pollo, Agnieszka ; Stawarz, Łukasz</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c322t-ad92719654ec99e9a077f4a9a8cc2f2eca453b8ce51ee3db77dff4c3067f040d3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2024</creationdate><topic>Accretion disks</topic><topic>Accuracy</topic><topic>Active galactic nuclei</topic><topic>Cosmic dust</topic><topic>Data points</topic><topic>Datasets</topic><topic>Evolution</topic><topic>Luminosity</topic><topic>Parameters</topic><topic>Photometry</topic><topic>Power law</topic><topic>Quasars</topic><topic>Red shift</topic><topic>Statistical tests</topic><topic>Supermassive black holes</topic><topic>Toruses</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Rałowski, Mateusz</creatorcontrib><creatorcontrib>Hryniewicz, Krzysztof</creatorcontrib><creatorcontrib>Pollo, Agnieszka</creatorcontrib><creatorcontrib>Stawarz, Łukasz</creatorcontrib><collection>CrossRef</collection><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Astronomy and astrophysics (Berlin)</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Rałowski, Mateusz</au><au>Hryniewicz, Krzysztof</au><au>Pollo, Agnieszka</au><au>Stawarz, Łukasz</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Covering factor in AGNs: Evolution versus selection</atitle><jtitle>Astronomy and astrophysics (Berlin)</jtitle><date>2024-02-01</date><risdate>2024</risdate><volume>682</volume><spage>A120</spage><pages>A120-</pages><issn>0004-6361</issn><eissn>1432-0746</eissn><abstract>Aims.
In every proposed unification scheme for active galactic nuclei (AGNs), an integral element is the presence of circumnuclear dust arranged in torus-like structures, partially obscuring the nuclear (accretion-associated) radiation. A crucial model parameter in this context is the covering factor (CF), which can be defined as the ratio of the infrared luminosity of the dusty torus,
L
IR
, to the accretion disk bolometric luminosity,
L
agn
. Recent research has discussed the potential redshift evolution of the CF. Our study aims to determine whether this observed evolution is genuine or if selection effects significantly influence it.
Methods.
Based on cross-matched multiwavelength photometrical data from the five major surveys (SDSS, GALEX, UKIDSS, WISE,
Spitzer
), a sample of over 17 000 quasars was derived. The main parameters of quasars, such as black hole masses and the Eddington ratios, were calculated based on the spectroscopic data. The data were divided into two redshift bins: low-
z
quasars (redshift from 0.7 to 1.1) and high-
z
quasars (from 2.0 to 2.4). The associated smaller datasets with higher quality data were constructed from the WISE
W
3 and
W
4 detections with
S
/
N
> 5 and the
Spitzer
MIPS 24 μm photometry. The CF was determined by computing the ratio of integrated luminosities,
L
IR
and
L
agn
, using two methods: power-law fitting and the area between all photometric points. We explored different selection effects and their influence on CF estimates. Finally, statistical tests were employed to assess the hypothesis of CF evolution within the higher-quality datasets.
Results.
We identified an issue with the accuracy of the WISE
W
4 filter. Whenever feasible, it is recommended to utilize
Spitzer
MIPS 24 μm data. Luminosities obtained through direct integration of all photometric data points exhibit higher accuracy compared to values derived from a power-law approximation. The Efron & Petrosian test confirmed the presence of luminosity evolution with redshift for both
L
IR
and
L
agn
. The low-
z
and high-
z
samples both exhibit a similar correlation between
L
agn
and
L
IR
. The calculated median CF values are comparable within the errors: log CF
low-
z
= −0.18 ± 0.11 and log CF
high-
z
= −0.01 ± 0.13. Additionally, the
Spitzer
photometry dataset reinforces this consistency with log CF
low-
z
= −0.19 ± 0.11 and log CF
high-
z
= −0.18 ± 0.11.
Conclusions.
No discernible evolution of the CF was observed in the subsample of quasars with high supermassive black hole (SMBH) mass bin or high luminosities, as the CF values for low-
z
and high-
z
quasars have the same distributions. The relationship between
L
IR
and
L
agn
deviates slightly from the expected 1:1 scaling, suggesting a more intricate connection between CF and
L
agn
. However, no statistically significant dependence of CF on luminosities could be claimed across the entire dataset (merged redshifts). It is worth noting that the low-
z
/low-luminosity portion of the CF distribution is influenced by contamination, possibly due to polar dust, as suggested in the literature, while the high-
z
/high-luminosity segment is affected by observational biases.</abstract><cop>Heidelberg</cop><pub>EDP Sciences</pub><doi>10.1051/0004-6361/202245487</doi><orcidid>https://orcid.org/0000-0002-0297-3346</orcidid><oa>free_for_read</oa></addata></record> |
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subjects | Accretion disks Accuracy Active galactic nuclei Cosmic dust Data points Datasets Evolution Luminosity Parameters Photometry Power law Quasars Red shift Statistical tests Supermassive black holes Toruses |
title | Covering factor in AGNs: Evolution versus selection |
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