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The Link Between the Hidden Broad Line Region and the Accretion Rate in Seyfert 2 Galaxies

Cosmology and Nongalactic Astrophysics · Submitted 25 Jan 2012

abstract compiled · 2026-09-23 · no language-model review

The authors' main claim In the following, we will present evidence that accretion rate is also a key parameter for the presence of Hidden Broad Line Regions in Seyfert 2 galaxies.

how it is stated · asserted 0.81 read the record →

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arXiv ID1201.5397 (version 1)
Pith ID2F6U6VEY, Pith's permanent record of this paper and its review
CitationAndrea Marinucci, Andy D. Goulding, Fabrizio Nicastro, Giorgio Matt, Stefano Bianchi. "The Link Between the Hidden Broad Line Region and the Accretion Rate in Seyfert 2 Galaxies." arXiv:1201.5397 (2012). https://pith.science/paper/2F6U6VEY
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The compiled record

The paper's own sentences, arranged. Each label is drawn from a closed vocabulary; the number beside it is the probability the classifier gave that label. Numbers in the tables are the authors', checked by code. No sentence in this record was written by a model.

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Compiled by classifier-1.13-20260917 via OpenRouter, question bank abstract-p1-20260923, 2026-09-23: 1 request, 8,593 input tokens, $0.0004 reported.

What the abstract itself states, as probabilities: claims first 0.03 · states limitation 0.83 · human participants 0.01 · controlled comparison 0.73 · randomized assignment 0.01 · states quantitative result 0.98 · compares with prior results 0.53 · mentions code or data availability 0.02.

The abstract, sentence by sentence

arXiv listing abstract v1. Results and the main claim are underlined; .

In the past few years more and more pieces of evidence have been presented for a revision of the widely accepted Unified Model of Active Galactic Nuclei. A model based solely on orientation cannot explain all the observed phenomenology. In the following, we will present evidence that accretion rate is also a key parameter for the presence of Hidden Broad Line Regions in Seyfert 2 galaxies. Our sample consists of 21 sources with polarized Hidden Broad Lines and 18 sources without Hidden Broad Lines. We use stellar velocity dispersions from several studies on the CaII and Mg b triplets in Seyfert 2 galaxies, to estimate the mass of the central black holes via the Mbh-{\sigma}\ast relation. The ratio between the bolometric luminosity, derived from the intrinsic (i.e. unabsorbed) X-ray luminosity, and the Eddington luminosity is a measure of the rate at which matter accretes onto the central supermassive black hole. A separation between Compton-thin HBLR and non-HBLR sources is clear, both in accretion rate (log Lbol/LEdd = -1.9) and in luminosity (log Lbol = 43.90). When, properly luminosity-corrected, Compton-thick sources are included, the separation between HBLR and non-HBLR is less sharp but no HBLR source falls below the Eddington ratio threshold. We speculate that non-HBLR Compton-thick sources with accretion rate higher than the threshold, do possess a BLR, but something, probably related to their heavy absorption, is preventing us from observing it even in polarized light. Our results for Compton-thin sources support theoretical expectations. In a model presented by Nicastro (2000), the presence of broad emission lines is intrinsically connected with disk instabilities occuring in proximity of a transition radius, which is a function of the accretion rate, becoming smaller than the innermost stable orbit for very low accretion rates and therefore luminosities.

background contribution method result interpretation main claim

What the classifier reports for each sentence. The number is the probability it gave the label.
#sentencerolethe authors' own workstates the main conclusionstrength
s0 In the past few years more and more pieces of evidence have been presented for a revision of the widely accepted Unified Model of Active Galactic Nuclei. background 1.00 0.04 0.02 asserted 0.98
s1 A model based solely on orientation cannot explain all the observed phenomenology. background 0.76 0.07 0.04 asserted 1.00
s2 In the following, we will present evidence that accretion rate is also a key parameter for the presence of Hidden Broad Line Regions in Seyfert 2 galaxies. contribution 0.96 0.33 0.70 asserted 0.81
s3 Our sample consists of 21 sources with polarized Hidden Broad Lines and 18 sources without Hidden Broad Lines. method 0.85 0.79 0.02 asserted 0.96
s4 We use stellar velocity dispersions from several studies on the CaII and Mg b triplets in Seyfert 2 galaxies, to estimate the mass of the central black holes via the Mbh-{\sigma}\ast relation. method 1.00 0.73 0.02 asserted 0.99
s5 The ratio between the bolometric luminosity, derived from the intrinsic (i.e. unabsorbed) X-ray luminosity, and the Eddington luminosity is a measure of the rate at which matter accretes onto the central supermassive black hole. method 0.87 0.19 0.03 asserted 1.00
s6 A separation between Compton-thin HBLR and non-HBLR sources is clear, both in accretion rate (log Lbol/LEdd = -1.9) and in luminosity (log Lbol = 43.90). result 1.00 0.90 0.44 asserted 1.00
s7 When, properly luminosity-corrected, Compton-thick sources are included, the separation between HBLR and non-HBLR is less sharp but no HBLR source falls below the Eddington ratio threshold. result 0.98 0.88 0.19 asserted 0.99
s8 We speculate that non-HBLR Compton-thick sources with accretion rate higher than the threshold, do possess a BLR, but something, probably related to their heavy absorption, is preventing us from observing it even in polarized light. interpretation 1.00 0.31 0.12 speculative 1.00
s9 Our results for Compton-thin sources support theoretical expectations. interpretation 0.89 0.76 0.09 asserted 0.89
s10 In a model presented by Nicastro (2000), the presence of broad emission lines is intrinsically connected with disk instabilities occuring in proximity of a transition radius, which is a function of the accretion rate, becoming smaller than the innermost stable orbit for very low accretion rates and therefore luminosities. interpretation 0.60 0.04 0.07 asserted 0.87

What kind of paper the classifier reports this is: empirical study 1.00 · evidence from analysis of existing data 0.98.

What was examined, and what was not

sources read
  • arXiv listing abstract v1
not examined
  • full text
  • figures and tables
  • references and citing sentences
  • relations to other papers
levels run
  • P abstract
not run
  • S sections
  • T body sentences
  • C citations
  • R cross-paper relations

Every quoted sentence on this record is the authors'. Every label is from Pith's closed vocabulary, with the probability shown beside it. Every number in the measurements table is the authors', checked by code. Record as JSON

The paper
Original abstract

In the past few years more and more pieces of evidence have been presented for a revision of the widely accepted Unified Model of Active Galactic Nuclei. A model based solely on orientation cannot explain all the observed phenomenology. In the following, we will present evidence that accretion rate is also a key parameter for the presence of Hidden Broad Line Regions in Seyfert 2 galaxies. Our sample consists of 21 sources with polarized Hidden Broad Lines and 18 sources without Hidden Broad Lines. We use stellar velocity dispersions from several studies on the CaII and Mg b triplets in Seyfert 2 galaxies, to estimate the mass of the central black holes via the Mbh-{\sigma}\ast relation. The ratio between the bolometric luminosity, derived from the intrinsic (i.e. unabsorbed) X-ray luminosity, and the Eddington luminosity is a measure of the rate at which matter accretes onto the central supermassive black hole. A separation between Compton-thin HBLR and non-HBLR sources is clear, both in accretion rate (log Lbol/LEdd = -1.9) and in luminosity (log Lbol = 43.90). When, properly luminosity-corrected, Compton-thick sources are included, the separation between HBLR and non-HBLR is less sharp but no HBLR source falls below the Eddington ratio threshold. We speculate that non-HBLR Compton-thick sources with accretion rate higher than the threshold, do possess a BLR, but something, probably related to their heavy absorption, is preventing us from observing it even in polarized light. Our results for Compton-thin sources support theoretical expectations. In a model presented by Nicastro (2000), the presence of broad emission lines is intrinsically connected with disk instabilities occuring in proximity of a transition radius, which is a function of the accretion rate, becoming smaller than the innermost stable orbit for very low accretion rates and therefore luminosities.

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References
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What this paper does with the arXiv papers it cites

Each citing sentence is taken from the citing paper's LaTeX source and typed by Pith's classifier. A label appears at probability 0.8 or more (0.95 for support), a contest at 0.7 or more; the quoted words are the citing authors'. How each label was checked · JSON

Papers whose main result relates to this one's

Found among the papers closest to this one by title and main claim. Pith's classifier compared each pair's main results and a second model family confirmed the relation; checked against two further families, shown conflicts agreed 118 times in 120 and shown same results 218 times in 239. The quoted sentence is the other paper's main claim.

States the same result 2 papers

What it cites · 7 sentences without a confident label

Uses the method or tool of 1 paper
Uses data or values from 6 papers
  • Our starting sample is mostly based on the spectropolarimetric surveys performed by [ref] on the Seyfert 2 galaxies included in the CfA [ref] and 12 $μ$m [ref] samples.

    The Extended 12 Micron Galaxy Sample · The Sample · 0.93

  • Stellar velocity dispersions ($σ_*$) were mainly taken from [ref] and [ref] .

    An atlas of Calcium triplet spectra of active galaxies · The BH mass sub-selection · 1.00

  • Columns: (a) Name of the object; (b) Instrument (AS: Chandra ACIS-S; PN: XMM-Newton EPIC pn; XIS: Suzaku XIS0+3) and obsid; (c) if Compton-thin, X if Compton-thick; (d) Stellar velocity dispersions; (e) Mass of the central BH in solar mass units; (f) Absorbing column density in $10^22$ cm$^-2$ units (g) Absorption corrected 2-10 keV luminosity; (h) Bolometric luminosity; (i) Accretion rate in Eddington units; (l) Extinction-corrected O [iii] ($λ 5007$ ) luminosity; (m) O [iv] ($λ25.89 μm$ ) luminosity (n) Reference for stellar velocity dispersions, HBLR (in order); References: (1) [ref] , (2) [ref] , (3) [ref] , (4) [ref] , (5) [ref] , (6) [ref] , (7) [ref] , (8) [ref] , (9 ) [ref] , (10) [ref] , (11) [ref] , (12) [ref] , (13) Other surveys

    A Study of the Direct-Fitting Method for Measurement of Galaxy Velocity Dispersions · The Sample · 0.98

Compares with 1 paper
Cites as background 2 papers

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