1. The Size, Structure & Ionization of the Broad-Line Region in NGC 3227 and NGC 4051 Nick Devereux (ERAU) Emily Heaton (ERAU) May 22 nd, 2013 Naples, Italy

2. NGC 3227 D = 21 Mpc Low luminosity, L bol /L edd < 10 -3

3. NGC 3227 D = 21 Mpc Low luminosity, L bol /L edd < 10 -3 Current paradigm is that BLR is small

4. NGC 3227 D = 21 Mpc Low luminosity, L bol /L edd < 10 -3 Current paradigm is that BLR is small New result: the reverberation radius marks just the inner radius of a much larger volume of ionized gas

5. BH mass in NGC 3227 is constrained by gas kinematics, reverberation mapping & stellar velocity dispersion; M  = (7 - 20) x 10 6 M  Davies et al., 2006, ApJ 646, 754 Hicks & Malkan 2008, ApJS 174, 31 Denney et al. 2010, ApJ 721, 715

6. HST spectra showing the time variable broad H  emission line.

7. The broad H  line in NGC 3227 with the narrow lines subtracted illustrating the line profile expected for the inflow model.

8. There are good reasons to consider an inflow All AGN pundits agree that AGN activity is fueled by gas flowing into a super-massive black hole. Stellar mass loss provides an abundant source of fuel. Since only zero angular momentum gas can free- fall into the BH, the inflowing gas has no rotation by definition.

9. Visualization of the Inflow

10. Gas is in spherically symmetric free-fall, v(r) = √ 2 GM(r)/r Mass, M(r) includes central MBH + stars Number density of inflowing points, N(r) Mass inflow rate, dm/dt  4πr 2 N(r) v(r) Steady State inflow, dm/dt  f(r) which implies N(r)  r -3/2 since r 2 r -3/2 r -1/2  f(r) Consequently, there are just 2 free parameters to model the shape of the broad emission line – the inner and outer radius of the ionized volume emitting Balmer lines. Inflow Model Parameters

11. The broad H  line in NGC 3227 with the narrow lines subtracted illustrating the line profile expected for the inflow model.

12. Uncertainties on the inner and outer radii are ~ 20% - 30% Inner radius, r i Outer radius, r o Χ 2 Surface

13. the inner radius uniquely defines the full width at zero intensity of the broad H  line

14. The inner radius of the inflow coincides with the reverberation radius! F var ~8%

15. Suggesting a new way to compute BH Masses using reverberation radii using the free-fall equation; M = R ΔV 2 /2G where ΔV is the half-width at zero intensity and R is the reverberation radius. This method negates the large ~ 5.5 correction factor, f, required for the virial product advocated by Peterson et al. (2004, ApJ 613, 682) and Onken et al., 2004, ApJ 615, 645. See Devereux & Heaton (2013), ApJ in press for more details.

16. Photoionization Model Analogous to that developed for HII regions by Osterbrock. The only difference is that the ionization is provided by the AGN Basic concept: Ionization balance Number of ionizing photons = number of recombinations

17. Photoionization Model Results

18. The outer radius of the BLR is ionization bounded.

20. Photoionization Model Results.

21. Electron density is low Ionization parameter is high

22. The size of the BLR depends, at least, on the neutral H gas density, n H ionizing photon rate, N ion For a given N ion, Low n H Large BLR“narrow line” NLS1, NGC 4051 High n H Small BLR “broad line” S1, NGC 3227

23. Kaspi et al., 2005, ApJ 629, 61

25. Please visit Poster # 15 by Emily Heaton!

29. In Summary…. The line profile modeling shows that the reverberation radius marks just the inner radius of a much larger volume of partially ionized gas. Consequently, the BLRs of LLAGNs are actually much larger than previously believed!

30. In Summary…. The line profile modeling shows that the reverberation radius marks just the inner radius of a much larger volume of partially ionized gas. Consequently, the BLRs of LLAGNs are actually much larger than previously believed! The photoionization modeling shows that the reverberation radius marks a transition from partially ionized gas to completely ionized gas as the AGN is approached.

31. In Summary…. The line profile modeling shows that the reverberation radius marks just the inner radius of a much larger volume of partially ionized gas. Consequently, the BLRs of LLAGNs are actually much larger than previously believed! The photoionization modeling shows that the reverberation radius marks a transition from partially ionized gas to completely ionized gas as the AGN is approached. Collectively, a spherically symmetric inflow is able to mimic the broad emission line profile shape. Further, the inner radius of the inflow coincides with the reverberation radius, suggesting a new way to compute BH masses using the free-fall equation.

32. Future Work will be to populate this diagram with approximately 24 additional AGNs listed in Peterson et al. (2004, ApJ 613, 682).

33. Backup Slides

34. Cloudy thinking? Our perception that the electron density, n, is high > 10 9 cm -3 is based primarily on Cloudy (Ferland et al., 1988, PASP, 110, 761). The problem with Cloudy is that it models the BLR as a single slab of fixed column density, N H = 10 23 cm -2, which it certainly is not! From which it follows that if r_ BLR is of the order of 10 17 - 10 18 cm, then, given the fixed column density, n ~ must be of the order of 10 5 - 10 6 cm -3, not > 10 9 cm -3, predicted by Cloudy for certain density sensitive emission line ratios.

35. Condition for a radiatively driven outflow, κL/4  cG > M  Where κ is the Thompson scattering opacity For NGC 3227, the condition is not satisfied by 2 orders of magnitude! ie. the AGN in NGC 3227 radiates substantially below the Eddington luminosity limit. Radiative outflow - not possible given the low luminosity of the AGN

36. Outer radius of the inflow ~ 90 lt-days. Inner radius of the inflow ~ 3 lt-days and coincides with the reverberation radius (Denney et al. 2010, 721,715). Inflow Gas Number Density, n > 10 6 cm -3 at the reverberation radius Inflow Filling Factor ~ 1 Mass Inflow Rate ~ 2 x 10 -2 M  /yr. Physical Properties of the Broad Line Region in NGC 3227 Inflow Properties