[GEMINI]GEMINI OBSERVATORY
observing time request (HTML summary)
[GEMINI]

Semester: 2011BObserving Mode: queuePartner Lead Scientist:
Neil Nagar
Universidad de Concepcion
Instruments:
GMOS South
Gemini Reference:
Not Available
Partner:
Chile
Time Awarded:
Not Available
Thesis:
No
Band 3 Acceptable:
No


Title:Tracing gas flows in Active Galactic Nuclei down to the innermost few parsecs: Completion of a statistically meaningful "sample"
Partner Lead Scientist: Neil Nagar
Universidad de Concepcion
Principal Investigator:Neil Nagar
PI institution:Universidad de Concepcion, Departamento de Astronomia,Casilla 160 - C,Concepcion - Chile,Chile
PI status:PhD/Doctorate
PI phone / fax / e-mail:+56 (0)41 220 7171 / / nagar@astro-udec.cl
Co-investigators:Thaisa Storchi-Bergmann: Universidade Federal do Rio Grande do Sul (UFRGS), thaisa@ufrgs.br
Allan Schnorr Muller: Universidade Federal do Rio Grande do Sul (UFRGS), allan.schnorr@ufrgs.br

Partner Submission Details (multiple entries for joint proposals)
NTAC
PartnerPartner Lead
Scientist
Time
Requested
Minimum
Time
Requested
Reference
number
Recommended
time
Minimum
Recommended
Time
Rank
ChileNagar7.0 hours2.3 hoursNot Available0.0 hours0.0 hours

Total Time

7.0 hours


Abstract (199 words)

We propose GMOS IFU emission-line spectroscopy of the extended Halpha gas in the inner kiloparsec of nearby active galactic nuclei (AGN) hosts, selected for having dusty nuclear spirals, in order to test the hypothesis that these spirals trace the channels through which the nuclear supermassive black hole is being fed. This is a continuing study for which we have already data for 5 LINERs, 3 Seyfert 2 and 3 Seyfert 1 galaxies. The data in hand show that the Halpha kinematics within the inner kiloparsec presents streaming motions towards the nucleus with speeds of the order of 50 km/s. This result suggests that dusty nuclear spirals do trace inflows, and we now aim at correlating the mass inflow rates with the strength (luminosity) of the nuclear activity, in order to characterize the black hole accretion and growth in a statistically significant sample of galaxies, spanning a range of nuclear power. We thus need to include in our sample a range of AGN luminosities and, towards this goal, we now propose to use Gemini/GMOS-IFU to map the gas kinematics in the nearby Seyfert galaxies NGC1386, NGC1566 and NGC7213. Part of this sample will also be proposed to ALMA (Cycle 0).

Science Justification (999 words)

BACKGROUND: A long-standing problem in the study of the coeval evolution of galaxies and their black holes is understanding how mass is transferred from galactic scales down to nuclear scales to feed the supermassive black hole (hereafter SMBH). Many theoretical studies [1,2,3] and simulations have shown that non-axisymmetric potentials efficiently promote gas inflow towards the inner regions [4]. The large programs of Mundell & Nagar have shown that misaligned (by more than ~10degrees) stellar and gaseous kinematic axes leads to increased accretion rates in AGNs [5,6]. Recent observations have revealed that structures such as small-scale disks or nuclear bars and associated spiral arms are frequently observed in the inner kiloparsec of active galaxies [7,8,9]. The most common nuclear structures are dusty spirals, estimated to reside in more than half of active galaxies [10]. Further, a strong correlation between the presence of nuclear dust structures (filaments, spirals and disks) and accretion-related activity in galaxies has recently been reported [11]. This correlation between dust structures and accretion activity in galaxies along with the enhanced frequency of dusty spirals supports the hypothesis that nuclear spirals are a mechanism for fuelling the nuclear SMBH, transporting gas from kiloparsec scales down to a few tens of parsecs of the active nucleus [12,13,14,15,16,17,18,19]. This hypothesis has recently been confirmed by our group [18,20,21] in the cases of the LINER galaxies NGC1097 and NGC6951. Using GMOS-IFU spectroscopy we could kinematically map streaming motions of gas towards the nucleus approximately along dusty spiral arms, which are observed in HST images.

We have also used GMOS-IFU to map the gas kinematics in the nuclear region of another LINER galaxy: M81[22]. In this case, instead of using models of circular rotation to isolate streaming motions from the orbital motions in the galaxy potential, we used the stellar velocity field. The results are shown in Fig.1. Also, in order to further investigate additional kinematic components in the emitting gas, we have applied the technique of principal component analysis (PCA) [23] to the datacube. Relevant results are illustrated in Fig.2, which shows the "eigen-spectra" PC3 and PC4 in the bottom panels, and the corresponding tomograms in the top panels. These eigen-spectra and tomograms reveal two kinematic components: (1) a compact rotating disk (PC3), with radius of ~20 pc; (2) a compact outflow (PC4) perpendicular to the disk, whose presence is supported by previous radio data showing a compact jet.

GOALS OF THE PRESENT PROPOSAL: We aim to apply the techniques we have recently developed and described above to: (1) obtain the stellar kinematics from the fitting of the stellar absorption bands using the pPXF method [24]; (2) map the inflows around nearby AGN, as well as possible outflows, using models of circular rotation and the stellar kinematics as references for rotation in the galaxy gravitational field; (3) look for the association of inflows with nuclear spirals and outflows with radio components; (4) constrain physical parameters of the inflows and outflows such as the mass flow rate, geometry and gas density; (5) correlate these parameters with other properties of the galaxies and their active nuclei, such as the nuclear accretion rate, molecular gas content and host galaxy morphology.

SAMPLE: This is a continuing study for which we have already data for 5 LINERs, 3 Seyfert 2 and 3 Seyfert 1 galaxies. The data we have in hand show that the Halpha kinematics within the inner kiloparsec presents streaming motions towards the nucleus (see Fig. 1), suggesting that dusty nuclear spirals do trace inflows. We now aim at correlating the mass inflow rates with the strength (luminosity) of the nuclear activity, in order to characterize the black hole accretion and growth in a statistically significant sample of galaxies, spanning a range of nuclear power. In order to "fill the gaps" we have in nuclear power, we now propose to use Gemini/GMOS-IFU to map the gas kinematics in the nearby Seyfert galaxies NGC1386 (Seyfert 2), NGC1566 (Seyfert 1) and NGC7213 (Seyfert 1). With these galaxies we will complete a sample covering a range of nuclear power and activity types, comprising 5 LINERs, 4 Seyfert 2 and 4 Seyfert 1 galaxies. Preliminary results we have obtained for the galaxies NGC1358, NGC1667 and NGC2110 are shown in Fig.3, namely nuclear spiral structures in Halpha.

Althought there is publically availiable GMOS-IFU data of NGC1566 in the archive, the Halpha and [NII]6585A lines, both crucial to our analysis, are not measurable in this data, as they are affected by the gap between the CCDs. It is then necessary for us to observe this galaxy again.

REFERENCES: [1] Shlosman, I., Begelman, M. C., Frank, J. 1990, Nature, 345, 679. [2] Emsellem, E., Goudfrooij, P., Ferruit, P. 2003, MNRAS, 345, 1297. [3] Knapen, J. H. 2005, ApSS, 295, 85. [4] Englmaier, P., Shlosman, I. 2004, ApJ, 617, L115. [5] Gaelle, Mundell, Emsellem & Nagar 2007, MNRAS, 379, 1249. [6] Westoby, Mundell, Nagar, et al. 2011, submitted to ApJ. [7] Erwin, P., Sparke, L. S. 1999, ASPC, 182, 243. [8] Pogge, R. W., Martini, P. 2002, ApJ, 569, 624. [9] Laine, S. et al. 2003, AJ, 126, 2717. [10] Martini, P., Regan, M. W., Mulchaey, J. S., Pogge, R. W. 2003, ApJ, 589, 77. [11] Simoes Lopes R. D. et al., 2007, ApJ, 655, 718. [12] Knapen, J. et al. 2000, ApJ, 528, 219. [13] Emsellem, E., et al. 2001, A&A, 368, 52. [14] Maciejewski, W., et al. 2002, MNRAS, 329, 502. [15] Marconi A., et al. 2003, ApJ, 586, 868. [16] Crenshaw, D. M., Kraemer, S. B., Gabel, J. R. 2003, AJ, 126, 1690. [17] Fathi K. et al. 2005, MNRAS, 364, 773. [18] Fathi K., Storchi-Bergmann, T., et al. 2006, ApJ, 641, L25. [19] Maciejewski, W. 2004, MNRAS, 354, 892. [20] Storchi-Bergmann et al. 2007, ApJ, 670,959 [21] Riffel R. A., Storchi-Bergmann T., et al. 2008, MNRAS, 385, 1129. [22] Schnorr Muller, Allan; Storchi-Bergmann, T., et al. 2011, MNRAS, In Press (arXiv:1012.3015). [23] Steiner J. et al., 2009, MNRAS, 395, 64. [24] Cappellari & Emsellem, 2007, PASP, 431, 465.

Attachments:

NameSourceType
Fig. 1: Results for M81: From left to right: gaseous velocity field, stellar velocity field and the residual between gaseous and stellar velocity field. The straight white line indicates the position of the line of nodes. Gemini Observatory Tracing gas flows in Active Galactic Nuclei down to the innermost few parsecs Page 4fig1.jpegJPEG
Fig. 2:Principal component (PC) 3 (left) and 4 (right). PC3 shows the presence of a compact rotating disk in the central region of the galaxy and PC4 shows an outflow perpendicular to the disk. Gemini Observatory Tracing gas flows in Active Galactic Nuclei down to the innermost few parsecs Page 5fig2.jpegJPEG
Fig. 3: Halpha flux for NGC1358, NGC1667 and NGC2110. Strong nuclear spiral structures are seen in both NGC1358 and NGC2110.fig3.jpgJPEG

Technical Justification (764 words)

DESCRIPTION OF OBSERVATIONS: In order to reach our scientific goals we propose to obtain the 2D gas and stellar kinematics within the inner kiloparsec of the galaxies NGC1386, NGC1566 and NGC7213 at sub-arcsecond spatial resolution. We propose to do that by measuring the emission-line profiles (wavelengths, fluxes, widths) of a few of the brightest emission lines of the spectra, namely Halpha, [NII]6548,84 and [SII]6717,31, as well as the stellar absorption features present in the covered wavelength interval (see below). The streaming gas motions towards the center will appear (if present) only after the subtraction of the rotation component. The rotation component will be derived via modelling (as done for NGC1097) or, if the gaseous velocity field is too disturbed to be modelled (as is the case of M81) then the rotation component will be obtained from the stellar kinematics. We will then estimate the mass inflow rate which will be compared with the nuclear accretion rate (to feed the SMBH). With a sample covering a range of activity types, we will be able to test if the streaming velocities and mass inflow rates are related to the type and strength of the nuclear activity. Besides obtaining the gas kinematics we will be able to derive the gas excitation through the [NII]/Halpha ratio and gas density through the ratio of the two [SII] lines. We will also apply the PCA technique to the data as an alternate method of mapping inflows and outflows. This technique was succesfully applied to the M81 datacube and it has allowed us to unveil faint components which seem to map the inflows and also outflows at the smallest scales around the SMBH.

We propose to use the GMOS IFU with grating R400 in combination with the r(630nm) filter in order to cover the wavelength range 560-700nm, which includes the above emission lines and a suitable number of stellar absorption features to allow the derivation of the stellar kinematics. For an effective output slit width for the IFU=0.31", the spectral resolution will be: R=3523, which is adequate for our purposes, according to the results we have obtained in our previous studies. We propose to observe in two slit mode, which will allow an angular coverage of 5"x7". At the typical distance of the targets, in order to cover a large enough field to map the kinematics we propose to observe two adjacent IFU fields with 1 arcseconds of overlap, covering 9 arcsec along the major axis and 7 arcseconds along the minor axis. The surface brightness in the continuum for the three galaxies is approximately 1 x 10^{-16} erg s^{-1} cm^{-2} A^{-1} arcsec^{-2}. Using the ITC, we obtain an integration time of 45 min to obtain S/N ratios of about 8 in the continuum. The total exposure time (for two fields) will then be 90 min on-source plus 25min overheads = 115min per galaxy. We intend to flux calibrate the data, in order to derive the mass flow rate towards the center, thus we need to observe one standard star. Time required for the standard star (25min) is mainly overhead. We propose three observations of the standard, considering the possibility that all three galaxies are observed at different nights. The total time will thus be: 3 x 115 + 3 x 25 = 420 min=7 hr. The minimum time requested is 2.3 h for the observation of only one galaxy and standard.

THE NEED FOR GEMINI AND GMOS IFU: We need the large aperture of Gemini to reach faint emission levels and obtain an adequate spatial coverage of the gas emission. The 2D coverage of the GMOS IFU is essential to adequately constrain the velocity field, at the necessary spatial resolution. Without the spatial resolution provided by the GMOS-IFU we would not have been able to kinematically map the streaming motions in narrow spiral arms as we successfully did for NGC1097 and NGC6951 [16,18].

MEASUREMENTS TO BE MADE FROM THE DATA: We will measure the emission-line fluxes (Halpha, [NII] and [SII]), central wavelengths and line widths in order to map the gaseous distribution, excitation, density and, most important, the gas kinematics. We will also obtain the stellar kinematics from the fitting of the stellar absorption bands using the pPXF method [22]. The two-dimensional measurements will allows us to appropriately deal with the non-circular kinematic components and constrain the circumnuclear disk geometry. We will use the technique successfully used by Fathi et al. [16] and Storchi-Bergmann et al. [18] as well as those we have used for M81 [20] to quantify the non-circular motions and to separate them from the circular velocity.

Attachments:

NameSourceType
Integration Time Calculator resultsGemini_Integration_Time_Calculator_4.pdfPDF

Band 3 Information

This proposal cannot be scheduled in Band 3.

Observation Details

ObservationRADecBrightnessTotal Time
(including overheads)
NGC138603:36:46.2-35:59:57.0V=12.09115.0 minutes
     109-008358(wfs)3:37:14.179-35:57:31.1111.080 UCmag,10.127 Jmag,9.800 Kmagseparation 6.16
     observing conditions: Mediumresources: GMOS South
NGC156604:20:0.4-54:56:16.0V=10.33115.0 minutes
     071-009425(wfs)4:19:49.577-54:51:03.4412.322 UCmag,11.030 Jmag,10.693 Kmagseparation 5.44
     observing conditions: Mediumresources: GMOS South
NGC721322:09:16.3-47:10:0.0V=11.01115.0 minutes
     086-422954(wfs)22:09:45.89-47:13:15.6110.744 UCmag,9.891 Jmag,9.608 Kmagseparation 5.99
     observing conditions: Mediumresources: GMOS South
LTT 241505:56:24.3-27:51:28.8V=12.2125.0 minutes
     125-019963(wfs)5:56:01.812-27:47:14.8712.492 UCmag,10.895 Jmag,10.323 Kmagseparation 6.53
     observing conditions: Mediumresources: GMOS South
LTT 241505:56:24.3-27:51:28.8V=12.2125.0 minutes
     125-019963(wfs)5:56:01.812-27:47:14.8712.492 UCmag,10.895 Jmag,10.323 Kmagseparation 6.53
     observing conditions: Mediumresources: GMOS South
LTT 241505:56:24.3-27:51:28.8V=12.2125.0 minutes
     125-019963(wfs)5:56:01.812-27:47:14.8712.492 UCmag,10.895 Jmag,10.323 Kmagseparation 6.53
     observing conditions: Mediumresources: GMOS South

Resources

Observing Conditions
NameImage QualitySky BackgroundWater VaporCloud Cover
Medium70%80%Any70%

Scheduling Information:

Synchronous dates:

Optimal dates:

Impossible dates:


Allocation Committee Comments


Additional Information


Keyword Category: Extra Galactic

Keywords: Active galaxies, Dynamics, Emission lines, Galaxy bulges, Galaxy centers, Intergalactic medium, Seyfert galaxies, Survey

Publications:

Allocations:
ReferenceTime% UsefulStatus of previous data
GS-2010B-Q-196.6 hours100P.I. Nagar. Observed on 26-28 January 2011 (i.e. 2 months ago). Data has been processed (see Fig.3 of this proposal) and reveal interesting details (specifically spiral structures, not necessarily related to the nuclear radio jets). Datacubes currently being analyzed in detail. Publication in process.
GN-2010A-Q428.0 hours100P.I. Riffel. Data processed, publication in process
GN-2008B-Q-305.5 hours100Three papers published (Riffel, Storchi-Bergmann & Nagar, 2010, MNRAS, 404, 166; Riffel et al., 2010, ApJ, 713, 469; and Riffel & Storchi-Bergmann 2011, MNRAS, 411, 469
GN-2006A-SV-124.25 hours100NIFS SV programme. Results published in Riffel et al. 2008, MNRAS, 385, 1129.
GS-2005B-Q-653.0 hours100GNIRS IFU Band 3 programme. Results published in Riffel et al. 2009, MNRAS, 393, 783
GS-2004B-Q-253.8 hours100Results published (also a Gemini press release) : Fathi, K., Storchi-Bergmann, T. , Riffel, R., Winge, C., Axon, D., Robinson, A., Capetti, A. & Marconi, A. 2006: "Streaming motions towards the supermassive black hole in NGC1097", ApJ Letters, 641, L25.
GS-2004B-SV-264.8 hours100GNIRS IFU SV programme. Results published in: Riffel, R. A., Storchi-Bergmann, T., Winge, C. Barbosa, F. K. B., 2006: Gemini near-infrared integral field spectroscopy of the narrow-line region of ESO428-G14: kinematics, excitation and the role of the radio jet, MNRAS, 373, 2.
GN-2004A-Q-13.5 hours100Same as next (GN-2002-Q-15)
GN-2003A-Q-13.5 hours100Same as next (GN-2002-Q-15)
GN-2002B-Q-153.5 hours100Results published in: Barbosa, F. K. B., Storchi-Bergmann, T., Cid Fernandes, R., Winge, C. & Schmitt, H., 2006: "Gemini/GMOS IFU stellar kinematics of the nuclear region of six nearby active galaxies", MNRAS 371, 170, Another paper, on the gas kinematics of the same 6 galaxies is accepted for publication in MNRAS. Partial results including the gas kinematics have been published in the Proceedings of IAU Symp. 222, 2004, eds. Storchi Bergmann, Ho & Schmitt.


Proposal Contents

Summary
Investigators
Partner Submission Details
Abstract
Science Justification
Technical Justification
Band 3 Information
Observation Details
Allocation Committee Comments
Additional Information