2015MNRAS.449..867B


Query : 2015MNRAS.449..867B

2015MNRAS.449..867B - Mon. Not. R. Astron. Soc., 449, 867-900 (2015/May-1)

P-MaNGA Galaxies: emission-lines properties - gas ionization and chemical abundances from prototype observations.

BELFIORE F., MAIOLINO R., BUNDY K., THOMAS D., MARASTON C., WILKINSON D., SANCHEZ S.F., BERSHADY M., BLANC G.A., BOTHWELL M., CALES S.L., COCCATO L., DRORY N., EMSELLEM E., FU H., GELFAND J., LAW D., MASTERS K., PAREJKO J., TREMONTI C., WAKE D., WEIJMANS A., YAN R., XIAO T., ZHANG K., ZHENG T., BIZYAEV D., KINEMUCHI K., ORAVETZ D. and SIMMONS A.

Abstract (from CDS):

MaNGA (Mapping Nearby Galaxies at Apache Point Observatory) is a 6-yr Sloan Digital Sky Survey (SDSS-IV) survey that will obtain spatially resolved spectroscopy from 3600 to 10 300Å for a representative sample of over 10 000 nearby galaxies. In this paper, we present the analysis of nebular emission-line properties using observations of 14 galaxies obtained with P-MaNGA, a prototype of the MaNGA instrument. By using spatially resolved diagnostic diagrams, we find extended star formation in galaxies that are centrally dominated by Seyfert/LINER-like emission, which illustrates that galaxy characterizations based on single fibre spectra are necessarily incomplete. We observe extended low ionization nuclear emission-line regions (LINER)-like emission (up to 1Re) in the central regions of three galaxies. We make use of the Hα equivalent width [EW(Hα)] to argue that the observed emission is consistent with ionization from hot evolved stars. We derive stellar population indices and demonstrate a clear correlation between Dn(4000) and EW(HδA) and the position in the ionization diagnostic diagram: resolved galactic regions which are ionized by a Seyfert/LINER-like radiation field are also devoid of recent star formation and host older and/or more metal-rich stellar populations. We also detect extraplanar LINER-like emission in two highly inclined galaxies, and identify it with diffuse ionized gas. We investigate spatially resolved metallicities and find a positive correlation between metallicity and star formation rate surface density. We further study the relation between N/O versus O/H on resolved scales. We find that, at given N/O, regions within individual galaxies are spread towards lower metallicities, deviating from the sequence defined by galactic central regions as traced by Sloan 3-arcsec fibre spectra. We suggest that the observed dispersion can be a tracer for gas flows in galaxies: infalls of pristine gas and/or the effect of a galactic fountain.

Abstract Copyright: © 2015 The Authors Published by Oxford University Press on behalf of the Royal Astronomical Society (2015)

Journal keyword(s): galaxies: abundances - galaxies: active - galaxies: evolution - galaxies: fundamental parameters - galaxies: ISM

Simbad objects: 15

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Number of rows : 15
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2024
#notes
1 NGC 891 H2G 02 22 32.907 +42 20 53.95 11.08 10.81 9.93 7.86   ~ 1669 2
2 NGC 2916 Sy2 09 34 57.5933209584 +21 42 18.960584796 12.81 12.74 12.05     ~ 153 1
3 Z 122-22 AG? 09 35 06.313 +21 37 39.89   15.6       ~ 19 0
4 UGC 5124 AG? 09 37 11.8172718720 +21 40 09.337997892   15.7       ~ 24 0
5 2MASS J09403025+2115136 G 09 40 30.2421564048 +21 15 13.691284920           ~ 7 0
6 2MASX J10495872+3624543 G 10 49 58.698 +36 24 54.03   16.5       ~ 12 0
7 MCG+06-24-030 LIN 10 52 59.0534371320 +37 36 48.297012588   15.1       ~ 17 0
8 UGC 6036 LIN 10 55 55.2559428168 +36 51 41.494143924   14.6       ~ 53 0
9 LEDA 2077998 G 10 57 46.620 +36 16 57.89           ~ 9 0
10 2MASX J11001209+3623137 G 11 00 12.109 +36 23 13.87           ~ 8 0
11 Mrk 796 AGN 13 46 49.486 +14 24 02.03   15.5       ~ 50 0
12 2MASX J13490999+1320492 G 13 49 10.0151401560 +13 20 49.400516400           ~ 7 0
13 IC 944 GiP 13 51 30.897 +14 05 31.66   14.7       ~ 78 0
14 2MASX J13521155+1359595 LIN 13 52 11.5543819776 +13 59 59.716058244   15.5       ~ 13 0
15 Z 74-13 AG? 13 56 55.397 +14 08 32.79   15.1       ~ 22 0

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