J/A+A/587/L7        Metallicity from Type II SN from (i)PTF  (Taddia+, 2016)

Metallicity from Type II supernovae from the (i)PTF. Taddia F., Moquist P., Sollerman J., Rubin A., Leloudas G., Gal-Yam A., Arcavi I., Cao Y., Filippenko A.V., Graham M.L., Mazzali P.A., Nugent P.E., Pan Y.-C., Silverman J.M., Xu D., Yaron O. <Astron. Astrophys., 587, L7-7 (2016)> =2016A&A...587L...7T 2016A&A...587L...7T (SIMBAD/NED BibCode)
ADC_Keywords: Galaxies, nearby ; Supernovae ; Abundances Keywords: supernovae: general - Galaxy: abundances Abstract: Type IIP supernovae (SNe IIP) have recently been proposed as metallicity (Z) probes. The spectral models of Dessart et al. (2014MNRAS.440.1856D 2014MNRAS.440.1856D) showed that the pseudo-equivalent width of FeII λ5018 (pEW5018) during the plateau phase depends on the primordial Z, but there was a paucity of SNe IIP exhibiting pEW5018 that were compatible with Z<0.4Z. This lack might be due to some physical property of the SN II population or to the fact that those SNe have been discovered in luminous, metal-rich targeted galaxies. Here we use SN II observations from the untargeted (intermediate) Palomar Transient Factory [(i)PTF] survey, aiming to investigate the pEW5018 distribution of this SN population and, in particular, to look for the presence of SNe II at lower Z. We perform pEW5018 measurements on the spectra of a sample of 39 (i)PTF SNe II, selected to have well-constrained explosion epochs and light-curve properties. Based on the comparison with the pEW5018 spectral models, we subgrouped our SNe into four Z bins from Z≃0.1 Z up to Z≃2 Z. We also independently investigated the Z of the hosts by using their absolute magnitudes and colors and, in a few cases, using strong-line diagnostics from spectra. We searched for possible correlations between SN observables, such as their peak magnitudes and the Z inferred from pEW5018. We found 11 events with pEW5018 that were small enough to indicate Z≃0.1 Z. The trend of pEW5018 with Z matches the Z estimates obtained from the host-galaxy photometry, although the significance of the correlation is weak. We also found that SNe with brighter peak magnitudes have smaller pEW5018 and occur at lower Z. Description: We collected the optical spectra of the 57 SNe II presented by R15, as obtained by the (i)PTF collaboration. The selected spectra were obtained with many different telescopes and instruments, as summarized in Table A.1. For each spectrum where FeIIλ5018 was identified, we established the phase, based on the explosion date reported by Rubin et al. (2016ApJ...820...33R 2016ApJ...820...33R). File Summary: -------------------------------------------------------------------------------- FileName Lrecl Records Explanations -------------------------------------------------------------------------------- ReadMe 80 . This file tablea1.dat 56 39 Log of spectral observations and pEW measurements tablea2.dat 109 39 Log of metallicity estimates and galaxy properties for our sample of (i)PTF SNe II -------------------------------------------------------------------------------- Byte-by-byte Description of file: tablea1.dat -------------------------------------------------------------------------------- Bytes Format Units Label Explanations -------------------------------------------------------------------------------- 1- 5 A5 --- SN (i)PTF SN designation (YYaaa) 6 A1 --- n_SN [*] Note on SN (G1) 8- 13 F6.2 d Phase Phase, from explosion date, and corrected for time dilation 15- 18 F4.2 d e_Phase rms uncertainty on Phase 20- 24 F5.2 0.1nm mpEW5018 Opposite of the pseudo equivalent width of FeII 5018Å, -pEW5018 26- 29 F4.2 0.1nm e_mpEW5018 rms uncertainty on mpEW5018 31- 44 A14 --- Tel Telescope+Instrument 47- 56 A10 "date" Obs.date Observation date -------------------------------------------------------------------------------- Byte-by-byte Description of file: tablea2.dat -------------------------------------------------------------------------------- Bytes Format Units Label Explanations -------------------------------------------------------------------------------- 1- 5 A5 --- SN (i)PTF SN designation (YYaaa) 6 A1 --- n_SN [*] Note on SN (G1) 8- 35 A28 --- Host Host-galaxy name 37- 38 I2 h RAh ? Host-galaxy right ascension (J2000) 40- 41 I2 min RAm ? Host-galaxy right ascension (J2000) 43- 48 F6.3 s RAs ? Host-galaxy right ascension (J2000) 50 A1 --- DE- Host-galaxy declination sign (J2000) 51- 52 I2 deg DEd ? Host-galaxy declination (J2000) 54- 55 I2 arcmin DEm ? Host-galaxy declination (J2000) 57- 61 F5.2 arcsec DEs ? Host-galaxy declination (J2000) 63- 66 F4.2 --- dSN/Rg ?=- Deprojected distance of each SN from its host-galaxy center (normalized by the De Vaucouleurs g-band radius of the host) 68- 73 F6.2 mag rMAG ?=- Absolute r-band magnitude of the host galaxy 75- 79 F5.2 mag g-r ?=- g-r color index of the host galaxy 81- 84 F4.2 Sun Zhost1 ?=- Host Z position as measured from the luminosity-metallicity relation (LZ) (2) 86- 89 F4.2 Sun Zhost2 ?=- Host Z position as measured from the luminosity-color-metallicity relation (LCZ) (2) 91- 94 F4.2 Sun Zhost3 ?=- Host Z position as measured from the strong-line diagnostic (O3N2; Pettini & Pagel, 2004MNRAS.348L..59P 2004MNRAS.348L..59P) (2) 96- 99 F4.2 Sun ZSN1 ?=- SN Z position as measured from the luminosity-metallicity relation (LZ) (2) 101-104 F4.2 Sun ZSN2 ?=- SN Z position as measured from the luminosity-color-metallicity relation (LCZ) (2) 106-109 F4.2 Sun ZSN3 ?=- Host Z position as measured from the strong-line diagnostic (O3N2; Pettini & Pagel, 2004MNRAS.348L..59P 2004MNRAS.348L..59P) (2) -------------------------------------------------------------------------------- Note (2): When computing the metallicity at the SN distance from the host-galaxy center, we converted the average Z gradient in units of DeVRad_g-1 by multiplying the metallicity gradient by 0.3, which is the typical ratio between DeVRad_g-1 and the isophotal radius in the g-band. The isophotal radius, isoA_g, is available only for the SDSS galaxies in the DR7. The host of PTF10vdl is not detected, those of PTF09fma, PTF11hsj, and PTF11hzt are not in the SDSS footprint. We exclude these hosts from the analysis presented in Fig. 3. The vast majority of our SN hosts are in the optimal Mg-(g-r) range where the LCZ relation was calibrated. The adoption of a standard gradient for all the host galaxies is a strong assumption and could lead to erroneous local metallicity estimates for some of the SNe if their actual gradient is significantly different from ours, as it could be for dwarf galaxies. -------------------------------------------------------------------------------- Glonal notes: Note (G1): *: SN IIL. The other objects are SNe IIP. -------------------------------------------------------------------------------- History: From electronic version of the journal
(End) Patricia Vannier [CDS] 09-Jun-2016
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