MPA-JHU catalogue (dr1.MPA)

The table has 100 rows, 40 columns.

Description

This table contains properties for CAVITY galaxies, directly taken from the MPA-JHU (Max-Planck-Institute for Astrophysics-John Hopkins University) Catalogue. Further information corresponding to the data present in this table can be consulted in the following data models:

Notes:

  1. All the fluxes reported here are computed from Gaussian fits to continuum subtracted data. Note that the fit is done simultaneously to all the lines so deblending happens automatically. For more information check [galSpecLine].

References:

  1. MPA-JHU survey.
  2. (Kauffmann et al., 2003).
  3. (Brinchmann et al., 2004).
  4. (Tremonti et al., 2004).
  5. (Salim et al., 2007).

Columns

Name Type UCD Unit Description
galaxy int meta.id
meta.main

CAVITY ID

bestObjID char meta.id
meta.corr

Unique ID in SDSS database

specObjID char meta.id
meta.corr

Spectral ID in SDSS database

sn_median float stat.snr
stat.median

Median S/N per pixel of the whole spectrum [from galSpecInfo]

oii_3726_flux float phot.flux
[10⁻¹⁷·erg·cm⁻²·s⁻¹]

[OII]3726 Flux from Gaussian fit to continuum subtracted data.

oii_3726_flux_err float stat.error
phot.flux
[10⁻¹⁷·erg·cm⁻²·s⁻¹]

Uncertainty in oii_3726_flux

oii_3729_flux float phot.flux
[10⁻¹⁷·erg·cm⁻²·s⁻¹]

[OII]3729 Flux from Gaussian fit to continuum subtracted data.

oii_3729_flux_err float stat.error
phot.flux
[10⁻¹⁷·erg·cm⁻²·s⁻¹]

Uncertainty in oii_3729_flux

h_beta_flux float phot.flux
[10⁻¹⁷·erg·cm⁻²·s⁻¹]

Hβ Flux from Gaussian fit to continuum subtracted data.

h_beta_flux_err float stat.error
phot.flux
[10⁻¹⁷·erg·cm⁻²·s⁻¹]

Uncertainty in the h_beta_flux

oiii_5007_flux float phot.flux
[10⁻¹⁷·erg·cm⁻²·s⁻¹]

[OIII]5007 Flux from Gaussian fit to continuum subtracted data.

oiii_5007_flux_err float stat.error
phot.flux
[10⁻¹⁷·erg·cm⁻²·s⁻¹]

Uncertainty in oiii_5007_flux

h_alpha_cont float phot.flux
spect.continuum
[10⁻¹⁷·erg·cm⁻²·s⁻¹·Å⁻¹]

Continuum at line center from 200 pixel median smoothing of the emission-line subtracted continuum

h_alpha_cont_err float stat.error
phot.flux
[10⁻¹⁷·erg·cm⁻²·s⁻¹·Å⁻¹]

Uncertainty in h_alpha_cont

h_alpha_reqw float spect.line.eqWidth
spect.continuum
Å

The equivalent width of the continuum-subtracted emission line computed from straight integration over the bandpasses listed in [galSpecLine] (emission is negative). In this case the continuum comes from a running 200 pixel median and does not properly account for stellar absorption. In general the EQW measurements provide a better measure of the true equivalent width. The purpose of this measurement is to help characterize the stellar absorption effecting the line. (EW_stellar = REQW – EQW)

h_alpha_reqw_err float stat.error
spect.line.eqWidth
Å

Uncertainty in h_alpha_reqw

h_alpha_eqw float spect.line.eqWidth
spect.continuum
Å

The equivalent width of the CB08 continuum-subtracted emission line computed from straight integration over the bandpasses listed in [galSpecLine] (emission is negative). This properly takes into account stellar absorption. Note that it will not be correct in the case of blended lines (i.e., NII & Hα)

h_alpha_eqw_err float stat.error
spect.line.eqWidth
Å

Uncertainty in h_alpha_eqw

h_alpha_flux float phot.flux
[10⁻¹⁷·erg·cm⁻²·s⁻¹]

Hα Flux from Gaussian fit to continuum subtracted data.

h_alpha_flux_err float stat.error
phot.flux
[10⁻¹⁷·erg·cm⁻²·s⁻¹]

Uncertainty in h_alpha_flux

nii_6584_flux float phot.flux
[10⁻¹⁷·erg·cm⁻²·s⁻¹]

[NII]6584 Flux from Gaussian fit to continuum subtracted data.

nii_6584_flux_err float stat.error
phot.flux
[10⁻¹⁷·erg·cm⁻²·s⁻¹]

Uncertainty in nii_6584_flux

sii_6717_flux float phot.flux
[10⁻¹⁷·erg·cm⁻²·s⁻¹]

[SII]6717 Flux from Gaussian fit to continuum subtracted data.

sii_6717_flux_err float stat.error
phot.flux
[10⁻¹⁷·erg·cm⁻²·s⁻¹]

Uncertainty in sii_6717_flux

sii_6731_flux float phot.flux
[10⁻¹⁷·erg·cm⁻²·s⁻¹]

[SII]6731 Flux from Gaussian fit to continuum subtracted data.

sii_6731_flux_err float stat.error
phot.flux
[10⁻¹⁷·erg·cm⁻²·s⁻¹]

Uncertainty in sii_6731_flux

oh_p16 float phys.abund
stat.median

The 16th percentile of the Oxygen abundance derived using Charlot & Longhetti models. The values are reported as 12 + Log O/H. See Tremonti et al (2004) and Brinchmann et al (2004) for details. [from galSpecExtra]

oh_p50 float phys.abund
stat.median

The median estimate of the Oxygen abundance derived using Charlot & Longhetti models. The values are reported as 12 + Log O/H. See Tremonti et al (2004) and Brinchmann et al (2004) for details. [from galSpecExtra]

oh_p84 float phys.abund
stat.median

The 84th percentile of the Oxygen abundance derived using Charlot & Longhetti models. The values are reported as 12 + Log O/H. See Tremonti et al (2004) and Brinchmann et al (2004) for details. [from galSpecExtra]

lgm_tot_p16 float phys.mass
stat.median
[log(M☉)]

The 16th percentile of the Log total stellar mass PDF using model photometry. [from galSpecExtra]

lgm_tot_p50 float phys.mass
stat.median
[log(M☉)]

The median estimate of the Log total stellar mass PDF using model photometry. [from galSpecExtra]

lgm_tot_p84 float phys.mass
stat.median
[log(M☉)]

The 84th percentile of the Log total stellar mass PDF using model photometry. [from galSpecExtra]

sfr_tot_p16 float phys.SFR
stat.median
[log(M☉·yr⁻¹)]

The 16th percentile of the Log total SFR PDF. This is derived by combining emission line measurements from within the fibre where possible and aperture corrections are done by fitting models ala Gallazzi et al (2005), Salim et al (2007) to the photometry outside the fibre. For those objects where the emission lines within the fibre do not provide an estimate of the SFR, model fits were made to the integrated photometry. [from galSpecExtra]

sfr_tot_p50 float phys.SFR
stat.median
[log(M☉·yr⁻¹)]

The median estimate of the Log total SFR PDF. This is derived by combining emission line measurements from within the fibre where possible and aperture corrections are done by fitting models ala Gallazzi et al (2005), Salim et al (2007) to the photometry outside the fibre. For those objects where the emission lines within the fibre do not provide an estimate of the SFR, model fits were made to the integrated photometry. [from galSpecExtra]

sfr_tot_p84 float phys.SFR
stat.median
[log(M☉·yr⁻¹)]

The 84th percentile of the Log total SFR PDF. This is derived by combining emission line measurements from within the fibre where possible and aperture corrections are done by fitting models ala Gallazzi et al (2005), Salim et al (2007) to the photometry outside the fibre. For those objects where the emission lines within the fibre do not provide an estimate of the SFR, model fits were made to the integrated photometry. [from galSpecExtra]

specsfr_tot_p16 float phys.SFR
stat.median
[log(yr⁻¹)]

The 16th percentile of the Log total SPECSFR PDF. This is derived by combining emission line measurements from within the fibre where possible and aperture corrections are done by fitting models ala Gallazzi et al (2005), Salim et al (2007) to the photometry outside the fibre. For those objects where the emission lines within the fibre do not provide an estimate of the SFR, model fits were made to the integrated photometry. [from galSpecExtra]

specsfr_tot_p50 float phys.SFR
stat.median
[log(yr⁻¹)]

The median estimate of the Log total SPECSFR PDF. This is derived by combining emission line measurements from within the fibre where possible and aperture corrections are done by fitting models ala Gallazzi et al (2005), Salim et al (2007) to the photometry outside the fibre. For those objects where the emission lines within the fibre do not provide an estimate of the SFR, model fits were made to the integrated photometry. [from galSpecExtra]

specsfr_tot_p84 float phys.SFR
stat.median
[log(yr⁻¹)]

The 84th percentile of the Log total SPECSFR PDF. This is derived by combining emission line measurements from within the fibre where possible and aperture corrections are done by fitting models ala Gallazzi et al (2005), Salim et al (2007) to the photometry outside the fibre. For those objects where the emission lines within the fibre do not provide an estimate of the SFR, model fits were made to the integrated photometry. [from galSpecExtra]

d4000_n float phot.flux.density
arith.ratio

4000AA break, Balogh et al (1999) definition. [from galSpecIndx]

d4000_n_err float stat.error
phot.flux.density
arith.ratio

Uncertainty in d4000_n