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:
- galSpecInfo (or alternative link);
- galSpecLine (or alternative link);
- galSpecExtra (or alternative link).
- galSpecIndx (or alternative link).
Notes:
References:
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 |