2011/06/30 by R. Nordon, D. Lutz, R. Genzel +34 · 2 citations
Physics and Astronomy · #Astronomy #Astronomy and Astrophysical Research #Astrophysics #Galaxies: Formation, Evolution, Phenomena #Galaxy #Gamma-ray bursts and supernovae #Infrared #Luminosity #Luminous infrared galaxy #Photometry (optics) #Physics #Redshift #Spectral energy distribution #Spectral line #Star formation #Stars #astro-ph.CO
paper · pdf · doi:10.1088/0004-637x/745/2/182
25 pages, 15 figures, accepted to ApJ; v3 include many minor modifications following the referee report, added a section comparing various z~2 IR template calibrations
arxiv created 2011/12/01 · openalex publication_date 2012/01/17 · arxiv updated 2015/05/28 · openalex created_date 2025/10/10 · openalex updated_date 2026/08/05
We combine Herschel -Photodetector Array Camera and Spectrometer (PACS) data from the PACS Evolutionary Probe (PEP) program with Spitzer 24 μm and 16 μm photometry and ultra deep Infrared Spectrograph (IRS) mid-infrared spectra to measure the mid- to far-infrared spectral energy distribution (SED) of 0.7 < z < 2.5 normal star-forming galaxies (SFGs) around the main sequence (the redshift-dependent relation of star formation rate (SFR) and stellar mass). Our very deep data confirm from individual far-infrared detections that z ∼ 2 SFRs are overestimated if based on 24 μm fluxes and SED templates that are calibrated via local trends with luminosity. Galaxies with similar ratios of rest-frame ν L ν (8) to 8–1000 μm infrared luminosity (LIR) tend to lie along lines of constant offset from the main sequence. We explore the relation between SED shape and offset in specific star formation rate (SSFR) from the redshift-dependent main sequence. Main-sequence galaxies tend to have a similar ν L ν (8)/LIR regardless of LIR and redshift, up to z ∼ 2.5, and ν L ν (8)/LIR decreases with increasing offset above the main sequence in a consistent way at the studied redshifts. We provide a redshift-independent calibration of SED templates in the range of 8–60 μm as a function of Δlog(SSFR) offset from the main sequence. Redshift dependency enters only through the evolution of the main sequence with time. Ultra deep IRS spectra match these SED trends well and verify that they are mostly due to a change in ratio of polycyclic aromatic hydrocarbon (PAH) to LIR rather than continua of hidden active galactic nuclei (AGNs). Alternatively, we discuss the dependence of ν L ν (8)/LIR on LIR. The same ν L ν (8)/LIR is reached at increasingly higher LIR at higher redshift, with shifts relative to local by 0.5 and 0.8 dex in log(LIR) at redshifts z ∼ 1 and z ∼ 2. Corresponding SED template calibrations are provided for use if no stellar masses are on hand. For most of those z ∼ 2 SFGs that also host an AGN, the mid-infrared is dominated by the star-forming component.