The physical processes driving the chemical evolution of galaxies in the last ∼ 11 Gyr cannot be understood without directly probing the dust-obscured phase of star-forming galaxies and active galactic nuclei. This phase, hidden to optical tracers, represents the bulk of star formation and black hole accretion activity in galaxies at 1 < z < 3. Spectroscopic observations with a cryogenic infrared (IR) observatory like SPICA will be sensitive enough to peer through the dustobscured regions of galaxies and access the rest-frame mid-to far-IR range in galaxies at high-z. This wavelength range contains a unique suite of spectral lines and dust features that serve as proxies for the abundances of heavy elements and the dust composition, providing tracers with a feeble response to both extinction and temperature. In this work, we investigate how SPICA observations could be exploited to understand key aspects in the chemical evolution of galaxies: the assembly of nearby galaxies based on the spatial distribution of heavy element abundances, the global content of metals in galaxies reaching the knee of the luminosity function up to z ∼ 3, and the dust composition of galaxies at high-z. Possible synergies with facilities available in the late 2020s are also discussed. Keywords: galaxies: evolution -galaxies: active -galaxies: starburst -infrared: galaxies -techniques: spectroscopic telescopes
PrefaceThe following set of papers describe in detail the science goals of the future Space Infrared telescope for Cosmology and Astrophysics (SPICA). The SPICA satellite will employ a 2.5-m telescope, actively cooled to around 6 K, and a suite of mid-to far-IR spectrometers and photometric cameras, equipped with state of the art detectors. In particular the SPICA Far-Infrared Instrument (SAFARI) will be a grating spectrograph with low (R = 300) and medium (R 3 000-11 000) resolution observing modes instantaneously covering the 35-230 µm wavelength range. The SPICA Mid-Infrared Instrument (SMI) will have three operating modes: a large field of view (12 × 10 ) low-resolution 17-36 µm spectroscopic (R ∼ 50-120) and photometric camera at 34 µm, a medium resolution (R 2 000) grating spectrometer covering wavelengths of 17-36 µm, and a high-resolution echelle module (R 28 000) for the 12-18 µm domain. A large field of view (80 × 80 ), three channel (110, 220 and 350 µm), polarimetric camera will also be part of the instrument complement. These articles will focus on some of the major sci- *