# Tracing the cosmological evolution of stars and cold gas with CMB spectral surveys

## TL;DR

This paper explores how CMB spectral surveys can trace galaxy evolution by measuring the intensity of CO and [CII] emissions across cosmic time, providing insights into star formation and cold gas abundance.

## Contribution

It demonstrates the potential of CMB spectral distortion instruments and intensity mapping, combined with cross-correlation techniques, to measure line brightness and galaxy evolution parameters.

## Key findings

- Cross-correlation allows unambiguous line brightness measurements.
- Instrument calibration is critical due to foreground contamination.
- Sensitivity estimates for PIXIE vary with redshift.

## Abstract

A full account of galaxy evolution in the context of LCDM cosmology requires measurements of the average star-formation rate (SFR) and cold gas abundance across cosmic time. Emission from the CO ladder traces cold gas, and [CII] fine structure emission at 158 um traces the SFR. Intensity mapping surveys the cumulative surface brightness of emitting lines as a function of redshift, rather than individual galaxies. CMB spectral distortion instruments are sensitive to both the mean and anisotropy of the intensity of redshifted CO and [CII] emission. Large-scale anisotropy is proportional to the product of the mean surface brightness and the line luminosity-weighted bias. The bias provides a connection between galaxy evolution and its cosmological context, and is a unique asset of intensity mapping. Cross-correlation with galaxy redshift surveys allows unambiguous measurements of redshifted line brightness despite residual continuum contamination and interlopers. Measurement of line brightness through cross-correlation also evades cosmic variance and suggests new observation strategies. Galactic foreground emission is $\sim 10^3$ times larger than the expected signals, and this places stringent requirements on instrument calibration and stability. Under a range of assumptions, a linear combination of bands cleans continuum contamination sufficiently that residuals produce a modest penalty over the instrumental noise. For PIXIE, the $2 \sigma$ sensitivity to CO and [CII] emission scales from $\sim 5 \times 10^{-2}$ kJy/sr at low redshift to ~2 kJy/sr by reionization.