Two decades ago, very large sources such as the building size ICF lasers were used as the energy sources to drive the first X‐ray lasers. Tremendous progress has been made over the last two decades to produce tabletop, high‐repetition rate X‐ray lasers that can be used as tools for applications. With the use of high‐reflectivity multilayer mirrors, many of the standard optical techniques such as interferometry can be extended to the soft X‐ray regime between wavelengths of 10 and 50 nm. The dominant X‐ray laser schemes are the monopole collisional excitation lasers either driven by chirped pulse amplification (CPA) laser systems or capillary discharge. The CPA systems drive lasing in neon‐like or nickel‐like ions, typically in the 10‐ to 30‐nm range, while the capillary system is currently limited to driving neon‐like ions at a longer wavelength near 50 nm. Most researchers use nickel‐like ion lasers near 14 nm because they are well matched to the Mo:Si multilayer mirrors, which have peak reflectivity near 13 nm, and are an essential component of applications such as X‐ray laser interferometry.