We report on the development of Microwave Kinetic Inductance Detectors (MKIDs) using platinum silicide as the sensor material. MKIDs are an emerging superconducting detector technology, capable of measuring the arrival times of single photons to better than two microseconds and their energies to around ten percent. Previously, MKIDs have been fabricated using either sub-stoichiometric titanium nitride or aluminum, but TiN suffers from spatial inhomogeneities in the superconducting critical temperature and Al has a low kinetic inductance fraction, causing low detector sensitivity. To address these issues, we have instead fabricated PtSi microresonators with superconducting critical temperatures of 944±12 mK and high internal quality factors (Q i 10 6 ). These devices show typical quasiparticle lifetimes of τ qp ≈ 30-40 µs and spectral resolution, R = λ/∆λ, of 8 at 406.6 nm. We compare PtSi MKIDs to those fabricated with TiN and detail the substantial advantages that PtSi MKIDs have to offer.Microwave Kinetic Inductance Detectors (MKIDs 1 ) are low-temperature detectors capable of measuring the arrival times of single photons to better than two microseconds and their energies to around ten percent. MKID operation depends on the kinetic inductance effect 2 , an additional inductance term which can be exploited for single photon detection. Cooper Pairs are broken when a superconductor below its T c absorbs a photon, creating a population of unpaired electrons called quasiparticles. The sudden decrease in Cooper Pair density temporarily increases the kinetic inductance of the superconducting film. If a thin film superconductor is lithographically patterned into a microresonator, a photon absorption event will then act to momentarily decrease the resonant frequency of the microresonator. The energy of the incident photon is proportional to the number of broken Cooper Pairs, and therefore the change in frequency, giving MKIDs spectral resolution. MKIDs are naturally multiplexed by assigning each microresonator in an array a unique frequency during lithography. They can then be read out 3 using a frequency domain multiplexing scheme. With this method employed on the latest generation of digital microwave electronics, thousands detectors can be coupled to and read out using a single microwave transmission line 4 . Because the bandgap ∆ of a superconductor is roughly 10 4 times smaller than that of the silicon used in conventional charge-coupled devices (CCDs), MKIDs are capable of detecting the long wavelength photons that would typically pass right through a CCD. MKIDs can be operated over a broad wavelength range and a handful of MKID astronomy instruments in the submillimeter 5,6 and the ultraviolet, optical, and nearinfrared (UVOIR) 7,8 wavelength bands have been commissioned. Although our work is primarily focused on the a) pszypryt@physics.ucsb.edu UVOIR regime, MKIDs operating at all wavelengths benefit from advances in the superconducting sensor layer.We have chosen platinum silicide as the superconductor in our ...