MKID

Contents

MKID#

API reference: MKID

As reported in [1], a superconducting microwave kinetic-inductance detector (MKID) is a novel concept of photo-detector tailored for wavelengths below a few millimetres [4]. Essentially, it is an LC micro-resonator with a superconducting photo-sensitive area, which is capable of detecting single photons; as well as providing a measurement on their arrival time and energy. Operationally, each photon impinging on the MKID breaks a number of superconducting charge carriers, called Cooper pairs, into quasi-particles. In turn, thanks to the principle of kinetic inductance, which becomes relevant only below a superconducting critical temperature, such a strike is converted into a sequence of microwave pulses (at a few $GHz$) with a wavelength-dependent profile; which are then read out one by one, on a single channel. An important caveat is that the photo-generated pulse profiles can be distinguished only if they do not overlap in time and if the read-out bandwidth is large enough. The situation is analogous to the “pulse pile-up” and “coincidence losses” of EM-CCDs, in photon-counting mode [e.g., Wilkins et al., 2014]. In other words, there is a maximum limit to the achievable count rate, which is inversely proportional to the minimum distance in time between distinguishable pulse profiles: the so-called “dead time”, which is fundamentally determined by the recombination time of quasi-particles re-forming Cooper pairs. Given this, an MKID-array per se can serve as an intrinsic integral-field spectrograph, at low resolution, without any dispersive elements or chromatic filters [5].

Below all available models for MKID are listed.

Available models#