&lt;p&gt;The following are the objectives of this project:&lt;br /&gt;&lt;br /&gt;(1) Demonstration of 1600-element Kinetic Inductance Detector (KID) imaging array operating at 350 micron with near background-limited sensitivity, a critical development step for the Short Wavelength Camera (SWCam) on CCAT;&lt;br /&gt;&lt;br /&gt;(2) Demonstration of 400-element KID imaging array operating at 850 micron with near background-limited sensitivity, also a critical development step for CCAT cameras;&lt;br /&gt;&lt;br /&gt;(3) Phase-contrast wavefront sensing at 850 micron with improved sensitivity and accuracy, targeting the eventual measurement of the CCAT telescope surface.&amp;nbsp;&lt;br /&gt;&lt;br /&gt;The current worldwide state-of-the art for submillimeter imaging detectors is the U.K.&amp;rsquo;s SCUBA2 instrument, which has 5000 Transition-Edge Sensor (TES) detectors each at 450 and 850 micron. TES&amp;rsquo;s work well, but may have reached practical limits for a ground-based project in part due to the high detector cost (&amp;gt; $100/pixel).&amp;nbsp; KIDs, on the other hand, should achieve a detector cost of &amp;lt;$10/pixel in the medium term and are therefore the baseline for CCAT&amp;rsquo;s short-wavelength camera SWCam, which requires 50,000 detectors. KIDs&lt;br /&gt;manufactured at JPL have shown background-limited performance in the lab at 350 micron, and a 400-element first-generation prototype was tested at CSO in April 2013 (see Figure) with promising results. The SWCam detectors operate by absorbing radiation directly in the inductive element of a TiN film and are fabricated by remarkably simple lithography. 350 micron is the key band for CCAT, and the SWCam detector work to date has concentrated on this band.&amp;nbsp; By re-optimizing the detailed design according to the operating background power, KIDs can work at fundamental background-limited sensitivity limits over a wide range of applications. Given that 850 micron is also an important band for CCAT, we propose to test an 850 micron imaging KID array at CSO in FY14.&lt;br /&gt;&lt;br /&gt;In FY12 and FY13, JPL and Caltech demonstrated the first (to our knowledge) implementation of phase-contrast (or Zernike) wavefront sensing applied to a submillimeter telescope (see Figure). In this approach, the detector images the power distribution incident on the pupil (primary mirror), and the phase of the field from a point source is modulated in the image plane in order to map the wavefront in the pupil plane. The resolution in the wavefront mapping improves as the number of imaging elements available grows. The testing demonstrated basic operation of the wavefront sensor, with induced ~&amp;pi;/4 wavefront shifts over ~3&#37; of the telescope surface detectable in a few minutes. This testing has been done so far at 850 micron with the (aging) SHARC2 instrument that was not originally designed for operation at that wavelength. One should be able to do much better with an improved detector.&lt;/p&gt;