Abstract: Systems, devices, and methods are disclosed for testing the boresight of a gimbaled camera and laser system, such as an infrared countermeasures (IRCM) system, in extreme environments. Light simulating a target is reflected through an optics system to the camera, with a portion of the light reflected back from a corner cube reflector through the optics system as a reference. A laser beam from the laser is received through the same optics system, and a position of the corner cube reflected reference and laser beam are compared in order to determine whether the camera and laser are properly aligned. A spherical shell adapted to position the camera at its geometric center keeps misaligned laser pulses from reflecting back into the camera.

Abstract: Systems, devices, and methods are disclosed for testing the boresight of a gimbaled camera and laser system, such as an infrared countermeasures (IRCM) system, in extreme environments. Light simulating a target is reflected through an optics system to the camera, with a portion of the light reflected back from a corner cube reflector through the optics system as a reference. A laser beam from the laser is received through the same optics system, and a position of the corner cube reflected reference and laser beam are compared in order to determine whether the camera and laser are properly aligned. A spherical shell adapted to position the camera at its geometric center keeps misaligned laser pulses from reflecting back into the camera.

Abstract: The absolute distance measuring interferometer (ADMI) is a multi-pass interferometer which is a resonant cavity consisting of two plane parallel mirrors whose length is referenced to a stabilized laser system. The resonant cavity can be used in order to measure very precisely (to within a fraction of a wavelength) the distance between a reference plane and an object. Due to its multi-pass nature, the length of the cavity can be measured much more accurately than for a conventional interferometer. The optical transmission bandwidth of the resonant cavity is inversely proportional to its length. A direct measure of the transmission bandwidth provides an extremely precise (to within a fraction of a wavelength) absolute measure of the length of the cavity. This eliminates the need for careful alignment during the motion of one of the mirrors of the multi-pass interferometer.