摘要:
Objective (1) having a first partial objective (3) which projects a first field plane (7) onto an intermediate image (11) and comprises a first convex mirror (13) with a first central mirror aperture (15) and a second concave mirror (17) with a second central mirror aperture (19), the first mirror (13) having a first axial spacing from the second mirror (17 )', and the second mirror (17) having a second axial spacing from the intermediate image (11), and the ratio of the first axial spacing to the second axial spacing having a value of between 0.95 and 1.05, in particular between 0.98 and 1.02, and a second partial objective (5), which projects the intermediate image (11) onto a second field plane (9) and comprises a third concave mirror (21) with a third central mirror aperture (23) and a fourth concave mirror (25) with a fourth central mirror aperture (27) 1 the third mirror (21) having from the second field plane (9) a third axial spacing ZM3-IM which has the following relationship with a numerical aperture NA in the second field plane (9) and with a diameter DUM3 of the third mirror (21) : (I), the objective (1) having a Petzval radius whose absolute value is greater than the axial spacing of the first field plane (7) from the second field plane (9) .
摘要:
A mirror system has four mirrors with a common optical axis, i.e. a first collecting mirror (1), a second smaller dispersing mirror (2), a third collecting mirror (3) and a fourth collecting mirror (4), seen in the direction of light incidence. Mirror (1) reflects incident light on mirror (2) that forms an intermediate image (5) of the light. The dispersed light then reaches mirror (3) that acts as a collimator and reflects parallel light on mirror (4), that in turn reflects the light on image field (6) in which a detector (7) is arranged. Mirror (1) has a central bore (10). Flat mirrors (8) fold the path of the light and are preferably arranged in the plane of intermediate image (5). An image field flattening lens (9) can flatten image field (6). Both classical Cassegrain systems and Ritchey-Chretien systems that consist of mirrors (1) and (2) may be aplanatically and anastigmatically corrected with a flat image field (6) by means of the disclosed two-mirror corrector made of mirrors (3) and (4).
摘要:
In mirror systems with three mirrors, light falls in its direction of displacement on a primary mirror (1), is reflected on a secondary mirror (2), then on a tertiary mirror (3) that bundles the light in a focal plane (4) into which a detector (5) may be introduced. The disclosed mirror systems may be designed to be free from spherical aberration, coma and astigmatism. In addition, the curvature radius of mirrors (1, 2 and 3) may be selected in mirror systems with at least one divergent mirror (1, 2 or 3) in such a way that the Petzval sum be also equal to zero, so that besides eliminating astigmatism a flat image field is obtained. Otherwise, the image field may be flattened by an image field flattening lens (6). The path of the beams may be folded by plane mirrors (7). The surface of mirrors (1, 2, 3 and 7) may be designed as holograms or as multilayered mirrors. The disclosed mirror systems may be designed as objective lenses, as magnifying or diminishing projection lenses, as afocal systems, as collimators and as real or virtual point light sources.
摘要:
A low cost infrared camera (1) for night vision. The camera (1) is disposed within a housing (2) having an infrared transmissive window (6) disposed at an input aperture (5) thereof. A compact reflective optical arrangement (10) is disposed within the housing (2) to focus energy from the window (5) onto a focal plane array (20). A chopper disk (19) is positioned between the reflective optical arrangement (10) and the focal plane array (20) to establish a reference level for the array (20) and to facilitate a sequential readout thereof. A signal processing circuit (100) is included for processing the output of the array (20) for display on a standard video screen. Thus, the problems with uncooled detectors are overcome by use of a fast reflective optical system in combination with an uncooled detector. The fast reflective optical system provides a high signal level to the uncooled detector, thereby compensating for losses in collection of thermal radiation. Reflective optical systems can be manufactured inexpensively from plastic or aluminum and reduce the needed for expensive infrared materials commonly used in military systems. The combination of the fast reflective optics and uncooled detector provides a truly low cost thermal camera for night vision.