Abstract: A lighting device with variable angle of emission includes a light source, and a lens system comprising two lenses, a primary lens and a secondary lens. The two lenses and the light source are arranged along an optical axis and the distance between the primary lens and the secondary lens is variable, in order to vary the angle of emission of the cone of light rays generated by the lighting device. In one example, the primary lens has a numerical aperture of at least 0.7, the primary lens is an aplanat, and the secondary lens is designed so as to image to infinity, at a certain distance of the secondary lens from the primary lens, a virtual image of the light source generated by the primary lens. According to a second aspect, the illumination factors are distinguished by the fact that the primary lens has a numerical aperture of at least 0.

Abstract: An apparatus and method for non-imaging optical systems to couple incoherent light from a source such as high-brightness lamps into optical fibers, and to deliver the light into the human body for photothermal and/or photochemical surgery. The incoherent light radiated from the light source is concentrated with a non-imaging light concentrator and the light is delivered to a body tissue for photothermal and/or photochemical medical treatment. The concentrator captures nearly the light source's full radiative output, and concentrates the collected radiation back to power densities close to the power densities of the hot plasma regions at the core of the light source. The concentrator couples the light into a photonic conduit such as optical fibers, and the photonic conduit delivers the concentrated intense light to surgical applications including contact (interstitial) procedures and non-contact treatments (within the internal body cavities as well as the surfaces of organs), and inside the body.

Abstract: A system and method for concentrating the intensity of light emitted by a high-intensity source for delivery to a remote target, so that the power density of the active radiating region of the source is nearly restored at the target. The source is surrounded by a plurality of nonimaging concentrators. If the source is elongated, the concentrators are similarly elongated and parallel to the source. If the source is compact, the preferred geometric pattern of the concentrators is dodecahedral. The geometry of the concentrators is designed in accordance with the edge-ray principle of nonimaging optics. Channels such as optical fibers or light pipes are coupled optically to the absorbers of the concentrators, to conduct the concentrated light to the remote target.

Abstract: A nonimaging illumination optical device for producing a selected far field illuminance over an angular range. The optical device includes a light source 102, a light reflecting surface 108, and a family of light edge rays defined along a reference line 104 with the reflecting surface 108 defined in terms of the reference line 104 as a parametric function R(t) where t is a scalar parameter position and R(t)=k(t)+Du(t) where k(t) is a parameterization of the reference line 104, and D is a distance from a point on the reference line 104 to the reflection surface 108 along the desired edge ray through the point.

Abstract: A nonimaging illumination optical device for producing a selected far field illuminance over an angular range. The optical device includes a light source 102, a light reflecting surface 108, and a family of light edge rays defined along a reference line 104 with the reflecting surface 108 defined in terms of the reference line 104 as a parametric function R(t) where t is a scalar parameter position and R(t)=k(t)+Du(t) where k(t) is a parameterization of the reference line 104, and D is a distance from a point on the reference line 104 to the reflection surface 108 along the desired edge ray through the point.

Abstract: A method of delivering guided radiation arriving via a first transparent medium having a first refractive index into a second transparent medium having a second refractive index that is smaller than the first refractive index, comprising: providing a transparent radiation delivery waveguide capable of admitting concentrated radiation and having a longitudinal axis and a third refractive index substantially equal to or greater than the first refractive index and adapted to guide the radiation along the longitudinal axis. The waveguide having a tapered radiation delivery portion of non-circular cross-sectional shape. Mounting the waveguide in optical contact with the first transparent medium so that the radiation delivery portion projects inside the second transparent medium.

Abstract: A nonimaging illumination optical device for producing a selected far field illuminance over an angular range. The optical device includes a light source 102, a light reflecting surface 108, and a family of light edge rays defined along a reference line 104 with the reflecting surface 108 defined in terms of the reference line 104 as a parametric function R(t) where t is a scalar parameter position and R(t)=k(t)+Du(t) where k(t) is a parameterization of the reference line 104, and D is a distance from a point on the reference line 104 to the reflection surface 108 along the desired edge ray through the point.