Light Prescriptions Innovators, LLC

Other

Tesseland, LLC

Lpi-europe, S.l.

Juan Carlos Miñano

Pablo Benitez

Pablo Benítez

Waqidi Falicoff

William A Parkyn, Jr

Maikel Hernandez

Oliver Dross

Julio Cesar Chaves

Julio C Chaves

Roberto Alvarez

Aleksandra Cvetkovic

Rubén Mohedano

Fernando Muñoz

William Arthur Parkyn, Jr

Yupin Sun

Dejan Grabovickic

Pablo Zamora

José Blen Flores

José Blen

Bharathwaj Narasimhan

A display device arranged to generate a light field to illuminate a human eye. The light field comprising a plurality of pencils that virtually intersect a first reference surface and a second reference surface, said first reference surface being the plane passing through the eye ball sphere center and is perpendicular to the skull frontward direction, and said second reference surface located at a distance from the user's skull and being a portion of a sphere centered the eye hall sphere center. The center of said second reference surface defined as the intersection point of the line passing through the eye ball sphere center and pointing in the skull's frontwards direction. Each pencil is a set of straight lines, segments of said lines coincident with light ray trajectories illuminating the eye having approximately equal luminance and color at any time.

Human vision-adapted light field displays

A display device includes a display operable to generate a real image and an optical system including: a plurality of optical channel bundles, each bundle comprising one or more channels, each channel comprising a lenslet arranged to generate a sub-image from a respective partial real image on the display, Each lenslet is configured to project light from the display to a corresponding eye position among two eye positions. The sub-images combine to form two virtual images so that different optical channel bundles image a same portion of the display to different portions of the virtual images. The optical system is configured to allow light to flow through selected channels and prevent, light from flowing through other selected channels. The system successively opens the optical channel bundles and displays partial real images associated with the channels of the corresponding optical channel bundle.

Visual display with time multiplexing for stereoscopic view

An optical component called the Phase Space Combiner (PSC) is designed to join several bundles of rays. The bundles of rays, when represented in ray phase-space, occupy non-connected regions before passing through the PSC, while their representation in ray phase space occupies a single simply connected region (without holes) after passing through the PSC. Obviously, when used in reverse way it splits one bundle in several parts. We present herein the idea of using Multiple Individual Optics, MIO, not for collimating the light from the LEDs but as a PSC. Then a Single Common Optics, SCO, which can be an optical train, is used to get the desired intensity pattern. This hybrid SCO and MIO strategy combines most of the advantages of both approaches.

Optical phase space combiner

Some photovoltaic cells have a front face accepting incoming incident light and opaque gridlines overlying part of the front face, electrically bonded to the face, with upper reflective facets oblique to the plane of the front face and producing outgoing reflected light. An optical interface parallel to and in front of the front face transmits incoming light to the front face and to the gridlines and reflects back towards the front face by total internal reflection at least some of the outgoing reflected light. Some photovoltaic devices have a triple junction photovoltaic cell, a single junction photovoltaic cell, and a reflective surface arranged to distribute incoming light between the cells. The surface may be a frequency-selective mirror that apportions light so when the cells are in series the power produced, and preferably the photocurrent, is greater than if all the light fell on the triple junction cell alone.

Photovoltaic device

One optical system comprises a first optical surface, a faceted second optical surface, and a faceted third optical surface. The optical system is operative to convert a first bundle of rays that is continuous in phase space outside the first optical surface into a second bundle of rays that is continuous in phase space outside the third optical surface. Between the second and third optical surfaces the rays making up the first and second bundles form discrete sub-bundles each passing from a facet of the second optical surface to a facet of the third optical surface. The sub-bundles do not form a continuous bundle in a phase space that has dimensions representing the position and angle at which rays cross a surface transverse to the bundle of rays.

Stepped flow-line concentrators and collimators

An embodiment of a method of designing a grooved reflector comprises selecting two given wavefronts; and designing two surfaces meeting at an edge to form a groove such that the rays of each of the given wavefront become rays of a respective one of the given wavefronts after a reflection at each of the surfaces. Multiple grooves may be combined to form a mirror covering a desired area. A mirror may be manufactured according to the design.

Reflectors made of linear grooves

A condenser for directing light from a UHP arc lamp or other generally cylindrical source onto a target such as a microdisplay in line with a front end of the lamp comprises a primary mirror to direct light from the source towards the back end of the condenser, and a secondary mirror at the back end of the condenser to direct the light from the primary mirror onto the target.

Free-form condenser optic

In one embodiment of a solar concentrator, a tailored aspheric lens augments the solar-concentrator performance of a concave mirror, widening its acceptance angle for easier solar tracking, making it more cost-competitive for ultra-large arrays. The molded-glass secondary lens also includes a short rod for reducing the peak concentration on a photovoltaic cell that is optically bonded to the end of the rod. The Simultaneous Multiple Surface method produces lens shapes suitable for a variety of medium and high concentrations by mirrored dishes. Besides the rotationally symmetric parabolic mirror itself, other aspheric deviations therefrom are described, including a free-form rectangular mirror that has its focal region at its edge.

Optical concentrator, especially for solar photovoltaics

One embodiment of a method of calculating an optical surface comprises calculating a meridional optical line of the surface. A ray is selected that passes a known point defining an end of a part of the optical line already calculated. The optical line is extrapolated from the known point to meet the ray using a polynomial with at least one degree of freedom. The polynomial is adjusted as necessary so that the selected ray is deflected at the extrapolated optical line to a desired target point. The polynomial is added to the optical line up to the point where the selected ray is deflected. The point where the selected ray is deflected is used as the known point in a repetition of those steps.

Imaging optics designed by the simultaneous multiple surface method

One example of a solar voltaic concentrator has a primary Fresnel lens with multiple panels, each of which forms a K&#xf6;hler integrator with a respective panel of a lenticular secondary lens. The resulting plurality of integrators all concentrate sunlight onto a common photovoltaic cell. Luminaires using a similar geometry are also described.

K&#xf6;hler concentrator

The diffuse reflectivity of an LED source is utilized to recycle some of its emission, thereby enabling a luminaire to escape the &#xe9;tendue limit. Retroreflectors intercept the rays destined for the outer part of the luminaire aperture, which can then be truncated. The resulting smaller aperture has the same beam-width as the full original, albeit with lesser flux due to recycling losses. A reduction to half the original area is possible.

LED luminance-augmentation via specular retroreflection, including collimators that escape the &#xe9;tendue limit

A waveguide version of a Kohler integrator is disclosed, utilizing geodesic lenses with a surface that can be mapped to a gradient-index Luneburg lens or to a nonfull-aperture Luneburg lens in such a way that the light paths in the gradient index lenses map into the geodesics of the surface, with the outer region of the gradient index lenses mapped into a flat surface. Arrays of these can be applied to lines of LEDs, as in CHMSLs, to mix light in intensity and in illumination as well as to avoid the deleterious effects of binning and burnout, or in multicolor arrays, to ensure complete chromatic mixing.

Waveguide-optical Kohler integrator utilizing geodesic lenses

An embodiment of an optical manifold has first and second collimators, each arranged to receive light from a source and transmit the light to an exit port of the collimator, and a separator arranged to emit some of the light from the exit ports of the first and second collimators and to recycle some of the light into the collimators. Another embodiment has at least three collimators of substantially equal length and having central axes, respective light sources at entry ports of the collimators, the collimators being arranged with their central axes parallel and with their light sources in a common plane and reflectors positioned to direct light from exit ports of the collimators to a selectively reflective component that guides all the light into a common exit beam.

Combining outputs of different light sources

Optical systems are described that have at least one source of a beam of blue light with divergence under 15&#xb0;. A phosphor emits yellow light when excited by the blue light. A collimator is disposed with the phosphor and forms a yellow beam with divergence under 15&#xb0;. A dichroic filter is positioned to transmit the beam of blue light to the phosphor and to reflect the beam of yellow light to an exit aperture. In different embodiments, the beams of blue and yellow light are incident upon said filter with central angles of 15&#xb0;, 22&#xb0;, and 45&#xb0;. The filter may reflect all of one polarization and part of the other polarization, and a polarization rotating retroreflector may then be provided to return the unreflected light to the filter.

Growing community of inventors

Madrid, Spain

Juan Carlos Miñano