The present invention relates to optics, and more particularly to extending light paths.
Providing multiple focal planes, or discrete steps of focus adjustment, is useful for a number of applications. It can be part of creating a more realistic three dimensional display, as well as the ability to capture three dimensional data. In the prior art, multiple focus capture utilized mechanical movement such as gears or liquid lenses. Such mechanisms are expensive, slow, and relatively fragile. Another prior art method of capturing multiple focal lengths uses multiple mirrors and lenses. This is like having multiple cameras; it is bulky and expensive. Because of the bulk and expense, it also limits the number of focal lengths that can be simultaneously captured. A large beam splitter has also been used in the prior art to create two light path lengths. However, this is also a bulky solution.
Such prior art solutions are some combination of large, expensive, and slow. Liquid lenses are expensive and slow, and large beam splitters are large. This makes them difficult to use, and not useful for size or cost constrained systems, particularly portable or worn devices.
The present invention is illustrated by way of example, and not by way of limitation, in the figures of the accompanying drawings and in which like reference numerals refer to similar elements and in which:
A digital light path length modulator is described. The digital light path length modulator includes an optical path length extender (OPLE) and a polarization modulator, and can be used to adjust the path length of light. In one embodiment, light with state 2 polarization travels through a longer path in the OPLE than light with state 1 polarization. This can be used to create two focal planes.
In one embodiment, an OPLE is made up of one or more polarization sensitive reflective elements, which cause light of one polarization state to travel a longer path than light of the other polarization state. In one embodiment, the OPLE comprises a cuboid with one or two diagonal polarization sensitive reflective elements, and quarter wave plate and a mirror on both sides. Light of a second polarization state is reflected by the polarization sensitive reflective element, passes through the quarter wave plate, is reflected by the mirror and passes through the quarter wave plate for the second time. This reverses the polarization of the light, which is reflected at least once more prior to exiting the orthogonal OPLE. In one embodiment, the structure supporting the polarization sensitive reflective elements are four triangular prisms arranged in a cuboid, which support two differently oriented angled polarization sensitive reflective elements and with a light path extender on one side. In one embodiment, the angled polarization sensitive reflective element comprises a wire grid polarizer or a thin-film polarizer coating. In one embodiment, the OPLE may be made up of one or more plates with a plurality of polarization sensitive reflective elements. A plurality of digital light path length modulators create a modulation stack.
In one embodiment, by using a modulation stack, the number of focal planes can be increased. This provides the capacity to build a system that can meet the physiological requirements of human vision, by creating a display in which the 3D cues of overlap, focus, and vergence match. This produces a better quality 3D display and can prevent the headaches associated with 3D displays.
This mechanism in one embodiment can also be used for image capture, and various other uses in which light waves or other waves in a similar spectrum are either projected or captured, including but not limited to cameras, binoculars, 3D printing, lithography, medical imaging, etc. Creating a simple, easy to manufacture digital light path length modulator is like the step from vacuum tubes to transistors; it enables more complex, cheaper, and much more dense digitally controlled elements, which can become building blocks for a wide range of uses.
The following detailed description of embodiments of the invention makes reference to the accompanying drawings in which like references indicate similar elements, showing by way of illustration specific embodiments of practicing the invention. Description of these embodiments is in sufficient detail to enable those skilled in the art to practice the invention. One skilled in the art understands that other embodiments may be utilized and that logical, mechanical, electrical, functional and other changes may be made without departing from the scope of the present invention. The following detailed description is, therefore, not to be taken in a limiting sense, and the scope of the present invention is defined only by the appended claims.
Between the contact areas of the prisms 110A, 110B, 110C, 110D are angled polarization sensitive reflective elements (in one embodiment wire grid polarizers) 130A, 130B, 140A, 140B. The first diagonal formed by the prisms, formed by the shared edges prisms 110A and 110B and the shared edges of prisms 110C and 110D, has a wire grid polarizer in a first orientation 130A, 130B, and the perpendicular diagonal, formed by the shared edges of prisms 110B and 110C and the shared edges of prisms 110A and 110D, has a wire grid polarizer in a second orientation 140A, 140B.
A path length extender 120 is positioned at one side of the OPLE 100, here on the base of prism 110D. In one embodiment, the height of the path length extender 120 (h2) is between ¼ mm to 30 mm.
On both sides of the OPLE 100 there is a quarter wave plate 150A, 150B and mirror 160A, 160B. In one embodiment, the quarter wave plate 150A, 150B is a birefringent material such as mica. In one embodiment, the quarter wave plate 150A, 150B is a polycarbonate film, which may be applied to the base of the side prism 110B and the base of the path length extender 120. In another embodiment, the quarter wave plate 150B may be applied to the top of the path length extender 120 or the bottom of prism 110D.
In one embodiment, the prisms 110A, 110B, 110C, 110D and path length extender 120 are made of material transparent to the wavelengths being used, e.g. optically transparent for light in optical wavelengths. The prisms 110A, 110B, 110C, 110D and path length extender 120 are glued together, in one embodiment.
Additionally, in one embodiment there is a small non-reflective area 170 on the tip of the prisms forming the intersection of the prisms 110A, 110B, 110C, 180. In one embodiment, the non-reflective area 170 may be a black spot in the cross section. The non-reflective area 170 ensures that light hitting the intersection point does not cause scattering of the light.
The embodiments of
In one embodiment, this configuration does not utilize a light path extender, in one embodiment, because there is a single polarization sensitive reflective element only the light with the second polarization is reflected. Light with the first polarization 325 passes straight through the OPLE 305. Light with the second polarization 327 is reflected by the polarization sensitive reflective element 310, passes through the quarter wave plate 320B, is reflected by the mirror, and passes through the quarter wave plate 320B again. It now has the first polarization and thus passes through the polarization sensitive reflective element 310 before encountering the second quarter wave plate 320A, and being bounced back once more, with the polarization rotated back to the second polarization. It then impacts the polarization sensitive reflective element 310 for the third and last time, and is reflected out of the OPLE 305. Thus, for a square cross-section of orthogonal OPLE 305, the path length for the light with the first polarization is W, the width of the polarizer 305, while the path length for the light with the second polarization is 2H+W (or 3H), since it bounces twice between the sides of the OPLE 305.
The wire grid or other polarization sensitive reflective element (not shown) is placed on the prisms. In one embodiment, wire grids may be placed on the prisms, glued onto the prisms, or nano-imprinted on the prisms. In one embodiment, one side of each prism 410, 415, 420, 425 has a wire grid placed on it, such that there are two prisms with polarization sensitive reflective elements of each orientation. In another embodiment, two prisms may have polarization sensitive reflective elements of opposite orientations placed on the two sides of the prism.
Once the polarization sensitive reflective elements are applied, the prisms 410, 415, 420, 425 may be attached to each other. In one embodiment, the prisms are glued together with index matched glue, which does not have an optical effect.
The path length extender 430 is then attached to a base of a prism, here prism 4440. In one embodiment, the path length extender 430 is also made of glass or plastic transparent to the wavelengths used by the system, and it is glued using index matched glue. In another embodiment, as shown above in
The quarter wave plates 435, 445 are then coupled to the sides of the cuboid formed by the prisms 410, 415, 420, 425 and the light path extender 430. In one embodiment, the quarter wave plates 435, 445 may be a film applied to the base of the prism 415 and path length extender 430. Mirrors 440, 447 are coupled to the quarter wave plates 435, 445. In one embodiment, the mirrors are glued on, using index matched glue.
Although the prisms 410, 415, 420, 425 here are shown as relatively short pieces, in one embodiment the system may be assembled as a large rectangle, and then cut to an appropriate size. The size, in one embodiment, depends on the aperture of the system. In one exemplary embodiment, the face formed by the prisms is 5 mm×5 mm (H), and the length of the OPLE (L) is 12 mm. The length may be between 5 mm and 100 mm.
In one embodiment, in this configuration the center of the OPLE has a non-reflective area to ensure that no negative optical effects are introduced into the system. In one embodiment, the OPLE includes the polarization sensitive reflective elements 450, 455, quarter wave plates 470, 480, and mirrors 480, 485.
The structure is supported by a framework 460, illustrated for simplicity by framing elements. The framework in one embodiment may be plastic, glass, or another material, and need not be transparent as long as it is capable of supporting the mirror and polarization sensitive reflective elements. In one embodiment, the quarter wave plates 470, 480 may be attached to the mirror 475, 485. In one embodiment, there may be a path length extender (not shown). In another embodiment, the bottom of polarization sensitive reflective elements 450, 455 is positioned a height h2 above the quarter wave plate 470 and mirror 475 to create the spacing of the path length extender without requiring a physical object.
From
In one embodiment, because the light exits from both sides of a longitudinal OPLE, the longitudinal OPLE 535 is preferentially a first OPLE in a modulation stack 510 that includes longitudinal OPLEs.
In the foregoing specification, the invention has been described with reference to specific exemplary embodiments thereof. It will, however, be evident that various modifications and changes may be made thereto without departing from the broader spirit and scope of the invention as set forth in the appended claims. The specification and drawings are, accordingly, to be regarded in an illustrative rather than a restrictive sense.
The present application is a continuation of U.S. patent application Ser. No. 15/675,659, filed on Aug. 11, 2017, issuing as U.S. Pat. No. 10,185,153, on Jan. 22, 2019, which claims priority to U.S. patent application Ser. No. 15/236,101, filed on Aug. 12, 2016, U.S. patent application Ser. No. 15/358,040 filed on Nov. 21, 2016, and U.S. patent application Ser. No. 15/491,792 filed Apr. 19, 2017. All of the above applications are incorporated herein by reference.
Number | Name | Date | Kind |
---|---|---|---|
6134031 | Nishi et al. | Oct 2000 | A |
7798648 | Ijzerman et al. | Sep 2010 | B2 |
20090021824 | Ijzerman et al. | Jan 2009 | A1 |
20090052838 | McDowall et al. | Feb 2009 | A1 |
20110075257 | Hua et al. | Mar 2011 | A1 |
20120113092 | Bar-Zeev et al. | May 2012 | A1 |
20140176818 | Watson | Jun 2014 | A1 |
20170146803 | Kishigami | May 2017 | A1 |
20170227770 | Carollo et al. | Aug 2017 | A1 |
20170269369 | Qin | Sep 2017 | A1 |
20190086675 | Carollo et al. | Mar 2019 | A1 |
Number | Date | Country |
---|---|---|
102566049 | Jul 2012 | CN |
105739093 | Jul 2016 | CN |
109997357 | Jul 2019 | CN |
0195584 | Sep 1986 | EP |
H06258673 | Sep 1994 | JP |
3384149 | Mar 2003 | JP |
Entry |
---|
Pate, Michael, Polarization Conversion Systems for Digital Projectors, Web Publication, Apr. 21, 2006, Downloaded from http://www.zemax.com/os/resources/learn/knowledgebase/polarization-conversion-systems-for-digital-projectors on Jun. 17, 2016 (8 pages). |
Number | Date | Country | |
---|---|---|---|
20190155045 A1 | May 2019 | US |
Number | Date | Country | |
---|---|---|---|
Parent | 15675659 | Aug 2017 | US |
Child | 16253149 | US | |
Parent | 15491792 | Apr 2017 | US |
Child | 15675659 | US | |
Parent | 15236101 | Aug 2016 | US |
Child | 15335298 | US | |
Parent | 15398705 | Jan 2017 | US |
Child | 15675659 | US | |
Parent | 15377938 | Dec 2016 | US |
Child | 15675659 | US |
Number | Date | Country | |
---|---|---|---|
Parent | 15358040 | Nov 2016 | US |
Child | 15491792 | US | |
Parent | 15236101 | Aug 2016 | US |
Child | 15358040 | US | |
Parent | 15335298 | Oct 2016 | US |
Child | 15491792 | US | |
Parent | 15358040 | Nov 2016 | US |
Child | 15398705 | US | |
Parent | 15358040 | Nov 2016 | US |
Child | 15377938 | US | |
Parent | 15335298 | Oct 2016 | US |
Child | 15358040 | US |