3D eyewear adapted for facial geometry
11385472 · 2022-07-12
Assignee
Inventors
- Barret LIPPEY (Foster City, CA, US)
- Martin J. Richards (Gig Harbor, WA, US)
- Christopher L. Huang (Walnut Creek, CA, US)
- Thao Hovanky (San Francisco, CA)
- Wilson Heaton Allen (Mill Valley, CA, US)
Cpc classification
G02B30/23
PHYSICS
International classification
G02B30/00
PHYSICS
G02B30/23
PHYSICS
Abstract
Three dimensional (3D) glasses suited for wearers with varying facial geometries may include a frame adapted to position spectrally filtering lenses at a particular distance from the eyes of the wearer. The 3D glasses may include a means for adjusting the distance between the lenses and the eyes of the wearer. The lenses may include positive runout.
Claims
1. Eyewear for viewing 3D images, each 3D image including a left eye image and a right eye image, said eyewear including: a left lens including a first set of spectral filters adapted to pass said left eye images and to block said right eye images; a right lens including a second set of spectral filters adapted to pass said right eye images and to block said left eye images; and a frame for holding said left lens and said right lens, said frame including one or more positioning surfaces disposed to abut the face of a wearer and to position said left lens and said right lens within a distance range of 15-20 mm from left and right eyes of said wearer, wherein said positioning surfaces include a nose piece that is mounted to said frame at an adjustable position relative to said frame to adapt said distance range when said frame is worn by a person having a nose bridge between a first length and a second length shorter than said first length, wherein said nose piece is mounted to said frame via a fastener passing through a hole in said frame, wherein said fastener threads into an alternate threaded opening in said nose piece, and wherein said frame further comprises an adjustment wheel forming a threaded engagement with said fastener to adjust said position of said nose piece relative to said frame.
2. The eyewear of claim 1, wherein said positioning surfaces include a brow engaging surface.
3. The eyewear of claim 1, wherein the first set of spectral filters have a thickness that is greater near edges of the left lens than near a center of the left lens and wherein the second set of spectral filters have a thickness that is greater near edges of the right lens than near a center of the right lens.
4. The eyewear of claim 1, wherein said nose piece simultaneously contacts, when said eyewear is worn by a person, a left side and a right side of said person's nose.
5. Eyewear for viewing 3D images, each 3D image including a left eye image and a right eye image, said eyewear including: a left lens including a first set of spectral filters adapted to pass said left eye images and to block said right eye images; a right lens including a second set of spectral filters adapted to pass said right eye images and to block said left eye images; and a frame for holding said left lens and said right lens, said frame including one or more positioning surfaces disposed to abut the face of a wearer and to position said left lens and said right lens within a distance range of 15-20 mm from left and right eyes of said wearer, wherein said positioning surfaces include a nose piece that is mounted to said frame at an adjustable position relative to said frame to adapt said distance range when said frame is worn by a person having a nose bridge between a first length and a second length shorter than said first length, wherein said nose piece travels along an axis during adjustment of the position of said nose piece relative to said frame, wherein said axis is substantially parallel to a wearer's straight-ahead line of sight, wherein said nose piece is mounted to said frame via a fastener passing through a hole in said frame, wherein said fastener threads into an alternate threaded opening in said nose piece, and wherein said frame further comprises an adjustment wheel forming a threaded engagement with said fastener to adjust said position of said nose piece relative to said frame by moving said nose piece along said axis.
6. The eyewear of claim 5, wherein the position of said nose piece relative to said frame is non-destructively adjustable.
7. The eyewear of claim 5, wherein said nose piece simultaneously contacts, when said eyewear is worn by a person, a left side and a right side of said person's nose.
8. The eyewear of claim 5, wherein the first set of spectral filters have a thickness that is greater near edges of the left lens than near a center of the left lens and wherein the second set of spectral filters have a thickness that is greater near edges of the right lens than near a center of the right lens.
Description
BRIEF DESCRIPTION OF THE DRAWINGS
(1) The present invention is described with reference to the following drawings, wherein like reference numbers denote substantially similar elements:
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DETAILED DESCRIPTION
(12) The present invention overcomes the problems associated with the prior art, by providing three dimensional (3D) eyewear that is suited for users of varying facial geometries. In the following description, numerous specific details are set forth (e.g., widths of spectral bands, lens characteristics, etc.) in order to provide a thorough understanding of the invention. Those skilled in the art will recognize, however, that the invention may be practiced apart from these specific details. In other instances, details of well-known 3D projection practices (e.g., image generation and filtering) and components have been omitted, so as not to unnecessarily obscure the present invention.
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(15) A single ray of light 206, originating from a point (A), is shown incident on lens 201 in both first position 202 and second position 204 and entering a pupil 208 of eye 200. Because of the difference in the ETL distances of positions 202 and 204 and the curvature of lens 201, the angle of incidence of ray 206 with lens 201 in first position 202 (φ.sub.snb) is larger than the angle of incidence of ray 206 with lens 201 in second position 204 (φ.sub.lnb). The relative dimensions (e.g., the ETL difference and the curvature of lens 201) in
(16) The AOIs of the viewed light can adversely affect the operation of lens 201. Particularly, there is a shift of the wavelength of incident light (i.e. the wavelength of the light becomes shorter or longer) depending on the AOI. The magnitude of the wavelength shift is modeled by the following equation:
λ.sub.φ=λ.sub.0√{square root over (1−(sin φ/n.sub.eff).sup.2)}, (Eq. 1)
where λ.sub.φ denotes the wavelength of the shifted light, λ.sub.0 denotes the original wavelength of the incident light, φ denotes the AOI of the incident light, and n.sub.eff denotes the effective index of refraction of the lens, which is dependent on the material and thicknesses of the coating layers (among other things). For most 3D projection applications, wavelength shifts typically act to blue-shift the coating (i.e. the coating is shifted to shorter wavelengths).
(17) Because lenses utilized in 3D glasses only transmit light within predetermined ranges of wavelengths, the shifting of the coating adversely impacts the intended images viewed through lens 201. The shift causes lens 201 to transmit light that otherwise would have been blocked and vice versa. The problems associated with the wavelength shift are discussed below. An angle as small as 26 degrees can cause a wavelength shift of about 14 nm, which is significant for the proper functioning of lens 201.
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(19) In the example embodiment, spectral band 300 includes light of wavelengths within a range from 438.0 nm to 449.5 nm, and spectral band 306 includes light of wavelengths within a range of wavelengths from 458.5 nm to 472.0 nm. In alternate embodiments, spectral bands 300 and 306 can include light within larger or smaller ranges of wavelengths, based on tradeoffs between color fidelity and image separation, among other things. Spectral bands 300 and 306 can also be made to correspond to the opposite eyes (i.e. spectral band 300 can be transmitted by the right eye lens and spectral band 306 can be transmitted by the left eye lens). Additionally, spectral bands 302 and 308 include light of wavelengths within ranges between 520.0 nm and 529.0 nm and between 543.0 nm and 551.0 nm, respectively. Spectral bands 304 and 310 include light of wavelengths within ranges between 631.0 nm and 638.0 nm and between 652.0 nm and 662.0 nm, respectively. Spectral bands 304, 306, 308 and 310 can also be tuned based on various factors and/or be made to correspond to either eye.
(20) In order to create depth in 3D images, the left eye and right eye images must be different, and should be viewed by the corresponding eye only. Therefore, spectral bands 300 and 306 are separated by a blue band gap 312, spectral bands 302 and 308 are separated by a green band gap 314, and spectral bands 304 and 310 are separated by a red band gap 316. For viewers with long nose bridges, band gaps 312, 314, and 316 are sufficiently wide to prevent crosstalk between right eye images and the left eye lens. However, for viewers with short nose bridges, the angle of incidence (obliqueness of light passing through the lenses) may be significant enough that the spectral properties (or wavelength properties) of the filters or passbands of the filters blue-shift enough to create crosstalk, by, for example, allowing one or more wavelengths of light intended to pass through the left eye lens to instead to pass through the right eye lens.
(21) The potential problem of blue-shift of filter properties for a right eye filter when used by viewers with a short nose bridge is illustrated by
(22) Although not explicitly shown, passbands (or pass areas) of the left eye filter are also blue-shifted at large angles of incidence. As with the right eye, only a portion of the shifted left eye filter pass areas will overlap with their corresponding spectral bands (300, 302, and 304 in the left eye case), and, therefore, only a portion of the light comprising the left eye images is transmitted by the left eye lens. Therefore, blue-shifting of the left eye spectral bands causes a significant decrease in the optical efficiency of the 3D system and can reduce a viewer's field of view to only a small portion of the screen. In the case that the left eye images are composed of light in the longwave bands and right eye images are composed of light in the shortwave bands, similar problems will occur with the other channel. In particular, the right eye images will crosstalk into the left eye images due to the blue shifted properties of the passbands (or pass areas) of the left eye lens (or filter), and right eye images will only be partially transmitted by the blue-shifted right eye lens (or filter).
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(24) In order to decrease the AOI of incoming light for the wearer, frame 402 includes a brow shelf 412, which is wider than on the frame of a typical pair of 3D glasses (illustrated by the dotted line). Brow shelf 412 is adapted to abut the wearer's brow or forehead to hold frame 402 and, thus, lenses 404 and 406 at a predetermined distance from the eyes of the viewer. In other words, brow shelf 412 ensures a minimum ETL distance. Inventors have discovered that the ideal ETL distance is between 15 and 20 millimeters (mm). Additionally, frame 402 includes a nose piece 500 (
(25) In one embodiment, the brow shelf (and/or other positioning surfaces) are adjustable to accommodate for variances in brow or other feature locations relative to the eye. The present invention includes 3D glasses with an adjustable ETL distance. The present invention includes 3D glasses with more than one adjustable member each effecting ETL distance. In one embodiment, a theater or other venue (such as an amusement park ride, museum, or tourist attraction) displays a test image (e.g., on the screen or other surface) with instructions for adjusting the brow shelf (or other adjustable points) so that each viewer may easily customize the relative positions and/or ETL distance for best image performance.
(26) Left temple piece 408 is coupled to frame 402 at a left temple region 414 and right temple piece 410 is coupled to frame 402 at a right temple region 416. Left temple portion 408 and right temple portion 410 are adapted to rest upon the left and right ears of the wearer, respectively, to provide additional support for frame 402.
(27) In the example embodiment, frame 402 and temple portions 408 and 410 are molded from plastic to form an integral piece. In alternate embodiments, frame 402 and temple portions 408 and 410 can be formed separately and coupled together via screws or some other fasteners. Additionally, temple portions 408 and 410 are rigidly fixed to frame 402 in the example embodiment. In alternate embodiments, temple portions 408 and 410 can be hinged to better fit the heads of a wide range of users or to be folded and stored.
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(30) Frame 604 is designed for a wearer with a long nose bridge, but detachable nose adapter 602 adapts 3D glasses 600 for a wearer with a short nose bridge. Adapter 602 is configured to mount to frame 604 via a screw 618. Screw 618 passes through a hole 620 in frame 604 and threads into a threaded opening 622 in adapter 602. Hole 620 is recessed to allow a head 624 of screw 618 to sit flush with respect to the front surface of frame 604. When screw 618 is threaded completely into threaded opening 622, adapter 602 is pulled tight against frame 604 and is fixed with respect to frame 604. An engaging surface 626 of adapter 602 is configured to abut a rear surface of frame 604 between lenses 606 and 608. Adapter 602 also includes a nose pad 628 configured to rest upon the nose of the wearer. Nose pad 628 is shaped to comfortably fit around the bridge of the wearer's nose and to function as a positioning surface. Nose pad 628 is fixed to a bridge portion 630, which is fixed to a pair of engaging surfaces 632. Engaging surfaces 632 are shaped to abut a nose piece (not shown) of 3D glasses 600, in order to seat adapter 602 securely against frame 604. When adapter 602 is coupled to frame 604, the ETL distance is increased, thus decreasing the AOI of incident light (as described above with reference to
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(33) Additionally, the spectral filters of lenses 700 are designed to permit only a predetermined amount of wavelength shift at the AOIs specified above. The wavelength shift is measured using the following equation:
WS=(λ.sub.SP,Measured−λ.sub.SP,Designed)/λ.sub.SP,Designed,SP=1,C,T,B,N, (Eq. 2)
where λ.sub.SP,Measured denotes a spectral average of the wavelengths of the shifted light at a given point on the lens, and λ.sub.SP,Designed denotes a spectral average of the wavelengths of the rising or falling edges of the spectral bands at a given point on the lens as specified above. Additionally, 1 refers to point 706, C refers to point 708, T refers to point 710, B refers to point 712, and N refers to point 714. To calculate the wavelength shift, first, a spectral average of the wavelengths, at which 50% of light is observed to pass through the spectral filters, is calculated. For example, if 50% of light of wavelengths of 450 nm, 530 nm, and 645 nm is observed passing through the spectral filters at point 706 of lens 702 at an AOI of 0 degrees, then λ.sub.1,Measured is equal to 450 nm+530 nm+645 nm/3≈542 nm. Next, a spectral average of the wavelengths of the falling edge of the associated spectral band is calculated. For example, at point 706 of lens 702 at an AOI of 0 degrees, the spectral filter is designed to transmit 50% of light at 455 nm, 540 nm, and 650 nm, so λ.sub.1,Designed is equal to 455 nm+540 nm+650 nm/3≈548 nm. Finally, the wavelength shift is calculated as (542 nm-548 nm)/548 nm≈−0.010 or −1.0%.
(34) Lenses 702 and 704 are each designed to provide a predetermined amount of bandpass wavelength shift at each of points 706, 708, 710, 712, and 714. For example, the spectral filter of lens 702 at point 706 provides approximately 0.4% of wavelength shift, where a negative value denotes blue-shift and a positive value denotes red-shift. At point 708, the spectral filter of lens 702 provides approximately −0.4% of wavelength shift. At point 710, the spectral filter of lens 702 provides approximately 1.7% of wavelength shift. At point 712, the spectral filter of lens 702 provides approximately −0.2% of wavelength shift. At point 714, the spectral filter of lens 702 provides approximately 1% of wavelength shift. Additionally, the spectral filter of lens 704 at point 706 provides approximately −0.2% of wavelength shift. At point 708, the spectral filter of lens 704 provides approximately −0.2% of wavelength shift. At point 710, the spectral filter of lens 704 provides approximately 1.7% of wavelength shift. At point 712, the spectral filter of lens 704 provides approximately −0.2% wavelength shift. At point 714, the spectral filter of lens 704 provides approximately 1% of wavelength shift. In alternate embodiments these specifications can be tightened, relaxed, or translated based on the needs of the wearer and/or manufacturer.
(35) The percentage wavelength shifts at each point are at least partially determined by the thickness of the spectral coating at that point.
(36) Spectral coating 718 affects the amount of wavelength shift of the filter properties, because the effective index of refraction (n.sub.eff in Eq. 2) is determined, at least partially, by the geometric characteristics of the lens. For example, in areas where spectral coating 718 is thicker (meaning the layers of the spectral coating are thicker), the blue shift of the filter properties will be reduced at any given AOI. In areas where spectral coating 718 is thinner, the blue shift of the filter properties will be increased at the same AOIs. Therefore, spectral coating 718 is thinner in the center of lens 704 than it is at the edges of lens 704 (i.e. spectral coating 718 has positive runout). Positive runout helps to eliminate some of the blue shift that occurs when the ETL distance is shorter than the ideal range. It should be noted that too much positive runout can cause its own problem for viewers with a long nose bridge in that positive runout shifts the filter properties to longer wavelengths and if shifted too far (too much positive runout), light incident at normal angles [or perhaps even less oblique angles] for example at the edges of the filter (or wherever the positive runout is applied) may pass through the opposite eye filter passbands (or pass areas). For example, portions of the right eye image (e.g., 306, 308, 310) may pass through the left eye filters if positive runout places the left eye filter passbands (or pass areas) at wavelengths corresponding to the right eye image. This problem is slightly reduced because it will mainly occur toward the edges of the filters and normally incident light at the edges is less likely to enter the pupil. Nonetheless with the variances in facial features and individual positioning of glasses and the range of angles in which viewers are subject themselves (or are subjected to, for example in a theme park ride), the problem exists.
(37) The present invention includes customizing glasses in frame structure (mainly ETL) and positive runout as fitting the average audience member. For example, viewers in China have customized glasses and positive runout which is different from glasses and positive runout in Europe, which is different from that used in Africa, or the Americas. Further, the present invention includes the disclosed amount of positive runout which yields lenses that can be used for all viewers. In particular, these lenses can be utilized in various frames that are designed for viewers with different facial geometry, including both long nose bridge and short nose bridge viewers. The combination of lenses with positive runout and frames adapted to control the ETL distance provides a significant improvement over 3D eyewear of the prior art.
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(39) The description of particular embodiments of the present invention is now complete. Many of the described features may be substituted, altered or omitted without departing from the scope of the invention. For example, alternate spectral bands may be substituted for the spectral bands illustrated in