US20150335241A1

US20150335241A1 - Apparatus for obtaining status information of crystalline lens and equipment including the same

Info

Publication number: US20150335241A1
Application number: US14/818,613
Authority: US
Inventors: Dae-Shik Seo; Byoung-Yong Kim
Original assignee: University Industry Foundation UIF of Yonsei University
Current assignee: University Industry Foundation UIF of Yonsei University
Priority date: 2011-01-18
Filing date: 2015-08-05
Publication date: 2015-11-26
Also published as: US9131839B2; KR20120083580A; US20120182398A1

Abstract

In one example embodiment, an apparatus for obtaining status information of a crystalline lens of an eye includes a light projector configured to project a reference light to the crystalline lens; an intensity detector configured to detect an intensity of scattered light that is generated from the reference light by being scattered at the crystalline lens; and a calculator configured to calculate thickness information of the crystalline lens based on the intensity of scattered light.

Description

CROSS-REFERENCE TO RELATED APPLICATION(S)

This is a continuation application of U.S. patent application Ser. No. 13/332,735, filed on Dec. 21, 2011 which claims the benefit under 35 U.S.C. §119(a) of a Korean Patent Application No. 10-2011-0004767, filed on Jan. 18, 2011, in the Korean Intellectual Property Office, the entire disclosure of which is incorporated herein by reference for all purposes.

BACKGROUND

1. FIELD
The following description relates to an apparatus for obtaining status information about a crystalline lens of a person's eyeball, and optical/electronic equipment including the apparatus.
2. Description of the Related Art
A person has an eyeball structure that may adjust a thickness of a crystalline lens to focus objects with different distances from the crystalline lens. A person's eyeball focuses on objects by increasing the thickness of the crystalline lens while the person views objects located close to the crystalline lens and by decreasing the thickness of the crystalline lens while viewing objects far from the crystalline lens. Accordingly, the radius of curvature of the crystalline lens (specifically, the cornea surrounding the crystalline lens) also decreases or increases depending on a distance from the crystalline lens to an object.
Optical devices, such as a telescope, a microscope, a camera, and the like, or direct view displays such as a head-mount display, generally include an external focusing terminal or a mechanical focusing device that may correct focus deviations based on a person's sights and/or various environments. A person who utilizes such an optical device or direct view display may manually manipulate the external focusing terminal to correct focus deviations or conduct refocusing.
Various methods for detecting changes in thickness of a crystalline lens to obtain status information of the crystalline lens have been proposed. For example, Japanese Laid-open Patent Application No. 2000-139841, entitled “a Method of Measuring Changes in Thickness of Crystalline Lens, and a Training System for Self-Care of Pseudomyopia Using the Method” relates to a method of irradiating an infrared light on an eyeball, photographing the eyeball with a CCD camera, and analyzing the photographed images using a computer to measure changes in thickness of a crystalline lens. Also, Japanese Laid-open Patent Application No. 2006-195084 entitled “display apparatus” relates to a display apparatus for estimating the thickness of a crystalline lens using light reflected from an eyeball and displaying images adaptively according to the status of the eyeball. According to the conventional techniques, a light emitted from a light source is incident to an eyeball via a translucent mirror and a pair of convex lenses, and a reflection light that is to be measured by a crystalline lens thickness measurer passes through the convex lenses and is deflected by the translucent mirror, so that the path of the reflection light is directed towards the crystalline lens thickness measurer.
Meanwhile, there are currently many displays that support Full High Definition. Thus, in spite of development of data compression technologies, an amount of video data that has to be processed is increasing as a result of the high resolution. The increase in the amount of video data that has to be processed increases the load of an encoder (or an image acquisition apparatus having an encoder). In this example, an image acquisition apparatus for acquiring stereoscopic images or a display for reproducing the stereoscopic images has greater load because the apparatus has to process left-eye and right-eye images.

SUMMARY

In one exemplary embodiment, there may be provided an apparatus for obtaining status information of a crystalline lens of an eye. The apparatus includes a light projector configured to project a reference light to the crystalline lens, an intensity detector configured to detect an intensity of scattered light that is generated from the reference light by being scattered at the crystalline lens; and, a calculator configured to calculate thickness information of the crystalline lens based on the intensity of scattered light.
In another exemplary embodiment, there may be provided a three-dimensional (3D) glasses apparatus. The 3D glasses apparatus includes a light projector configured to project a reference light to a crystalline lens of an eye of a user wearing the 3D glasses, an intensity detector configured to detect an intensity of scattered light that is generated from the reference light by being scattered at the crystalline lens, a calculator configured to calculate thickness information of the crystalline lens based on the intensity of scattered light; and a transmitter configured to transmit the thickness information of the crystalline lens to an external device.
In yet another exemplary embodiment, there may be provided a three-dimensional (3D) image display system. The 3D image display system includes a 3D image reproducing apparatus configured to reproduce 3D images on a 3D display and a 3D glasses used to view the 3D images displayed on the 3D display. The 3D glasses includes a crystalline lens thickness detector configured to detect thickness information of a crystalline lens of an eye of a wearer, and a transmitter configured to transmit the thickness information of the crystalline lens to the 3D image reproducing apparatus. The 3D image reproducing apparatus includes a receiver configured to receive the thickness information of the crystalline lens from the 3D glasses, and a controller configured to adjust the 3D images based on the thickness information of the crystalline lens. The crystalline lens thickness detector includes a light projector configured to project a reference light to the crystalline lens of the eye of the wearer, an intensity detector configured to detect an intensity of scattered light that is generated from the reference light by being scattered at the crystalline lens and a calculator configured to calculate the thickness information of the crystalline lens based on the intensity of scattered light.
In still another exemplary embodiment, there may be provided a three-dimensional (3D) image acquisition apparatus. The 3D image acquisition apparatus includes a left camera, a right camera spaced away from the left camera, a crystalline lens thickness detector positioned on at least one of the left camera and right camera, and configured to detect thickness information of a crystalline lens of an eye of a user who is photographing with the 3D image acquisition apparatus and an image processor configured to encode at least one of a left image acquired by the left camera and a right image acquired by the right camera based on the thickness information of the crystalline lens. The crystalline lens thickness detector includes a light projector configured to project a reference light to the crystalline lens of the eye of the wearer, an intensity detector configured to detect an intensity of scattered light that is generated from the reference light by being scattered at the crystalline lens and a calculator configured to calculate the thickness information of the crystalline lens based on the intensity of scattered light.
In still another exemplary embodiment, there may be provided a method for obtaining information of a crystalline lens of an eye. The method includes projecting a reference light to the crystalline lens of the eye, detecting an intensity of scattered light that is generated from the reference light by being scattered at the crystalline lens and calculating the thickness information of the crystalline lens based on the intensity of scattered light.
Other features and aspects will be apparent from the following detailed description, the drawings, and the claims.

BRIEF DESCRIPTION OF THE DRAWINGS

FIGS. 1A and 1B are diagrams illustrating examples of a focal length of a human being's eyeball varying according to a distance to an object.

FIGS. 2A and 2B are diagrams illustrating examples of lights perpendicularly incident to crystalline lenses having different radiuses of curvature.

FIG. 3 is a diagram illustrating an example of an apparatus for obtaining status information of a crystalline lens.

FIG. 4 is a diagram illustrating an example of a 3D image display system.

FIG. 5 is a diagram illustrating an example of a 3D image acquisition apparatus.

FIG. 6 is a diagram illustrating an example of a 3D imaging method.

Throughout the drawings and the detailed description, unless otherwise described, the same drawing reference numerals will be understood to refer to the same elements, features, and structures. The relative size and depiction of these elements may be exaggerated for clarity, illustration, and convenience.

DETAILED DESCRIPTION

The following description is provided to assist the reader in gaining a comprehensive understanding of the methods, apparatuses, and/or systems described herein. Accordingly, various changes, modifications, and equivalents of the methods, apparatuses, and/or systems described herein will be suggested to those of ordinary skill in the art. Also, descriptions of well-known functions and constructions may be omitted for increased clarity and conciseness.
The following description relates to an apparatus capable of accurately measuring the thickness of a crystalline lens and of obtaining status information of the crystalline lens without deteriorating the staring capacity, and optical/electronic equipment including the same.
The following description also relates to an optical/electronic device that can perform automatic control according to the focal length of a user's eyeball.
The following description also relates to a 3D image acquisition apparatus or a 3D image display capable of reducing the amount of data that has to be processed.
FIGS. 1A and 1B illustrate examples of a focal length of a human being's eyeball varying according to a distance to an object. For example, FIG. 1A is the case in which an object 2 a is located relatively close to the eyeball and FIG. 1B is the case in which an object 2 b is located relatively far from the eyeball.
Referring to FIGS. 1A and 1B, a thickness of the crystalline lens (4 a, 4 b) of a human being's eyeball adjusts based on the distances to the objects 2 a and 2 b so that the focal length is controlled. For example, as illustrated in FIG. 1A, if the object 2 a is located relatively close to the eyeball, the crystalline lens 4 a is thickened so that the focal length of the eyeball is shortened. In this example, the radius of curvature of the crystalline lens 4 a is relatively small. Meanwhile, as illustrated in FIG. 1B, if the object 2 b is located farther from the eyeball, the crystalline lens 4 b becomes thinner so that the focal length of the eyeball is lengthened. In this example, the radius of curvature of the crystalline lens 4 b is relatively great.
FIGS. 2A and 2B illustrate examples of light that is perpendicularly incident to crystalline lenses having different radiuses of curvature.
Typically, light scattering is a phenomenon in which light is scattered in all directions when it encounters a certain object having a rough surface. That is, scattered lights mean lights that have directions that change by scattering of light. As described herein, the term “scattered lights” is not limited to lights that are scattered by light scattering, and includes all lights scattered in all directions from a certain light perpendicularly incident to a surface having a predetermined radius of curvature. It should also be understood that a light reflected through the same path as a light incident to a crystalline lens does not belong to the “scattered lights”.
When a certain light is incident to a crystalline lens, the light may have different scattering ranges according to a radius of curvature of the crystalline lens. For example, a scattering range θ₁of scattered lights L_2awhen the radius of curvature of the crystalline lens 4 a (specifically, the cornea surrounding the crystalline lens 4 a) is small, as illustrated in FIG. 2A, is relatively larger than a scattering range θ₂of scattered lights L_2bwhen the radius of curvature of the crystalline lens 4 b is great, as illustrated in FIG. 2B (θ₁>θ₂). As a result, when the radius of curvature of the crystalline lens 4 a is small, the intensity (that is, the intensity of scattered lights per a unit area) of the scattered lights L_2abecomes weaker, while when the radius of curvature of the crystalline lens 4 b is great, the intensity of the scattered lights L_2bbecomes stronger. In the current example, changes in intensity of scattered lights according to changes in radius of curvature of a crystalline lens are used to obtain status information of the crystalline lens. The status information may include thickness information about the crystalline lens.
FIG. 3 illustrates an example of an apparatus for obtaining status information of a crystalline lens.
Referring to FIG. 3, the apparatus for obtaining status information of a crystalline lens includes a light source unit 10, a light receiving unit 20, and a calculating unit 30. The light source unit 10 creates a reference light L₁and directs the reference light L₁incident to a crystalline lens 4 of a person. In order to directly measure scattered lights L₂beyond the visual field of an eyeball and efficiently measure changes in intensity of the scattered lights L₂according to changes in radius of curvature of the crystalline lens 4, the light source unit 10 may direct the reference light L₁straightly incident to the crystalline lens 4. A part of the reference light L₁that is straightly incident to the crystalline lens 4 becomes a reflection light that reflects back along the incident path of the reference light L₁, however, the remaining part of the reference light L₂becomes scattered lights L₂.
The light source unit 10 may be disposed between the eyeball and an object 2. For example, the light source unit 10 may be disposed at an arbitrary location on an imaginary line connecting the eyeball to the object 2. In this example, the light source unit 10 may become an obstacle in the visual field. The apparatus for obtaining the status information of a crystalline lens may be applied to applications in which it does not matter that the light source unit 10 becomes an obstacle in the visual field.
As another example, the light source unit 10 may be spaced a predetermined distance away from an imaginary line connecting the eyeball to the object 2. In this example, the light source unit 10 may be disposed as far away from the imaginary connection line as possible in order not to become an obstacle in the visual field. However, if the light source unit 10 is spaced too far from the imaginary connection line and accordingly it has too large angle with the reference light L₁, the intensity of scattered lights received by the light receiving unit 20 may become weak and also measurement sensitivity in measuring changes in thickness of the crystalline lens may deteriorate.
In order to overcome these potential drawbacks, the light source unit 10 may direct the reference light L₁straightly incident to the eyeball along the imaginary line connecting the eyeball to the object 2, so that the light source unit 10 does not become an obstacle in the visual field of the eyeball. For example, the light source unit 10 may include a light source 12 for generating the reference light L₁and a light path changing unit 14 for changing a path of the reference light L₁emitted from the light source 12. In this example, the light source 12 may be disposed beyond the visual field so that it does not become an obstacle in the visual field. For example, the light source 12 may be disposed above or below the imaginary line connecting the eyeball to the object 2.
In this example, light generated by the separate light source 12, instead of a peripheral light, is used as the reference light L₁. In the case of using a peripheral light as the reference light L₁, it is needed to accurately measure the intensity, amount, and the like, of the peripheral light in order to obtain status information of the crystalline lens 4. However, if a light from the separate light source 12 is used as the reference light L₁, the intensity, amount, and the like, of the reference light L₁may be arbitrarily adjusted to ensure a sufficient intensity and amount of light for enabling the light receiving unit 20 to measure status information of the crystalline lens 4. In this case, in order to avoid the reference light L₁from blurring vision, an invisible light, such as ultraviolet, infrared, and the like, may be used as the reference light L₁.
In the example of FIG. 3, the light path changing unit 14 is disposed on the imaginary line connecting the eyeball to the object 2. The light path changing unit 14 changes the path of the reference light L₁emitted from the light source 12 toward the eyeball. For example, the path of the reference light L₁may be changed approximately 90 degrees by means of the light path changing unit 14. It will be also apparent to one skilled in the art that the path of the reference light L₁can be changed by another angle than 90 degrees. The reference light L₁that has a path that is changed by means of the light path changing unit 14 may be straightly incident to the crystalline lens 4.
For example, the light path changing unit 14 may be a prism. As illustrated in FIG. 3, the prism 14 may change the path of the reference light L₁by 90 degrees to make the reference light L₁straightly incident to the crystalline lens 4. In this example, the prism 14 may have an optical characteristic that it is shown transparent in the direction of a line of sight, in order not to become an obstacle in the visual field. As another example, the prism 14 may have a very small size that cannot be recognized with the naked eye or at least that becomes no obstacle in the visual field. For example, the prism 14 may be a dot prism pattern formed on a transparent lens, and the like.
The apparatus for obtaining status information of a crystalline lens may include at least one light receiving unit 20. The light receiving unit 20 may receive scattered lights L₂of a reference light L₁that is incident to the crystalline lens 4, convert information about the scattered lights L₂to an electrical signal, and output the electrical signal. For example, the light receiving unit 20 may include a photosensitive device, such as a CMOS image sensor or a CCD, in order to receive the scattered lights L₂. The type of the photosensitive device is not limited thereto. The photosensitive device may sense lights corresponding to the wavelength of the reference light L₁.
The light receiving unit 20 may have an entrance with a predetermined width. As illustrated in FIG. 2A, in the case where the distance between an eyeball and an object is relatively short so that the radius of curvature of the crystalline lens is small, a scattering range of scattered lights L₂is wide. Accordingly, the intensity of the scattered lights L₂that are received by the light receiving unit 20 is relatively weak. On the contrary, as illustrated in FIG. 2B, if the distance between an eyeball and an object is relatively distant so that the radius of curvature of the crystalline lens is great, a scattering range of scattered lights L₂is narrow. Accordingly, the intensity of the scattered lights L₂that are received by the light receiving unit 20 is relatively strong. In order to efficiently receive the scattered lights L₂passing through the entrance of the light receiving unit 20, a predetermined optical lens may be positioned between the entrance of the light receiving unit 20 and the photosensitive device.
The light receiving unit 20 directly receives scattered lights L₂that are scattered against the crystalline lens 4, for example, against the surface of the cornea surrounding the crystalline lens 4. In this example, there is no subsidiary optical means such as a reflector for changing the path of light between the crystalline lens 4 and the light receiving unit 20. Therefore, loss of the scattered lights L₂due to reflection, and the like, can be prevented, which improves the measurement accuracy of the light receiving unit 20. As another example, in consideration of polarization degrees (for example, ¼ of the wavelength of the reference light L₁) of the scattered lights L₂with respect to the reference light L₁, a polarizer (not shown) for efficiently passing polarized ones of the scattered lights L₂through may be positioned at the entrance of the light receiving unit 20.
The light receiving unit 20 may be disposed beyond the visual field of the eyeball in order to not be an obstacle in the visual field. For example, the light receiving unit 20 may be disposed at an angle of about 15 through 60 degrees with respect to the incident path of the reference light L₁, or at an arbitrary location in which the light receiving unit 20 is not an obstacle in the visual field according to an application. If the light receiving unit 20 is disposed beyond the visual field and close to the crystalline lens 4 as much as possible, the measurement efficiency of the scattered light L₂can be improved.
The calculating unit 30 may obtain thickness information of the crystalline lens 4 using information about the scattered lights L₂received by the light receiving unit 20. The calculating unit 30 may be electrically connected to the light receiving unit 20 and may obtain thickness information of the crystalline lens 4 using information (for example, intensity) about the scattered lights L₂output from the light receiving unit 20. This distinction between the calculating unit 30 and the light receiving unit 20 is only functional distinction. For example, the calculating unit 30 and the light receiving unit 20 may be implemented as two physically separated units or may be integrated into a single unit.
For example, the calculating unit 30 may be means for calculating a change in thickness of the crystalline lens 4 or a relative thickness of the crystalline lens 4, instead of being a means for calculating an absolute thickness of the crystalline lens 4. For example, the calculating unit 30 may compare the intensity of the scattered lights L₂measured by the light receiving unit 20 to a predetermined reference value or a previously measured value, in order to calculate a change in thickness of the crystalline lens 4. As another example, the calculating unit 30 may determine only whether the measured intensity of the scattered lights L₂is above or below a predetermined reference value.
Because the thicknesses, radiuses of curvature, surface roughness, and the like, of crystalline lenses have deviations, a reference value that is used in calculating a change in thickness of a crystalline lens may be set differently for each user. For example, the light receiving unit 20 may measure the intensity of scattered lights L₂from a reference light L₁generated by the light source unit 10 and incident to the crystalline lens of a specific user who views an object placed at a predetermined distance from the crystalline lens. The predetermined distance may be based on an application type of the apparatus for obtaining status information of a crystalline lens, and the measured intensity of the scattered lights L₂may be used as a reference value. As another example, the calculating unit 30 may estimate a change in thickness of the crystalline lens 4 using a difference between a value previously measured by the light receiving unit 20 and a value currently measured by the light receiving unit 20.
In this example, the apparatus for obtaining status information of a crystalline lens may obtain status information of a crystalline lens by directly receiving scattered lights from a reference light straightly incident to the crystalline lens. Also, the apparatus for obtaining status information of a crystalline lens may use a prism to change a path of a reference light generated by a light source disposed at a location in which the prism is not an obstacle in the visual field, thereby making the reference light straightly incident to the crystalline lens. Accordingly, it is unnecessary to provide a separate translucent mirror for passing a reference light through to change the path of a reflection light. Also, the light receiving unit 20 has excellent measurement efficiency because it directly receives scattered lights and measures the intensity of the scattered lights.
FIG. 4 illustrates an example of a 3D image display system. The 3D image display system is an example of an application apparatus for obtaining status information of a crystalline lens, as described herein with reference to FIG. 3. Referring to FIG. 4, the 3D image display system includes 3D glasses 110 which a user may wear to view 3D images that are displayed on a 3D display, and a 3D image reproducing apparatus 120 for reproducing the 3D images on the 3D display.
The type of the 3D glasses 110 is not limited. For example, the 3D glasses 110 may be active shutter glasses or polarization glasses. As another example, the 3D glasses 110 may be new type glasses that will be developed in the future.
The 3D glasses 110 include a frame 112 and lenses 114. The frame 112 includes a pair of frame bodies 112 a (also, 112 a for each) surrounding the lenses 114 (also, 114 for each), and frame legs 112 b (also, 112 b for each) that respectively extend from the frame bodies 112 a and are to be placed on a user's ears. The frame 112 of the 3D glasses 110 may further include additional means (for example, a pair of nose supporting plates attached to a connection point of the frame bodies 112 a, which are not shown in the drawing) for assisting a user wearing the 3D glasses 110.
As another example, the 3D glasses 110 may be rimless glasses without frame bodies. In this example, the light source 12 of the apparatus for obtaining status information of a crystalline lens may be disposed, instead of at the frame body 112 a, at the frame leg 112 b, for example, at a connection point between the frame leg 112 b and the lens 114. Other components except for the light source 12 may be disposed at the same locations as in the 3D glasses 110, which is described later. Hereinafter, the 3D glasses 110 having the frame bodies 112 a are described.
The 3D glasses 110 include the apparatus for obtaining status information of a crystalline lens, as described above with reference to FIG. 3. For example, the 3D glasses 110 include the light source unit 10, the light receiving unit 20, and the calculating unit 30. The 3D glasses 110 may have one apparatus for obtaining status information of a crystalline lens, or multiple apparatuses of obtaining status information of a crystalline lens at the left and right sides.
The light source unit 10 includes a light source 12 for generating a reference light, and a light path changing unit 14 for changing the path of the reference light emitted from the light source 12 toward crystalline lens. The light source 12 may be disposed at a predetermined location on the frame body 112 a. For example, the light source 12 may be disposed between the lenses 114 or at a connection point between the lens 114 and the frame leg 12 b in order not to become an obstacle in the visual field. As another example, the light source 12 may be disposed at a frame leg part connected to the frame body 112 a. Also, the light path changing unit 14 may be formed at the center portion of the lens 14, as a dot for creating a micro-sized prism that cannot be recognized with a naked eye or that becomes a very little obstacle in the visual field. The light path changing unit 14 formed in the center portion of the lens 114 may reflect a reference light emitted from the light source 12 at a predetermined angle to make the reference light straightly incident to the crystalline lens of a user who wears the 3D glasses 110.
The light receiving unit 20 which receives scattered lights may be disposed at a predetermined location on the frame leg 112 b. For example, the light receiving unit 20 may be disposed at a frame leg portion that is closest to the eyeball of the user who is wearing the 3D glasses. In this example, the light receiving unit 20 may be disposed slightly in front of the eyeball in order to efficiently receive the scattered lights. The calculating unit 30 may be integrated with the light receiving unit 20 or disposed adjacent to the light receiving unit 20. As described above, the calculating unit 30 may obtain thickness information of a crystalline lens using the intensity of scattered lights or obtain changes in intensity of the scattered lights, which is measured by the light receiving unit 20.
The 3D glasses 110 further include a transmission unit 116. The transmission unit 116 is used to transmit thickness information of a crystalline lens obtained by the calculating unit 30 to an external electronic device. For example, the transmission unit 116 may transmit thickness information of a crystalline lens to a 3D image reproducing apparatus 120 of a 3D image display system. For example, the transmission unit 116 may be a transmitter, such as BLUETOOTH® or Zigbee, based on a Near Field Communication (NFC) standard.
The thickness information that is transmitted by the transmission unit 116 may relate to the radius of curvature of the crystalline lens. For example, the thickness information may indicate that the radius of curvature of the crystalline lens is above or below a predetermined reference value. As another example, the thickness information may include a degree at which the radius of curvature (or the thickness) of the crystalline lens increases or decreases, or information about an amount of deviation from a reference value.
As described above, the 3D image display system includes the 3D image reproducing apparatus 120 for reproducing 3D images on a 3D display. The 3D image reproducing apparatus 120 may reproduce 3D images on the 3D display by decrypting encrypted 3D video content. Operation of decrypting encrypted 3D video content may be performed by an image processor 126 of the 3D image reproducing apparatus 120. For example, the 3D image reproducing apparatus 120 may be installed in a television, a computer monitor, a display of a mobile terminal, or in an external electronic apparatus electrically connected to the electronic appliance so that 3D images can be reproduced on the electronic appliance.
For example, the 3D image reproducing apparatus 120 may receive thickness information of a crystalline lens from the 3D glasses 110 and change the format of 3D images that are to be reproduced on a display adaptively based on the thickness information. For example, if the thickness of the crystalline lens exceeds a predetermined reference value, the 3D image reproducing apparatus 120 may reproduce 3D images based on binocular disparity. As another example, if the thickness of the crystalline lens is less than the predetermined reference value, the 3D image reproducing apparatus 120 may reproduce 2D images based on brightness or depth perception, or reproduce new 3D images that can be represented with a small amount of data compared to existing 3D images.
The images may be reproduced based on the assumption that when an object is relatively far away from a crystalline lens, binocular disparity is small and also a human being's vision is not easy to recognize a cubic effect. In the case in which an object is far away from a crystalline lens, a viewer may little recognize deterioration of cubic effect although 2D images are reproduced. Meanwhile, if the distance between an object and a crystalline lens is longer than a predetermined distance (for example, 3 m), the 3D image reproducing apparatus 120 reproduces 2D images or new 3D images that can be represented with a relatively small amount of data, on the 3D display, resulting in reduction of an amount of data processing and improvement of processing speed.
For this operation, the 3D image reproducing apparatus 120 includes a receiving unit 122 and a control unit 124. The receiving unit 122 may be used to receive thickness information transmitted from the transmission unit 116 of the 3D glasses 110. A communication method of the receiving unit 122 corresponds to a communication method of the transmission unit 116, and the configuration of the receiving unit 122 is not limited. The control unit 124 may control the format of 3D images that are reproduced on the display, based on the thickness information. For example, the controller 124 may control the image processing unit 126 of the 3D image reproducing apparatus 120 to decrypt encrypted 3D video content and restore 3D or 2D images based on binocular disparity, thereby adaptively changing the format of images that are restored by the 3D image reproducing apparatus 120 and transferred to the display.
FIG. 5 illustrates an example of a 3D image acquisition apparatus.
The 3D image acquisition apparatus is another example of an application apparatus that uses status information of a crystalline lens, as described above with reference to FIG. 3.
Referring to FIG. 5, the 3D image acquisition apparatus includes a pair of cameras (that is, a left camera 202 and a right camera 204), an apparatus 206 for obtaining status information of a crystalline lens, and an image processor 210.
The configuration of the cameras 202 and 204, which are image acquisition devices for photographing 3D images, is not limited thereto. In this example, the left camera 202 is spaced a predetermined distance from the right camera 204. The distance between the left and right cameras 202 and 204 may be fixed or may not be fixed. The distance between the left and right cameras 202 and 204 may correspond to the distance between a human being's eyes. The left camera 202 photographs a left image of a 3D image and the right camera 204 photographs a right image of the 3D image. One or both of the left and right cameras 202 and 204 may include the apparatus 206 for obtaining status information of a crystalline lens. The apparatus 206 for obtaining status information of a crystalline lens may have the configuration illustrated in FIG. 3. Accordingly, the apparatus 206 for obtaining status information of a crystalline lens includes the light source unit 10, the light receiving unit 20, and the calculating unit 30.
Referring again to FIG. 3, the light source unit 10 includes the light source 12 for generating a reference light, and the light path changing unit 14 for changing the path of the reference light emitted from the light source 12 toward crystalline lens. For example, the light source 12 may be installed at or around an eyepiece frame into which an eyepiece of the left and/or right camera 202 and/or 204 is inserted. The light path changing unit 14 is formed at the center of the eyepiece, as a dot for creating a micro-sized prism that cannot be recognized with a naked eye or that is a little obstacle in the visual field. The light path changing unit 14 formed at the center of the eyepiece reflects a reference light emitted from the light source 12 at a predetermined angle, to make the reference light straight incident to the crystalline lens of a user who photographs 3D images through a 3D image acquisition apparatus. In addition, the light receiving unit 20 for receiving scattered lights may be disposed at or around the eyepiece frame. Also, the calculating unit 30 may be integrated with the light receiving unit 20 or disposed adjacent to the light receiving unit 20.
The image processor 210 may encode one or both of left and right images acquired by the left and right cameras 202 and 204 based on thickness information that is received from the apparatus 206 for acquiring status information of a crystalline lens. For example, if the thickness of the crystalline lens exceeds a predetermined reference value, the image processor 210 may encode both the left and right images, and if the thickness of the crystalline lens is below the predetermined reference value, the image processor 210 may encode one of the left and right images.
The operation of the image processor 210 may be controlled by the control unit 208. Like the 3D image display system illustrated in FIG. 4, the current example is also based on the assumption that when an object is relatively far away from a crystalline lens, binocular disparity is small and also a human being′ vision is not easy to recognize a cubic effect. Accordingly, if the distance from a crystalline lens to an object is longer than a predetermined distance (for example, 3 meters), the image processor 210 encodes only one of the left and right images, thereby reducing the amount of data processing and increasing processing speed. For example, image data processed by the image processor 210 may be stored in a memory 212.
FIG. 6 illustrates an example of a 3D imaging method. For example, the method may be used to obtain information of a crystalline lens of an eyeball of a person.
Referring to FIG. 6, in 601, light is directed towards the crystalline lens of the eyeball. For example, the directing may be performed by a source that is not in the field of view of the person. As merely one example, the source may be included in a pair of three-dimensional (3D) glasses.
In 602, light scattered against the crystalline lens of the eyeball is received. For example, light may be directed in 601 to be perpendicularly incident on the crystalline lens of the eyeball. As a result, the light may reflect in a scattered pattern and may be received by an imaging element in 602.
In 603, thickness information of the crystalline lens is calculated based on the received scattered lights.
The Examples described herein with respect to FIGS. 1-5 are also applicable to the method of FIG. 6, however, additional description thereof is omitted here for conciseness.
A number of examples have been described above. Nevertheless, it will be understood that various modifications may be made. For example, suitable results may be achieved if the described techniques are performed in a different order and/or if components in a described system, architecture, device, or circuit are combined in a different manner and/or replaced or supplemented by other components or their equivalents. Accordingly, other implementations are within the scope of the following claims.

Claims

What is claimed is:

1. An apparatus for obtaining status information of a crystalline lens of an eye, the apparatus comprising:

a light projector configured to project a reference light to the crystalline lens;

an intensity detector configured to detect an intensity of scattered light that is generated from the reference light by being scattered at the crystalline lens; and

a calculator configured to calculate thickness information of the crystalline lens based on the intensity of scattered light.

2. The apparatus of claim 1, wherein the light projector comprises:

a light source positioned outside of a visual field of the eye and configured to generate the reference light; and

a light path changer configured to change a direction of the reference light received from the light source to a direction in which the reference light perpendicularly enters the crystalline lens.

3. The apparatus of claim 2, wherein the light path changer comprises a prism that is positioned at an approximately center of the visual field of the eye.

4. The apparatus of claim 1, wherein the reference light is an invisible light.

5. The apparatus of claim 1, wherein the calculator is further configured to calculate a change amount of a thickness of the crystalline lens based on a change amount of the intensity of the scattered light.

6. The apparatus of claim 1, wherein the calculator is further configured to calculate a thickness of the crystalline lens based on the intensity of the scattered light and a predetermined reference value.

7. The apparatus of claim 1, further comprising a polarizer positioned at an entrance of the intensity detector.

8. A three-dimensional (3D) glasses apparatus comprising:

a light projector configured to project a reference light to a crystalline lens of an eye of a user wearing the 3D glasses;

an intensity detector configured to detect an intensity of scattered light that is generated from the reference light by being scattered at the crystalline lens;

a calculator configured to calculate thickness information of the crystalline lens based on the intensity of scattered light; and

a transmitter configured to transmit the thickness information of the crystalline lens to an external device.

9. The 3D glasses of claim 8, wherein the light projector comprises:

a light source positioned at a frame body of the 3D glasses and configured to generate the reference light; and

a light path changer positioned on a lens of the 3D glasses and configured to change a direction of the reference light received from the light source to a direction in which the reference light perpendicularly enters the crystalline lens.

10. The 3D glasses of claim 9, wherein the light path changer comprises a micro-sized prism.

11. A three-dimensional (3D) image display system comprising:

a 3D image reproducing apparatus configured to reproduce 3D images on a 3D display; and

a 3D glasses used to view the 3D images displayed on the 3D display,

wherein the 3D glasses comprise:

a crystalline lens thickness detector configured to detect thickness information of a crystalline lens of an eye of a wearer, and

a transmitter configured to transmit the thickness information of the crystalline lens to the 3D image reproducing apparatus, and

wherein the 3D image reproducing apparatus comprises:

a receiver configured to receive the thickness information of the crystalline lens from the 3D glasses, and

a controller configured to adjust the 3D images based on the thickness information of the crystalline lens,

wherein the crystalline lens thickness detector comprises:

a light projector configured to project a reference light to the crystalline lens of the eye of the wearer;

a calculator configured to calculate the thickness information of the crystalline lens based on the intensity of scattered light.

12. The 3D image display system of claim 11, wherein the controller is further configured to display the 3D images based on binocular disparity, if the thickness of the crystalline lens is less than a predetermined reference value, and display 2D images if the thickness of the crystalline lens is greater than the predetermined reference value.

13. A three-dimensional (3D) image acquisition apparatus comprising:

a left camera;

a right camera spaced away from the left camera;

a crystalline lens thickness detector positioned on at least one of the left camera and right camera, and configured to detect thickness information of a crystalline lens of an eye of a user who is photographing with the 3D image acquisition apparatus; and

an image processor configured to encode at least one of a left image acquired by the left camera and a right image acquired by the right camera based on the thickness information of the crystalline lens,

wherein the crystalline lens thickness detector comprises:

14. The 3D image acquisition apparatus of claim 14, wherein the image processor is further configured to encode both of the left image and right image, if the thickness of the crystalline lens is less than a predetermined reference value, and encode one of the left image and right image if the thickness of the crystalline lens is greater than the predetermined reference value.

15. A method for obtaining information of a crystalline lens of an eye, the method comprising:

projecting a reference light to the crystalline lens of the eye;

detecting an intensity of scattered light that is generated from the reference light by being scattered at the crystalline lens; and

calculating the thickness information of the crystalline lens based on the intensity of scattered light.

16. The method of claim 15, wherein the projecting is performed by a light source that is positioned outside of a field of view of the eye.

17. The method of claim 16, wherein the projecting comprises:

projecting the reference light, by the light source, to a light path changer that is positioned in the field of view of the eye, and

changing a direction of the reference light, by the light path changer, to a direction in which the reference light perpendicularly enters the crystalline lens.

calculating thickness information of the crystalline lens based on the received scattered lights.

18. The method of claim 17, wherein the directing is performed by a source that is not in the field of view of the person.

19. The method of claim 18, wherein the source is included in a pair of three-dimensional (3D) glasses.

20. The method of claim 17, wherein the directing comprises directing the light to be perpendicularly incident on the crystalline lens of the eyeball.