The present application is the U.S. national phase entry of the international application PCT/CN2017/110412, with an international filing date of Nov. 10, 2017, which claims the benefit of Chinese Patent Application No. 201610815306.1, filed on Sep. 9, 2016, and Chinese Patent Application No. 201710166323.1, filed on Mar. 20, 2017, the entire disclosures of which are incorporated herein by reference.
The present disclosure relates to the field of display technology, and particularly to a holographic display panel and a holographic display device.
Stereoscopic display based on holographic information is getting more and more attention. In the recording of holographic information, two laser beams traveling along different paths (i.e., a reference beam and an object beam) interfere with each other to form an optical interference pattern. The optical interference pattern causes a chemical or physical change in the photosensitive recording medium so that information relating to the object to be reconstructed is recorded in the recording medium. In the reconstruction of the holographic information, a reference beam similar to the reference beam for recording is irradiated to the recording medium so that the optical interference pattern in the recording medium diffracts the reference beam to reconstruct the object beam, thereby reconstructing the holographic information. With the continuous development of display technologies, stereoscopic display technologies have become increasingly popular. Typically, dynamic display of a hologram image can be achieved by using e.g. a combination of a liquid crystal display panel and a phase plate. In realizing stereoscopic display, different views with a horizontal parallax are provided to the user's left and right eyes, respectively. Through the fusion of the brain, a stereoscopic image with depth perception is finally formed.
The embodiments of the present disclosure provide a holographic display panel, a holographic display device and a holographic display method.
According to an aspect of the present disclosure, an embodiment of the present disclosure provides a holographic display panel. The holographic display panel includes: a plurality of sub-pixels arranged in an array and a phase plate disposed on a light exit side of the plurality of sub-pixels; and a blocking member disposed between the plurality of sub-pixels and the phase plate; an orthogonal projection of the blocking member on a plane where the plurality of sub-pixels are located is arranged between adjacent sub-pixels for blocking an edge portion of a light beam diffracted by the sub-pixel.
Optionally, a width a of the blocking member satisfies: a=0.61λd/w, where λ is a wavelength of the light beam, w is a width of the sub-pixel, and d is a distance between the blocking member and the sub-pixel.
Optionally, the holographic display panel further includes a first substrate disposed on the light exit side of the plurality of sub-pixels. The phase plate is disposed on a surface of the first substrate facing away from the plurality of sub-pixels, and the blocking member is disposed on a surface of the first substrate facing the plurality of sub-pixels.
Optionally, the holographic display panel further includes a color film substrate disposed on the light exit side of the plurality of sub-pixels, and the blocking member is disposed on a surface of the color film substrate facing away from the plurality of sub-pixels.
Optionally, the phase plate is configured to adjust an angle of a light beam from the plurality of sub-pixels, and/or the phase plate includes a plurality of sub-phase plates corresponding to the plurality of sub-pixels one-to-one.
Optionally, the phase plate is a diffraction grating.
Optionally, the holographic display panel further includes a plurality of depth display units; each depth display unit includes at least two adjacent pixels, and each pixel includes a plurality of sub-pixels; each depth display unit further includes a plurality of phase plates, each sub-pixel corresponds to a phase plate along a direction of light emitted from the sub-pixel, the phase plate is configured to control a diffraction angle of light emitted through the phase plate; wherein phase plates corresponding to sub-pixels of a same pixel have a same diffraction angle, diffraction angles of light beams emitted by different pixels in a same depth display unit after passing through the phase plate are different, so that reverse extension lines of the light beams emitted from the same depth display unit intersect at a depth position.
Optionally, the plurality of depth display units are divided into display groups arranged in an array, each display group is composed of at least two depth display units adjacent to each other; wherein depths of field of depth display units in a same display group are different.
Optionally, two adjacent depth display units have different depths of field.
According to another aspect of the present disclosure, an embodiment of the present disclosure provides a holographic display device. The holographic display device includes the holographic display panel as described in the above embodiments.
In the following, the technical solutions in embodiments of the disclosure will be described clearly and completely in connection with the drawings in the embodiments of the disclosure. Obviously, the described embodiments are only part of the embodiments of the disclosure, and not all of the embodiments. Based on the embodiments in the disclosure, all other embodiments obtained by those of ordinary skills in the art under the premise of not paying out creative work pertain to the protection scope of the disclosure.
When implementing a near-eye display or using a virtual reality display device, the virtual image or point in the space is determined by the angle of divergence or convergence of the incident light, and such a display device is generally required to have a high resolution (i.e., the number of sub-pixels per inch, PPI). However, the inventors have found that as the resolution increases, the size of the sub-pixels decreases and Fraunhofer diffraction will occur between the sub-pixels and the phase plate of the display panel. The presence of the Fraunhofer diffraction angle results in crosstalk between the light beams from adjacent sub-pixels, which greatly affects the depth of field and position of the stereoscopic image and reduces the display effect.
According to an aspect of the present disclosure, an embodiment of the present disclosure provides a holographic display panel. As shown in
In the embodiment of the present disclosure, by using the blocking member, the problem of beam crosstalk caused by the Fraunhofer diffraction angle of small-size sub-pixels is well solved. Therefore, with the configuration of the embodiments of the present disclosure, clear sub-pixel edges can be obtained, color crosstalk and grayscale crosstalk can be eliminated, and an accurate depth of field of an image can also be provided, improving the visual effect of the holographic display.
As shown in
As shown in
Due to the reduction in the size of the sub-pixel, Fraunhofer diffraction is a major factor in limiting the display resolution. The width condition of the blocking member can be deduced from the Fraunhofer diffraction angle. With the above width condition, the blocking member can block the edge portion of the light beam diffracted by the sub-pixel, avoiding the edge portion from being incident on the portions of the phase plate corresponding to the adjacent sub-pixels.
For a given sub-pixel, the Fraunhofer diffraction angle θ=1.22λ/w. For a smaller angle θ, θ/2≈tgθ/2=a/d. Thus, the width a of the blocking member 103 can be obtained as a=0.61λd/w.
It can be seen from the above relationship that as the distance d increases, the width a of the blocking member 103 also increases accordingly. For a given width w of the sub-pixel, a large blocking member 103 may instead block the portion of the light beam 104 close to the optical axis, thereby losing light intensity. Therefore, the width a of the blocking member 103 (or, the distance d between the blocking member 103 and the sub-pixel 101) should be limited to an appropriate range. Assuming that the interval between two adjacent sub-pixels 101 is p, the width a of the blocking member 103 should be smaller than p. Therefore, 0.61λd/w≤p, that is, the distance d between the blocking member 103 and the sub-pixel 101 is d≤wp/0.61λ.
Optionally, as shown in
Optionally, as shown in
Optionally, as shown in
In practical applications, the phase plate can be integrated or can be composed of a plurality of sub-phase plates arranged on a substrate (as shown in
Similarly, a phase plate composed of an integrated phase plate or a plurality of sub-phase plates can also be disposed on the surface of the first substrate facing away from the plurality of sub-pixels, and the blocking member is disposed on the surface of the first substrate facing the plurality of sub-pixels. In this case, the blocking member can be fabricated using e.g. a black matrix process in the liquid crystal display panel. Therefore, the blocking member can have a plurality of openings that are in one-to-one correspondence with the plurality of effective regions or the plurality of sub-phase plates.
Optionally, the phase plate 102 is a diffraction grating.
With diffraction gratings having different parameters, the light beams from the sub-pixels can be adjusted to desired directions. Thus, as shown in
It should be noted that since the phase plate 102 is used to diffract the incident light, the phase plate 102 can be a phase grating, i.e., a diffraction grating. On this basis, in order to increase the utilization of light, a transmission grating can be selected as the phase plate 102 described above. In this case, since light has different phases in the convex and concave portions of the transmission grating, it is possible to cause diffraction for light passing through the transmission grating.
Specifically, if the phase plate 102 is a transmission grating, the transmission grating can be a single-step grating as shown in
Optionally, as shown in
The plurality of sub-pixels of the holographic display panel can be divided into a plurality of pixel groups, and each pixel group is configured for displaying an image with a specific depth of field. Thus, by applying e.g. time division multiplexing and persistence of vision, the holographic display panel can be used to display a plurality of images having different depths of field, thereby providing a picture having a plurality of depths of field.
Specifically, as shown in
Therefore, optionally, the holographic display panel further includes a plurality of depth display units; each depth display unit includes at least two adjacent pixels, and each pixel includes a plurality of sub-pixels; each depth display unit further includes a plurality of phase plates, each sub-pixel corresponds to a phase plate along a direction of light emitted from the sub-pixel, the phase plate is configured to control a diffraction angle of light emitted through the phase plate; wherein phase plates corresponding to sub-pixels of a same pixel have a same diffraction angle, diffraction angles of light beams emitted by different pixels in a same depth display unit after passing through the phase plate are different, so that reverse extension lines of the light beams emitted from the same depth display unit intersect at a depth position.
Optionally, the plurality of depth display units are divided into display groups arranged in an array, each display group is composed of at least two depth display units adjacent to each other; wherein depths of field of depth display units in a same display group are different.
Optionally, two adjacent depth display units have different depths of field.
According to another aspect of the present disclosure, an embodiment of the present disclosure provides a holographic display device. As shown in
The holographic display device can be any product or component with display function, such as mobile phone, tablet computer, TV, display, notebook computer, digital photo frame and navigator.
According to the holographic display panel and the holographic display device provided by the embodiments of the present disclosure, by using the blocking member, the problem of beam crosstalk caused by the Fraunhofer diffraction angle of small-size sub-pixels is well solved. Therefore, with the configuration of the embodiments of the present disclosure, clear sub-pixel edges can be obtained, color crosstalk and grayscale crosstalk can be eliminated, and an accurate depth of field of an image can also be provided, improving the visual effect of the holographic display.
Apparently, the person skilled in the art may make various alterations and variations to the disclosure without departing the spirit and scope of the disclosure. As such, provided that these modifications and variations of the disclosure pertain to the scope of the claims of the disclosure and their equivalents, the disclosure is intended to embrace these alterations and variations.
Number | Date | Country | Kind |
---|---|---|---|
2016 1 0815306 | Sep 2016 | CN | national |
2017 1 0166323 | Mar 2017 | CN | national |
Filing Document | Filing Date | Country | Kind |
---|---|---|---|
PCT/CN2017/110412 | 11/10/2017 | WO | 00 |
Publishing Document | Publishing Date | Country | Kind |
---|---|---|---|
WO2018/046025 | 3/15/2018 | WO | A |
Number | Name | Date | Kind |
---|---|---|---|
20070188667 | Schwerdtner | Aug 2007 | A1 |
20100027083 | Kroll et al. | Feb 2010 | A1 |
20100253995 | Reichelt | Oct 2010 | A1 |
20100297538 | Chang et al. | Nov 2010 | A1 |
20120120059 | Bratkovski et al. | May 2012 | A1 |
20130300956 | Chen et al. | Nov 2013 | A1 |
20140300711 | Kroon et al. | Oct 2014 | A1 |
20160223860 | Wang et al. | Aug 2016 | A1 |
20160327906 | Futterer | Nov 2016 | A1 |
20160349702 | Sung | Dec 2016 | A1 |
20160373732 | Kim et al. | Dec 2016 | A1 |
20170017086 | Wei | Jan 2017 | A1 |
Number | Date | Country |
---|---|---|
1894976 | Jan 2007 | CN |
101568888 | Oct 2009 | CN |
202025132 | Nov 2011 | CN |
103918257 | Jul 2014 | CN |
104024349 | Sep 2014 | CN |
104111560 | Oct 2014 | CN |
104570370 | Apr 2015 | CN |
105917277 | Aug 2016 | CN |
106154797 | Nov 2016 | CN |
206002848 | Mar 2017 | CN |
106646905 | May 2017 | CN |
Entry |
---|
Second Office Action for Chinese Patent Application No. 201710166323.1 dated Apr. 1, 2019. |
First Office Action for Chinese Patent Application No. 201610815306.1 dated Apr. 16, 2018. |
Search Report for International Application No. PCT/CN2017/110412 dated Jan. 3, 2018. |
Number | Date | Country | |
---|---|---|---|
20180321499 A1 | Nov 2018 | US |