Open Access
10 September 2013 One-dimensional integral imaging display using a variable parallax barrier
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Abstract
We analyze the effect of aperture width of the parallax barrier on the viewing angle of one-dimensional integral imaging (1-DII) display and propose a 1-DII display that consists of a display panel and a variable parallax barrier. When the variable parallax barrier changes its aperture width, the viewing angle and the optical efficiency of the proposed 1-DII display are compared. The viewing angle is increased by decreasing the aperture width of the variable parallax barrier, while the optical efficiency is increased by increasing the aperture width of the variable parallax barrier.

1.

Introduction

Integral imaging (II) display that presents true three-dimensional (3-D) images with full parallax and continuous viewpoints is regarded as a promising 3-D display.1 But it is difficult to realize high resolution, wide viewing angle, and large depth display.24 To overcome these disadvantages, a number of methods have been proposed.57 A conventional one-dimensional integral imaging (1-DII) display reduces ray information by removing vertical parallax and provides 3-D images with high resolution in the vertical direction.810 Although 1-DII autostereoscopic display resembles a multiview display, an important difference between the 1-DII display and the multiview autostereoscopic display is defined in terms of the position and the interval of beam condensing points. There is no need to predetermine the observer’s viewpoints in the 1-DII display. However, the observer’s viewpoints are light ray converging points and are an important design parameter in the multiview autostereoscopic display. The 1-DII displays have been implemented by using a parallax barrier or a lenticular lens array. The 1-DII display using a parallax barrier uses less space and a lower cost than that using a lenticular lens array.11 Moreover, using the parallax barrier is simpler and has a lower cost than using the lenticular lens array. So the 1-DII display using a parallax barrier is a practical solution for a low cost and easy-viewable 3-D display. However, the relationship between the aperture width of the parallax barrier and the viewing angle of the 1-DII display has not been studied. Therefore, we analyze the effect of aperture width of the parallax barrier on the viewing angle of the 1-DII display. Moreover, we propose a 1-DII display using a variable parallax barrier. The viewing angle and the optical efficiency can be adjusted by adjusting the aperture width of the variable parallax barrier.

2.

Structure and Principle

The primary viewing zone of the 1-DII display using a parallax barrier is shown in Fig. 1. Lights emitted from an elemental image displayed on the display panel are modulated by the corresponding slit and the theoretical viewing zone, in which the observer can theoretically see 3-D images is determined by the solid lines. However, flipping images are seen in part of the theoretical viewing zone which is determined by the long-dashed lines. Therefore, orthoscopic images are only seen in the primary viewing zone which is determined by the short-dashed lines.

Fig. 1

Primary viewing zone of the one-dimensional integral imaging (1-DII) display using a parallax barrier.

OE_52_9_093102_f001.png

Suppose that each parallax barrier ideally integrates the light into one line, point A is one point of the ideal line, L is the distance between the parallax barrier and the observer, g is the gap between the parallax barrier and the display panel, and l is the distance between the point A and the display panel. The pitch and the aperture width of the parallax barrier are PB and PW, respectively. Based on the geometric relationships in Fig. 1, the viewing angle θ can be obtained as

Eq. (1)

θ=2arctan(PB2l).

The relationship between l and PW exists as

Eq. (2)

l=PBgPBPW.

From Eqs. (1) and (2), the relationship between the aperture width and the viewing angle is obtained as

Eq. (3)

θ=2arctan(PBPW2g).

From Eq. (3), we can see that when PB and g are fixed, the viewing angle θ can be increased by decreasing the aperture width and vice verse. The relationship between the aperture width and the viewing angle are not only obtained in 1-DII display using a parallax barrier but also in two-dimensional integral imaging display using a pinhole array.

The optical efficiency of the 1-DII display using a parallax barrier φ is12

Eq. (4)

φ=PWPB.

It is obvious that the optical efficiency of the 1-DII display is increased by increasing the aperture width of the parallax barrier and vice verse. As mentioned above, the viewing angle and the optical efficiency of the 1-DII display using a parallax barrier cannot be simultaneously improved by adjusting the aperture width of the parallax barrier. Therefore, we proposed a 1-DII display using a variable parallax barrier. Figure 2 illustrates the structure of the proposed 1-DII display. It consists of a display panel and a variable parallax barrier. Aperture centers of the variable parallax barrier are located at the centers of the corresponding elemental images on the display panel. Lights from the elemental image array (EIA) displayed on the display panel are modulated by the variable parallax barrier, which reconstructs the angular distribution of the rays and hence displays the 3-D images.

Fig. 2

Structure of the proposed 1-DII display.

OE_52_9_093102_f002.png

There is only an elemental image integrated in Fig. 1. In practice, the more elemental images that are integrated, the smaller the viewing angle becomes.13 The viewing angle of the proposed 1-DII display θ can be obtained as

Eq. (5)

θ=2arctan[PBPW2g(N1)PB2L],
where N is the number of the elemental images in the horizontal direction. Whatever the number of the elemental images integrated, the viewing angle of the proposed 1-DII display can also be increased by decreasing the aperture width of the variable parallax barrier and vice verse.

3.

Experiments and Results

We performed an experiment to verify the proposed 1-DII display. In our experiment, a back light unit and a printed film were combined as a display panel with a high resolution. The display panel was used to generate three identical EIAs, simultaneously. Another printed film was used to generate three parallax barriers with different aperture widths. A high-resolution printer, SCREEN Tanto 6120, was used to print two films, and two printed films are stuck well on a glass substrate. The parameters of the prototype are shown in Table 1.

Table 1

Parameters of the prototype.

SpecificationsValues
PB (mm)5
g (mm)5
L (mm)390
N51

The EIA of 3-D scenes “SC” is generated by using a computer.14 The EIA consists of 51 elemental images and each elemental image has 60×2100pixels. The letters “S” and “C” are located 60 mm in front of and behind the display panel, respectively.

The top, center, and bottom scene “SC”s are behind the three parallax barriers with the aperture widths are 0.25, 0.5, and 0.75 mm, respectively. Corresponding to the aperture widths of three parallax barriers, the viewing angles are 18, 14.6, and 12 deg, respectively. When the viewing angle is 8 deg to the left, there are flipping images in the center and bottom scenes, as shown in Fig. 3(a). Decreasing the viewing angle to 7 deg to the left, there are also flipping images in the bottom scene, as shown in Fig. 3(b). Decreasing the viewing angle to the middle, the full white luminances of 3-D images reconstructed through three parallax barriers are 10.2, 20.1, and 30.6cd/m2, as shown in Fig. 3(c). The optical efficiencies of three 3-D images are 5.1%, 10.05%, and 15.3%, respectively. When the viewing angle increases to 7 deg to the right, there are flipping images in the bottom scene, as shown in Fig. 3(d). Increasing the viewing angle to 8 deg to the right, there are also flipping images in the center and bottom scenes, as shown in Fig. 3(e).

Fig. 3

Images viewed from (a) left 8 deg, (b) left 7 deg, (c) middle, (d) right 7 deg, and (e) right 8 deg.

OE_52_9_093102_f003.png

The experimental results proved that the viewing angle of the proposed 1-DII display is increased by decreasing the aperture width of the parallax barrier. The experimental results also show that the optical efficiency of the proposed 1-DII display is increased by increasing the aperture width of the parallax barrier. For multiple observers, the viewing angle is more important than the optical efficiency. For a single observer, the optical efficiency is more important than the viewing angle. Viewing angle priority 1-DII display is obtained by decreasing the aperture width of the variable parallax barrier, while brightness priority 1-DII display is obtained by increasing the aperture width of the variable parallax barrier. Therefore, the aperture width of the variable parallax barrier can be adjusted to satisfy the observers’ requirements in the real time.

4.

Conclusions

A 1-DII display using a variable parallax barrier is proposed. Its operation principle and calculation equations are described in detail. The viewing angle and the optical efficiency of the proposed 1-DII display are adjusted by adjusting the aperture width of the variable parallax barrier. It could be helpful for mobile applications.

Acknowledgments

The work is supported by the NSFC under Grant Nos. 61225022 and 61036008, the “973” Program under Grant No. 2013CB328802, and the “863” Program under Grant Nos. 2012AA011901 and 2012AA03A301.

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Biography

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Fei Wu is working toward the PhD degree in optical engineering from the School of Electronics and Information Engineering, Sichuan University, China. He has published 15 papers. His recent research interest is information display technologies including three-dimensional (3-D) displays.

OE_52_9_093102_d002.png

Huan Deng is a lecturer of optical engineering at the School of Electronic and Information Engineering, Sichuan University. She has published more than 10 papers. Her recent research interest is information display technologies including 3-D displays.

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Da-Hai Li is a professor of optics at the School of Electronics and Information Engineering, Sichuan University. He received his MS degree from the University of Electronic Science and Technology of China in 1996 and his PhD degree from the Sichuan University in 2002, respectively. He has published more than 30 papers. His recent research interests include optics and optoelectronics, especial display technologies and optical measurements.

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Qiong-Hua Wang is a professor of optics at the School of Electronics and Information Engineering, Sichuan University. She was a postdoctoral research fellow in the School of Optics/CREOL, University of Central Florida, in 2001 to 2004. She received her MS and PhD degrees from the University of Electronic Science and Technology of China (UESTC) in 1995 and 2001, respectively. She worked at UESTC in 1995 to 2001, and at Philips Mobile Display Systems, Philips Shanghai, in 2004. She has published 170 papers on display devices and systems. She holds five US patents and 21 Chinese patents. She is a senior member of Society for Information Display. Her recent research interests include optics and optoelectronics, especial display technologies.

CC BY: © The Authors. Published by SPIE under a Creative Commons Attribution 4.0 Unported License. Distribution or reproduction of this work in whole or in part requires full attribution of the original publication, including its DOI.
Fei Wu, Huan Deng, Da-Hai Li, and Qiong-Hua Wang "One-dimensional integral imaging display using a variable parallax barrier," Optical Engineering 52(9), 093102 (10 September 2013). https://doi.org/10.1117/1.OE.52.9.093102
Published: 10 September 2013
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Cited by 5 scholarly publications.
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KEYWORDS
Integral imaging

3D displays

3D image processing

Autostereoscopic displays

Communication engineering

Lenticular lenses

Image resolution

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