1. Field of the Invention
This invention generally relates to electronic displays and, more particularly, to a display capable of operation using both ambient and internally generated illumination sources.
2. Description of the Related Art
As the thickness of flat-panel liquid crystal (LC) displays is reduced to below 1 centimeter (cm), conventional backlight designs such as compact fluorescent lamp (CFL), which require that the light sources be distributed across the backlight panels, cannot be used due to the geometry limitations of these light sources. Ultra-thin display designs might be implemented using LEDs with small-volume packages. But the cost of these implementations can be high since a large number of LEDs would be required.
Display designs with edge-coupled LEDs using large-size multiple-mode waveguide light pipes enable ultra-thin LC display designs while reducing the number of LEDs used in those displays as well. The edge-coupled schemes reduce the cost of backlight dramatically in addition to supporting the stylish thin look of the displays.
However, the image quality of these edge-coupled displays cannot match that of displays using distributed LEDs as backlight light sources in the backlight panels. For the latter case, each LED light extraction cell of the backlight systems can be individually addressed to create low resolution images of desired images. With the synchronization of backlight low resolution images, in time and spatial domain, to the images on the front high-resolution LC panels, high quality images can be realized with higher contrasts and dynamic responses. In this kind of display implementation, the capability to address desired backlight light extraction cells is the key enabling technology, which is not easily achievable using edge-coupled LED backlight systems.
Regardless of whether an LED or CFL light source is used, LCD panel displays require a significant amount of power to operate, which is a disadvantage if the display is a portable battery-operated unit. Reflective display technology is attractive because these displays consume substantially less power than LCDs displays, by eliminating the power consumption of the backlight source. Some examples of reflective display technologies include electrophoretic, electrowetting, electrochromic, and interference-based MEMS displays. However, the operation of these types of displays completely depends on the availability of ambient light, dramatically limiting their application as a consumer product capable of operating in all kinds of environments, including dark or very dim ambient light conditions.
It would be advantageous if a reflective display could be operated with a backlight when ambient light conditions are dim.
Disclosed herein is a display that can be operated in both reflection and transmission modes to meet everyday operational demands, while keeping power consumption low. The display is based upon a pixel micro-scattering mechanism. This mechanism permits the consistent operation of display pixels in both the reflection and transmission modes. The consistency of operational modes enables uniform display controls under either operational mode, dramatically reducing design and algorithm development.
Accordingly, a scattering tunable display method is provided that uses reflection and edge-lit waveguide transmission modes of illumination. A front panel is provided with an array of selectable display pixels arranged in a plurality of sequences. A backlight panel includes a plurality of edge-coupled waveguide pipes formed in a plurality of rows. Each waveguide pipe has an optical input connected to a corresponding light emitting diode (LED), and an optical output index-matched to a corresponding sequence of display pixels. A high absorption layer underlies the backlight panel. The method selects a display pixel to enable, and measures ambient visible spectrum illumination incident to a top surface of the front panel. In response to the measured ambient illumination being above a first minimum threshold, the display pixel is operated in a reflective illumination mode. In response to the measured ambient illumination being below the first minimum threshold, the display pixel is operated in a transmissive illumination mode.
If the measured ambient illumination is below the first minimum threshold, but above a second minimum threshold, the display pixel is operated in a combination of both reflective and transmissive illumination modes. If the measured ambient light is above the first minimum threshold, the selected display pixel is operated exclusively in the reflective mode. If the measuring ambient illumination is below the second minimum threshold, the display pixel is operated primarily in the transmissive illumination mode.
The front panel selectable display pixels include a medium of liquid crystal molecules, embedded in a polymer network, and interposed between transparent electrodes, and the display pixels are operated by creating a biased potential between the electrodes of a selected display pixel. By supplying an ON voltage, the medium in the selected display pixel operates at a high scattering strength, returning incident light with a maximum reflection efficiency. By enabling an LED corresponding to a waveguide pipe underlying the selected display pixel and supplying the ON voltage, the medium in the selected display pixel operates at the high scattering strength, and extracts light received from the waveguide pipe with a maximum extraction efficiency.
Additional details of the above-described method and a scattering tunable display using reflection and edge-lit waveguide transmission modes of illumination are presented below.
A plurality of light emitting diodes (LEDs) 114-0 through 114-m are shown. Each LED 114 has an optical output connected to a corresponding waveguide pipe edge 112. In one aspect not shown, more than one LED may be interfaced to the waveguide pipe edge. In other aspects not shown, an LED may be interfaced to both edges (ends) of every waveguide pipe. An index-matching layer 116 is interposed between the backlight panel 106 and the front panel 102. A high absorption layer 118 underlies the backlight panel 106. This layer (118) has low reflectivity through the whole visible spectrum, turning the incidental light into heat. Ideally, layer 118 is a black-body in physics.
A light gauge 120 is mounted to the front panel 102, and has an electrical output on line 122 to supply a measurement signal responsive to the intensity of ambient visible spectrum light incident to the front panel. An illumination control module 124 has an input on line 122 to accept the measurement signal and an output on line 126 to supply an LED enable signal responsive to the measurement signal. In response to an ambient illumination measurement above a first minimum threshold, the illumination control module 124 operates selected display pixels in a reflective illumination mode. In response to the ambient illumination measurement being below the first minimum threshold, the illumination control module 124 operates the selected display pixels in a transmissive illumination mode.
In one aspect as shown in
If the illumination control module enables an LED 114 corresponding to a waveguide pipe 108 underlying the selected display pixel 104-1, as shown, the medium 200 in the selected display pixel operates with a high scattering strength in responsive to an ON voltage between the electrodes 202, extracting light (whitearrow) from the waveguide pipe 108 with a first extraction efficiency. The medium 200 in non-selected display pixel 104-0 operates with a low scattering strength in responsive to an OFF voltage between the electrodes 202, extracting light from the waveguide pipe 108 with a second extraction efficiency, less than the first extraction efficiency. Note: most of the light transmitted to pixel 104-0 from the waveguide pipe is reflected back to the light absorption layer 118.
The response of polymer network liquid crystal molecules to an electric field is the major characteristic utilized in industrial applications. The ability of the director to align along an external field is caused by the electric nature of the molecules. Permanent electric dipoles result when one end of a molecule has a net positive charge while the other end has a net negative charge. When an external electric field is applied to the liquid crystal, the dipole molecules tend to orient themselves along the direction of the field. Even if a molecule does not form a permanent dipole, it can still be influenced by an electric field. In some cases, the field produces a slight re-arrangement of electrons and protons in molecules such that an induced electric dipole results. While not as strong as permanent dipoles, an orientation with the external field still occurs.
Because of the birefringence of liquid crystal materials, the effective refractive index may be a squared average of the indexes along two directions. Therefore, depending on the LC molecule alignment, different effective indexes can be achieved. If all the LC molecules are aligned in parallel to an incident light ray, the effective index reaches its minimum value no, i.e., the ordinary refractive index value. If the LC molecules are aligned perpendicular, the effective index reaches the maximum value square root of ((nc2+no2)/2). This refractive index change is the largest value that can be achieved with a nematic liquid crystal. In summary, and as explained in more detail below, the scattering characteristics in an LC cell change in response to the local orientation of the LC dipoles in polymer networks.
In one aspect, the medium 200 (see
Likewise, if the medium in the selected display pixel operates with a medium scattering strength in responsive to the MID voltage, light is extracted from the waveguide pipe 108 with a third extraction efficiency, less than the first extraction efficiency, but greater than the second extraction efficiency.
Numerical models have been developed that show that the scattered light from waveguide light pipes is strongly angular dependent due to a scattering mechanism based on the relative ratio between the dimension scale of the scatters and light wavelengths. Most of the scattering events can be regarded as Mie scattering. Mie theory, also called Lorenz-Mie theory or Lorenz-Mie-Debye theory, is an analytical solution of Maxwell's equations for the scattering of electromagnetic radiation by spherical particles (also called Mie scattering). This approach is used to explain the behavior of light in interactions with particles having a size similar to that of the wavelength of light.
Since Mie scattering is the dominate scattering mechanism inside the addressable scattering LC cells, it is convenient to define a scattering mean free path, Lmean, which is inversely proportional to the product of average scattering cross-section of scatters, σsc, and scatter density, N, where N is defined as the average particle numbers inside a unit volume.
L
mean˜1/(σsc×N) Equation 1
As shown in
Step 902 provides a front panel with an array of selectable display pixels arranged in a plurality of sequences. Step 904 provides a backlight panel with a plurality of edgecoupled waveguide pipes formed in a plurality of rows. Each waveguide pipe has an optical input connected to a corresponding light emitting diode (LED), and an optical output index-matched to a corresponding sequence of display pixels. Step 906 provides a high absorption layer underlying the backlight panel. Step 908 selects a display pixel to enable. Step 910 measures ambient visible spectrum illumination incident to a top surface of the front panel. In response to the measured ambient illumination being above a first minimum threshold, Step 912 operates the display pixel in a reflective illumination mode. In response to the measured ambient illumination being below the first minimum threshold, Step 914 operates the display pixel in a transmissive illumination mode.
In one aspect, Step 902 provides selectable display pixels with a medium of liquid crystal molecules, embedded in a polymer network, and interposed between transparent electrodes. Then, operating the display pixel in Step 912 and 914 includes creating a biased potential between the electrodes of the selected display pixel.
In another aspect, operating the display pixels in the reflective illumination mode (Step 912) includes substeps. Step 912a supplies an ON voltage to the selected display pixel. In Step 912b, the medium in the selected display pixel operates at a high scattering strength in response to the ON voltage. In Step 916 the selected display pixel returns incident light with a first reflection efficiency. In Step 918 non-selected display pixels return incident light with a second reflection efficiency, less than the first reflection efficiency.
In one variation, Step 912a supplies a MID voltage to the selected display pixel, and in Step 912b the medium in the selected display pixel operates at a medium scattering strength, less than the high scattering strength, in response to the MID voltage. Then, in Step 916 the selected pixel returns incident light with a third reflection efficiency, less than the first reflection efficiency, but greater than the second reflection efficiency.
Operating the display pixels in a transmissive illumination mode may include the following substeps. Step 914a enables a first LED corresponding to a waveguide pipe underlying the selected display pixel. Step 914b supplies an ON voltage to the selected display pixel. In Step 914c the medium in the selected display pixel operates at a high scattering strength in response to the ON voltage. In Step 920 the selected display pixel extracts light received from the waveguide pipe with a first extraction efficiency. In Step 922 non-selected display pixels in the same sequence as the selected display pixel extract light from the waveguide pipe with a second extraction efficiency, less than the first extraction efficiency.
In one variation, Step 914b supplies a MID voltage to the selected display pixel, and in Step 914c the medium in the selected display pixel operates at a medium scattering strength, less than the high scattering strength, in response to the MID voltage. Then, in Step 920 the selected display pixel extracts light received from the waveguide pipe with a third extraction efficiency, less than the first extraction efficiency, but greater than the second extraction efficiency.
In one aspect, Step 910 measures ambient illumination below the first minimum threshold, but above a second minimum threshold. Then, Steps 912 and 914 operate the display pixel in a combination of both reflective and transmissive illumination modes. If Step 910 measures ambient illumination above the first minimum threshold, Step 912 operates the selected display pixel exclusively in the reflective mode. If Step 910 measures ambient illumination below the second minimum threshold, Step 914 operates the display pixel primarily in the transmissive illumination mode.
A display has been provided that uses both reflective and transmissive modes of illumination. Examples of particular materials and dimensions have been given to illustrate the invention, but the invention is not limited to just these examples. Other variations and embodiments of the invention will occur to those skilled in the art.
The application is a Continuation-in-Part of a pending application entitled, THREE-DIMENSIONAL DISPLAY USING ANGULAR PROJECTION BACKLIGHT, invented by Huang et al., Ser. No. 12/873,188, filed on Aug. 31, 2010, Attorney Docket No. SLA2739.
Number | Date | Country | |
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Parent | 12873188 | Aug 2010 | US |
Child | 12877017 | US |