Depth of mirror d (m)
Number of rays leaving through grating
Width of mirrors, w (m) (100 sampling point)
Number of rays leaving outside of the grating apertures
log ( depth of mirrors, d ) (m)
- The authors want to thank the IEE for awarding K.Wang a Research Scholarship
- The authors acknowledge technical support from Breault Research Organization, Inc. for use of the modeling CAD package ASAP 7.1.8.
- The authors thank T. Kataoka from the Department of Electronic & Electrical Engineering, University College London for helpful theoretical discussions on the structure of nematic liquid crystal.
- We would also like to thank the SID reviewer of this paper for giving helpful advice and thank the SID for awarding K.Wang Student Travel Grant.
Number of rays leaving through grating
Number of rays leaving from opposite side of the lightguide
Width of mirrors, w (m)
- We use two cylindrical microlens arrays which give more design variables to enable optimization of collimation.
- The microlenses convert the angular separation of the three color beams into a spatial separation and collimate the beams so that they provide illumination normal to the LCD and separate them sufficiently and narrow the beams so that they pass thorough the centre of each corresponding LCD pixel.
Total Internal Reflection (TIR) Lightguide
- The total internal reflection light guide is fabricated without cladding, from a transparent polymer with a refractive index of 1.50 giving a critical angle by the formula, of
- The light generated from LEDs enters the lightguide, the angular distribution of rays is bound within
- Tracing back the critical ray at the lightguide side wall to the entrance face of the guide, the refractive angle of the ray at the internal surface of the lightguide is , which is larger than .
- According to Snell’s Law, all rays incident on the entrance of the lightguide at angles less than will strike the interior wall at angles greater than
and so will be totally internally reflected and will travel along the lightguide.
- This means that all beams incident on the input face of the guide are guided.
Position and Width of Micro-mirror Array
- We modeled the full backlight structure so that the optimum size, position and width of the micro-mirrors could be established for this backlight structure.
To Establish the Optimum Depth of the Micro-mirror Array
- We fixed the width of the mirrors and varied the depth.
- When the mirrors move from the upper surface to the lower surface of the light guide, the number of rays leaving the guide at the grating increased.
- When the micro-mirrors were placed deeper than 10 µm some light exited the lightguide at the top surface but outside the grating region.
- Mirrors too close to the upper lightguide surface can block the light from reaching the grating “windows” so the output is reduced.
- In the range of mirror depths, d = 0 to 10 m, the maximum output occurs at 10 m.
- The best position was found to be at 10 m which is a conveniently small figure to envisage realistic fabrication procedures for this internal or embedded micro-mirror array layer.
To Establish the Optimum Width of the Micro-mirror Array
- We fixed the mirror depth at the optimum of 10 m below the upper surface of the light guide and varied the width from the minimum of 0.1 m to the maximum of 331 m.
- If the width is set to be too small, some first order reflected light passes through the gaps between the micro-mirrors and exits the lower surface of the guide.
- If the mirror is too wide it will block the rays from the light guide from reaching the grating and so reduce the rays reaching the LCD cutting down the brightness and efficiency.
- The optimum mirror widths were found to be at 160 ± 3 m, to give the maximum output.
Micro-mirror Depth/Width Coupling
- In fact the micro-mirror depth and width are coupled in their effects and so cannot be correctly considered independently of each other.
- We have calculated and plotted a contour map showing their inter-relationship. The optimum occurs at the marked point at
- The contour plot shows that the light at the LCD panel at this point increases by 38.2% ( ).
- A thin, efficient backlight illumination system was modeled and designed which did not require the usual power absorbing colour filters.
- A micro-mirror array layer inside the multimode lightguide reduces the light lost from the opposite side of lightguide improving light intensity by 38.2%
- A microlens system was designed to collimate and to direct the light normal to the display for optimum contrast.
- Periodic, limited length, discrete gratings are used instead of a continuous grating surface. It also allows us to control the strength of each grating window individually to abstain better uniformity.