WO2001035128A9

WO2001035128A9 - Subwavelength optical microstructure light collimating films

Info

Publication number: WO2001035128A9
Application number: PCT/US2000/042002
Authority: WO
Inventors: Robert B Nilsen; Patrick W Mullen; Xiao-Jing Lu
Original assignee: Reflexite Corp
Priority date: 1999-11-12
Filing date: 2000-11-08
Publication date: 2002-08-15
Also published as: US6570710B1; WO2001035128A2; EP1248958A2; CN1278139C; US20040027676A1; WO2001035128A3; US6891677B2; JP2003518263A; CN1434928A

Abstract

A light collimating film has a sheeting having a first side and a second side, wherein the first side includes a series of linear optical elements having a primary axis running the length of the optical elements, and the second side includes a plurality of subwavelength optical microstructures being oriented at about ninety degrees relative to the primary axis of the linear optical elements. Another embodiment includes a back lighting display device having a lighting device, a display panel, and a sheeting having a first side and a second side, wherein the first side includes a series of linear prisms having peaks, and the second side includes a plurality of subwavelength optical microstructures being oriented at about ninety degrees relative to the peaks of the linear prisms.

Description

SUB WAVELENGTH OPTICAL MICROSTRUCTURE LIGHT COLLΓMATΓNG FΓLMS

BACKGROUND OF THE INVENTION

Brightness enhancing films (BEF) have been used in lighting panels for directing light from lighting fixtures through luminaires and laptop computers displays. The brightness enhancing films, which can have linear prisms, diffuse light with a desired directionality. Often the films have been used in combination with a fluorescent light source. The films have had partial success in improving luminair or display brightness by controlling the angle at which light emerges. However, a need still exists for improved control of lighting and enhancement of brightness for laptop computer screens.

SUMMARY OF THE INVENTION

The present invention includes a light collimating film having a sheeting having a first side and a second side, wherein the first side includes a series of linear optical elements having a primary axis running the length of the optical elements, and the second side includes a plurality of subwavelength structures being oriented at about ninety degrees relative to the primary axis of the linear optical elements. The subwavelength structures can include linear moth-eye structures. In one embodiment, the linear optical elements are linear prisms having an included angle in the range of between about sixty and 120 degrees. In another embodiment, the linear optical elements include lenticular linear elements. In a particular embodiment, the prisms have an included angle of about eighty-eight degrees. In another particular embodiment, the prisms have an included angle of about eighty- nine degrees. In another embodiment, the invention includes a back lighting display device having a lighting device, a display panel, and a sheeting having a first side and a second side, wherein the first side includes a series of linear prisms having peaks, and the second side includes a plurality of subwavelength structures, the subwavelength structures being oriented at about ninety degrees relative to the peaks of the linear prisms. In another embodiment, the back lighting display device can have a first collimating film having a first surface with subwavelength structures thereon and a second surface with linear prisms having an included angle of greater than about ninety-five degrees, and a second collimating film having a first surface with a moth-eye structure thereon and a second surface with linear prisms having an included angle of less than about eighty-five degrees.

In a further embodiment, the invention includes a light collimating structure having a first collimating film having a first surface with a plurality of linear moth- eye structures thereon and a second surface with first linear prisms having peaks, the linear moth-eye structures being oriented at about ninety degrees relative to the peaks of the first linear prisms, and a second collimating film having a first surface with a plurality of linear moth-eye structures thereon and a second surface with second linear prisms having peaks, the moth-eye structures being oriented at about ninety degrees relative to the peaks of the second linear prisms. A method of forming a light collimating film is also provided which includes the steps of forming a series of linear prisms, which include peaks, on a first side of a sheeting, and forming a plurality of linear moth-eye structures on a second side of the sheeting with the linear moth-eye structures being oriented at about ninety degrees relative to the peaks of the linear prisms. The method can further include the steps of forming a series of linear prisms, which also include peaks, on a first side of a second sheeting, and forming a plurality of linear moth-eye structures on a second side of the second sheeting with the linear moth-eye structures being oriented at about ninety degrees relative to the peaks of the linear prisms. In one embodiment, the first and second sheetings are arranged such that the moth-eye structures of the first sheeting face the moth-eye structures of the second sheeting. BRIEF DESCRIPTION OF THE DRAWINGS

Figure 1 illustrates a cross-sectional view of a backlighting system.

Figure 2 illustrates a perspective view of a linear prism structure.

Figure 3 illustrates a side view of the linear prism structure shown in Figure 2.

Figure 4 illustrates a cross-sectional view of a second embodiment of a back lighting system.

Figure 5 shows a plot of reflectance as a function of angles of incidence and polarization for a moth-eye structure with 3,300 grooves per millimeter at a light wavelength of 514.5 nm.

Figure 6 shows a plot of reflectance as a function of angles of incidence and polarization for a moth-eye structure with 3,300 grooves per millimeter at a light wavelength of 647.1 nm.

Figure 7 shows a plot of reflectance for a dielectric having an index of refraction and a smooth non-moth-eye surface.

Figure 8 shows a theoretical plot of output from a uniform light distribution X-profile for one and two films of 0.0019 inch (48 μm) pitch linear prisms having a prism angle of ninety degrees.

Figure 9 shows a theoretical plot of output from a uniform light distribution Y-profile for one and two films of 0.0019 inch (48 μm) pitch linear prisms having a prism angle of ninety degrees.

Figure 10 shows a theoretical plot of output from a uniform light distribution X-profile for one and two films of 0.0019 inch (48 μm) pitch linear prisms having a prism angle of seventy-five and ninety-five degrees, respectively. Figure 11 shows a theoretical plot of output from a uniform light distribution

Y-profile for one and two films of 0.0019 inch (48 μm) pitch linear prisms having a prism angle of seventy-five and ninety-five degrees, respectively.

Figure 12 shows a theoretical plot of output from a uniform light distribution X-profile for one and two films of 0.0019 inch (48 μm) linear prisms having a prism angle of seventy-five degrees . Figure 13 shows a theoretical plot of output from a uniform light distribution Y-profile for one and two films of 0.0019 inch (48 μm) linear prisms having a prism angle of seventy-five degrees.

Figure 14 shows a theoretical plot of output from a cosine light distribution X-profile for one and two films of 0.0019 inch (48 μm) pitch linear prisms having a prism angle of ninety degrees.

Figure 15 shows a theoretical plot of output from a cosine light distribution Y-profile for one and two films of 0.0019 inch (48 μm) pitch linear prisms having a prism angle of ninety degrees. Figure 16 shows a theoretical plot of output from a cosine light distribution

X-profile for one and two films of 0.0019 inch (48 μm) pitch linear prisms having a prism angle of seventy-five and ninety-five degrees, respectively.

Figure 17 shows a theoretical plot of output from a cosine light distribution Y-profile for one and two films of 0.0019 inch (48 μm) pitch linear prisms having a prism angle of seventy-five and ninety-five degrees, respectively.

Figure 18 shows a theoretical plot of output from a cosine light, distribution X-profile for one and two films of 0.0019 inch (48 μm) linear prisms having a prism angle of seventy-five degrees.

Figure 19 shows a theoretical plot of output from a cosine light distribution Y-profile for one and two films of 0.0019 inch (48 μm) linear prisms having a prism angle of seventy-five degrees.

Figure 20 illustrates a side view of a subwavelength optical microstructure.

Figure 21 shows a plot of relative response versus wavelength of light for a 0.002 inch (51 μm) thick film of polyester, 0.002 inch (51 μm) thick film of polyester with one side having moth-eye structures, 0.002 inch (51 μm) thick film of polyester with two sides having moth-eye structures, and a reference with a detector located normal to the surface of the film.

Figure 22 shows a plot of relative response versus wavelength of light for a 0.002 inch (51 μm) thick film of polyester, 0.002 inch (51 μm) thick film of polyester with one side having moth-eye structures, 0.002 inch (51 μm) thick films of polyester with two sides having moth-eye structures, and a reference with a detector located at an angle thirty degrees from the normal to the surface of the film. Figure 23 shows a plot of light transmission versus angle from the normal of a 0.002 inch (51 μm) polyester film with and without a moth-eye structure on one side at the zero and ninety degree profile.

Figure 24 shows a plot of color versus angle from the normal of a 0.002 inch (51 μm) thick polyester film with and without moth-eye structures on both sides observed at zero degree orientation.

Figure 25 shows a plot of color versus angle from the normal of a 0.004 inch (102 μm) thick polyester film with and without moth-eye structures on both sides observed at zero degree X-orientation and ninety degree Y-orientation.

Figure 26 is a plot of luminance cross section versus observation angle from the normal at zero degree orientation of a film with moth-eye structures having a period of about 0.2 μm and a height of about 0.4 μm and linear prisms with ninety- five degree included angle and a pitch of 0.0019 inches (48 μm).

Figure 27 is a plot of luminance cross section versus observation angle from the normal at ninety degrees orientation of a film with moth-eye structures having a period of about 0.2 μm and a height of about 0.4 μm and linear prisms with a ninety- five degree included angle and a pitch of 0.0019 inches (48 μm). Figure 28 is a plot of luminance cross section versus observation angle from the normal at zero degree orientation of a film without moth-eye structures and linear prisms with ninety-five degree included angle and a pitch of 0.0019 inches (48 μm).

Figure 29 is a plot of luminance cross section versus observation angle from the normal at zero degree orientation of a film without moth-eye structures and linear prisms with ninety-five degree included angle and a pitch of 0.0019 inches (48 μm).

Figure 30 shows a plot of light transmission versus angle from the normal of a film with ninety degree linear prisms having a pitch of 0.002 inches (51 μm) with and without moth-eye structures on the window side of the films. The foregoing and other objects, features and advantages of the invention will be apparent from the following more particular description of preferred embodiments of the invention, as illustrated in the accompanying drawings in which like reference characters refer to the same parts throughout the different views. The drawings are not necessarily to scale, emphasis instead being placed upon illustrating the principles of the invention. All percentages and parts are by weight unless otherwise indicated.

DETAILED DESCRIPTION OF THE INVENTION

With respect to the optical performance of a collimating film, it has been found that for individual AMLCD (active matrix liquid crystal display) back lighting system designs, the optical efficiency of the particular lamp, waveguide and diffuser system can be improved by designing a collimating film to maximize the use of the diffraction and refraction effects. For example, as shown in Figure 1, a back lighting system 10 includes a light source 12 and light reflector 14. Light source 12 can be a fluorescent light, incandescent light or other suitable light source. Waveguide 16, which is for directing light out of back lighting system, can be formed of a transparent solid material and is often wedge shaped. On one side of waveguide 16 is waveguide reflector 18 formed of a specular material, such as aluminum or a coated white surface, for reflecting light back to waveguide 16. Waveguide reflector 18 can be curved or flat. Diffuser 20 is a film that diffuses the light from the waveguide into a substantially uniform distribution. An example of a suitable diffuser is a randomly textured surface or gradient index film or engineered diffractive structure.

Above diffuser 20, first collimating film 22 has moth-eye structure 24 on a first side adjacent waveguide 16. Second side of first collimating film 22 has prism structure 25. An optional abrasion reduction layer 26 is between first collimating film 22 and second collimating film 28. The abrasion reduction layer can have a moth-eye structure on one or two surfaces to improve performance. Second collimating film 28 has moth-eye structure 30 on a first side adjacent first collimating film 22 and prism structure 32. Prism structure 32 of second collimating fil 28 can be oriented in the- same direction as the prisms on first collimating film 22. Alternatively, it may be offset by rotating the prism orientation up to about 180 degrees. In a preferred embodiment, the second collimating film is rotated about ninety degrees with respect to the first collimating film to reduce moire fringe formation and improve the uniformity of the exiting light distribution. Above the second collimating film is a liquid crystal display 34. A collimating film which has linear prisms designed with a tilt, size and included angle which match the light source, waveguide and diffuser properties provides enhanced performance. The advantages of employing linear prism arrays with included angles which range from ninety- five degrees to 120 degrees provides a light distribution which is optimized for viewing angles of a computer screen. The included angle is considered the top angle of a triangular linear prism structure.

An example of a linear prism film is shown in a perspective view in Figure 2 and in a side view in Figure 3. Linear prism film 40 has prism surface 42 and window surface 44 and is formed of a transparent polymeric material. Prisms 46 have sides 48 with peaks 50 and valleys 52. The pitch (p) of the prisms 46 is measures from valley 52 to next valley 52. The pitch can be in the range of between ¹0.001 and 0.003 inches (25 and 76 μm). The height (h) of the linear prisms is measured by the vertical distance from the valley 52 to peak 50. The height can be in the range of between 0.0003 and 0.0015 inches (7.6 and 38 μm). The included angle (<*) is measured between the two sides that meet at peak 50. ^' The angle («) can range from about sixty to 120 degrees, i a preferred embodiment, the angle (< ) is in a range of between about sixty and eighty-five degrees or between about ninety- five and 120 degrees. Sides 48 on each side of the peak 50 can be the side length (1) from valley 52 to peak 50 to fonn an isosceles triangle. Alternatively, the sides can have different lengths, thereby tilting or canting the prisms. The tilting angle (β) of the prisms is between the optical axis 54 and a line 56 perpendicular to the window side 44. The prisms can be tilted in the range of between about -44 and +44 degrees. In a preferred embodiment, the tilting is about seven degrees. h other embodiments, prism stractures 22, 32 can include lenticular linear elements, such as disclosed in U.S. Patent 5,592,332, issued to Nishio et al. on January 7, 1997.

Another embodiment of the present invention is shown in Figure 4. A back lighting system 100 includes a light source 102 and a light reflector 104. Waveguide 106 can be formed of a transparent solid material and is preferably wedge shaped. Adjacent to the first side 108 of waveguide 106 is waveguide reflector 110 formed of a specular material. The reflector 110 is spaced slightly away from surface 108 to allow total internal reflection at surface 108 to take place. First side 108 can be stepped in shape. Second side 112 of waveguide 106 is on the opposite side away from waveguide reflector 110. Second side 112 has moth-eye structures 114.

Above waveguide 106, first collimating film 116 has first prism structure 118 with peaks 120 pointed toward waveguide 106 and first moth-eye structures 122 on the window side of first prism structure 118. Preferably, the peaks of linear prisms on first collimating film 116 run parallel to light source 102. Above first collimating film 116, second collimating film 124 has second moth-eye structure 126 and second prism structure 128. Peaks 130 of second prism structure 128 point away from waveguide 106. Preferably, the peaks 130 of second prism structure 128 is oriented in a non-parallel direction to peaks 120 of first prism structure 118. A more preferred orientation is ninety degrees.

In one embodiment, the first moth-eye structures 122 are oriented at about ninety degrees relative to the peaks of the linear prisms on the first collimating film 116. hi one embodiment, angle («) of the linear prisms on the first collimating film 116 is about eighty-eight degrees, hi another embodiment, angle (<*) is about eighty- nine degrees.

The second moth-eye structures 126 can be oriented at about ninety degrees relative to the peaks of the second collimating film 124. In one embodiment, angle (°O of the linear prisms on the collimating film 116 is about eighty-eight degrees. In another embodiment, angle (<*) is about eighty-nine degrees. The moth-eye structures 122, 126 are oriented at about ninety degrees relative to the linear prisms of respective collimating films 116, 124 to minimize, and preferable eliminate, the deep blue to deep green color that is produced by light resonance, and which is visible, at wide entrance angles. h one embodiment having the moth-eye structures 122, 126 oriented ninety degrees relative to the linear prisms of respective collimating films 116, 124, only a small amount of green color shows at very wide viewing angles, for example, seventy to eighty degrees from normal, hi contrast, when the moth-eye structures 122, 126 are oriented parallel to the linear prisms of respective collimating films 116, 124, the off axis color becomes a very vivid purple-blue at a viewing angle of about forty-five degrees from normal. In some applications, this vivid color may be desirable where a narrow useable viewing is needed, such as in security/privacy applications.

In the embodiment having eighty-eight degree linear prisms on collimating films 116, 124 with moth-eye structures 122, .126 oriented at about ninety degrees relative to respective linear prisms, a 4% performance increase over commercially available brightness enhancing films having ninety degree prisms has been realized. In the embodiment having eighty-nine degree linear prisms on collimating films 116, 124 with moth-eye structures 122, 126 oriented at about ninety degrees relative to respective linear prisms, a 6% performance increase over commercially available brightness films having ninety degree prisms has been realized. The performance of TIR (total internally reflecting) films, often called BEF

(brightness enhancing film), which are used to increase the light output from back lighting systems in AMLCD flat panel displays can be improved by changing the tilt angle of the linear prism, the linear prism included angle and also the pitch of the linear prism array. A further improvement can be made by making the film monolithic or polylithic. A monolithic film removes one material interface (at the substrate) and improves optical transmission. In the case of the polylithic film, a diffuser can be incorporated into the film structure saving the need to fabricate a separate diffuser and dependent on the degree of collimation required.

A fine pitch of a linear comer cube prism structure provides excellent performance as a first layer in a back lighting system if a diffuser is not used between the top smooth surface of a waveguide and a flat surface of the linear micro corner cube sheet. A fine pitch, preferably in the range of between about 0.00005 and 0.0001 inches (1.3 and 2.5 μm), of the comer cube array helps to spread the refracted and retroreflected light by diffraction creating increase diffusion of recycled light. In a more preferred embodiment, the pitch is about 0.000075 inches (1.9 μm). The refracted and retroreflected light is spread by one to two degrees depending on the accuracy of the linear comer cube array dihedral angles. This spreading is then increased by diffuse structures on the second surface of the waveguide creating a smooth diffuse light pattern without the need of the diffuser between the waveguide and linear comer cube collimating sheet. In addition, the groove pattern in the linear comer cube array is oriented in directions which do not modulate with the diffuse dot pattern on the rear of the waveguide. Therefore, moire fringes are not created. A surface is disclosed in U.S. Patent 5,600,462, issued to Suzuki et al. on February 4, 1997, which employs a rough structure (0.004 inches, 10 μm) for performing diffuse transmission to create a "ground glass-type diffusion."

Also, it has been found that the addition of one or two ninety-five degree linear prism sheet(s) with 0.0019 inch (48 μm) pitch above the fine pitch linear corner cube sheet and with the smooth surface oriented toward the comer cube array further enhances the brightness. The second linear prism sheet is oriented about ninety degrees with respect to the first sheet.

The materials that work well for optical microstructured films are an ultraviolet cured polymers bonded to a polyester substrate, which can have abrasion resistance which is important during handling of the collimating films. If the prism tips are damaged during handling, the resulting display can have fine lines that appear as less bright than surrounding areas on axis and brighter than surrounding areas off-axis. The films can be formed of suitable polymers such as polycarbonate. The films can be constructed from a polycarbonate material, acrylic, or other suitable material, such as disclosed in U.S. Patent 5,396,350, issued to Beeson et al. on March 7, 1995. An abrasion reduction sheeting, such as a thin polypropylene film or similar material can be placed in between the collimating film layers to help to reduce any effect from abrasion without losing significant brightness. Subwavelength visible light moth-eye stractures can be used on these overleaf films to effectively eliminate Fresnel reflection light losses. The softer films do not abrade the linear prism peaks as easily as hard films. A semi-soft substrate, such as a polyvinyl chloride film can be used in place of the polyester substrate to make collimating films and reduce abrasion. However, one must be careful of out-gassing and resulting surface contamination which can occur with polyvinyl chloride.

A linear non-isosceles prism array tilted or canted in the range of between about -45 and +45 degrees and preferably at seven degrees, having a ninety-five degree included angle and a 0.0019 inch (48 μm) pitch as a first layer and a linear isosceles prism (with zero tilt), having a ninety-five degree included angle and a 0.0019 inch (48 μm) pitch as a second layer can significantly improve the amount of light that is directed through an AMLCD to the angles (geometry's) desired for optimum user viewing angles. The tilt or canting of the optical axis of the first layer linear prism anay corrects the skewed direction of the light distribution coming from the waveguide and diffuser. A 0.0019 inch (48 μm) pitch can cause diffraction spreading, which smooths the light distribution and maximizes the light directed toward the angles most beneficial or desired for a AMLCD display user. The ninety- five degree included angle further optimizes the field of view of the light distribution for the display user while still recycling light which is headed in the incorcect direction back into the display where it is used again.

Therefore, a prefereed collimating film combination for a wedge waveguide includes a first collimating film which has prisms tilted to conect for the skew created by the waveguide wedge and diffuser layers and has a prism angle designed to maximize the user field of view plus a second collimating film oriented at ninety degrees to the first and with a symmetrical linear prism pattern. In the second collimating film the prisms can be tilted uniformly in both directions (tilt every other prism in the opposite direction) to have a prism angle that optimizes the user field of view for this axis. Further, performance change can be achieved by combining the diffuser into the first zone of the first collimating film to eliminate one film component. However, the focusing effect of the first surface is lost. The diffuser can be made by employing textured films and casting the linear prisms onto the smooth side of the film, by rotary screen printing a diffuse layer onto the polyester tie coat prior to casting the linear prisms onto the diffuse layer (in this embodiment the diffuse layer is sandwiched between the linear prisms and the substrate film), by rotary screen printing a diffuse layer onto a canier film and then casting linear prisms onto the diffuse layer. The prism and diffuse layer can be made of the same material and finish cured together, by adding particles into the tie coat prior to casting the linear prisms onto the tie coat and by dispersing particles in the substrate sheet followed by casting linear prisms onto the substrate sheet.

The addition of the moth-eye structure to the window side of the collimating films increases the system brightness by about 6% to 8%, which is significantly brighter (by 10% to 12%) than the previously known brightness enhancing film systems with a similar pitch. These improved results are believed to be due to a combination of micro structured optical effects. The uniform white light, such as a fluorescent bulb which causes this light to have a cool appearance because of the blue shift, has distribution coming from the diffuser which is incident on the first layer moth-eye surface. At angles of incidence of +/-60 degrees, 2% or less of the light is reflected at the first layer moth-eye to air interface. Plots of the reflectance are shown in Figures 5 and 6 for a subwavelength microstracture having 3,300 grooves per millimeter of light having wavelengths of 514.5 nm and 647.1 nm, respectively. The S line represents light perpendicular to the plane of incidence, and the P line represents light parallel to the plane of incidence. Shown in Figure 5, the average reflectance (linear average between S and P lines) is about 0.8% at sixty degrees and shown in Figure 6, the average reflectance is about 2% at sixty degrees. This is compared to an average of about 10% of the light that is reflected at a smooth non-moth-eye surface at a sixty degree angle of incidence. Figure 7 shows a plot of an average of about 10% reflectance at a sixty degree incident angle. Also at normal incidence, a typical 4% reflectance due to a smooth surface is reduced to less than 1% with a moth-eye structure. At angles of incidence that are greater than seventy-five degrees, a green and then a blue color can be observed. The color is a result of diffraction scattering as the short wavelengths enter the moth-eye structure from an angle which causes the aperture of the moth-eye elements to become diffractive and resonate. This diffraction scattered light is processed by the linear prism film differently than the light that passes through a non-moth-eye smooth surface, i this embodiment, the green to blue light is more uniformly distributed throughout the film creating a more uniform illumination. A significant amount of green light is light piped by total internal reflection within the film and is partially filtered out of the light that becomes available to illuminate an LCD panel. Different size (frequency and amplitude) moth-eye stractures can be used to create different illumination effects depending on the light source and optical components used in the illumination system. By changing the size of the moth-eye structures in the range from subwavelength to larger than wavelength scale structures, for example, moth-eye stractures having a period of between about 0.15 and 10.0 micrometers, the diffraction properties of the surface can be optimized to help smooth the resulting light distribution and improve wide angle light distribution.

After the light has passed through the first moth-eye layer, it is collimated to about forty-two degrees and the ninety-five degree linear prism second surface of the first film layer through refraction collimates the light to approximately +/-30 degrees. Then the light enters the moth-eye surface on the first surface of the second layer film where it is further collimated by refraction. The majority of the light is at +/-30 degrees from the normal as it enters the moth-eye surface and passes through the moth-eye layer with little intensity loss. The light passes through the second layer film and is further redirected through refraction and recycling by the ninety- five degree linear prism structure. The ninety-five degree prism shape helps to recycle any of the light that is still traveling at wide angles of incidence. This light eventually emerges from the lighting system within a final +/-29 degree light distribution in both the X and Y axes. If two crossed seventy-five degree linear prism films with moth-eye smooth surfaces are used in the illumination system, a light intensity distribution width of +/-18 degrees and an intensity of 2.63 can be achieved. The light intensity distribution X-profile and Y-profile for uniform light through a film with ninety degree, seventy-five degree and ninety-five degree prism films are shown. Figures 8 and 9 show plots of output uniform light distribution of the X-profile and Y-profile, respectively, for one and two films of 0.0019 inch (48 μm) pitch for linear prisms having a prism angle of ninety degrees. Figures 10 and 11 show plots of output for uniform light distribution X-profile and Y-profile, respectively, for one and two films of 0.0019 inch (48 μm) pitch for linear prisms having a prism angle of seventy-five and ninety-five degrees, respectively. Figures 12 and 13 show plots of output for umform light distribution X-profile and Y-profile, respectively, for one and two films of 0.0019 inch (48 μm) linear prisms having a prism angle of seventy- five degrees. Figures 14 and 15 show plots of output cosine light distribution of the X-profile and Y-profile, respectively, for one and two films of 0.0019 inch (48 μm) pitch for linear prisms having a prism angle of ninety degrees. Figures 16 and 17 show plots of output for cosine light distribution X-profile and Y-profile, respectively, for one and two fihns of 0.0019 inch (48 μm) pitch for linear prisms having a prism angle of seventy-five and ninety- five degrees respectively. Figures 18 and 19 show plots of output for cosine light distribution X-profile and Y-profile, respectively, for one and two films of 0.0019 inch (48 μm) linear prisms having a prism angle of seventy-five degrees. Additional optimization of the angles allows a near +/-10 degree intensity distribution. One disadvantage with this configuration is an approximate +/-2.0 degree void that appears at the center of the light intensity distribution. This effect is visible in Figures 12 and 13. Slight curvature or positive- negative canting in the prism facets can reduce this void. The application of a moth-eye structure to the smooth surface of the linear prism films improves significantly the light collimating capability of the films by increasing light throughput at the moth-eye structured surface and redirecting wide incident angle light rays. Diffraction effects also play a significant role in the improved performance of the system. The resulting color of the backlight assembly is warmer in appearance than the same assembly without the addition of the moth- eye structures. This color shift can have a beneficial effect on the contrast within the final back light display.

As shown in Figure 20, the moth-eye structure applied preferably has an amplitude (A) of about 0.4 micrometers and a period (P) of less than about 0.2 micrometers. The structure is sinusoidal in appearance and can provide a deep green to deep blue color when viewed at grazing angles of incidence. Preferably, the amplitude is about three times the period to provide a three to one aspect ratio.

Figures 21 and 22 show a plot of the improvement in transmission by wavelength for 0.002 inch (51 μm) thick PET having moth-eye stractures on one side and having moth-eye structures on both sides at zero degrees and at thirty degree angles from the normal, respectively. The moth-eye structures have a period of about 0.2 μm and a height of about 0.4 μm. The reference is a uniform light distribution coming from a diffuser positioned above the waveguide. Figure 23 shows a plot of the improvement in transmission by angle from the normal for 0.002 inch (51 μm) PET with moth-eye stractures. In this figure, the fluorescent tube light bulb is at a +80 degree position for the ninety degree orientation. Figure 24 shows a plot of the color shift which occurs for 0.002 inch (51 μm) thick PET with moth-eye structures on one side and with moth-eye stractures on both sides. Figure 25 shows a plot of the color shift that occurs for 0.004 inch (102 μm) thick PET with ninety- five degree linear prisms on the side away from the diffuser and with and without moth eye on the side close to the diffuser. For all measurements, the samples were placed on top of the diffuser in a standard LCD back light assembly and the Photon Research detector, Model PR650 was supported eighteen inches (45.7 cm) above the part surface. The moth-eye structure provides anti-reflection properties to the previously smooth light entrance surface of the substrate even at entrance angles that are near grazing incidence. The moth-eye stracture is more effective than standard thin film anti-reflection coatings at wide angles of incidence especially angles of incidence beyond thirty degrees up to eighty degrees. This characteristic causes many types of optical microstructure films including linear prism films to process light very differently than the standard linear prism collimating films which have smooth entrance surfaces with or without standard anti-reflection thin film (vacuum deposited or liquid applied) coatings. The addition of the moth-eye structures helps to more efficiently recycle light and also redirects the normally reflected grazing angle incidence rays into the optical microstracture (such as linear prisms) sheet where the rays are refracted, reflected or retroreflected depending on the respective angles of incidence. This moth-eye improvement concept can be added to many types of brightness enhancement films (BEF). An advantage is that functional optical microstructures can be applied to both sides of a film or substrate.

A moth-eye anti-reflection surface is one in which the reflection of light is reduced by the presence of a regular areay of small protuberances covering the surface. The spacing of the protuberances is less than the wavelength of light for which anti-reflection is sought. A moth-eye surface can be understood in tenns of a surface layer in which the refractive index varies gradually from unity to that of the bulk material. Without such a layer the Fresnel reflection coefficient at an interface of two media is equal to ((n_t - n₂) (n_! + n₂))², where n_j and n₂ are the refractive indices of the media. However, if there is a gradual change of index, net reflectance can be regarded as the result of an infinite series of reflections at each incremental change in index. Since each reflection comes from a different depth from the surface, each has a different phase. If a transition takes place over an optical distance of λ/2, all phases are present, there is destructive interference and the reflectance falls to zero.

When the height of the protuberance (h) is significantly less than the wavelength (λ), the interface appears relatively sharp and the reflectance is essentially that of a discontinuous boundary. As the ratio of h/λ increases, the reflectance decreases to a minimum value at about h/λ=0.4. Further increases in h/λ show a series of successive maxima and minima, but the value does not again approach that of a sharp interface. The details of the curve shown in Figure 20 vary depending on the profile of the change of the index of refraction, but if the thickness is of the order of half a wavelength or more the reflectance is considerably reduced. The spacing of the protuberances should be sufficiently fine to avoid losses by diffraction. Preferably, it should be less than the shortest wavelength involved divided by the refractive index of the material.

It is important that the spacing d between the peaks of the protuberances on the moth-eye surface is sufficiently small that the anay cannot be resolved by incident light. If this is not the case, the array can act as a diffraction grating and, although there may well be a reduction in the specular reflection (zero order), the light is simply redistributed into the diffracted orders. In other words, we require that d<λ for normal incidence and d<λ/2 for oblique incidence if for reflection only, and that d<λ/2n in the case of transmission where diffraction inside the material is suppressed.

For a given moth-eye surface, where the height of the protuberances is h and the spacing is d, the reflectance is expected to be very low for wavelengths less than about 2.5h and greater than d at normal incidence, and for wavelengths greater than 2d for oblique incidence. Preferably, the spacing is as close as possible, and the depth as great as possible, in order to give the widest possible bandwidth. For example, a h/d ratio is preferably about three.

The moth-eye effect should not be confused with that of reducing the specular reflectance by roughening. Roughness merely redistributes the reflected light as diffuse scattering and degrades the transmitted wavefront. With the moth- eye stracture, there is no increase in diffuse scattering, the transmitted wavefront is not degraded and the reduction in reflection gives rise to a conesponding increase in transmission.

The moth-eye stracture has many advantages. There is no extra coating process necessary. The structure can be transfened to the sheet by a pressure molding process, such as with a Fresnel stracture. The reflection reduction does not depend on the wavelength. There is only a lower limit (on the ultraviolet side of the spectrum) set by the structure period. If the wavelength is too small compared to the period, the light is diffracted. In regard to angular dependence, with conventional anti-reflective coatings, the transmission curve shifts with the light incidence angle. With the moth-eye structure, the critical wavelength for diffraction shifts to higher values, but there are no changes above this wavelength. Another advantage for moth-eye structures is that there are no adhesion problems between lens and gradient layer because it can be one bulk material. From a high incident angle, the surfaces can appear blue or violet.

To form a moth-eye stracture, the structure is first produced on a photoresist- covered glass substrate by a holographic exposure using an ultraviolet laser. A suitable device is available from Holographic Lithography Systems of Bedford, Massachusetts 01730. An example of a method is disclosed in U.S. Patent 4,013,465, issued to Clapham et al. on March 22, 1977. This method is sensitive to any changes in the environment, such as temperature and dust, and care must taken. The structure is then transfened to a nickel shim by an electro forming process. In a prefereed embodiment, the shims are about 300 micrometers thick or less.

The moth-eye structures can be made one dimensional in a grating type pattern. In this embodiment, the stracture has a nearly rectangular profile, which means they have no gradient layers, but more of a one layer anti-reflective coating with a lowered refractive index in the stracture region. Control of the grating depth is important as is control of thickness for the evaporated layers. Control of depth and thickness is achieved by maintaining uniformity of beam exposure, substrate flatness and exposure time.

A two-dimensional structure is formed by two exposures with a linear sinus- grid, turned by ninety degrees for the second exposure. A third type of structure is formed by three exposures with turns of sixty degrees to provide a hexagonal or honeycomb shape.

When measured at a four inch (10.2 cm) distance from the display Photon Research Model No. PR650, the results with two ninety-five degree linear prism films each having a moth-eye stracture on the previously smooth side show about the same brightness on axis as two ninety degree BEF films, a large improvement in brightness off axis in both vertical and horizontal axis and a warmer color to the light emerging from the display, hi Figures 26, 27, 28 and 29, the total integrated light intensity for the ninety-five degree prisms with moth-eye stracture films is 6,686.8 lm/m² with a maximum of 4,460 cd/m² and a minimum of 554.0 cd/m². For the ninety degree prisms without moth-eye stracture films, the integrated light intensity is 5,698.8 lm m² with a maximum of 4,685.0 cd/m² and a minimum of 295.9 cd/m².

Through analysis and experimental results, a prefened embodiment includes a seventy-five degree linear prism film can be used as the first layer above a uniform light output diffuser to collimate the light to about a +/-30 degree angle. The prism grooves in this first layer are oriented parallel to the light source that illuminates the waveguide which is below the diffuser. On top of this film can be a ninety-five degree linear prism film which is oriented at ninety degrees with respect to the seventy- five degree film to collimate the light to about +/-25 degrees with a small percentage of the light at +/-30 degrees as shown in Figures 10, 11, 16 and 17. The final intensity of the collimated light is excellent and comparable to results obtained with two crossed ninety degrees BEF films, as shown in Figures 8, 9, 14 and 15. These ninety degree BEF films do not allow for the recycled component (Note that •there is no recycled light with the seventy-five degree film) but allowing for the recycled light the peak intensities become 2.15 for the seventy-five degree plus ninety-five degree collimating films and 2.06 for the BEF films. The prism apex angle of the second ninety-five degree film can be increased to about 100 degrees if the spread in the collimated light beam is too narrow.

Figure 30 shows a comparative plot of light transmission versus angle from the normal of a film with ninety degree linear prisms having a pitch of 0.002 inches (51 μm) with moth-eye stractures on the window side of the film and a film with ninety degree linear prisms having a pitch of 0.002 inches (51 μm) without moth-eye structures on the side of the film. The comparative plot shows a substantial improvement in transmission, particularly at zero degrees, when employing a moth- eye stracture on the window side of the film as compared to a similar film without a moth-eye structure.

While this invention has been particularly shown and described with references to prefened embodiments thereof, it will be understood by those skilled in the art that various changes in form and details may be made therein without departing from the scope of the invention encompassed by the appended claims.

Claims

CLATMSWhat is claimed is:

1. A light collimating film comprising: a sheeting having a first side and a second side, wherein said first side includes a series of prisms, and said second side includes a plurality of moth- eye stractures.

2. The light collimating film of Claim 1, wherein said first side includes a series of linear optical elements having a primary axis running the length of the optical elements, and said second side includes a plurality of moth-eye stractures, said moth-eye structures being oriented at about ninety degrees relative to the primary axis of said linear optical elements.

3. The light collimating film of Claim 1 wherein said linear optical elements include linear prisms that run the width of the sheeting.

4. The light collimating film of Claim 1 wherein said linear optical elements include linear prisms having triangular prisms arranged side-by-side.

5. The light collimating film of Claim 4 wherein said triangular prisms include a top angle in a range of between about sixty and 120 degrees.

6. The light collimating film of Claim 5 wherein said linear prisms include triangular prisms that are isosceles in shape.

7. The light collimating film of Claim 4 wherein said triangular prisms include a top angle in a range of between about sixty and eighty-five degrees.

8. The light collimating film of Claim 4 wherein said triangular prisms include a top angle in a range of between about ninety-five and 120 degrees.

9. The light collimating film of Claim 4 wherein said triangular prisms include a top angle of about eighty-eight degrees.

10. The light collimating film of Claim 3 wherein said triangular prisms include a top angle of about eighty-nine degrees.

11. The light collimating film of Claim 1 wherein said linear optical elements are pitched at regular intervals.

12. The light collimating film of Claim 1 wherein said linear optical elements include lenticular linear elements.

13. The light collimating film of Claim 1 wherein said linear optical elements are pitched in the range of between about 0.0127 and 6.35 millimeters.

14. The light collimating film of Claim 1 wherein said moth-eye structures include linear moth-eye structures.

15. The light collimating film of Claim 14 wherein said second side includes linear moth-eye stractures spaced about 0.15 micrometers apart.

16. The light collimating film of Claim 14 wherein said linear moth-eye stractures have depth to width ratio in range of between about one and three.

17. The light collimating film of Claim 14 wherein said linear moth-eye structures include a period in the range of between about 0.15 and 10.0 micrometers.

18. A back lighting display device, comprising: a) a lighting means; b) a display panel; and c) a sheeting having a first side and a second side, wherein said first side includes a series of prisms, and said second side includes a plurality of moth-eye stractures.

19. The back lighting display device of Claim 18 wherein said first side includes a series of linear prisms having peaks, and said second side includes a plurality of linear moth-eye structures, said linear moth-eye structures being oriented at about ninety degrees relative to the peaks of said linear prisms.

20. The back lighting display device of Claim 18 further comprising a second sheeting having a first side and a second side, said second side includes a plurality of moth-eye structures.

21. The back lighting display device of Claim 20, wherein said first side includes a series of linear prisms having peaks, and said second side includes a plurality of linear moth-eye stractures, said linear moth-eye structures being oriented at about ninety degrees relative to the peaks of said linear prisms.

22. The back lighting display device of Claim 18 wherein said linear prisms include triangular prisms having a top angle of about eighty-eight degrees.

23. The back lighting display device of Claim 18 wherein said linear prisms include triangular prisms having a top angle of about eighty-nine degrees.

24. A light collimating stracture, comprising: a) a first collimating film having a first surface with a moth-eye stracture thereon and a second surface with linear prisms; and b) a second collimating film having a first surface with a moth-eye structure thereon and a second surface with linear prisms.

25. The light collimating structure of Claim 24 wherein the linear prisms of the second surface of the first collimating film includes an included angle of equal or greater than about ninety-five degrees.

26. The light collimating structure of Claim 24 wherein the linear prisms of the second surface of the second collimating film includes an included angle of equal or less than about eighty-five degrees.

27. The light collimating structure of Claim 24 wherein the moth-eye structure of the first collimating film and the moth-eye structure of the second collimating film face each other.

28. The light collimating structure of Claim 24 wherein the first collimating film includes the linear moth-eye structures being oriented at about ninety degrees relative to the peaks of said first linear prisms; and

29. The light collimating structure of Claim 24 wherein the second collimating film includes the linear moth-eye stractures being oriented at about ninety degrees relative to the peaks of said second linear prisms.

30. A method for fonning a light collimating film, comprising: forming a series of linear prisms on a first side of a sheeting, the linear prisms including peaks; and forming a plurality of linear moth-eye structures on a second side of the sheeting with the linear moth-eye stractures being oriented at about ninety degrees relative to the peaks of the linear prisms.

31. The method of Claim 30 further comprising the steps of: forming a series of linear prisms on a first side of a second sheeting, the linear prisms also including peaks; and forming a plurality of linear moth-eye structures on a second side of the second sheeting with the linear moth-eye stractures being oriented at about ninety degrees relative to the peaks of the linear prisms.

32. The method of Claim 31 further comprising the step of arranging the first and second sheetings such that the moth-eye stractures of the first sheeting face the linear moth-eye stractures of the second sheeting.

33. A waveguide having a moth-eye structure on a surface.

34. The waveguide of Claim 30 wherein the waveguide is wedge shaped.