Motor vehicle windshield having an antireflective transparent coating

Abstract: An anti-reflective coating employing Si 1-x H x as a high refractive index material in a film pair together with SiO₂ as a low refractive index material is found to be substantially transparent to visible light and to provide good anti-reflectance where the Si 1-x H x film is ultra-thin, preferably less than about 80 Angstroms, and the thickness of the SiO₂ film is matched to that of the Si 1-x H x film. Laminated glazing units having such anti-reflective film can be used, for example, even in applications requiring high transmittance of visible light, such as motor vehicle windshields, in view of the substantial transparency of the coating.

Description: The present invention relates to an anti-reflective coating which is substantially transparent to visible light wavelengths. The anti-reflective coating of the invention is particularly suitable for use on glazing units, such as automotive and architectural windows. Anti-reflective coatings have been used in various applications for some time. Exemplary applications include lenses, glazing units, mirrors and the like. It is becoming desirable to use anti-reflective coatings on architectural and automotive glazing units, especially on the inside and/or outside surfaces of motor vehicle windshields. A suitable anti-reflective coating on the inside surface of a motor vehicle windshield would facilitate the use of lighter coloured instrument panel materials. Without an anti-reflective coating, vision through the windshield might be impaired by light from the upper surface of such lighter coloured instrument panel reflecting on the inside surface of the windshield. An anti-reflective coating on the outside of a windshield increases transmitted light intensity and helps meet applicable minimum transparency requirements. Presently, minimum transmittance of visible light for motor vehicle windshields is 70% in the United States and 75% in Europe. Therefore, to be suitable for use in a vehicle windshield or other glazing application, the anti-reflective coating must not reduce the transparency of the glazing unit to an unacceptable degree. Numerous anti-reflective coatings are known, many of which comprise a film stack in which a first film of relatively high refractive index material is paired with a second film of lower refractive index material. Thus, for example, U.S. patent No. 4,846,151 to Simko, Jr. suggests that various surfaces of transparent plates used in solar collectors can be coated with an anti-reflective material. Exemplary materials are listed, including multi-layer coatings such as silicon dioxide paired with aluminium oxide or titanium dioxide. Similarly, U.S. Patent No. 4,822,748 to Janesick et al suggests the use of an anti-reflective coating on glass used in picture frames and the like. Specifically, it suggests the preparation of a triple layer film stack in which a film of titanium oxide is sandwiched between films of silicon dioxide. Other materials, such as zirconium oxide, tantalum oxide and magnesium oxide also are mentioned. The use of silicon monoxide is suggested as an anti-reflective coating for optical parts made of synthetic resin in U.S. patent No. 4,497,539 to Sakurai et al. Silicon monoxide also is suggested, as is silicon dioxide, as an anti-reflective layer having high infrared reflectivity and high visible light transmission suitable for use in heat-mirrors in U.S. patent No. 4,822,120 to Fan et al. In U.S. patent No. 4,815,821 to Nonogaki et al a light transmitting glass panel is suggested having on its surface a coating consisting of a silicon monoxide layer over a titanium oxide layer. The silicon monoxide layer is said to be intermittently spaced from the titanium dioxide layer by a light absorbing layer of colloidal carbon. A transparent optical article, such as a lens, is suggested in U.S. patent No. 4,765,729 to Taniguchi. Silicon dioxide is suggested as a suitable anti-reflective coating for the surface of the article. The use of an anti-reflective coating on both the inside and the outside of an ophthalmic lens is suggested in U.S. patent No. 4,070,097 to Gelber. Each of the two coatings is said to have two layers, a dielectric layer and a metal layer. For the metal layer, suitable materials are said to include nickel, chromium, Inconel and Nichrome (a material comprised essentially of nickel and chromium). The metal layer is said typically to have a thickness ranging from 1-4 nm (10 to 40 Angstroms). Various the materials, including silicon dioxide, are listed for the dielectric layer. A second U.S. patent to Gelber, No. 3,990,784, is directed to coated architectural glass having a multi-layer coating on its surface. The coating is said to comprise first and second metal layers spaced from each other by a dielectric layer disposed between them. An additional metal oxide layer is said to be used optionally for anti-reflective purposes. Nickel is mentioned as being a suitable metal together with silicon dioxide as the dielectric layer. The optical properties of silicon/silicon dioxide multi-layer systems are discussed in Stone et al., Reflectance, Transmittance and Lost Spectra of Multi-layer Si/SiO 2 Thin Film Mirrors and Antireflection Coatings For 1.5 um , Applied Optics, Vol. 29, No. 4 (1 February 1990). Stone et al suggest that in the spectral region between 1.0 and 1.6 um, a useful and easy to handle combination of paired layers is silicon and silica. The paper is directed to the fabrication of multi-layer systems. It is noted therein that the greater the difference in the index of refraction of the paired layers, the fewer the number of layers will be needed to obtain a desired level of reflectance. Silicon is noted to have a relatively high index of refraction. The paper states that silicon cannot be used as a material in the film pair for light below about 1.0 µm wavelength, for visible light, for example, due to its high absorption of light in that range. Visible light has a wavelength in the range of about 0.4 to 0.75 µm. Thus, while suggesting that a simple two layer anti-reflection coating can be made using silicon and silicon dioxide, the article clearly teaches that such anti-reflection coating is not suitable for applications requiring transparency to visible light. The article notes that Si/SiO 2 film pairs for high reflectance mirrors and anti-reflection coatings have been deposited by reactive sputtering. The coatings discussed in the paper are said to have been deposited by electron beam evaporation onto glass substrates. The anti-reflection coatings described in the Stone et al article are said to consist of a layer of silicon about 15 nm (150 Angstroms) thick with a layer of SiO 2 thereover having a thickness selected to yield minimum reflection. A silicon layer of that thickness is substantially opaque to visible light and reflectance percentage is shown in the paper only for light far above the visible wavelength range. For a layer of silicon of that thickness, a SiO 2 layer of about 280 nm (2800 Angstroms) is employed by Stone et al. It is further stated that the minimum reflectance value is not very sensitive to the thickness to the silicon layer over a thickness range between 7,5 and 20 nm (75 and 200 Angstroms). Even at the low end of this thickness range, however, the layer of silicon would be substantially opaque to the visible light component of ordinary sunlight. Similar teaching is presented in Pawlewicz et al., 1315 nm Dielectric Mirror Fabrication By Reactive Sputtering presented at the Topical Meeting on High Power Laser Optical Components held at Boulder, Colorado on October 18-19, 1984. Low levels of light absorption are reported in that paper for five reactively sputtered amorphous optical coating materials, including a Si:H/SiO 2 film pair. The low absorption was measured for light in the 1.3 µm range and it is taught in the conclusion of the paper that the Si:H material is not usable at visible wavelengths. The same point is made in Pawlewicz et al., Optical Thin Films-Recent Developments In Reactively Sputtered Optical Thin Films, Proceedings of the SPIE, Vol. 325, pp. 105-112 (January 26-27, 1982). Table 1 of that paper lists light wavelengths of 1,000 to 9,000 nm (1.0 to 9.0 µm) as the range for which optical coatings of silicon are useful. Thin film coatings of Si 1-x H x for reducing light absorption of infrared laser wavelengths 1.06, 1.315 and 2.7µm are discussed in Pawlewicz et al., Improved Si-Based Coating Materials for High Power Infrared Lasers (November, 1981). The optical properties of Si:H are discussed also in Martin et al., Optical Coatings for Energy Efficiency and Solar Applications , Proceeding of the SPIE, Vol. 324, pp. 184-190 (January 28-29, 1982). The effect is discussed of hydrogen content and Si:H bonding on various optical properties at 2 µm, a non-visible wavelength. Multi-layer Si:H/SiO 2 laser mirrors with reflectance greater than 99% at non-visible wavelengths 1.315, 2.7 and 3.8 µm also are described. The article notes that Si:H/SiO 2 multi-layer coatings are easily fabricated by sputtering, since only a single Si target is required, with either H 2 or O 2 being introduced into the sputtering chamber to form Si:H and SiO 2 layers, respectively. The high absorption coefficient in the visible region is said to make thin films of Si:H suitable for use in solar cells to absorb solar radiation. Various glazing product needs would be met by a new anti-reflective coating system which is substantially transparent to visible light and which can be deposited onto a substrate surface by economical and industrially feasible techniques. In addition, certain glazing applications, such as the above mentioned inside surface of a motor vehicle windshield, require relatively hard and durable anti-reflective coating systems. It is an object of the present invention to provide a motor vehicle windshield having on its inside surface an anti-reflective coating, which meets one or more of these product needs. Additional features and aspects of the invention will be understood from the following disclosure and description thereof. According to a first aspect of the invention, a motor vehicle windshield has on its inside surface an anti-reflective coating system that comprises a film stack having a high index of refraction material paired with a low index of refraction material, specifically, an ultra-thin film of hydrogenated silicon, Si 1-x H x is paired with a thicker film of silicon dioxide, x being a positive number less than about .4. The anti-reflective coatings of the invention are substantially transparent to visible light. This is surprising, since it is well known that Si 1-x H x exhibits strong absorption in the visible wavelength region. For that reason Si 1-x H x has not previously been considered suitable for use in anti-reflective coatings on glazing units, that is, applications requiring transparency. Because of its high absorption of visible light, it would not have been thought possible prior to the present invention to use Si 1-x H x alone or in a film pair with silicon dioxide or other material for an anti-reflective coating which is substantially transparent to visible light. Nevertheless, the present invention employs Si 1-x H x effectively in a substantially transparent anti-reflective coating system. Specifically, an ultra-thin film of Si 1-x H x , preferably about 3 nm (30 Angstroms) to about 8 nm (80 Angstroms) thick, is surprisingly found to be able to function effectively as the high refractive index material in a film pair with silicon dioxide if the silicon dioxide is appropriately matched in film thickness to the Si 1-x H x film. That is, it is found able to operate together with a film of silicon dioxide of appropriate thickness as a high refractive index/low refractive index film pair. According to another aspect of the present invention, a motor vehicle windshield is provided having on one or more surfaces an anti-reflective coating as described above. The silicon dioxide film, as the exterior film of the film pair, is found to act as a hard protective layer, providing good durability for the anti-reflective coating. The anti-reflective coating of the motor vehicle windshield functions on the inside surface to reduce reflected light from the dashboard. On the outside surface it increases transmittance of visible light to the interior. The Si 1-x H x and silicon dioxide films can be deposited by sputtering and other methods which are commercially known and economically and industrially feasible. The coating is especially suitable for use on silicon based glass, in which applications especially durable interfacial adhesion is obtained. Additional features and advantages of the invention will be understood by those skilled in the art in view of the foregoing disclosure and the following detailed description of certain preferred embodiments. The invention will now be described further, by way of example, with reference to the accompanying drawings, in which : Fig. 1 is a cross-sectional view of a laminated motor vehicle windshield comprising an anti-reflective coating in accordance with a preferred embodiment of the present invention; Fig. 2 is a graph showing percent transmittance of visible light through the glazing unit of Fig. 1 as a function of the degree of hydrogenation of the Si 1-x H x film, that is, as a function of the value of x; Fig. 3 is a graph showing percent reflectance of visible light from the glazing unit of Fig. 1 as a function of the degree of hydrogenation of the Si 1-x H x film; Fig. 4 is a graph showing percent transmittance of visible light through the glazing unit of Fig. 1, as a function of Si 1-x H x film thickness, for several silicon dioxide film thicknesses; and Fig. 5 is a graph showing percent reflectance of visible light from the glazing unit of Fig. 1 (i.e., from the surface bearing the anti-reflective coating of the invention), as a function of Si .85 H .15 film thickness, for several silicon dioxide film thicknesses. It should be understood that features and elements of the embodiments of the invention illustrated in Fig. 1 are not necessarily precisely to scale. The thicknesses of the films of the anti-reflective coating are shown larger than true scale, for example, for ease of illustration and understanding. For purposes of exemplification, the invention is described with reference to certain preferred embodiments comprising a motor vehicle windshield having an anti-reflective coating in accordance with the invention on its inside surface (i.e., the surface exposed to the passenger compartment of the motor vehicle). This anti-reflective coating provides several significant advantages. The glass currently used in motor vehicle windshields is typically a silicon based composition. The silicon based anti-reflective coatings of the windshield according to the invention are found to have good interfacial adhesion with a silicon based glass substrate. In addition, the silicon dioxide film forming the exposed surface of the glazing unit provides a hard and durable surface well adapted to the use environment experienced by a motor vehicle windshield. It should be understood that reference to the windshields comprising the antireflective coating according to the invention as being substantially transparent to visible light will generally, unless otherwise stated, mean a transmittance value of at least about 50%, and preferably at least about 70%, to meet current federal guidelines for motor vehicle windshields and also product specifications for certain architectural applications. The term visible light is used broadly to mean light anywhere in a wavelength range which is perceptible to a human observer. It is generally accepted that visible light is in the wavelength range of about 400 to 750 nm. In the visible wavelength range, percent transmittance plus percent absorption plus percent reflection equals 100%. For glazing units in which the substrate is untinted glass or the like, the absorption of visible wavelength light is negligible, such that the percent transmittance plus the percent reflectance can be taken as equaling 100% for the purposes of this discussion. Referring now to Fig. 1, a cross sectional view of a motor vehicle windshield 10 is seen to comprise an exterior ply 12 laminated by a polyvinylbutyral (PVB) laminating ply 14 to a substrate ply 16. An anti-reflective coating 20 at this windshield in accordance with the invention is carried on exposed surface 18 of substrate ply 16. Exterior ply 12 and substrate ply 16 each can be made of plastic or, more preferably, glass. In any event, substrate ply 16 preferably is substantially rigid and inextensible, such that the thin films making up anti-reflective coating 20 are not disrupted by stretching of substrate ply 16 during the lamination process or during the installation or use of the glazing unit. Anti-reflective coating 20 in the preferred embodiment of Fig. 1 consists of film 22 of hydrogenated silicon, Si 1-x H x , carried directly on surface 18 of substrate ply 16. Film 24 of silicon dioxide is carried directly over Si 1-x H x film 22. It will be recognised by those skilled in the art that the thicknesses of the various plys and films are not to scale. Films 22 and 24 are exaggerated for ease of illustration and better understanding. Although not necessary in all applications, an anti-reflective coating on a windshield typically will be coextensive with the inside surface thereof. Si 1-x H x has a refractive index which varies with the value of x. At a value of .11 the index of refraction of a sputtered Si 1-x H x film, at 2um wavelength, is about 3.45. The above-mentioned Martin et al paper, Optical Coatings for Energy Efficiency and Solar Applications , presents a plot (Fig. 5) of the refractive index of a sputtered Si 1-x H x film as a function of the value of x at 2um wavelength, the same being hereby incorporated by reference. As discussed above, the usefulness of Si 1-x H x as the high refractive index material in a film pair intended for use as a transparent anti-reflective coating is highly surprising in view of the strong absorption of Si 1-x H x in the visible wavelength region. The present invention overcomes this difficulty, in part, through the use of an ultra-thin film of Si 1-x H x . Anti-reflective efficacy is obtained notwithstanding that the high refractive index material is so thin. Specifically, it has been found that anti-reflective efficacy is achieved with an ultra-thin Si 1-x H x film coupled with a film of silicon dioxide of appropriate thickness as the low refractive index material. Silicon dioxide has a refractive index of about 1.46. The Si 1-x H X film preferably is about 3-8 nm (30 to 80 Angstroms) thick, more preferably about 4-6 nm (40 to 60 Angstroms), and most preferably about 5 nm (50 Angstroms). The value of x preferably is about .05 to .2, most preferably about .11. The SiO 2 film preferably is about 100-170 nm (1000 to 1700 Angstroms), more preferably about 120-160 nm (1200 to 1600 Angstroms), most preferably about 140 nm (1400 Angstroms). These preferences are based on the optical properties of the resulting anti-reflective coating, including especially the percent reflectance and percent transmittance of a coated glazing unit. As discussed further below in connection with Figs. 1-5, a most preferred embodiment, specifically, a laminated motor vehicle windshield having an anti-reflective coating comprising a 140 nm (1400 Angstrom) thick film of SiO 2 directly over a 5 nm (50 Angstrom) thick film of Si 1-x H x , where x is about .11, is found to have only about 4% total reflectance of visible light. This is half the anti-reflectance of the same glazing unit without the anti-reflective coating of the invention. Reflectance from the coated glass surface is reduced very nearly to zero percent. The glass maintained its substantial transparency to visible light. The Si 1-x H x and silicon dioxide films of the anti-reflective coatings of the windshield of the invention can be made employing equipment and techniques which are commercially available and well known to those skilled in the art. Thus, the films can be deposited onto a glass or other substrate surface by reactive sputtering and can also be deposited by chemical vapour deposition techniques, preferably using silane or higher order silanes as a donor gas and helium as a carrier gas. It is contemplated that increases in the thickness of the films may be achievable while still meeting a given transparency requirement by appropriately 5 adjusting the deposition parameters or technique or by using alternative deposition methods. In general, it is an advantage of the invention that the Si 1-x H x film can be deposited quickly and, hence, economically because it is so thin. Typically, the Si 1-x H x film is deposited onto a surface of a ply, for example, a glass sheet, and the silicon dioxide film is deposited over the Si 1-x H x film. In one alternative method, a thin interface film of silicon, preferably about 5-15 nm (50 to 150 Angstroms), is deposited on the glass surface and then heated, preferably at the glass bending temperature, while bending the glass in air, prior to depositing the Si 1-x H x and SiO 2 films. The silicon film is sufficiently thin that the glass clears during the heating and bending. While not intending to be bound by theory, it is believed that the silicon is oxidised. In any event, the heating improves adhesion of the antireflective coating to the glass substrate. It also improves the mechanical, and likely the chemical, durability of the film stack. It appears that this method provides a diffuse interface between the anti-reflective coating and the glass substrate. According to a preferred embodiment of this coating method, a silicon film is deposited, on the surface of a glass ply. The glass ply then is heated to an elevated temperature, typically at least about 1000°F, for example 1040°F, and preferably to the bending temperature of the glass, typically about 1250°F. After heating at such elevated temperature for a time sufficient to alter the optical properties of the silicon, preferably at least about fifteen minutes at 1250°F, the glass is slowly cooled to room temperature. After such process, the Si 1-x H x /SiO 2 coating is applied. In a preferred method of the invention a substantially transparent laminated glazing unit is fabricated by sputtering a 3-8 nm (30 to 80 Angstroms), more preferably about 4-6 nm (40 to 60 Angstroms), thick Si 1-x H x film onto a major surface of a substantially inextensible substrate ply. A 100-170 nm (1000 to 1700 Angstroms), more preferably about 120-160 nm (1200 to 1600 Angstroms), thick silicon dioxide film is sputtered over the Si 1-x H x film. The substrate ply then is laminated to another ply of glass, plastic, etc. by means of a laminating ply of PVB or other flexible polymeric material. Specifically, the laminating ply is sandwiched between the substrate ply and the additional ply and they are laminated, usually by application of heat and pressure and perhaps vacuum. Preferably the surface of the substrate ply carrying the anti-reflective coating is positioned as an exterior surface of the glazing unit closest to the viewer. The path of incident light through a glazing unit having an anti-reflective coating in accordance with the invention is illustrated in Fig. 1. Specifically, incident light 30 strikes the surface 26 of the anti-reflective film 20 and a substantial portion thereof passes through the anti-reflective coating and the remainder of the glazing unit to exit through surface 13 of exterior ply 12 as transmitted light 32. Typically, a portion of incident light is reflected back at each interface between materials of different refractive indexes. Virtually no light is reflected back at either of the two glass/PVB interfaces 31a and 31b, because the refractive index of glass is so close to that of PVB. Normally, approximately 4% of incident light is reflected back at a glass/air interface. Thus, as noted above and as marked in Fig. 2, bare glass has a total reflectance R of about 8%, that is, 4% from each surface of the glass. In certain most preferred embodiments of the present invention, total reflectance is reduced to as low as about 4% using an anti-reflective coating on one surface. Specifically, the reflectance from the surface carrying the anti-reflective coating of the invention is reduced nearly to 0%, leaving only the 4% from the air/glass interface at the opposite glass surface. In another preferred embodiment an anti-reflective coating is employed on both surfaces and reflectance is reduced nearly to zero for the windshield. This can be better understood with reference to Fig. 1. Incident light 30 strikes surface 26 of anti-reflective coating 20. Total reflectance R, expressed as a percentage of incident light 30, includes: (i) light 34 reflected at the air/SiO 2 interface at surface 26; (ii) light 35 reflected at the SiO 2 /Si 1-x H x interface 27; (iii) light 36 reflected at the Si 1-x H x /glass interface at surface 18 and (iv) light 37 reflected from the glass/air interface at surface 28. As noted above, the two glass/PVB interfaces can be ignored, since the refractive index of the two materials is almost identical. The percentage passing through surface 13 is the transmittance percentage T%. Reflectance from glass surface 18 without the anti-reflective coating of the invention would be about 4%, as noted above. According to certain most preferred embodiments of the invention, such reflectance with anti-reflective coating 20 thereon, i.e., the sum of 34 plus 35 plus 36, equals approximately zero. Thus, the reflectance for the glazing unit is only about 4% in total, virtually all of that amount being contributed by reflectance 37. While substantial reflectance would have been expected at the Si 1-x H x /glass interface, because of the large difference in the refractive index of those materials, reflectance 36 is, in fact, essentially zero. While not intending to be bound by theory, it presently is understood that reflectance 36 is essentially zero because the ultra-thin Si 1-x H x film is too thin to establish an optically significant interface with the glass. As noted above, of course, it has been found nevertheless sufficient to act as the high refractive index material with SiO 2 in the anti-reflective film pair of the invention. It will be understood from the foregoing that an embodiment of the invention further comprising an anti-reflective coating on surface 13 of exterior glass ply 12 would have total reflectance of approximately zero. The optical properties, specifically transmittance and reflectance, of anti-reflective coatings of the invention are shown in the graphs of Figs. 2 through 5. Spectrophotometric reflectance (R%) and transmittance (T%) values were calculated using a computer program adapted to give integrated R and T values of UV, visible, and IR regions for a given angle of incidence on a multi-film coating on a glass substrate. Literature values of the optical constants, the refractive index and extinction coefficient of Si 1-x H x and silicon dioxide films, were used in calculating the R and T values. The computer program was provided T% and R% values for d Si and d SiO2 parametric values. Plots were drawn for R as a function of d Si and T as a function of d Si for parametric thicknesses of SiO 2 films. These curves were used to decide the thicknesses of experimentally deposited Si 1-x H x and SiO 2 pairs providing minimum reflection with maximum transmission. The following actual pairs of Si 1-x H x /SiO 2 (for x=0) were sputtered from a Si target: 60/1000; 40/1000; 20/1000; 20/1200; 30/1200; 25/1200; 27/1500; 27/2000. Spectrophotometer reflectance and transmittance plots of these actual samples were obtained using a Perkin-Elmer Lambda 9 spectrophotometer. The experimental results agreed very well with values predicted by the multi-film computer program. The results shown in Figs. 2 through 5 were then determined by the computer program for coatings according to the present invention, employing hydrogenated silicon. The values were calculated for normal incidence. A similar procedure was applied to oblique incidence, including 65° which is the installation angle of a typical motor vehicle windshield (as viewed by a driver of the vehicle). The best results were obtained for a Si 1-x H x /SiO 2 film pair having a 140 nm (1400 Angstrom) thick SiO 2 film directly over a 5 nm (50 Angstrom) thick Si 1-x H x film where x was .11. In Fig. 2 the percent transmittance T of middle visible light (approximately 550 nm) is shown as a function of the value of x for an Si 1-x H x /SiO 2 anti-reflective coating on a glass substrate. The Si 1-x H x film thickness is 5 nm (50 Angstroms) and the SiO 2 film thickness is 140 nm (1400 Angstroms), in accordance with a highly preferred embodiment of the invention. Percent reflectance R is shown for this windshield in Fig. 3, again as a function of the value of x. It can be seen from Figs. 2 and 3 that transmittance is maximised and reflectance minimised for values of x between about .05 and .2, with an optimal value being about .11. In Fig. 4 the percent transmittance of visible light is shown as a function of the thickness d SiH of the hydrogenated silicon film for several different silicon dioxide film thicknesses d SiO2 . The silicon film was 15% hydrogenated. That is, x was about .15. The 92% transmittance of the bare glass substrate used for the test samples is indicated in the graph. Also the 70% transmittance T min currently required by United States federal guidelines for motor vehicle windshields is indicated. It can be seen that where the SiO 2 film is 140 nm (1400 Angstroms) thick, transmittance is optimal at about 5 nm (50 Angstroms) of Si .85 H .15 . Thinner films are generally preferred over thicker films, if performance requirements are met, since they can be deposited by sputtering or other method more quickly and, hence, are generally more economical and result in higher productivity. Referring now to Fig. 5, the percent reflectance of the laminated windshield for which transmittance is shown in Fig. 4, having an anti-reflective coating according to the invention, is shown as a function of hydrogenated silicon film thickness for a variety of silicon dioxide film thicknesses. The 8% reflectance of bare glass is indicated in the graph. It can be seen that a film pair having about 5 nm (50 Angstroms) hydrogenated silicon (x=.15) and 140 nm (1400 Angstroms) silicon dioxide has reflectance of visible light as low as about 4%.

Claims: A motor vehicle windshield having on its inside surface an anti-reflective coating which is substantially transparent to visible light said anti-reflective coating comprising a Si 1-x H x film (22) having a thickness between 3 and 8 nm (30-80 Angstroms) and a silicon dioxide film (24) over the Si 1-x H x film (22) having a thickness between 100 to 170 nm (1000 to 1700 Angstroms), x being a positive number less than about .4. A motor vehicle windshield as claimed in claim 1, wherein the silicon dioxide film (24) has a thickness between 120 and 160 nm (1200 and 1600 Angstroms) and x is between .05 and .2. A motor vehicle windshield as claimed in claim 1 wherein the Si 1-x H x film has a thickness of about 5 nm (50 Angstroms) and having a SiO 2 film having a thickness of about 140 nm (1400 Angstroms) applied directly on the Si 1-x H x film and in which x is about .11, the resulting anti-reflective coating having at least about 70% transmittance and less than about 8% reflectance of visible light incident on the anti-reflective coating. A motor vehicle windshield as claimed in any one of the preceding claims in which the windshield comprises a first ply and a substantially inextensible substrate ply having a first surface laminated to the first ply by a laminating layer of flexible polymeric material, the second surface being substantially parallel and coextensive with, and opposite to, the first surface. A motor vehicle windshield as claimed in claim 5, wherein the first and substrate plys each is glass and the laminating ply is polyvinylbutyral. A method of providing a substantially transparent motor vehicle windshield with an anti-reflective coating, the method comprising depositing an Si 1x H x film with a thickness between about 3 and 8 nm (30-80 Angstroms) on the inside surface of the windshield and then depositing a SiO 2 film with a thickness between 100 and 170 nm (1000-1700 Angstroms) over the Si 1-x H x film, wherein x is a positive number less than about .4. A method as claimed in claim 6, wherein said films are deposited by sputtering, the silicon dioxide film being between about 120 and 160 nm (1200 and 1600 Angstroms) thick. A method as claimed in claim 6, wherein windshield has a glass substrate ply with a thin interfacial film of silicon directly on the surface thereof and the method further comprises heating the glass ply with the silicon film thereon to an elevated temperature for a period of time sufficient to alter its optical properties prior to depositing the Si 1-x H x film and SiO 2 films thereon. A method as claimed in claim 6, comprising the steps of: a) depositing a 3 to 8 nm (30 to 80 Angstroms) thick Si 1-x H x film onto a major surface of a substantially inextensible substrate ply thereof, wherein x is a positive number less than about .40, by sputtering silicon in an atmosphere comprising hydrogen; b) then depositing a 120 to 160 nm (1200 to 1600 Angstrom) thick SiO 2 film directly over the Si 1-x H x film by sputtering silicon in an atmosphere comprising oxygen; and c) then sandwiching a flexible polymeric laminating ply between the substrate ply and an additional ply and laminating the same, the major surface with the anti-reflective coating thereon being what will be the interior surface of the windshield when the windshield is assembled in the motor vehicle.

Inventors: DEMIRYONT HULYA, SUROWIEC ROMAN, DEMIRYONT, HULYA, SUROWIEC, ROMAN
Applicants: FORD FRANCE, FORD MOTOR CO, FORD WERKE AG, FORD FRANCE S. A., FORD MOTOR COMPANY LIMITED, FORD-WERKE AKTIENGESELLSCHAFT
Application year: 1991
Main classification: G02B1
IPC codes: C03C17, G02B1