SOLAR CONTROL COATED GLASS

Abstract: A solar-control glass that has acceptable visible light transmission, absorbs near infrared wavelength light (NIR) and reflects midrange infrared light (low emissivity mid IR) along with a preselected color within the visible light spectrum for reflected light is provided. Also provided is a method of producing the improved, coated, solar-controlled glass. The improved glass has a solar energy (NIR) absorbing layer comprising tin oxide having a dopant such as antimony and a low emissivity control layer (low emissivity) capable of reflecting midrange infrared light and comprising tin oxide having fluorine and/or phosphorus dopant. A separate iridescence color suppressing layer as described in the prior art is generally not needed to achieve a neutral (colorless) appearance for the coated glass, however an iridescence suppressing layer or other layers may be combined with the two layer assemblage provided by the present invention. Ifdesired, multiple solar control and/or multiple low emissivity layers can be utilized. The NIR layer and the low emissivity layer can be separate portions ofa single tin oxide film since both layers are composed of doped tin oxide. A method of producing the coated solar control glass is also provided.

Description: Background This invention relates to coated glass used in residential, architectural and vehicle windows and miscellaneous applications where both solar control and low emissivity properties are desired. The coatings for solar control and low emissivity contain tin oxide having various dopants. The invention avoids the need for an anti-iridescence underlayer. The glass articles may be of any shape but are typically flat or curved. The glass composition can vary widely but is typically soda lime glass produced by the float process. It may be annealed, heat strengthened or tempered. Solar-control is a term describing the property of regulating the amount of solar heat energy which is allowed to pass through a glass article into an enclosed space such as a building or an automobile interior. Low emissivity is a term describing the property of an article's surface wherein the absorption and emission of mid-range infrared radiation is suppressed, making the surface a mid-range infrared reflector and thereby reducing heat flux through the article by attenuating the radiative component of heat transfer to and from the low emissivity surface (sometimes referred to as Low E). By suppressing solar heat gain, building and automobile interiors are kept cooler; allowing a reduction in air conditioning requirements and costs. Efficient low emissivity coatings improve comfort during both summer and winter by increasing the thermal insulating performance of a window. Important to commercially acceptable coated glass articles which possess both solar-control and low emissivity properties are, of course, economic processes for producing the articles and durability and maintenance of associated properties such as light transmission, visibility, color, clarity and reflection. As explained below, various technologies have been employed to meet the requirement for solar-control and low emissivity glass, however, no one system has successfully met all of the performance requirements in an economic manner. Many coatings and coating systems cause iridescent colors to develop in the coated article. This may be caused by the chemical composition of the coating, the thickness ofan individual layer or layers, or an interaction of the substrate and coatings to incident light. Such iridescence can, in some cases, be minimized or eliminated by placing an anti-iridescence layer between the glass substrate and the first coating. The use of an interference layer between the glass and a subsequent functional layer or layers to suppress iridescence or color reflection was first demonstrated by Roy G. Gordon, and was the subject of U. S. Patent 4,187,336, issued Feb 5, 1980. The Gordon technology has been the state of the art for coated solar control glass as evidenced by recently issued U.S. Patent 5,780,149 (McCurdy el al, July 14, 1998) which applied two layers to obtain solar control on top of a Gordon type interference layer. The interference layer frequently contains silicon dioxide. Surprisingly, the present invention represents a dramatic breakthrough and eliminates the need for a Gordon type underlayer to control reflected color. US Patent 3,149,989 discloses compositions of coatings useful in producing radiation reflecting (solar-control) glass. At least two coatings are used with the first coating, adhered to the glass substrate, being comprised of tin oxide doped with a relatively high level of antimony. The second coating is also comprised of tin oxide and is doped with a relatively low level of antimony. The two films may be superimposed, one on another, or may be applied to opposite sides of the glass substrate. In either case, these solar-control coatings do not contribute significant low emissivity properties to the glass article. US Patent 4,601,917 teaches liquid coating compositions for producing high-quality, high-performance, fluorine-doped tin oxide coatings by chemical vapor deposition. One of the uses of such coatings is in the production of energy-efficient windows, also known in the trade as low-E or low-E windows. Methods of producing the coated glass are also described. This patent does not teach how to produce coated glass articles which possess both solar-control and low emissivity properties. US Patent 4,504,109, assigned to Kabushiki Kaisha Toyota Chou, describes glass coated with infrared shielding multilayers comprising a visible light transparent substrate and an overlying component lamination consisting of "at least one infrared shield layer and at least one interferential reflection layer alternatively lying on each other ...." Indium oxide doped with Sn is used in the examples as the infrared shield layer and TiO 2 was used as the interferential shield layer. In order to reduce iridescence the infrared shield layer and the interferential reflection layer thickness must have a value of one quarter lambda (lambda/4) with a permissible deviation of from 75% to 130% of lambda/4. Although other formulations are disclosed for the infrared shield layer and the interferential reflection layer such as SnO 2 with or without dopants, (see column 6 lines 12 to 27), however, the specific combination of doped SnO 2 layers of the present invention that accomplishes solar control, low emissivity and anti-iridescence without requiring a lambda/4 thickness limitation is neither disclosed nor exemplified to suppress iridescence or color reflection. US Patent 4,583,815, also assigned to Kabushiki Kaisha Toyota Chou describes a heat wave shield laminate consisting of two indium tin oxide overlayers containing different amounts of tin. Antireflection layers, above or below the indium tin oxide layers are also described. Other formulations are disclosed for the infrared shield layer and the interferential reflection layer such as SnO 2 with a dopant that becomes a positive ion with a valence of +5 such as Sb, P, As, Nb, Ta, W, or Mo or an element such as F which readily becomes a negative ion with a valence of -1, (see column 22 lines 17 to 23). However, the specific combination of doped SnO 2 layers of the present invention that accomplishes solar shielding, low emissivity and anti-iridescence is neither disclosed nor exemplified. There is no claim to tin oxide layers nor any teaching in the specification to describe the composition of such layers, e.g. the ratio of dopant to tin oxide. It should also be noted that the teaching leads to the use of the same dopant in both layers (indium tin oxide) whereas in the instant patent application, one layer must contain a different dopant than the other layer. US Patent 4,828,880, assigned to Pilkington PLC, describes barrier layers which act to inhibit migration of alkali metal ions from a glass surface and/or act as color suppressing underlayers for overlying infrared reflecting or electrically conducting layers. Some of these color suppressing layers are used in solar-control or low emissivity glass construction. US Patent 5,168,003, assigned to Ford Motor Company, describes a glazing article bearing a substantially transparent coating comprising an optically functional layer (which may be low emissivity or solar control) and a thinner anti-iridescence layer which is a multiple gradient step zone layer. Antimony doped tin oxide is mentioned as a possible alternative or optional component ofthe exemplified low emissivity layer. US Patent 5,780,149 , assigned to Libbey-Owens-Ford describes solar control coated glass wherein at least three coating layers are present, first and second transparent coatings and an iridescence suppressing layer lying between the glass substrate and the transparent upper layers. The invention relies upon the transparent layers having a difference in refractive indices in the near infrared region greater than the difference of indices in the visible region. This difference causes solar heat to be reflected in the near IR region as opposed to being absorbed. Doped metal oxides which have low emissivity properties, such as fluorine doped tin oxide, are used as the first transparent layer. Metal oxides such as undoped tin oxide are used as the second layer. No NIR absorbing combinations are described. EP 0-546-302-B1 issued July 16,1997 and is assigned to Asahi Glass Co. This patent describes coating systems for solar-control, heat treated (tempered or bent) glass comprising a protection layer based on a metal nitride. The protection layer or layers are used to overcoat the solar-control layer (to prevent it from oxidizing during thermal treatment). As a solar control layer, many examples are provided including tin oxide doped with antimony or fluorine. However, the specific combination of doped SnO 2 layers of the present invention that accomplishes solar control, low emissivity and anti-iridescence without following Gordon's teachings is neither disclosed nor exemplified. EP 0-735-009-A1 is a patent application that was published in February 1996 and is assigned to Central Glass Co. This patent application describes a heat-reflecting glass pane having a multilayer coating comprising a glass plate and two layers. The first layer is a high refractive index metal oxide based on Cr, Mn, Fe, Co, Ni or Cu, the second layer is a lower refractive index film based on a metal oxide such as tin oxide. Doped layers and low emissivity or NIR absorbing combinations are not disclosed. WO 98/11031 This patent application was published in March 1998 and assigned to Pilkington PLC. It describes a high performance solar-control glass comprising a glass substrate with coatings comprising a heat-absorbing layer and a low emissivity layer ofa metal oxide. The heat-absorbing layer may be a metal oxide layer. This layer may be doped tungsten, cobalt, chromium, iron molybdenum, niobium or vanadium oxide or mixtures thereof. The low emissivity layer may be doped tin oxide. In a preferred aspect of the invention, an iridescence-suppressing layer or layers is incorporated under the coating comprising a heat-absorbing layer and a low emissivity layer. This application does not disclose or suggest the specific combination of doped SnO 2 layers ofthe present invention that accomplishes solar control, low emissivity and anti-iridescence without requiring a "Gordon" type underlayer to suppress iridescence or color reflection. Canadian Patent 2,193,158 discloses an antimony doped tin oxide layer on glass with a tin to antimony molar ratio o 1:0.2 to 1:0.5 that reduces the light transmission of the glass. Dopant Effects in Sprayed Tin Oxide Films , by E. Shanthi, A. Banerjee and K.L. Chopra, Thin Solid Films, Vol 88, 1981 pages 93 to 100 discusses the effects of antimony, fluorine, and antimony-fluorine dopants on the electrical properties of tin oxide films. The article does not disclose any optical properties of the antimony-fluorine films nor the effect on transmitted or reflected color. UK Patent Application GB 2,302, 101 A assigned to Glaverbel describes a glass article coated with an antimony/tin oxide film of at least 400 nm containing an Sb/Sn molar ratio from 0.05 to 0.5, with a visible transmittance of less than 35%. The films are applied by aqueous spray CVD and are intended for privacy glass applications. Haze reducing undercoats are taught as well as thick layers with low Sb/Sn ratios which have low emissivity properties as well as high solar absorbency. It also teaches that it is possible to provide one or more additional coating layers to achieve certain desirable optical properties. None of these properties other than haze are mentioned. The application teaches nothing about thinner layers, the use of more than one dopant, or the control of film color. UK Patent Application GB 2,302,102 A also assigned to Glaverbel describes a glass substrate coated with a Sn/Sb oxide layer containing tin and antimony in a molar ratio of from 0.01 to 0.5, said layer having been deposited by CVD , whereby the coated substrate has a solar factor(solar heat gain coefficient) of less than 0.7. The coatings are intended for window applications and have luminous transmittances between 40 and 65% and thicknesses ranging from 100 to 500 nm. Haze reducing undercoats are claimed and low emissivity can be imparted to the coatings by a judicious choice of the Sb/Sn ratio. Like the previous application, the teaching of providing one or more additional coating layers to achieve certain desirable optical properties is mentioned. Also low emissivity layers of fluorine doped tin oxide can be deposited over the Sb/Sn layers or fluorine components can be added to the Sb/Sn reactants to give low emissivity films which contain F, Sb and Sn. The last two methods were not favored because of the added time and cost of adding a third layer and the fact that the emissivity of the Sb/F films was raised and not lowered. No mention of color control or color neutrality is found. GB 2,200139, assigned to Glaverbel teaches a method of depositing a coating by the spray application of solutions containing tin precursors, fluorine containing compounds and at least one other dopant selected from the group antimony, arsenic, vanadium, cobalt, zinc, cadmium, tungsten, tellurium or manganese. Previously, glass manufacturers have managed heat transport through windows by the use of absorbing and/or reflecting coatings, glass tints, and post-applied films. Most of these coatings and films are designed to control only one portion of the solar heat spectrum, either the NIR, i.e. near infra red component of the electromagnetic spectrum having a wavelength in the range of 750 - 2500 nm or the mid IR component of the electromagnetic spectrum having a wavelength on the range of 2.5 - 25 microns. A product has been designed to control the entire heat spectrum, however Sputtered metal/dielectric film stacks while effective, have limited durability and must be protected and sealed within the center section of a multipane insulated glass unit (IGU). What is needed is a total solar control film or combination of films that can be easily applied by pyrolytic deposition during the glass making operation which yields an article which has an acceptable visible transmission, reflects or absorbs the NIR, reflects the mid-IR, and is neutral or close to neutral in color. The above references either alone or in combination do not teach or suggest the specific combination of doped SnO 2 layers of the present invention that accomplishes solar control, low emissivity and anti-iridescence without requiring a "Gordon" type underlayer. The present application discloses novel solar-control glass that has acceptable visible light transmission, absorbs near infrared wavelength light (NIR) and reflects midrange infrared light (low emissivity or Low E) along with a preselected color within the visible spectrum for reflected light that can be controlled to a specific color or be made essentially colorless ("neutral" as defined hereinafter). Also provided are methods of producing such coated, solar-control glass. The glass has a solar energy (NIR) absorbing layer comprising tin oxide having a dopant such as antimony and a low emissivity control layer capable of reflecting midrange infrared light and comprising tin oxide having fluorine and/or phosphorus dopant. A separate iridescence color suppressing layer as described in the prior art is not needed to achieve a neutral (colorless) appearance for light reflected off the coated glass. If desired, multiple solar control and/or multiple low emissivity layers can be utilized. The NIR layer and the low emissivity layer can be separate portions ofa single tin oxide film since both layers are composed of doped tin oxide. A method of producing the coated solar control glass is also provided. In addition, some of these measures may control or change the color of transmitted light through the addition of color additives to the NIR layer. Surprisingly we have found that the dopant fluorine that produces a noncolored tin oxide film functions as a color additive when added as an additional dopant to the NIR layer and modifies the colour of transmitted light through the NIR film. Brief Description of the Drawings Figures 1 through 4 and 8 through 13 depict a cross-section of coated glass having different numbers of layers or films in different stacking sequences for the layers on glass substrates. Figures 5 and 6 graphically depict the solar control achieved with antimony doped films at various concentrations ofdopant and various film thicknesses on window panes, i.e. a single pane of glass, or on insulated glass units (IGU) which are a composite of at least two glass panes. Figure 7 depicts the color spectrum in terms of Commission Internationale de L'Exclairage (C.I.E.) x and y coordinates and the specific color achievable with various film thickness and dopant concentrations. The English translation for C.I.E. is International Commission on Illumination Preferred Aims One preferred aim is to prepare a transparent article with controlled reflected color (even neutral color as defined herein,) that will absorb solar near infrared (NIR) wavelength radiation and reflect mid-range infrared heat (low emissivity) comprising two thin film layers containing doped SnO 2 . Another is the application of the layers by atmospheric pressure chemical vapor deposition (CVD) techniques, or by other processes such as solution spray or vaporized/sublimed liquids/solids can be utilized. The preferred method of application for this invention is atmospheric pressure CVD using vaporized liquid precursors. Another is to provide multiple solar control and/or low emissivity layers along with other layers in combination with the solar control or low emissivity layer. Another is to provide a solar control film or combination of films that can be easily applied by pyrolytic deposition during the glass making operation which yields an article which has an acceptable visible transmission, reflects or absorbs the NIR, reflects the mid-IR (low-E), and is neutral or close to neutral in color, the production of which is an object of the present invention. Another preferred aim is to control the color of transmitted light independently from the color of reflected light by the addition of color additives in the NIR layer. Detailed Descriptions, Explanations, Preferred Embodiments Solar control and low emissivity coated glass is produced by depositing preferably on a heated transparent substrate at least two layers, a low emissivity layer comprising a SnO 2 film containing fluorine and/or phosphorus dopant and a NIR absorbing layer comprising a SnO 2 film containing as a dopant antimony, tungsten, vanadium, iron, chromium, molybdenum, niobium, cobalt, nickel or mixtures thereof. This combination has been found to effectively control the solar and radiative heat portions of the electromagnetic spectrum such that a window coated with these films will have greatly enhanced properties. Solar control properties are typically expressed in terms of solar heat gain coefficient (SHGC) and U-value. SHGC is a measure of the total solar heat gain through a window system relative to the incident solar radiation , while the U-value (U) is the total heat transfer coefficient for the window. The SHGC of the coated glass is primarily dependent on the thickness and the antimony content of the NIR absorbing film (see Figures 5 and 6) while the U-value depends primarily on the film's emissivity and the window construction. SHGC measured at center of glass can range from about 0.40 to 0.80 while U values measured at center of glass can vary from about 0.7-1.2 for a single pane coated with the preferred embodiment films. In an insulated glass unit (IGU) the SHGC's decrease to ∼0.30 with U-values as low as ∼0.28. We have found that both the reflected and transmitted color of the coated glass can be controlled. In addition the amount ofvisible light transmitted through the coated glass can be controlled between about 25-80% by controlling the thickness of the NIR and low emmisivity films and the concentration of dopant in the NIR film. Transmitted color, i.e. the color of light transmitted through the coated glass can be controlled separately from the reflected color by the addition of a color-effective quantity of a color additive to the NIR layer of the coating. The reflected color can vary from almost neutral to red, yellow, blue or green and can be controlled by varying the film thickness and dopant content of the layers. Surprisingly, near color neutrality as defined herein can be achieved for reflected color without the need of an anti-iridescent layer. Although the refractive indices of the NIR and low emissivity films are different, the reflected color does not depend on classical interference phenomena originally discovered by Gordon (U.S. Patent 4,1887,336). Observed reflected color is unexpectedly controlled by the combination ofabsorption and reflection achieved by the NIR layer (absorption) and the reflection achieved by the low-emissivity layer or layers. The absorption of the NIR layer can be controlled by varying the thickness of its SnO 2 layer and the concentration of the dopant in the NIR layer, usually antimony. The reflectance of the low emissivity layer can be controlled by varying the thickness of its SnO 2 layer and the concentration of the dopant in the low emmisivity layer, usually fluorine. The low emissivity layer composed of SnO 2 containing a fluorine or phosphorous dopant is sometimes abbreviated herein as TOF or TOP while the NIR layer of SnO 2 when it contains an antimony dopant is sometimes abbreviated herein as TOSb. A preferred embodiment of this invention utilizes a combination of a fluorine doped tin oxide (TOF) film as the low emmisivity layer with an antimony doped tin oxide (TOSb) film as the NIR layer. TOF films and their deposition processes onto glass are known in the art and referred to as low emissivity films. The NIR absorbing film is also a SnO 2 film but contains a different dopant than the low emissivity layer. The dopant in the NIR layer is preferably antimony although the dopant can be an element selected from the group consisting of antimony, tungsten vanadium, iron, chromium, molybdenum, niobium, cobalt, nickel, and mixtures thereof. A mixture of one or more dopants can be used in the NIR layer, however the low emissivity layer must contain a low emissivity dopant that imparts significant conductivity to the layer such as fluorine or phosphorous, although other dopants may be used in combination with the low emissivity dopant. Since the low emissivity and the NIR layers of the present invention both utilize SnO 2 as the metal oxide matrix containing a dopant, the NIR and the low emissivity layers can be part of a single film having a dopant gradient. A single film utilizing a dopant gradient is depicted in Figure 3 as film 16. In film 16 there is a dopant gradient with the NIR dopant having a higher concentration than the other dopant(s) at one surface of the film, either surface 18 or 22, and the low emissivity dopant having a higher concentration than the other dopants at the other surface of the film. This results in a change or gradient in the concentrations of the NIR and low emissivity dopants between surface 18 and surface 22. At some intermediate point 20 between surface 18 and surface 22 the concentration of the NIR dopant changes from being the highest concentration dopant on one side of point 22 to no longer being the highest concentration dopant on the other side of point 22. Figure 8 show the low E film, 10, above the NIR film 12, The NIR film 12 in Figure 8 has a concentration gradient for the NIR dopant in the tin oxide film with a lower concentration of the dopant closer to the low E film 10. The coated glass of Figure 9 is similar to the structure shown in figure 8 with the exception that the concentration gradient of the NIR dopant, usually antimony, is higher near the low E film 10 and lower nearer the substrate. Film 12 is different then film 16 shown in Figure 3 in that film 12 is a NIR film while film 16 has both NIR and low E properties and contains both a low e dopant and a NIR dopant with a concentration gradient for the low e dopant and a concentration gradient for the NIR dopant. Figures 10, 11, 12 and 13 show the NIR layer as two distinct films,28 and 30,. Film 28 is shown as being thicker than film 30 and the total thickness of the NIR layer is the sum of the thicknesses of films 28 and 30 and should be within the range of thicknesses stated above for the NIR layer and preferably from 80 to 300nm. In Figures 10 and 11, films 28 and 30 are adjacent each other, while in Figures 12 and 13, films 28and 30 are on opposite sides of low E film 10. The concentration of dopant in film 28 is preferably different than the concentration of dopant in film 30. The preferred embodiment ofthis invention uses an antimony doped film as the NIR film. Such a film can be deposited by a number of techniques including spray pyrolysis, PVD and CVD methods. Spray pyrolysis is known and disclosed in patents such as Canadian patent 2,193,158. CVD methods for depositing SnO 2 films with or without dopants and the chemical precursors for forming SnO 2 films containing dopants are well known and disclosed in U.S. Patents 4,601,917, and 4,285,974. Preferred is CVD deposition of the SnO 2 layers containing dopants according to known methods directly on a float glass manufacturing line outside ofor within the float glass chamber utilizing conventional on-line deposition techniques and chemical precursors as taught by U.S. Patent 4,853,257 (Henery). However the SnO 2 films containing dopants can be applied as layers on glass utilizing other processes such as solution spray or vaporized/sublimed liquids/solids at atmospheric pressure. The preferred method of application for this invention is atmospheric pressure CVD using vaporized liquid precursors. The process is very amenable to existing commercial on-line deposition systems. The precursors of the preferred embodiments are economical to apply, will enable long coating times, will reduce the frequency of system clean-out, and should be able to be used with little or no modification to existing glass float line coating equipment, The coatings function by a combination of reflection and absorption. The low emissivity film reflects mid-IR heat in the 2.5-25 micron region of the spectrum while the NIR absorbing film absorbs heat primarily in the 750- 2500 nm region. While not to be bound thereby, the theory upon which we account for this effect is that in the NIR region, the plasma wavelength (PL - the wavelength where the low emissivity film changes from a transmitter to a reflector of light energy) for the low emissivity film falls in the NIR region. In the area around the PL, the NIR absorption is the highest for the low emissivity film and when combined with a NIR absorbing film, increased absorbency takes place. The NIR absorbing films of our preferred embodiments are also doped semi-conductors and hence have reflective properties in the mid IR. This reflection coupled with the low emissivity film reflection gives an overall higher heat reflectance in the mid IR. Preferably the SnO 2 is pyrolytically deposited on the glass using a tin precursor, especially an organotin precursor compound such as monobutyltin trichloride (MBTC), dimethyltin dichloride, dibutyltin diacetate, methyl tin trichloride or any of the known precursors for CVD deposition of SnO 2 such as those disclosed in US 4,601,917 incorporated herein by reference. Often such organotin compounds used as precursors for pyrolytic deposition of SnO 2 contain stabilizers such as ethanol. Preferably the concentration ofstabilizers is less than 1% in order to reduce fire risks when contacting hot glass with such chemicals in the presence of oxygen. Precursors for the dopant in the NIR layer (antimony, tungsten, vanadium, iron, chromium, molybdenum, niobium, cobalt and nickel) are preferably halides such as antimony trichloride, however alkoxides, esters, acetylacetonates and carbonyls can be used as well. Other suitable precursors for the dopant and SnO 2 are well known to those skilled in the art. Suitable precursors and quantities for the fluorine dopant in the low emissivity SnO 2 layer are disclosed in U.S. Patent 4,601,917 and include trifluoroacetic acid, ethyltrifluoroacetate, ammonium fluoride, and hydrofluoric acid. Concentration of low emissivity dopant is usually less then 30% with preferred concentrations of low emissivity dopant from 1% to 15% by weight of dopant precursor based upon the combined weight of dopant precursor and tin precursor. This generally correlates to a dopant concentration in the low E film of from 1% to 5% percent based upon the weight of tin oxide in the low E film. In our preferred embodiments, the properties depend on the thickness of the low emissivity and absorbing layers as well as the antimony content of the absorbing (NIR) film. The low emissivity film thickness ranges from 200-450 nm with 280 to 320nm being most preferred. The preferred NIR absorbing films can be deposited in a similar fashion as the low emissivity films using such methods as disclosed in U.S. Patent 4,601,917. The organotin precursors for the SnO 2 can be vaporized in air or other suitable carrier gases containing a source of O 2 and in precursor concentrations from 0.25 - 4.0 mol% (0.5 - 3.0 mol% more preferred). SnO 2 precursor concentrations are expressed herein as a percentage based upon the moles of precursor and the moles of carrier gas. Preferred concentrations of NIR dopant precursor are from about 1% to about 20% (2.5% to 7.5% more preferred and 3.0% to 6.0% most preferred) and are calculated using the weight of dopant precursor and the weight of SnO 2 precursor. Particularly preferred is an antimony dopant using antimony trichloride as the precursor at about 2% to about 8% by weight with about 4.0% by weight particularly preferred. This correlates to a similar antimony mass percent in the tin oxide NIR film. A coated glass exemplifying the invention is depicted in the figures. Figure I shows the films in cross section. The film thicknesses range from 200 to 450 nm for the low emissivity film (item 10) and for the NIR film (item 12) from 80 to 300 nm. The preferred thickness is 250 to 350 nm for the low emmisivity film and 200 to 280 nm for the NIR film. Most preferred is 280 to 320nm for the low E film and 220-260 nm for NIR film. Using films of the preferred embodiments, solar control coated glass can be produced with a Neutral-blue Color which is defined herein as coated glass having reflected light predominately within C.I.E. chromaticity coordinates values of x between 0.285 and 0.310 and y between 0.295 and 0.325. The definition of Neutral-blue is shown in Figure 7 by the area within the box labeled Neutral-blue Color. As shown in Figure 7 the data for examples 15, 20 and 22, controlled or preselected reflected color close to neutral color but slightly to the red shade from neutral can be produced (x values of up to 0.325 and y values of up to 0.33), but such essentially neutral to slightly red shades of reflected color are not appealing to consumers. Figure 2 shows the two films or layers in the opposite sequence than that shown in Figure 1. In Figure 2, the low emissivity film is closer to the glass 14 than the NIR film 12. Figure 3 shows the NIR and the low emissivity layers integrated into a single SnO 2 film 16 having a dopant gradient within film 16. Film 16 has a preponderance of one dopant (e.g. the low emissivity dopant, fluorine) at the upper surface, 18, away from the glass 14 and a preponderance of the other dopant (e.g. the NIR dopant such as antimony) at the film surface 22 nearer the glass. The concentration of dopant changes from surface 18 to surface 22, so that one dopant changes from greater than 50% of the dopants at surface 18 to approximately 0% at surface 22. At an intermediate point 20, below upper surface 18, the predominant dopant at that point in the film changes from the predominant dopant at surface 18 to the predominant dopant at surface 22. Either the NIR dopant or the low emissivity dopant (fluorine) can be the predominant dopant at surface 18 with the other dopant the predominant dopant at surface 22. Figure 4 depicts a coated glass having additional layers 24 and 26 in addition to a low emissivity layer 10 and NIR layer 12. The additional layers 24 and 26 can be additional low emissivity and/or NIR layers or other conventional layers used to coat glass such as a tinting layer. For example 12 can be a NIR layer (e.g .antimony doped tin), 10 a low emissivity layer (fluorine doped tin) and 24 another NIR layer. 26 can be another low emissivity layer or some other conventional layer. The concentration of dopant when more than one low emissivity layer is utilized may be the same or different and the thickness of each low emmisivity layers may also be the same or different. Likewise, when more than one NIR layer is utilized, the concentration ofdopant and the selection of dopant (antimony, tungsten, vanadium, iron, chromium, molybdenum, niobium, cobalt and nickel) can be the same or different and the thickness of each NIR layer can be the same or different. Generally the dopant for the NIR layer has been discussed herein mostly in terms of antimony, it must be understood that the dopant in the NIR layer can be selected from the group consisting of antimony, tungsten, vanadium, iron, chromium, molybdenum, niobium, cobalt, nickel and mixtures thereof. Likewise, in the gradient layer embodiment of the invention as depicted in Figure 3, the predominant dopant at the NIR surface either surface 18 or 22 can be selected from the group consisting of antimony, tungsten, vanadium, iron, chromium, molybdenum, niobium, cobalt, nickel and mixtures thereof, it only being essential that the low e dopant, e.g. fluorine, be the predominant dopant at the opposite surface. Combined with a gradient layer can be one or more NIR or low emissivity layers such as layers 10 and 12 in figures 1 to 3 and/or other conventional layers. Water is preferably used to accelerate the deposition of SnO 2 film onto glass as taught by U.S. Patent 4,590,096 (Lindner) and used in concentrations from ~0.75 to 12.0 mol% H 2 O based upon the gas composition. The preferred embodiments of our invention will be exemplified by the following examples. The most preferred embodiment at this time to obtain a coated glass with low E and NIR properties with neutral reflected color with only two films on glass is about a 3000Å thick TO:F film (fluorine doped tin oxide) in combination with about a 2400Å TO:Sb (antimony doped tin oxide) film on glass. The film thickness for the TO:F layer can range from ∼2800-3200Å and still achieve the surprising result of a neutral reflected color. The fluorine concentration can range from ∼1-5 atomic%. The TO:Sb film thickness can range from ∼2200-2600Å with an antimony concentration from ∼3-8% and still achieve the surprising result of a neutral reflected color for the coated glass. Within the preferred thickness and dopant concentration ranges of the present invention, a solar control coated glass can be produced having a NIR layer and a low E layer and having a Neutral-blue Color for reflected light, i.e. coated glass having reflected light predominately within C.I.E. chromaticity coordinates values of x between 0.285 and 0.310 and y between 0.295 and 0.325 as shown in Figure 7 by a box labeled Neutral-blue Color or close to the Neutral-blue Color with x values as high as about 0.32 as shown by Examples 15, 20 and 22. Examples 1 to 30 A 2.2 mm thick glass substrate (soda lime silica), two inches square, was heated on a hot block to 605 to 625°C. The substrate was positioned 25 mm under the center section of a vertical concentric tube coating nozzle. A carrier gas of dry air flowing at a rate of 15 liters per minute (l/min) was heated to 160°C and passed through a hot wall vertical vaporizer. A liquid coating solution containing ∼95 wt% monobutyltin trichloride and ∼5 wt% antimony trichloride was fed to the vaporizer via a syringe pump at a volume flow designed to give a 0.5 mol% organotin concentration in the gas composition. A quantity of water was also fed into the vaporizer at a flow designed to give a 1.5 mol% water vapor in the gas mixture. The gas mixture was allowed to impinge on the glass substrate at a face velocity of0.9 m/sec for ∼6.1 seconds resulting in the deposition of a film of antimony doped tin oxide ∼240 nm thick. Immediately following, a second gas mixture was used consisting of a precursor composition of 95 wt% monobutyltin trichloride and 5 wt% trifluoroacetic acid, along with water in the same concentrations and carrier gas as used before to deposit the antimony doped SnO 2 layer. This second gas mixture was allowed to impinge on the coated substrate for ~6.7 seconds. A film of ∼280nm of fluorine doped tin oxide was deposited. The bilayer film was very light blue in transmission and reflection. The optical properties were measured on a UV/VIS/NIR spectrophotometer and the sheet resistance was measured on a standard four point probe. The solar heat gain coefficient, U value and visible transmission for the center of the glass were calculated using the Window 4.1 program developed by Lawrence Berkeley National Laboratory, Windows and Daylight Group, Building Technologies Program, Energy and Environmental Division. The C.I.E. chromaticity x and y color coordinates were calculated using ASTM E308-96 from the visible reflectance data between 380-770 nm and the tristimulus values for Illuminant C. The analysis results for this film appears in Table 1, number 19. The procedure of this example was repeated 29 additional times with concentrations of chemical precursors and deposition times varied in order to produce coated glass samples having different thicknesses for the NIR and low emissivity layers and different dopant concentrations. The results are presented in Table 1. Example 31 to 38 The procedure of Example 1 was repeated, except that the vapor feed order was reversed. The fluorine doped tin oxide film was deposited first for ∼8 seconds followed by the antimony doped tin oxide film for -6 seconds. The resulting film was ∼540 nm thick and composed of a low emissivity layer (TOF) of about 300 nm and a NIR layer (TOSb) of about 240 nm and had a similar appearance and reflected light color (Neutral-blue Color) as the film in example 19. The analysis results appear in Table 2, number 31. The procedure of this example was repeated 7 additional times with concentrations of chemical precursors and deposition times varied in order to produce coated glass samples having different thicknesses for the NIR and low emissivity layers and different dopant concentrations. The results are presented in Table 2 Example 39 The procedure of Example 1 was repeated but utilizing three precursor feed mixtures. The composition of the third mixture was 90 wt% monobutyltin trichloride, 5 wt% trifluoroacetic acid, and 5 wt% antimony trichloride. A gradient film was deposited by first depositing only the antimony doped tin oxide precursor of Example 1 for 70% of the time needed to deposit 240 nm. Then the mixed antimony/fluorine doped precursor was started. Both precursor mixtures would continue for 20 % of the total deposition time at which point the antimony precursor mixture was turned off. The antimony/fluorine mixed precursor was continued for the remaining 10% of the total deposition time for the 240 nm antimony film. At this point, the fluorine doped tin oxide film precursor feed was turned on. Both feeds were continued for 20% of the total time needed to deposit 300 nm of fluorine doped tin oxide. The mixed antimony/fluorine precursor feed was turned off and the fluorine doped tin precursor was continued for the remaining deposition time for the fluorine doped film. The resultant gradient coating layer is light blue in transmitted and reflected color (x=0.292, y=0.316) a SHGC = 0.50, a U value = 0.6, and a visible transmission about 45%. As shown in Figure 3, surface 22 of gradient film 16 would have essentially 100% antimony dopant while surface 18 would have essentially 100% fluorine dopant with a gradient in dopant concentration between surfaces 18 and 22 and all within a film matrix of SnO 2 . Examples 40 to 43 The procedure of Example 1 was used in Examples 40 to 43. The coating composition for the NIR layer in Examples 41 and 43 was composed of a fluorine, antimony, and tin precursor made by adding SbC13 and TFA to MBTC. This precursor contained 0-5% by weight TFA, 5.2-5.5% by weight SbCl3, and the remainder MBTC, and was co-fed with water into the second vaporizer. The carrier gas used for the second vaporizer was dry air at a rate of 15 l/min. The fluorine/antimony/tin precursor was added at a rate of 0.5 mole percent of total carrier gas flow, the water was added at a rate of 1.5 mole percent total carrier gas flow, and the vaporizer temperature was maintained at 160C. A soda-lime-silica glass substrate two inches square and 2.2 mm thick was preheated on a heater block to 605 to 625C. The heater block and substrate were then moved to a position directly beneath the vertical coater nozzle, with the substrate being 25mm beneath the coater nozzle. F/Sb/Sn/H2O vapors from the second vaporizer were then directed onto the glass substrate, depositing an antimony and fluorine doped tin oxide undercoat layer in examples 41 and 43. The velocity of the carrier gas was 0.9 m/s and the thickness of the fluorine and antimony doped tin oxide film was ∼240 nm. Reaction byproducts and unreacted precursor vapors were exhausted from the substrate at a rate of 18 l/min. After the antimony and fluorine doped tin oxide undercoat was deposited, the coater nozzle valve was switched from the second vaporizer feed to the first vaporizer feed. MBTC/TFA/H2O vapors from the first vaporizer feed were then directed onto the substrate, depositing a layer of fluorine doped tin oxide directly on top ofthe antimony/fluorine doped tin oxide undercoat. The velocity of the carrier gas was 0.9 m/s and the thickness of the fluorine doped tin oxide film was ∼300 nm. The bilayer films in examples 41 and 43 (containing both F and Sb in the NIR undercoat) were light grey in transmitted color and neutral in reflected color. Examples 40 and 42 essentially reproduce examples 40 and 43 respectively but without fluorine dopant in the NIR undercoat layer. The properties were measured and the results appear in Table 3. The results show how fluorine, as an additional dopant in the NIR layer, acts as a color modifier for both reflected and transmitted color. The transmitted colors, T vis , x and y, of the films made with the TFA and Sb dopants in the NIR layer, Examples 41 and 43, are more neutral in reflected color and greyer in transmitted color then those which only contained Sb as a dopant in the antimony doped tin oxide NIR layer in examples 40 and 42. Furthermore, the antimony doped NIR layer with a color effecting quantity of fluorine dopant has greater transmission of visible light (increase in T VIS from 54.5 to 58.5 in example 41 versus example 42 with the some level of antimony dopant). Examples 44 through 47 demonstrate the deposition of films with the following composition: TOF/TOSb (low Sb conc.)/TOSb (high Sb conc.)/Glass, TOF/TOSb (high Sb conc.)/TOSb (low Sb cone.)/Glass, TOSb (low Sb)/TOF/TOSb (high Sb conc.)/Glass, and TOSb (high Sb)/TOF/TOSb (low Sb conc.)/Glass Examples 44 The procedure of Example 1 was repeated except that the glass temperature was about 610°C and the concentration of reagents was about 0.63 mol% in air flowing at a rate of 20 liters per minute. About 400Å of antimony doped tin oxide was deposited first from a liquid coating solution composed of about 10 wt% antimony trichloride and ∼90% monobutyltin trichloride. Immediately following, a second layer of about 2000 Å of antimony doped tin oxide from a liquid coating solution composed of 3.25% antimony trichloride and 96.75% monobutlytin trichloride was deposited. A third layer composed of about 3000 Å of fluorine doped tin oxide was deposited from a solution containing 5 wt% trifluoroacetic acid and 95 wt% monobutyltin trichloride. The resulting film appeared to have a light green-blue color for reflected light and light blue color for transmitted light. The film properties were measured as described in Example 1. The visible light transmission was 64% and the SHGC was calculated to be 0.56. The x and y coordinates for the color of reflected light were 0.304 and 0.299, respectively, putting the film in the neutral-blue color quadrant of C.I.E. color space as defined earlier. Example 45 The procedure of Example 44 was repeated, but this time the TOSb layers were deposited in reverse order. The resulting film was blue-red in reflected color with color coordinates of (x) 0.330 and (y) 0.293, respectively. A visible transmission of 59% and a SHGC of 0.54 were obtained. One skilled in the art will realize that the TOSb layers can be of different thicknesses and concentrations than described herein and still be within the scope of this invention. Example 46 The procedure of Example 44 was repeated, but in this example the deposition sequence of the fluorine doped tin oxide layer and the 3.25% antimony trichloride solution layer were reversed. The resulting film had a visible transmission of about 62%, a SHGC of 0.55, and a neutral blue-red reflected color characterized by color coordinates (x) 0.311 and (y) 0.311. Example 47 The procedure of Example 45 was repeated, but in this example the deposition sequence of the fluorine doped tin oxide layer and the 10.0% antimony trichloride solution layer were reversed. The resulting film had a visible transmission of about 57%, a SHGC of 0.53, and a light green reflected color characterized by color coordinates (x) 0.308 and (y) 0.341. One skilled in the art will realize that the TOSb layers can be ofdifferent thicknesses and concentrations than described herein and still be within the scope of this invention. All SHGC and U values in the tables have been determined using the single band approach of the NFRC Window 4.1 program. Use of the more accurate multiband approach (spectral data file required) will improve the SHGC's by approximately 14%. The C.I.E. tristimulus values for the reflected and transmitted colors of the coated articles can be calculated according to ASTM Standard E 308, with Illuminant C used as the standard illuminant. From this ASTM Standard E 308, the color of an object can be specified with one of several different scales. The scale used for the coated articles in this invention is the C.I.E. 1931 chromaticity coordinates x and y. One can easily translate to the C.I.E. 1976 L*, a*, b* opponent-color scale by using the following equations: x = X/(X+Y+Z) y = Y/(X+Y+Z) L* = 116(Y/Y n ) 1/3 -16 a* = 500[(X/X n ) 1/3 -(Y/Y n ) 1/3 ] b* = 200[(Y/Y n ) 1/3 -(Z/Z n ) 1/3 ] where X, Y, and Z are the C.I.E. tristimulus values of the coated article, and X n , Y n , and Z n , are 98.074, 100.000, and 118.232, respectively, for Standard Illuminant C. from the L*, a*, b* values, the color saturation index, c*, can be calculated by the equation c*=[(a*) 2 + (b*) 2 ] 1/2 . A color saturation index of 12 or less is considered neutral. The definition of Neutral-blue Color for reflected light, i.e. coated glass having reflected light predominately within C.I.E. chromaticity coordinates values of x between 0.285 and 0.310 and y between 0.295 and 0.325 as shown in Figure 7 by a box labeled Neutral-blue Color correlates with C.I.E. 1976 L*, a*, b* of 37.85, -1.25, -5.9 and 39.62, -2.25, 1.5. A sample conversion follows: Example 40 (Table 3) 5.5 % SbCl 3 300/240 (F/Sb/Glass) X = 9.797 Y = 9.404 Z = 12.438 x = 0.310 y = 0.297 L* = 36.751 a* = 4.624 b* = -3.466 c* = 5.778 Solar control properties of glass windows has been evaluated and rated by the United States of America, Environmental Protection Agency using an Energy Star rating system. An Energy Star rating for the Central Region of the United States requires a U-factor rating of 0.40 or lower and a SHGC rating of 0.55 or below. An Energy Star rating for the Southern Region of the United States requires a U-factor rating of 0.75 or lower and a SHGC rating of 0.40 or below. Coated glass having the NIR and Low E coatings proposed herein when incorporated into windows of convention design may achieve the Energy Star ratings for the Central and/or Southern Region. For example a Vertical slider design window 3 feet wide by 4 feet high and having a frame absorption value of 0.5 as rated by the National Fenestration Rating Council (NFRC) and assembled with coated solar control glass of the present invention having a NIR film and a low E film within the preferred ranges for a Neutral-Blue Color achieves a SHGC of less than 0.40 and a U value of less than 0.64 for a monolith glass construction with a frame U-value of 0.7 or less and achieves a SHGC of less than 0.3 8 and a U value of less than 0.48 for an Insulated Glass Unit (IGU) construction made up with 2.5 mm clear lite, 0.5 inch air gap and NIR and Low e coatings on the #2 surface of the outer lite and a frame U-value of 1.0 or less. The examples substantiate that with a minimum of two doped SnO 2 layers, an excellent solar control coated glass can be produced having a preselected reflected color . Tables 1, 2 and 3 present the data while Figures 5 and 6 show graphically how the solar properties of the coated glass vary with dopant concentrations and film thickness primarily of the NIR film. Figure 7 plots the x and y C.I.E. chromaticity coordinates of a representative selection of coated glass of examples 1 to 39. As seen in Figure 7, specific combinations of film thicknesses for both the NIR and low emissivity films and specific dopant(s) concentrations can be utilized to produce a coated, solar control glass with any desired color for light reflected off the coated surface of the glass, such as red, green, yellow, blue and shades thereof or Neutral-blue Color. It is particularly surprising that a Neutral-blue Color can be achieved with a NIR and a low emissivity layers but without an anti-iridescence layer such as taught by Gordon. While the invention may be embodied with only two layers, a NIR layer and a low emissivity layer, multilayer embodiments are within the scope and content of the invention. The multilayers can be additional NIR and/or low emissivity layers or other functional or decorative layers. Multilayer embodiments include TOSb/TOF/TOSb/Glass, or TO/TOF/TOSb/Glass, or TO/TOSb/TOF/Glass with TO being just a tin oxide film. When multiple NIR or low emissivity layers are used, the dopant concentrations or dopant selection in each NIR or low emissivity film need not be the same. For example when two NIR layers are used in combination with at least one low emissivity layer, one NIR layer can have a low level of antimony dopant (e.g. 2.5%) to give some reflectance in the mid IR range and one layer can have a higher level (≥ 5%) to give NIR absorbency. The terms layer and film are generally used herein interchangeably except in the discussion ofgradient film depicted in Figure 3 in which a portion of the film is referred to as a layer having a dopant concentration different than the dopant concentration in another layer of the film. In the method of making the coated glass of the present invention as demonstrated in the examples, the glass is contacted sequentially with carrier gas containing precursors. Accordingly, the glass may have a coating on it when it is contacted a second time with a carrier gas containing precursors. Therefore, the term "contacting glass" refers to either direct contact or contact with one or more coatings previously deposited on the glass. Another embodiment of the invention provides the ability to change the transmitted color of the coated glass. Transmitted color refers to the color perceived by a viewer on the opposite side of the coated glass then the source of light being viewed while reflected color is the color perceived by a viewer on the same side as the source of light being viewed. Transmitted light can be effected by adding additional dopants to the NIR film. As previously explained, the NIR layer contains a dopant selected from the group consisting of antimony, tungsten, vanadium, iron, chromium, molybdenum, niobium, cobalt and nickel. The color of transmitted light through the NIR layer can be changed by adding an additional dopant different then the first dopant in the NIR layer and selected from the group consisting of tungsten, vanadium, iron, chromium, molybdenum, niobium, cobalt, nickel, and fluorine or a combination ofmore then one additional dopant to the NIR layer. As shown in examples 40-43, the addition of a fluorine precursor, such as trifluoroacetic acid (TFA) to a NIR precursor solution such as SbCl 3 /MBTC, produces a film containing fluorine as an additional dopant in the NIR layer of antimony doped tin oxide. When fluorine is present as an additional dopant in an antimony doped tin oxide layer, the transmitted color is gray versus a blue transmitted color for an antimony doped tin oxide layer without fluorine dopant. The additional dopant has little or no effect on reflected light and accordingly, a coated glass can be produced having a reflected light that is different then its transmitted light. Dopants in the NIR layer such as vanadium , nickel, chromium and non-traditional color additives such as trifluoroacetic acid (TFA) and HCl can be added to the TO:Sb precursors in 1-5 wt% (based on the total wt of precursor and additive) to effect transmitted color changes in the final film construction while not significantly affecting overall reflected color neutrality. Summary of Properties of Bilayer Films TOSb/TOF # 31 32 33 34 35 36 37 38 Composit. Sb/F/G Sb/F/G Sb/F/G Sb/F/G Sb/F/G Sb/F/G Sb/F/G Sb/F/G %Sb 5.6 5.6 5.6 5.6 5.6 5.6 5.6 5.6 Thick. nm 240/300 160/300 138/300 120/300 110/300 80/300 120/332 120/262 %Asol 47.9 36.1 29.2 27.2 25.6 23.5 28.5 26.8 %Tsol 45.9 55.5 61.1 63.3 64.3 65.8 62.5 63.4 %Rsol,1 6.1 8.3 9.7 9.6 10.2 10.7 9.0 9.8 %Rsol,2 8.2 9.3 10.1 9.5 9.2 9.2 9.2 9.6 %Tvis 53.2 63.2 67.2 69.0 69.5 71.8 69.0 68.1 %Rvis,1 6.1 7.6 9.3 9.1 10.1 10.9 7.8 9.9 %Rvis,2 7.6 8.9 10.7 10.4 10.5 10.9 8.9 11.6 %Tuv 38.5 43.4 47.0 48.7 49.2 49.1 47.7 49.6 S. R, 14.7 15.9 16.5 17.4 18.8 17.3 15 21.1 Emis-cal 0.14 0.15 0.15 0.16 0.17 0.16 0.14 0.19 SHGCc 0.54 0.61 0.66 0.68 0.69 0.7 0.67 0.68 " IG 0.45 0.53 0.58 0.6 0.61 0.62 0.59 0.6 Uc 0.73 0.74 0.74 0.74 0.75 0.74 0.73 0.76 " IG 0.28 0.28 0.29 0.29 0.29 0.29 0.28 0.3 Tvis-c 0.53 0.63 0.67 0.69 0.69 0.72 0.69 0.68 " IG 0.48 0.57 0.61 0.63 0.63 0.65 0.63 0.62 x 0.289 0.309 0.310 0.311 0.313 0.302 0.306 0.292 y 0.300 0.283 0.274 0.275 0.306 0.364 0.281 0.349 %Rvis 6.2 7.7 9.3 9.1 10.1 10.9 7.8 9.9 R Colors Blue Blue-Neu Blue-Gr Blue-Gr Neutral Greeen Blue-Neu Green Explanation key for Tables 1 and 2: Composit. F/Sb/G=Fluorine doped tin oxide/Antimony doped tin oxide/Glass Sb/F/G=Antimony doped tin oxide/Fluorine doped tin oxide/Glass %Sb % SbCl 3 (antimony trichloride) by weight in MBTC (monobutyltin trichloride) Thick. nm Profilometer measurement of individual TO:F (fluorine doped tin oxide) and TO:Sb (antimony doped tin oxide) films %Asol % solar absorbance 1 from film side of glass (= 100-(%Tsol+%Rsol, 1)) - 300-2500 nm %Tsol % solar transmission 1 from the film side of glass - 300-2500 nm %Rsol,1 % solar reflection 1 from film side of glass - 300-2500 nm %Rsol, 2 % solar reflection 1 from back side of glass - 300-2500 nm %Tvis % transmission 1 in the visible region of spectrum from film side of glass - 380-780 nm S.R. Sheet resistance as measured on a Alessi 4-point probe Emis. Cal Emissivity calculated from measured sheet resistance (= 1-(1+0.0053*S.R.) 2 ) SHGCc Solar heat gain coefficient 2 for center of glass/single pane "IG Solar heat gain coefficient 2 for center of glass in an IGU 3 Uc Total heat transfer coefficient 2 for center of glass/single pane "IG Total heat transfer coefficient 2 for center of glass in an IGU 3 Tvis-c transmission 1 in the visible region of spectrum center of glass/single pane - 380-780 nm "IG transmission 1 in the visible region of spectrum center of glass in an IGU 3 - 380-780 nm x,y color coordinates calculated from %Rvis according to ASTM E308-96, Illuminant C, 1931 Observer, 10 nm interval (Table 5.5) - 380-770 nm %Rvis % reflection 1 in the visible region of the spectrum from film side of glass - 380-770 nm Summary of Properties of Bilayer Films TOSb/TOF 40 41 42 43 Composit. F/Sb/G F/Sb-F/G F/Sb/G F/Sb-F/G %SbCl3 5.5 5.2 5.2 5.36 %TFA(under) 0 5 0 2.5 Thick. nm 300/240 300/240 300/240 300/240 %Asol 45.5 35.7 41.8 39.1 %Tsol 45.0 54.2 48.2 50.6 %Rsol,1 9.5 10.1 10.0 10.3 %Rsol,2 8.0 8.9 8.4 8.7 %Tvis 50.9 58.5 54.5 55.6 %Rvis,1 9.4 10.1 10.4 10.3 %Rvis,2 8.0 9.0 8.5 9.0 %Tuv 40.1 41.1 41.6 39.8 S. R, 11.9 13.7 11.8 12.5 Emis-cal 0.12 0.13 0.11 0.12 SHGCc 0.53 0.60 0.55 0.57 " IG 0.45 0.52 0.47 0.49 Uc 0.72 0.73 0.72 0.72 " IG 0.27 0.28 0.27 0.27 Tvis-c 0.51 0.59 0.55 0.56 " IG 0.46 0.53 0.50 0.51 R1 x 0.310 0.297 0.302 0.303 R1 y 0.297 0.313 0.299 0.307 %Rvis 9.4 10.1 10.4 10.3 Tvis x 0.295 0.308 0.297 0.304 Tvis y 0.308 0.315 0.310 0.314

Claims: A coated, solar control glass of preselected reflected colour, having an anti-iridescent SnO 2 coating containing at least two layers, one layer being a NIR solar absorbing layer comprising SnO 2 containing a dopant selected from antimony, tungsten, vanadium, iron, chromium, molybdenum, niobium, cobalt, nickel and mixtures thereof, and another layer being a low emissivity layer comprising SnO 2 containing fluorine and/or phosphorus dopant, wherein the thickness of the NIR solar absorbing layer is from 80 to 300 nm, the thickness of the low emissivity layer is from 200 to 450 nm, and the reflectance of visible light from the SnO 2 coating is at least 6.2%. The glass of claim 1 wherein the SnO 2 coating is in direct contact with the glass. The glass of claim 1 wherein the thickness of the NIR solar absorbing layer is from 200 to 280 nanometers (nm) and the thickness of the low emissivity layer is from 250 to 350 nm. A coated, solar control glass of predetermined reflected colour having a SnO 2 film in direct contact with the glass containing at least two dopants, where there is a difference in the concentration of the dopants from one surface of the film to the opposite surface of the film, a first dopant being selected from antimony, tungsten, vanadium, iron, chromium, molybdenum, niobium, cobalt, nickel and mixtures thereof, and a second dopant being fluorine or phosphorus, said first dopant comprising at least 50% of the dopants present at a first surface of said SnO 2 film to form a NIR solar absorbing layer within said SnO 2 film adjacent to said first surface, and said second dopant being present at a concentration of at least 50% of the dopant at a second surface of said film opposite said first surface to form a low emissivity layer within said SnO 2 film adjacent to said second surface. The coated, solar control glass of claim 4 wherein said first dopant comprises at least 75% of the dopants present in said SnO 2 film in a volume of the film commencing with said first surface and continuing into the SnO 2 film for a depth of at least 80 nm, and said second dopant comprises at least 75% of the dopants present in said SnO 2 film in a volume of the film commencing with said second surface and continuing into the SnO 2 film to a depth of at least 80 nm, wherein said area of said SnO 2 film having at least 75% of said second dopant functions as a low emissivity layer and said area of said SnO 2 film having at least 75% of said first dopant functions as a NIR solar absorbing layer. The coated, solar control glass of claim 1 wherein said solar absorbing layer has a thickness from 220 to 260 nm and a dopant concentration of from 2.5 % to 7 % by weight based upon the weight of SnO 2 in said solar absorbing layer; the low emissivity layer has a thickness of from 280 to 320 nm and a fluorine dopant concentration of from 1% to 5% by weight based upon the weight of SnO 2 in said low emissivity layer; and the coated glass has a Neutral-blue Color for reflected light. The glass of claim 1 wherein the solar absorbing layer is SnO 2 having an antimony dopant within the range of 3% to 6% by weight based upon the weight of SnO 2 tin oxide in the solar absorbing layer; the low emissivity control layer is SnO 2 having a fluorine dopant within range of 1% to 3% dopant by weight based upon the weight of SnO 2 in the low emissivity layer; and the improved glass has a Neutral-blue Color for reflected light. The glass ofclaim 1 wherein the solar absorbing layer is coated directly onto the glass and the low emissivity layer is coated on top of the solar control layer. The coated solar control glass of any one of claims 1 to 5 wherein the preselected reflected color is red. The coated solar control glass of any one of claims 1 to 5 wherein the preselected reflected color is yellow. The coated solar control glass of any one of claims 1 to 5 wherein the preselected reflected color is green. The coated solar control glass of any one of claims 1 to 5 wherein the preselected reflected color is blue. The coated solar control glass of any one of claims 1 to 5 wherein the preselected reflected color is Neutral-blue Color. A coated, solar control glass of preselected reflected colour, having an anti-iridescent SnO 2 coating containing at least two dopants, a first dopant selected from antimony, tungsten, vanadium, iron, chromium, molybdenum, niobium, cobalt, nickel and mixtures thereof, and a second dopant of fluorine and/or phosphorus, wherein the first dopant is at a higher concentration than the second dopant at a first surface of the film; the first dopant is at a lower concentration than the second dopant at a second surface of the film, opposite said first surface; the portion of film in proximity with the first surface functions as a NIR solar absorbing layer within the SnO 2 coating; the portion of film in proximity with the second surface functions as a low emissivity layer within the SnO 2 coating; and the reflectance of visible light from the SnO 2 coating is at least 6.2%. The coated glass of claim 1 wherein the dopant for the solar absorbing layer is antimony. The coated glass of claim 15 wherein the antimony dopant is obtained from a precursor containing antimony trichloride, antimony pentachloride, antimony triacetate, antimony triethoxide, antimony trifluoride, antimony pentafluoride, or antimony acetylacetonate. The coated glass of claim 1 wherein the dopant for the low emissivity layer is fluorine The coated glass of claim 17 wherein the fluorine dopant is obtained from a precursor containing trifluoroacetic acid, difluoroacetic acid, monofluoroacetic acid, ethyltrifluoroacetate, ammonium fluoride, ammonium bifluoride, or hydrofluoric acid. The coated glass ofclaim 1 wherein each of the SnO 2 layers is obtained by pyrolytic decomposition of a tin precursor. The coated glass of claim 19 wherein the tin precursor is selected from monobutyltin trichloride, methyltin trichloride, dimethyltin dichloride, dibutyltin diacetate, and tin tetrachloride. The coated glass of claim 1 wherein the solar absorbing layer is composed of at least two solar absorbing films and the total thickness of the solar absorbing films is from 80 to 320 nm. The coated glass of claim 21 wherein the concentration ofdopant in one of said solar absorbing films is different than the concentration of dopant in another of the solar absorbing films. The coated glass of claim 1 wherein the low emissivity layer is composed of at least two low emissivity films and the total thickness of the low emissivity films is from 200 to 450 nm. The coated glass of claim 23 wherein the concentration of dopant in one of said low emissivity films is different from the concentration of dopant in another of the low emissivity films. The coated glass of claim 1 further comprising a transmitted color modifying quantity of a dopant in said solar absorbing layer. The coated glass of claim 25 wherein said color modifying dopant is fluorine or chlorine. The coated glass of claim 1 further comprising chlorine as a dopant in said solar absorbing layer. A method of producing the coated glass of claim 1 comprising sequentially treating glass at a glass temperature above 400° C. with: a first carrier gas containing a source of oxygen, H 2 O, a tin precursor and a dopant precursor selected from antimony trichloride, antimony pentachloride, antimony triacetate, antimony triethoxide, antimony trifluoride, antimony pentafluoride, or antimony acetylacetonate; and, a second carrier gas containing a source of oxygen, H 2 O, a tin precursor and a dopant precursor selected from trifluoroacetic acid, ethyltrifluoroacetate, difluoroacetic acid, monofluoroacetic acid, ammonium fluoride, ammonium bifluoride, and hydrofluoric acid; to form by pyrolysis a NIR solar absorbing layer comprising SnO 2 containing an antimony dopant and a low emissivity layer comprising SnO 2 containing a fluorine dopant. A method of producing the coated glass of claim 1 comprising sequentially treating glass at a glass temperature above 400° C. with: a first carrier gas containing a source of oxygen, H 2 O, an organotin precursor and a dopant precursor containing a metal selected from antimony, tungsten, vanadium, iron, chromium, molybdenum, niobium, cobalt, and nickel, and, a second carrier gas containing a source of oxygen, H 2 O, an organotin precursor and a dopant precursor containing fluorine or phosphorus; to form by pyrolysis a NIR solar absorbing layer comprising SnO 2 containing an antimony, tungsten, vanadium, iron, chromium, molybdenum, niobium, cobalt, or nickel dopant or mixture ofdopants and a low emissivity layer comprising SnO 2 containing a fluorine or phosphorus dopant. The method of claim 28 or 29 wherein said glass is contacted with the first carrier gas before it is contacted with the second carrier gas. The method of claim 28 or 29 wherein said first carrier glass also contains the components of said second carrier gas to produce a product in which the NIR solar absorbing layer contains a fluorine or phosphorus dopant in addition to the dopant of antimony, tungsten, vanadium, iron, chromium, molybdenum, niobium, cobalt, or nickel. The method of claim 28 or 29 further wherein said first carrier gas also contains a dopant precursor containing fluorine, chlorine or phosphorous. The method of claim 32 wherein said dopant precursor containing fluorine, chlorine or phosphorous is either trifluoroacetic acid, HCI, or phosphorous trichloride. The method of claim 28 or 29 further wherein said first carrier gas also contains a film modifier selected from the dopant precursor containing fluorine or phosphorous. The product produced by the process of any one of claims 28 to 34 The coated glass of claim 1 further comprising fluorine dopant in said NIR solar absorbing layer and wherein the reflected color of said glass is different from the transmitted color. The coated glass of claim 36 wherein the reflected color is Neutral Blue Color and the transmitted color is blue. The method of claim 28 or 29 wherein said first carrier gas also contains a second dopant precursor containing fluorine or phosphorus or a second dopant precursor containing a metal selected from antimony, tungsten, vanadium, iron, chromium, molybdenum, niobium, cobalt, and nickel. The method of claim 38 wherein said second dopant precursor is selected from trifluoroacetic acid, ethyltrifluoroacetate, difluoroacetic acid, monofluoroacetic acid, ammonium fluoride, ammonium bifluoride, and hydrofluoric acid. The product produced by the process of claim 38 or claim 39. A NIR film comprising tin oxide containing a NIR dopant selected from antimony, tungsten, vanadium, iron, chromium, molybdenum, niobium, cobalt, and nickel and containing a fluorine dopant at an atomic concentration less then the concentration of the NIR dopant . The film of claim 41 wherein the fluorine dopant is present in a quantity sufficient to modify the transmitted color of light through the film. A NIR film comprising tin oxide containing a NIR dopant selected from antimony, tungsten, vanadium, iron, chromium, molybdenum, niobium, cobalt, and nickel and containing a color modifying dopant present in a quantity sufficient to modify the transmitted color of light through the film and selected from antimony, tungsten, vanadium, iron, chromium, molybdenum, niobium, cobalt, nickel and fluorine, provided that the selection ofcolor modifying dopant is different then the selection ofNIR dopant and when fluorine is the selected dopant its atomic concentration is less then the concentration of the NIR dopant. A coated, solar control glass having Neutral-blue Color for reflected light and having a NIR solar absorbing layer and a low emissivity layer, comprising glass having a coating containing at least two layers with one layer being a solar absorbing layer comprising SnO 2 containing a dopant selected from the group consisting of antimony, tungsten, vanadium, iron, chromium, molybdenum, niobium, cobalt, nickel and mixtures thereof and another layer being a low emissivity layer comprising SnO 2 containing a dopant selected from the group fluorine or phosphorus. A coated, solar control glass having a color intensity index of 12 or less for reflected light and having a NIR solar absorbing layer and a low emissivity layer, comprising glass having a coating containing at least two layers with one layer being a solar absorbing layer comprising SnO 2 containing a dopant selected from the group consisting of antimony, tungsten, vanadium, iron, chromium, molybdenum, niobium, cobalt, nickel and mixtures thereof and another layer being a low emissivity layer comprising SnO 2 containing a dopant selected from the group fluorine or phosphorus A coated, solar control glass having C.I.E. 1931 color coordinates x between about 0.285 and 0.310 and y between about 0.295 and 0.325 for reflected light and having a NIR solar absorbing layer and a low emissivity layer, comprising glass having two layers coated thereon with one layer being a solar absorbing layer comprising SnO 2 containing a dopant selected from the group consisting of antimony, tungsten, vanadium, iron, chromium, molybdenum, niobium, cobalt, nickel and mixtures thereof and a second layer being a low emissivity layer comprising SnO 2 containing a dopant selected from the group fluorine or phosphorus. A coated, solar control glass having a C.I.E. 1931 color coordinates x between about 0.285 and 0.325 and y between about 0.295 and 0.33 for reflected light and having a NIR solar absorbing layer and a low emissivity layer, comprising glass having at least two layers coated thereon, with one layer being a solar absorbing layer comprising SnO 2 containing a dopant selected from the group consisting of antimony, tungsten, vanadium, iron, chromium, molybdenum, niobium, cobalt, nickel and mixtures thereof a second layer being a low emissivity layer comprising SnO 2 containing a dopant selected from the group fluorine or phosphorus

Inventors: MCKOWN CLEM STEFFLER, ROGER CHRISTOPHE, RUSSO DAVID ALAN, STRICKER JEFFREY LEE, MCKOWN, CLEM STEFFLER, ROGER, CHRISTOPHE, RUSSO, DAVID ALAN, STRICKER, JEFFREY LEE
Applicants: ATOFINA CHEM INC, ATOFINA CHEMICALS, INC.
Application year: 1999
Main classification: C03C17
IPC codes: C03C17, G02B5, B32B17