BACKGROUND OF THE INVENTION

1. Field of the Invention

The present invention concerns a controllable electrochromic indicator device consisting of an electrochromic layer and an adjacent charge-carrier-passing insulating layer located between two electrodes with at least one of the two electrodes attached to a supporting plate and at least one of the electrodes being transparent.

2. Description of the Prior Art

Such indicator devices are already known from U.S. Pat. No. 3,521,941. A particular embodiment is shown in FIG. 1. On a supporting plate 1, e.g., of glass or another transparent material, there are deposited in succession thin layers of tin oxide (SnO₂) as a transparent electrode 2, molybdenum oxide (MoO₃) as an electrochromic substance 3, silicon oxide (SiO) as a charge-carrier-passing insulator 4 and gold (Au) as the second electrode 5. A voltage AB of about 6V with the proper polarity applied to the electrodes 2, 5, the thickness of the charge-carrier-passing insulating layer 4 being about 0.2 μ and that of the electrochromic layer being about 1 μ, produces a blue coloration of the previously almost colorless indicator device after about 30 seconds. The color fades away about 15 seconds after reversal of the polarity of the voltage.

The charge carrier transmitting insulation layer 4 on the one hand is to prevent a short circuit between electrodes 2 and 5, but on the other hand it is also to supply a sufficient flow of charge carriers to the electrochromic layer 3. A satisfactory number of charge carriers pass through the insulating layer 4 only at very high field strengths, so as to produce coloration of the electrochromic layer 3. Since the speed of coloration and thus the response time of the device is determined by the number of charge carriers reaching the electrochromic layer per unit time and the field strength cannot be made arbitrarily high, such indicator devices exhibit a slow response and must always be operated at high field strengths, i.e., at relatively high voltages and very small thicknesses of the charge-carrier-transmitting layer 4. Moreover, electrolytic deposits form on the electrodes of such indicator devices in the course of time, thus shortening the lifetime of the electrochromic cell.

SUMMARY OF THE INVENTION

It is an aim of the invention, therefore, to develop a controllable electrochromic indicator device distinguished by a high time resolution even at low field strengths, endowed at the same time, however, with a high life expectancy through reversible coloration of the electrochromic layer and suitable configuration.

The aforementioned aim is attained in accordance with the invention by making the charge-carrier-passing insulation layer a good ion conductor with almost complete blockage against the passage of electrons, and by providing at least one non-polarizable electrode, preferably disposed next to the ion conductor.

With the use of good ion conductors as the charge-carrier-transmitting insulating layer, the color-producing ions pass out of the ion conductor into the electrochromic layer in sufficient quantity even with the application of a small voltage. The thickness of the ion-conducting layer is no longer so critical and can now be up to 30μ instead of 0.2μ. Along with easier fabrication of the indicator device, significantly improved insulation between the electrodes is attained, since the insulating inter-layer is thicker and exhibits none of the "patchiness" of thin films. By the inclusion of a non-polarizable electrode, deposits occurring at the electrodes of a state-of-the-art indicator device are avoided since, e.g., cationic secondary reactions produced at the junction of the cathode and the charge-carrier-transmitting insulation layer in which metals may be deposited are suppressed.

Particularly suitable for non-polarizable electrodes is a mixed ion-electron-conductor, e.g., a tungsten and/or molybdenum bronze with the composition M_x Y, where 0 < X < 1 and M = alkali-alkaline earth metals, Cu, Ag, NH₄ or H and Y = WO₃, MoO₃ and WO₃ /MoO₃, since in such a device reactive cations leaving the ion conductor are absorbed by the cathode and incorporated in the molecular structure of the bronze. In this way contact surface reactions of the cations with water or oxygen and thus the accumulation of troublesome deposits are avoided.

The foregoing and other objects are attained in accordance with one aspect of the present invention through the provision of a controllable electrochromic indicator device comprising: two electrodes, an electrochromic layer and an adjacent charge-carrier-transmitting insulator layer situated between the two electrodes, at least one of the electrodes being deposited on a supporting plate and at least one of the electrodes being transparent, the charge-carrier-transmitting insulator layer being a good ion conductor and functioning to almost completely block the flow of electrons, and at least one of the electrodes being non-polarizable and disposed in contact with the ion conductor.

BRIEF DESCRIPTION OF THE DRAWINGS

Various objects, features and attendant advantages of the present invention will be more fully appreciated as the same becomes better understood from the following detailed description of the present invention when considered in connection with the accompanying drawings in which:

FIG. 1 is a section through a state-of-the-art electrochromic indicator device, and

FIG. 2 is a section through an electrochromic indicator device conforming to the invention.

DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS

Referring now to the drawings, wherein like reference numerals designate identical or corresponding parts throughout the several views, and more particularly to FIG. 2 thereof, in FIG. 2 are shown applied to a supporting plate 1, and referenced by numbers 2, 3, 5, 6 and 7, layers of tin oxide (SnO₂)2, tungsten trioxide (WO₃)3, silver iodide (AgI) 5, tungsten trioxide (WO₃) 6 and gold 7. The supporting plate 1 is preferably of glass, but any other transparent material, e.g., plastic, could be used. The tin dioxide layer 2 deposited on the glass plate 1 is transparent and serves as an electrode. The first electrochromic film 3 of WO₃ is evaporated on in a high vacuum of about 10^{- 6} Torr. from a platinum-alloy boat electrically heated to about 300°C and it has a thickness of about 5μ. The ion-conducting silver iodide layer 5 of about 5μ thickness, in contrast, is evaporated onto the tungsten trioxide film at room temperature. Its film thickness is not very critical and can amount to as much as 50μ. The adjoining second electrochromic layer 6 is applied at room temperature and has the same thickness as the film 2. The final layer 7 of gold is about 1μ thick and provides the connection between the terminal A of a D.C. voltage source of about 3 V and the electrochromic layer 6 functioning as an electrode. The other terminal B of the D.C. voltage source is connected to the electrode 2.

If electrode 6 is at a positive potential, the WO₃ -layer 3 turns blue after about 5 seconds. An explanation of this phenomenon is probably that the silver ions Ag+ are formed in sufficient quantity in the silver iodide layer by the electric field and carried into the tungsten trioxide layer 3. Since charge neutrality must be maintained in the layers of the indicator device, electrons are supplied to the electrochromic layer 3 by the cathode 2 which causes a reduction of silver ions and tungsten trioxide to blue tungsten bronze. The excess negative charge carriers of the ion-conducting silver iodide layer 5 are drawn off by the WO₃ -layer 6 acting as anode. The tungsten bronze Ag_x WO₃, formed in the layer 3 exhibits various degrees of blue coloration for all x-values between 0 and 0.3, with bronzes of small x-values giving only a slight coloration to the initially colorless tungsten trioxide. The blue color is readily visible through the glass plate 1 and the tin dioxide electrode 2.

When the polarity of the voltage is reversed the coloring of the tungsten trioxide layer 3 disappears again in about 5 seconds. This process is most likely attributable to the formation of sufficient silver ions in the ion-conducting silver iodide film 5 and their transport into the tungsten trioxide layer 6. Thus, a gradient in the concentration of silver ions in the silver iodide layer develops so that silver ions diffuse through the ion-conducting layer 5 from the silver-rich region next to the electrochromic layer 3 to the silver-poor one next to the electrochromic layer 6. The surface of the silver iodide film 5 next to the electrochromic layer 3 now has too low a concentration of silver ions, so that silver ions diffuse into this region from layer 3. These ions are formed by oxidation of the tungsten bronze at the tin dioxide anode 2, and are continuously removed from the electrochromic layer 3 by reason of the electric field and the silver ion deficit in the contact surface of the ion conductor, so that the coloration almost completely disappears and only the yellowish silver iodide surface is visible. Of course, the electrochromic film 6 turns blue while the film 3 is losing its coloration, but this cannot be detected by an observer, since only the yellowish silver iodide film 5 is visible through the transparent bleached tungsten trioxide film 3.

Such a cell works reversibly and is still usable after several weeks' operation, since no elementary silver is deposited and thus short circuiting as well as discoloration and color suppression are avoided. It is most important for satisfactory operation of the cell that layer 5 be the best possible ion conductor, e.g., with a specific conductivity between 10^{- 1} and 10^{- 10} Ω ^{- 1} cm^{- 1}, and that it block the passage of electrons almost completely, thereby permitting a sufficiently high electric field to be established. Such a cell with a display area of about 0.1 cm² in the above-described example draws about 300μ A.

Together with silver iodide all the other ion-conducting crystals like β -alumina are candidates for the ion conductor, especially those which do not diffuse the ions Li⁺, Na⁺, K⁺, Rb⁺, Cs⁺, Be^{+ +}, Mg^{+ +}, Ca^{+ +}, Ba^{+ +}, Sr^{+ +}, H⁺, NH₄ ⁺, Cu⁺ or Ag⁺ into an electrochromic layer, e.g. LiCl, CuBr, CuI and Rb₄ AgI₅. Also very suitable are glasses with high ionic conductivity such as SiO₂ --B₂ O₃ glasses. Thus according to K. Otto, Physics and Chemistry of Glasses 7/1966/29, the ionic conductivity of a glass with the composition 25Li₂ O + 50 SiO₂ + 25 B₂ O₃ is between 10^{- 4} and 2 × 10^{- 4} Ω^{- 1} cm^{- 1} at room temperature and that of a glass with the composition 35 Li₂ O + 28 Li₂ SO₄ + 7(LiCl)₂ + 4SiO₂ + 26B₂ O₃ is about 5 - 10 × 10^{- 3} Ω^{- 1} cm^{- 1}. The advantages of such glasses over the crystalline ion conductors are above all that very thin but defect-free layers can be produced by cathodic sputtering or even by simple screen-print enameling techniques and that their ionic conductivity is not significantly impaired by random structural characteristics, such as occur in the production techniques for thin films, since they are already amorphous or polycrystalline. In addition such glasses give the indicator device a long life expectancy since, on account of their amorpous or polycrystalline structure, a structural change is hardly to be feared even with very frequent charge/discharge cycles. Ion conducting polymers, like perfluorated sulfonic acid, are also suitable ion conductors.

Satisfactory electrochromic materials, besides tungsten trioxide, are all oxides and oxide mixtures of the metals manganese, molybdenum, niobium, palladium, platinum, rhenium, titanium vanadium and tungsten, particularly MoO₃ and WO₃.

For use as non-polarizable electrodes there are the bronzes of the composition MxY where M = Li, Na, K, Rb, Cs, Be, Mg, Ca, Ba, Sr, H, NH₄, Cu and Ag, Y = WO₃ MoO₃ and WO₃ /MoO₃ and x lies between 0 and 1; further, hydrogen-bearing palladium and platinum, as well as graphite-alkali metal alloys like CNa_x with x < 0.1, and sulfides and selenides of silver and tungsten, like Ag₂ S, Ag₂ Se, WS₂ and WSe₂ with a slight alkali admixture are quite suited. Such bronzes furnish both ions and electrons and, at small x-values, change color or effect color changes in unbronzed electrochromic layers. At high x-values they contribute to a good color contrast with transparent ion conductors. If for electrode 6 opposite the observer something like Li_x WO₃ is used, with x ≈ 0.7 - 0.85, and for the ion conductor a transparent ion conducting glass, like SiO₂ -- B₂ O.sub. 3, is used then, with bleached front electrochromic layer 3, the gold-yellow color of the background is visible, which presents a sharp color contrast to the blue-green color of a partially decolorized electrochromic layer 3.

Obviously, numerous modifications and variations of the present invention are possible in light of the above teachings. It is therefore to be understood that within the scope of the appended claims the invention may be practiced otherwise than as specifically described herein.