Solid dielectric capacitor and method of manufacture

BACKGROUND OF THE INVENTION
Our invention relates to solid dielectric capacitors and more particularly to a monolithic ceramic capacitor comprising a single or multiple layered ceramic body and at least two electrodes in contact therewith. The invention also pertains to a method of fabrication of such capacitors.
Multilayered ceramic capacitors have long been known and used extensively which employ noble metals such as platinum and palladium as the electrode materials. Generally, for the fabrication of such capacitors, "green" (unsintered) dielectric sheets have first been prepared from the proportioned ingredients of a desired dielectric ceramic material in finely divided form. An electroconductive paste containing powdered platinum or palladium has then been "printed" on the green sheets in a desired pattern. Then a plurality of such printed green sheets have been stacked up, pressed together, and sintered in a temperature range of 1300 degrees to 1600 degrees C. in an oxidative atmosphere.
This conventional method makes possible the simultaneous firing (cosintering) of the dielectric ceramic layers and the film electrodes interleaved therewith. It is also an acknowledged advantage of this known method that the noble metal electrodes are totally unaffected by the high temperature sintering in an oxidative atmosphere. Offsetting all such advantages is the expensiveness of the noble metals, which add substantially to the manufacturing costs of the multilayered ceramic capacitors.
Wada et al. U.S. Pat. No. 4,610,969, assigned to the assignee of the instant application, suggests a solution to the above problem. It teaches dielectric ceramic compositions consisting of a major ingredient expressed by the formula, (Ba.sub.k-x M.sub.x)O.sub.k TiO.sub.2, where M is at least either of magnesium (Mg) and zinc (Zn), and additives consisting of lithium oxide (Li.sub.2 O) and silicon dioxide (SiO.sub.2). The compositions may, or may not, additionally include at least one metal oxide selected from among barium oxide (BaO), calcium oxide (CaO) and strontium oxide (SrO).
Another solution is found in Wada et al. U.S. Pat. No. 4,610,970, which proposes ceramic compositions whose major ingredient is expressed by the formula, (Ba.sub.k-x-y M.sub.x L.sub.y)O.sub.k TiO.sub.2, where M is at least either of Mg and Zn, and L is at least either of Sr and Ca. To this major ingredient are added Li.sub.2 O, SiO.sub.2 and, optionally, at least one other metal oxide selected from among BaO, CaO and SrO.
Wada et al. U.S. Pat. No. 4,610,971 suggests still another solution, teaching use of a major ingredient expressed by the formula, (Ba.sub.k-x M.sub.x)O.sub.x TiO.sub.2, where M is at least one of Mg, Zn, Sr and Ca. This major ingredient is admixed with boric oxide (B.sub.2 O.sub.3), SiO.sub.2 and, optionally, at least one other metal oxide selected from among BaO, MgO, ZnO, Sro and CaO.
A further solution is found in Wada et al. U.S. Pat. No. 4,610,968, which proposes ceramic compositions including a major ingredient expressed by the formula, (Ba.sub.k-x M.sub.x)O.sub.x TiO.sub.2, where M is at least one of Mg, Zn, Sr and Ca. This major ingredient is admixed with B.sub.2 O.sub.3 and at least one metal oxide selected from among BaO, MgO, ZnO, SrO and CaO.
All the foregoing known compositions make possible the fabrication of ceramic bodies by firing at temperatures of not more than 1200 degrees C. in a nonoxidative (reductive or neutral) atmosphere. The ceramic bodies may therefore be cosintered with electrodes of a base metal such as nickel. The resulting capacitors have specific dielectric constants of not less than 2000, and the temperature dependences of their capacitances are within plus or minus 10 percent in a temperature range of -25 degrees to +85 degrees C.
While these values are satisfactory for all practical purposes, we have nevertheless been hard pressed by our customers, with the recent development of microelectronics, for ceramic capacitors that have higher specific dielectric constants with no less temperature dependences.
SUMMARY OF THE INVENTION
We have hereby invented how to manufacture ceramic capacitors that have higher dielectric constants, with less temperature dependences over a wide temperature range, than heretofore and which can be formed by firing in a temperature range of not more than 1200 degrees C. in a nonoxidative atmosphere.
Briefly stated in one aspect thereof, our invention provides a solid dielectric capacitor of the above improved characteristics, comprising a low temperature sintered dielectric ceramic body and at least two electrodes in contact therewith. The ceramic body consists essentially of 100 parts by weight of a major ingredient that is expressed by the formula, (1-.alpha.){(Ba.sub.k-x M.sub.x)O.sub.k (Ti.sub.1-y R.sub.y)O.sub.2-(y/2) }+.alpha.CaZrO.sub.3, and 0.2 to 5.0 parts by weight of an additive mixture (hereinafter referred to as the additive ingredient) of at least two members selected from the group consisting of B.sub.2 O.sub.3 or Li.sub.2 O, SiO.sub.2 and at least one of BaO, SrO, CaO, MgO and ZnO. In the formula of the major ingredient, M is either or both of magnesium and zinc, R is at least one metal selected from scandium(Sc), yttrium(Y), gadolinium(Gd), dysprosium(Dy), holmium(Ho), erbium(Er), ytterbium(Yb), terbium(Tb), thulium(Tm) and lutetium(Lu), .alpha. is a numeral in the range of 0.005 to 0.040, k is a numeral not less than 1.00 and not more than 1.05, x is a numeral in the range of 0.01 to 0.10, and y is a numeral greater than 0 and not greater than 0.04. The relative proportions of B.sub.2 O.sub.3 or Li.sub.2 O, SiO.sub.2 and at least one selected metal oxide, altogether constituting the additive mixture, will be specified with reference to the ternary diagrams attached hereto.
Another aspect of our invention concerns a method of fabricating the ceramic capacitor having the ceramic body of the above specified composition. The method dictates, first of all, the preparation of a mixture of the above specified major ingredient and additives in finely divided form. This mixture is then molded into a body of desired shape and size, which is provided with at least two electrode portions of an electroconductive material in any convenient manner. Then the moldings with the electrode portions are consintered in a reductive or neutral atmosphere and is subsequently heated in an oxidative atmosphere.
The dielectric ceramic composition of our invention, set forth in the foregoing, makes it possible to sinter the moldings in a nonoxidative atmosphere at temperatures not exceeding 1200 degrees C. A preferred temperature range for this molding operation is from 1050 degrees to 1200 degrees C. The sintering temperatures of less than 1200 degrees C. enable the use of nickel or like low cost base metal as the electrode material in cosintering the ceramic boy and the electrodes.
Therefore, in the fabrication of ceramic capacitors by the method of our invention, an electroconductive paste of powdered nickel or like base metal may be printed, coated, or otherwise formed on green sheets of the dielectric ceramic compositions in accordance with our invention. The green sheets and the electroconductive layers thereon may be cosintered at temperatures of not more than 1200 degrees C.
The ceramic capacitors of our invention have proved to have very favorable physical and performance characteristics. The test capacitors manufactured in accordance with our invention, to be disclosed subsequently, had specific dielectric constants of more than 3000, dielectric losses of not more than 2.5%, and resistivities of not less than 1.times.10.sup.6 megohm-centimeters. Also the temperature dependences of their specific dielectric constants were from -15% to +15% of the value at 25 degrees C. in a temperature range of -55 degrees to +125 degrees C., and from -10% to +10% of the value at 20 degrees C. in a temperature range of -25 degrees to +85 degrees C.
The above and other features and advantages of our invention and the manner of realizing them will become more apparent, and the invention itself will best be understood, from a study of the following description and appended claims taken together with the attached drawings.

BRIEF DESCRIPTION OF THE DRAWINGS
FIG. 1 is a section through a monolithic, multilayered ceramic capacitor capable of fabrication in accordance with the teaching of our invention, the illustrated capacitor being representative of numerous test capacitors manufactured in the Examples of our invention to be presented subsequently;
FIG. 2 is a ternary diagram depicting the relative proportions of the second additives of the ceramic compositions in accordance with Examples 1-131 of our invention; and
FIG. 3 is a ternary diagram depicting the relative proportions of the second additives of the ceramic compositions in accordance with Examples 132-162 of our invention.

DETAILED DESCRIPTION
We have illustrated in FIG. 1 one of many monolithic ceramic capacitors of like construction fabricated in the subsequent Examples of our invention by way of a preferable embodiment thereof. Generally designated 10, the representative capacitor is shown to have an interlamination of three dielectric ceramic layers 12 and two film electrodes 14. The three ceramic layers 12 constitute in combination a solid dielectric body 15 having the low temperature sinterable ceramic compositions in accordance with our invention. The two film electrodes 14, which can be of a low cost base metal such as nickel, extend from both sides of the dielectric body 15 toward, and terminate short of, the opposite sides of the dielectric body and so have an overlapping, parallel spaced relation to each other.
The capacitor 10 also includes a pair of conductive terminations 16 which are formed on both sides of the dielectric body 15 and which contact the respective film electrodes 14. Each termination 16 is shown to comprise a baked on zinc layer 18, a plated on copper layer 20, and a plated on solder layer 22.
Typically, and as fabricated in the subsequent Examples of our invention, the intermediate one of the three dielectric layers 12 has a thickness of 0.02 millimeter (mm). The area of that part of each film electrode 14 which overlaps the other film electrode is 25 mm.sup.2 (5.times.5 mm).
EXAMPLES
We fabricated 162 different sets of test capacitors, each constructed as shown in FIG. 1, some having their dielectric bodies formulated in accordance with the ceramic compositions of our invention and others not. Then we measured the specific dielectric constant, dielectric loss, resistivity, and temperature dependence of capacitance of the test capacitors. Tables 1, 2 and 3 list the compositions of the dielectric bodies of all the test capacitors fabricated.
We have previously defined the major ingredient of the ceramic compositions in accordance with our invention by the general formula,
(1-.alpha.){(Ba.sub.k-x M.sub.x)O.sub.k (Ti.sub.1-y R.sub.y)O.sub.2-(y/2)}+.alpha.CaZrO.sub.3.
Thus, in Table 1, we have given various combinations of (1-.alpha.), .alpha., (k-x) and x in the formula to indicate the specific major ingredients employed in the various Tests. The (1-.alpha.) and .alpha. indicate the relative proportions of (Ba.sub.k-x M.sub.x)O.sub.k (Ti.sub.1-y R.sub.y)O.sub.2-(y/2) and CaZrO.sub.3 of the major ingredient in moles. The (k-x) and x indicate the atomicities of the associated elements. Since M can be either or both of Mg and Zn, the column under X is subdivided into the atomicities of these elements and their sum (X).
In Table 2, we have given various combinations of y and k in the formula to indicate the specific major ingredients employed in the various Tests. Since R is at least one metal selected from Sc, Y, Gd, Dy, Ho, Er and Yb, the column under y is subdivided into the atomicities of these elements and their sum(y). The k indicates the atmicity of the element (O).
The ceramic compositions of our invention also include an additive ingredient or glass ingredient. The additive ingredient is an additive mixture of B.sub.2 O.sub.3, SiO.sub.2 and MO or an additive mixture of Li.sub.2 O, SiO.sub.2 and MO. Table 3 specifies the proportions, in parts by weight, of the additive ingredient with respect to 100 parts by weight of the major ingredient. Also, Table 3 specifies the relative proportions, in mole percent, of the additive ingredients B.sub.2 O.sub.3, Li.sub.2 O, SiO.sub.2, and MO. Further, since MO can be any one or more of BaO, MgO, ZnO, SrO and CaO, Table 3 gives the relative proportions, in mole percent, of these metal oxides. In the Table 3, the additives of Tests Nos. 1-131 consist of Li.sub.2 O, SiO.sub.2 and MO, and the additive of Tests Nos. 132-162 consist of B.sub.2 O.sub.3, SiO.sub.2 and MO.
TABLE 1______________________________________Caramic CompositionsMajor Ingredient(100 wt. parts)Test XNo. 1 - .alpha. .alpha. k - x Mg Zn Sum______________________________________ 1 0.98 0.02 0.96 0.05 0.01 0.06 2 0.98 0.02 0.96 0.05 0.01 0.06 3 0.98 0.02 0.96 0.05 0.01 0.06 4 0.98 0.02 0.96 0.05 0.01 0.06 5 0.98 0.02 0.96 0.05 0.01 0.06 6 0.98 0.02 0.96 0.05 0.01 0.06 7 0.98 0.02 0.96 0.05 0.01 0.06 8 0.98 0.02 0.96 0.05 0.01 0.06 9 0.98 0.02 0.96 0.05 0.01 0.0610 0.98 0.02 0.96 0.05 0.01 0.0611 0.98 0.02 0.96 0.05 0.01 0.0612 0.98 0.02 0.96 0.05 0.01 0.0613 0.98 0.02 0.96 0.05 0.01 0.0614 0.98 0.02 0.96 0.05 0.01 0.0615 0.98 0.02 0.96 0.05 0.01 0.0616 0.98 0.02 0.96 0.05 0.01 0.0617 0.98 0.02 0.96 0.05 0.01 0.0618 0.98 0.02 0.96 0.05 0.01 0.0619 0.98 0.02 0.96 0.05 0.01 0.0620 0.98 0.02 0.96 0.05 0.01 0.0621 0.98 0.02 0.96 0.05 0.01 0.0622 0.98 0.02 0.96 0.05 0.01 0.0623 0.98 0.02 0.96 0.05 0.01 0.0624 0.98 0.02 0.96 0.05 0.01 0.0625 0.98 0.02 0.96 0.05 0.01 0.0626 0.98 0.02 0.96 0.05 0.01 0.0627 0.98 0.02 0.96 0.05 0.01 0.0628 0.98 0.02 0.96 0.05 0.01 0.0629 0.98 0.02 0.96 0.05 0.01 0.0630 0.98 0.02 0.96 0.05 0.01 0.0631 0.98 0.02 0.96 0.05 0.01 0.0632 0.98 0.02 0.96 0.05 0.01 0.0633 0.98 0.02 0.96 0.05 0.01 0.0634 0.98 0.02 0.96 0.05 0.01 0.0635 0.98 0.02 0.96 0.05 0.01 0.0636 0.98 0.02 0.96 0.05 0.01 0.0637 0.98 0.02 0.96 0.05 0.01 0.0638 0.98 0.02 0.96 0.05 0.01 0.0639 0.98 0.02 0.96 0.05 0.01 0.0640 0.98 0.02 0.96 0.05 0.01 0.0641 0.98 0.02 0.96 0.05 0.01 0.0642 0.98 0.02 0.96 0.05 0.01 0.0643 0.98 0.02 0.96 0.05 0.01 0.0644 0.98 0.02 0.96 0.05 0.01 0.0645 0.98 0.02 0.96 0.05 0.01 0.0646 0.98 0.02 0.96 0.05 0.01 0.0647 0.98 0.02 0.96 0.05 0.01 0.0648 0.995 0.005 0.96 0.06 0.02 0.0849 0.995 0.005 0.96 0.06 0.02 0.0850 0.995 0.005 0.96 0.06 0.02 0.0851 0.995 0.005 0.96 0.06 0.02 0.0852 0.995 0.005 0.96 0.06 0.02 0.0853 0.995 0.005 0.96 0.06 0.02 0.0854 0.96 0.04 0.96 0.05 0.03 0.0855 0.96 0.04 0.96 0.05 0.03 0.0856 0.96 0.04 0.96 0.05 0.03 0.0857 0.96 0.04 0.96 0.05 0.03 0.0858 0.96 0.04 0.96 0.05 0.03 0.0859 0.96 0.04 0.96 0.05 0.03 0.0860 0.96 0.04 0.96 0.05 0.03 0.0861 0.96 0.04 0.96 0.05 0.03 0.0862 0.96 0.04 0.96 0.05 0.03 0.0863 0.96 0.04 0.96 0.05 0.03 0.0864 0.96 0.04 0.96 0.05 0.03 0.0865 0.96 0.04 0.96 0.05 0.03 0.0866 0.96 0.04 0.96 0.05 0.03 0.0867 0.96 0.04 0.96 0.05 0.03 0.0868 0.96 0.04 0.96 0.05 0.03 0.0869 0.96 0.04 0.96 0.05 0.03 0.0870 0.96 0.04 0.96 0.05 0.03 0.0871 0.96 0.04 0.96 0.05 0.03 0.0872 0.96 0.04 0.96 0.05 0.03 0.0873 0.96 0.04 0.96 0.05 0.03 0.0874 0.96 0.04 0.96 0.05 0.03 0.0875 0.96 0.04 0.96 0.05 0.03 0.0876 0.96 0.04 0.96 0.05 0.03 0.0877 0.96 0.04 0.96 0.05 0.03 0.0878 1 0 0.91 0.05 0.05 0.179 0.995 0.005 0.91 0.05 0.05 0.180 0.98 0.02 0.91 0.05 0.05 0.181 0.96 0.04 0.91 0.05 0.05 0.182 0.95 0.05 0.91 0.05 0.05 0.183 1 0 0.97 0.02 0.05 0.0784 0.995 0.005 0.97 0.02 0.05 0.0785 0.98 0.02 0.97 0.02 0.05 0.0786 0.96 0.04 0.97 0.02 0.05 0.0787 0.95 0.05 0.97 0.02 0.05 0.0788 0.98 0.02 1 0 0 089 0.98 0.02 0.99 0.01 0 0.0190 0.98 0.02 0.99 0 0.01 0.0191 0.98 0.02 0.97 0.02 0.01 0.0392 0.98 0.02 0.95 0.01 0.04 0.0593 0.98 0.02 0.92 0.04 0.04 0.0894 0.98 0.02 0.9 0.1 0 0.195 0.98 0.02 0.9 0 0.1 0.196 0.98 0.02 0.88 0.12 0 0.1297 0.98 0.02 0.88 0 0.12 0.1298 0.97 0.03 1 0 0 099 0.97 0.03 1.04 0.01 0 0.01100 0.97 0.03 1.04 0 0.01 0.01101 0.97 0.03 1 0.03 0.02 0.05102 0.97 0.03 0.97 0.06 0.02 0.08103 0.97 0.03 0.95 0.06 0.04 0.1104 0.97 0.03 0.93 0.06 0.06 0.12105 0.98 0.02 0.94 0.04 0 0.04106 0.98 0.02 0.96 0.04 0 0.04107 0.98 0.02 0.99 0.04 0 0.04108 0.98 0.02 1.01 0.04 0 0.04109 0.98 0.02 1.03 0.04 0 0.04110 0.99 0.01 0.9 0.02 0.06 0.08111 0.99 0.01 0.92 0.02 0.06 0.08112 0.99 0.01 0.95 0.02 0.06 0.08113 0.99 0.01 0.97 0.02 0.06 0.08114 0.99 0.01 0.99 0.02 0.06 0.08115 0.98 0.02 0.96 0.04 0.02 0.06116 0.98 0.02 0.96 0.04 0.02 0.06117 0.98 0.02 0.96 0.04 0.02 0.06118 0.98 0.02 0.96 0.04 0.02 0.06119 0.98 0.02 0.96 0.04 0.02 0.06120 0.97 0.03 0.94 0.05 0.05 0.1121 0.97 0.03 0.94 0.05 0.05 0.1122 0.97 0.03 0.94 0.05 0.05 0.1123 0.97 0.03 0.94 0.05 0.05 0.1124 0.97 0.03 0.94 0.05 0.05 0.1125 0.97 0.03 0.94 0.05 0.05 0.1126 0.97 0.03 0.94 0.05 0.05 0.1127 0.97 0.03 0.94 0.05 0.05 0.1128 0.97 0.03 0.94 0.05 0.05 0.1129 0.97 0.03 0.94 0.05 0.05 0.1130 0.97 0.03 0.94 0.05 0.05 0.1131 0.97 0.03 0.94 0.05 0.05 0.1132 0.98 0.02 0.96 0.05 0.01 0.06133 0.98 0.02 0.96 0.05 0.01 0.06134 0.98 0.02 0.96 0.05 0.01 0.06135 0.98 0.02 0.96 0.05 0.01 0.06136 0.98 0.02 0.96 0.05 0.01 0.06137 0.98 0.02 0.96 0.05 0.01 0.06138 0.98 0.02 0.96 0.05 0.01 0.06139 0.98 0.02 0.96 0.05 0.01 0.06140 0.98 0.02 0.96 0.05 0.01 0.06141 0.98 0.02 0.96 0.05 0.01 0.06142 0.98 0.02 0.96 0.05 0.01 0.06143 0.98 0.02 0.96 0.05 0.01 0.06144 0.98 0.02 0.96 0.05 0.01 0.06145 0.98 0.02 0.96 0.05 0.01 0.06146 0.98 0.02 0.96 0.05 0.01 0.06147 0.98 0.02 0.96 0.05 0.01 0.06148 0.98 0.02 0.96 0.05 0.01 0.06149 0.98 0.02 0.96 0.05 0.01 0.06150 0.98 0.02 0.96 0.05 0.01 0.06151 0.995 0.005 0.96 0.07 0.01 0.08152 0.995 0.005 0.96 0.07 0.01 0.08153 0.995 0.005 0.96 0.07 0.01 0.08154 0.98 0.005 0.96 0.07 0.01 0.08155 0.995 0.005 0.96 0.07 0.01 0.08156 0.995 0.005 0.96 0.07 0.01 0.08157 0.96 0.04 0.98 0.03 0.02 0.05158 0.96 0.04 0.98 0.03 0.02 0.05159 0.96 0.04 0.98 0.03 0.02 0.05160 0.96 0.04 0.98 0.03 0.02 0.05161 0.96 0.04 0.98 0.03 0.02 0.05162 0.96 0.04 0.98 0.03 0.02 0.05______________________________________
TABLE 2______________________________________Caramic CompositionsMajor IngredientTest yNo. Sc Y Gd Dy Ho Er Yb Sum k______________________________________1 0 0 0 0 0 0 0.01 0.01 1.022 0 0 0 0 0 0 0.01 0.01 1.023 0 0 0 0 0 0 0.01 0.01 1.024 0 0 0 0 0 0 0.01 0.01 1.025 0 0 0 0 0 0 0.01 0.01 1.026 0 0 0 0 0 0 0.01 0.01 1.027 0 0 0 0 0 0 0.01 0.01 1.028 0 0 0 0 0 0 0.01 0.01 1.029 0 0 0 0 0 0 0.01 0.01 1.0210 0 0 0 0 0 0 0.01 0.01 1.0211 0 0 0 0 0 0 0.01 0.01 1.0212 0 0 0 0 0 0 0.01 0.01 1.0213 0 0 0 0 0 0 0.01 0.01 1.0214 0 0 0 0 0 0 0.01 0.01 1.0215 0 0 0 0 0 0 0.01 0.01 1.0216 0 0 0 0 0 0 0.01 0.01 1.0217 0 0 0 0 0 0 0.01 0.01 1.0218 0 0 0 0 0 0 0.01 0.01 1.0219 0 0 0 0 0 0 0.01 0.01 1.0220 0 0 0 0 0 0 0.01 0.01 1.0221 0 0 0 0 0 0 0.01 0.01 1.0222 0 0 0 0 0 0 0.01 0.01 1.0223 0 0 0 0 0 0 0.01 0.01 1.0224 0.01 0 0 0 0 0 0 0.01 1.0225 0.01 0 0 0 0 0 0 0.01 1.0226 0.01 0 0 0 0 0 0 0.01 1.0227 0 0.01 0 0 0 0 0 0.01 1.0228 0 0.01 0 0 0 0 0 0.01 1.0229 0 0.01 0 0 0 0 0 0.01 1.0230 0 0 0.01 0 0 0 0 0.01 1.0231 0 0 0.01 0 0 0 0 0.01 1.0232 0 0 0.01 0 0 0 0 0.01 1.0233 0 0 0 0.01 0 0 0 0.01 1.0234 0 0 0 0.01 0 0 0 0.01 1.0235 0 0 0 0.01 0 0 0 0.01 1.0236 0 0 0 0 0.01 0 0 0.01 1.0237 0 0 0 0 0.01 0 0 0.01 1.0238 0 0 0 0 0.01 0 0 0.01 1.0239 0 0 0 0 0 0.01 0 0.01 1.0240 0 0 0 0 0 0.01 0 0.01 1.0241 0 0 0 0 0 0.01 0 0.01 1.0242 0 0 0 0 0 0 0.01 0.01 1.0243 0 0 0 0 0 0 0.01 0.01 1.0244 0 0 0 0 0 0 0.01 0.01 1.0245 0 0 0 0 0 0 0.01 0.01 1.0246 0 0 0 0 0 0 0.01 0.01 1.0247 0 0 0 0 0 0 0.01 0.01 1.0248 0 0 0 0.01 0 0 0 0.01 1.0449 0 0 0 0.01 0 0 0 0.01 1.0450 0 0 0 0.01 0 0 0 0.01 1.0451 0 0 0 0.01 0 0 0 0.01 1.0452 0 0 0 0.01 0 0 0 0.01 1.0453 0 0 0 0.01 0 0 0 0.01 1.0454 0 0 0 0 0 0 0 0 1.0455 0 0 0 0 0 0 0.005 0.005 1.0456 0 0 0 0 0 0 0.01 0.01 1.0457 0 0 0 0 0 0 0.02 0.02 1.0458 0 0 0 0 0 0 0.04 0.04 1.0459 0 0 0 0 0 0 0.06 0.06 1.0460 0.005 0 0 0 0 0 0 0.005 1.0461 0.04 0 0 0 0 0 0 0.04 1.0462 0.06 0 0 0 0 0 0 0.06 1.0463 0 0.005 0 0 0 0 0 0.005 1.0464 0 0.04 0 0 0 0 0 0.04 1.0465 0 0.06 0 0 0 0 0 0.06 1.0466 0 0 0.005 0 0 0 0 0.005 1.0467 0 0 0.04 0 0 0 0 0.04 1.0468 0 0 0.06 0 0 0 0 0.06 1.0469 0 0 0 0.005 0 0 0 0.005 1.0470 0 0 0 0.04 0 0 0 0.04 1.0471 0 0 0 0.06 0 0 0 0.06 1.0472 0 0 0 0 0.005 0 0 0.005 1.0473 0 0 0 0 0.04 0 0 0.04 1.0474 0 0 0 0 0.06 0 0 0.06 1.0475 0 0 0 0 0 0.005 0 0.005 1.0476 0 0 0 0 0 0.04 0 0.04 1.0477 0 0 0 0 0 0.06 0 0.06 1.0478 0 0 0 0 0 0 0.02 0.02 1.0179 0 0 0 0 0 0 0.02 0.02 1.0180 0 0 0 0 0 0 0.02 0.02 1.0181 0 0 0 0 0 0 0.02 0.02 1.0182 0 0 0 0 0 0 0.02 0.02 1.0183 0 0 0 0.005 0 0 0 0.005 1.0484 0 0 0 0.005 0 0 0 0.005 1.0485 0 0 0 0.005 0 0 0 0.005 1.0486 0 0 0 0.005 0 0 0 0.005 1.0487 0 0 0 0.005 0 0 0 0.005 1.0488 0 0 0 0 0 0 0.02 0.02 189 0 0 0 0 0 0 0.02 0.02 190 0 0 0 0 0 0 0.02 0.02 191 0 0 0 0 0 0 0.02 0.02 192 0 0 0 0 0 0 0.02 0.02 193 0 0 0 0 0 0 0.02 0.02 194 0 0 0 0 0 0 0.02 0.02 195 0 0 0 0 0 0 0.02 0.02 196 0 0 0 0 0 0 0.02 0.02 197 0 0 0 0 0 0 0.02 0.02 198 0 0 0 0.04 0 0 0 0.04 199 0 0 0 0.04 0 0 0 0.04 1.05100 0 0 0 0.04 0 0 0 0.04 1.05101 0 0 0 0.04 0 0 0 0.04 1.05102 0 0 0 0.04 0 0 0 0.04 1.05103 0 0 0 0.04 0 0 0 0.04 1.05104 0 0 0 0.04 0 0 0 0.04 1.05105 0 0 0 0 0 0 0.005 0.005 0.98106 0 0 0 0 0 0 0.005 0.005 1107 0 0 0 0 0 0 0.005 0.005 1.03108 0 0 0 0 0 0 0.005 0.005 1.05109 0 0 0 0 0 0 0.005 0.005 1.07110 0 0 0 0.02 0 0 0 0.02 0.98111 0 0 0 0.02 0 0 0 0.02 1112 0 0 0 0.02 0 0 0 0.02 1.03113 0 0 0 0.02 0 0 0 0.02 1.05114 0 0 0 0.02 0 0 0 0.02 1.07115 0 0 0 0.001 0 0 0.001 0.002 1.02116 0 0 0 0.005 0 0 0.005 0.01 1.02117 0 0 0 0.01 0 0 0.01 0.02 1.02118 0 0 0 0.02 0 0 0.02 0.04 1.02119 0 0 0 0.03 0 0 0.03 0.06 1.02120 0 0 0 0.03 0 0 0.01 0.04 1.04121 0 0.01 0 0 0 0 0.01 0.02 1.04122 0.01 0 0 0 0.01 0 0 0.02 1.04123 0 0.02 0 0.02 0 0 0 0.04 1.04124 0 0 0 0 0 0.03 0.01 0.04 1.04125 0 0.01 0 0.01 0 0 0.01 0.03 1.04126 0.01 0 0 0.02 0 0 0.01 0.04 1.04127 0 0.01 0 0.01 0.01 0.01 0 0.04 1.04128 0.01 0.01 0 0.01 0 0 0.01 0.04 1.04129 0.005 0.002 0.003 0.005 0 0.005 0.005 0.025 1.04130 0.003 0.005 0.002 0.005 0.005 0.005 0.005 0.03 1.04131 0.01 0.01 0.005 0.01 0.01 0.01 0.01 0.065 1.04132 0 0 0 0 0 0 0.01 0.01 1.02133 0 0 0 0 0 0 0.01 0.01 1.02134 0 0 0 0 0 0 0.01 0.01 1.02135 0 0 0 0 0 0 0.01 0.01 1.02136 0 0 0 0 0 0 0.01 0.01 1.02137 0 0 0 0 0 0 0.01 0.01 1.02138 0 0 0 0 0 0 0.01 0.01 1.02139 0 0 0 0 0 0 0.01 0.01 1.02140 0 0 0 0 0 0 0.01 0.01 1.02141 0 0 0 0 0 0 0.01 0.01 1.02142 0 0 0 0 0 0 0.01 0.01 1.02143 0 0 0 0 0 0 0.01 0.01 1.02144 0 0 0 0 0 0 0.01 0.01 1.02145 0 0 0 0 0 0 0.01 0.01 1.02146 0 0 0 0 0 0 0.01 0.01 1.02147 0 0 0 0 0 0 0.01 0.01 1.02148 0 0 0 0 0 0 0.01 0.01 1.02149 0 0 0 0 0 0 0.01 0.01 1.02150 0 0 0 0 0 0 0.01 0.01 1.02151 0 0 0 0 0 0 0.01 0.01 1.04152 0 0 0 0 0 0 0.01 0.01 1.04153 0 0 0 0 0 0 0.01 0.01 1.04154 0 0 0 0 0 0 0.01 0.01 1.04155 0 0 0 0 0 0 0.01 0.01 1.04156 0 0 0 0 0 0 0.01 0.01 1.04157 0 0 0 0.01 0 0 0 0.01 1.03158 0 0 0 0.01 0 0 0 0.01 1.03159 0 0 0 0.01 0 0 0 0.01 1.03160 0 0 0 0.01 0 0 0 0.01 1.03161 0 0 0 0.01 0 0 0 0.01 1.03162 0 0 0 0.01 0 0 0 0.01 1.03______________________________________
TABLE 3__________________________________________________________________________Ceramic CompositionsAdditive IngredientTest Proportion Composition (mole %) MO (mole %)No. (wt. parts) B.sub.2 O.sub.3 Li.sub.2 O SiO.sub.2 MO BaO SrO CaO MgO ZnO__________________________________________________________________________1 2 -- 1 80 19 20 0 50 30 02 2 -- 1 39 60 20 0 50 30 03 2 -- 30 30 40 20 0 50 30 04 2 -- 50 50 0 0 0 0 0 05 2 -- 20 80 0 0 0 0 0 06 2 -- 10 50 40 20 0 50 30 07 2 -- 30 40 30 20 0 50 30 08 2 -- 20 60 20 20 0 50 30 09 2 -- 35 65 0 0 0 0 0 010 2 -- 1 59 40 20 0 50 30 011 2 -- 1 85 14 20 0 50 30 012 2 -- 20 29 51 20 0 50 30 013 2 -- 50 30 20 20 0 50 30 014 2 -- 60 30 10 20 0 50 30 015 2 -- 60 40 0 0 0 0 0 016 2 -- 10 90 0 0 0 0 0 017 2 -- 20 60 20 100 0 0 0 018 2 -- 20 60 20 0 100 0 0 019 2 -- 20 60 20 0 0 100 0 020 2 -- 20 60 20 0 0 0 100 021 2 -- 20 60 20 0 0 0 0 10022 2 -- 20 60 20 20 20 20 20 2023 2 -- 20 60 20 40 10 20 10 2024 2 -- 10 50 40 40 20 0 50 3025 2 -- 20 60 20 20 20 0 50 3026 2 -- 35 65 0 0 0 0 0 027 2 -- 10 50 40 40 20 0 50 3028 2 -- 20 60 20 20 20 0 50 3029 2 -- 35 65 0 0 0 0 0 030 2 -- 10 50 40 40 20 0 50 3031 2 -- 20 60 20 20 20 0 50 3032 2 -- 35 65 0 0 0 0 0 033 2 -- 10 50 40 40 20 0 50 3034 2 -- 20 60 20 20 20 0 50 3035 2 -- 35 65 0 0 0 0 0 036 2 -- 10 50 40 40 20 0 50 3037 2 -- 20 60 20 20 20 0 50 3038 2 -- 35 65 0 0 0 0 0 039 2 -- 10 50 40 40 20 0 50 3040 2 -- 20 60 20 20 20 0 50 3041 2 -- 35 65 0 0 0 0 0 042 0 -- 0 0 0 0 0 0 0 043 0.2 -- 15 75 10 30 10 10 30 2044 1 -- 15 75 10 30 10 10 30 2045 3 -- 15 75 10 30 10 10 30 2046 5 -- 15 75 10 30 10 10 30 2047 7 -- 15 75 10 30 10 10 30 2048 0 -- 0 0 100 0 0 0 0 049 0.2 -- 15 40 45 20 20 20 20 2050 1 -- 15 40 45 20 20 20 20 2051 3 -- 15 40 45 20 20 20 20 2052 5 -- 15 40 45 20 20 20 20 2053 7 -- 15 40 45 20 20 20 20 2054 1 -- 30 40 30 0 0 0 100 055 1 -- 30 40 30 0 0 0 100 056 1 -- 30 40 30 0 0 0 100 057 1 -- 30 40 30 0 0 0 100 058 1 -- 30 40 30 0 0 0 100 059 1 -- 30 40 30 0 0 0 100 060 1 -- 30 40 30 0 0 0 100 061 1 -- 30 40 30 0 0 0 100 062 1 -- 30 40 30 0 0 0 100 063 1 -- 30 40 30 0 0 0 100 064 1 -- 30 40 30 0 0 0 100 065 1 -- 30 40 30 0 0 0 100 066 1 -- 30 40 30 0 0 0 100 067 1 -- 30 40 30 0 0 0 100 068 1 -- 30 40 30 0 0 0 100 069 1 -- 30 40 30 0 0 0 100 070 1 -- 30 40 30 0 0 0 100 071 1 -- 30 40 30 0 0 0 100 072 1 -- 30 40 30 0 0 0 100 073 1 -- 30 40 30 0 0 0 100 074 1 -- 30 40 30 0 0 0 100 075 1 -- 30 40 30 0 0 0 100 076 1 -- 30 40 30 0 0 0 100 077 1 -- 30 40 30 0 0 0 100 078 3 -- 10 50 40 20 20 20 20 2079 3 -- 10 50 40 20 20 20 20 2080 3 -- 10 50 40 20 20 20 20 2081 3 -- 10 50 40 20 20 20 20 2082 3 -- 10 50 40 20 20 20 20 2083 1 -- 20 60 20 0 100 0 0 084 1 -- 20 60 20 0 100 0 0 085 1 -- 20 60 20 0 100 0 0 086 1 -- 20 60 20 0 100 0 0 087 1 -- 20 60 20 0 100 0 0 088 0.5 -- 30 40 30 0 0 0 100 089 0.5 -- 30 40 30 0 0 0 100 090 0.5 -- 30 40 30 0 0 0 100 091 0.5 -- 30 40 30 0 0 0 100 092 0.5 -- 30 40 30 0 0 0 100 093 0.5 -- 30 40 30 0 0 0 100 094 0.5 -- 30 40 30 0 0 0 100 095 0.5 -- 30 40 30 0 0 0 100 096 0.5 -- 30 40 30 0 0 0 100 097 0.5 -- 30 40 30 0 0 0 100 098 0.5 -- 30 40 30 0 0 0 100 099 3 -- 35 55 10 100 0 0 0 0100 3 -- 35 55 3 100 0 0 0 0101 3 -- 35 55 3 100 0 0 0 0102 3 -- 35 55 3 100 0 0 0 0103 3 -- 35 55 3 100 0 0 0 0104 3 -- 35 55 3 100 0 0 0 0105 1 -- 10 50 40 20 20 20 20 20106 1 -- 10 50 40 20 20 20 20 20107 1 -- 10 50 40 20 20 20 20 20108 1 -- 10 50 40 20 20 20 20 20109 1 -- 10 50 40 20 20 20 20 20110 2 -- 15 75 10 0 0 100 0 0111 2 -- 15 75 10 0 0 100 0 0112 2 -- 15 75 10 0 0 100 0 0113 2 -- 15 75 10 0 0 100 0 0114 2 -- 15 75 10 0 0 100 0 0115 0.5 -- 30 55 15 20 20 20 20 20116 0.5 -- 30 55 15 20 20 20 20 20117 0.5 -- 30 55 15 20 20 20 20 20118 0.5 -- 30 55 15 20 20 20 20 20119 0.5 -- 30 55 15 20 20 20 20 20120 5 -- 35 40 25 20 0 30 50 0121 5 -- 35 40 25 20 0 30 50 0122 5 -- 35 40 25 20 0 30 50 0123 5 -- 35 40 25 20 0 30 50 0124 5 -- 35 40 25 20 0 30 50 0125 5 -- 35 40 25 20 0 30 50 0126 5 -- 35 40 25 20 0 30 50 0127 5 -- 35 40 25 20 0 30 50 0128 5 -- 35 40 25 20 0 30 50 0129 5 -- 35 40 25 20 0 30 50 0130 5 -- 35 40 25 20 0 30 50 0131 5 -- 35 40 25 20 0 30 50 0132 2.00 1 -- 80 19 20 0 50 30 0133 2.00 1 -- 39 60 20 0 50 30 0134 2.00 30 -- 0 70 20 0 50 30 0135 2.00 90 -- 0 10 20 0 50 30 0136 2.00 90 -- 10 0 0 0 0 0 0137 2.00 20 -- 80 0 0 0 0 0 0138 2.00 15 -- 30 55 20 0 50 30 0139 2.00 45 -- 15 40 20 0 50 30 0140 2.00 20 -- 50 30 20 0 50 30 0141 2.00 50 -- 30 20 20 0 50 30 0142 2.00 10 -- 20 70 20 0 50 30 0143 2.00 95 -- 5 0 0 0 0 0 0144 2.00 10 -- 85 5 20 0 50 30 0145 2.00 20 -- 50 30 100 0 0 0 0146 2.00 20 -- 50 30 0 100 0 0 0147 2.00 20 -- 50 30 0 0 100 0 0148 2.00 20 -- 50 30 0 0 0 100 0149 2.00 20 -- 50 30 0 0 0 0 100150 2.00 20 -- 50 30 20 20 20 20 20151 0.00 0 -- 0 0 0 0 0 0 0152 0.20 15 -- 75 10 0 50 0 50 30153 1.00 15 -- 75 10 0 50 0 50 30154 3.00 15 -- 75 10 0 50 0 50 30155 5.00 15 -- 75 10 0 50 0 50 30156 7.00 15 -- 75 10 0 50 0 50 30157 0.00 0 -- 0 0 0 0 0 0 0158 0.20 45 -- 15 40 20 20 20 20 20159 1.00 45 -- 15 40 20 20 20 20 20160 3.00 45 -- 15 40 20 20 20 20 20161 5.00 45 -- 15 40 20 20 20 20 20162 7.00 45 -- 15 40 20 20 20 20 20__________________________________________________________________________
According to Tables 1 and 2, the major ingredient of the dielectric bodies of the capacitors of Test No. 1 was:
0.98{(Ba.sub.0.96 M.sub.0.06)O.sub.1.02 (Ti.sub.0.99 R.sub.0.01)O.sub.1.995 }+0.02CaZrO.sub.3
or, more specifically, since M.sub.0.06 =Mg.sub.0.05, Zn.sub.0.01, and R.sub.0.01 =Yb.sub.0.01,
0.98{(Ba.sub.0.96 Mg.sub.0.05 Zn.sub.0.01)O.sub.1.02 (Ti.sub.0.99 Yb.sub.0.01)O.sub.1.995 }+0.02CaZrO.sub.3
One hundred parts by weight of this major ingredient was admixed with 2.0 parts by weight of a additive mixture of one mole percent Li.sub.2 O, 80 mole percent SiO.sub.2 and 19 mole percent MO. The MO was a mixture of 20 mole percent BaO, 50 mole percent CaO, and 30 mole percent MgO.
For the fabrication of the capacitors of Test No. 1 we started with the preparation of the first component, (Ba.sub.0.96 Mg.sub.0.05 Zn.sub.0.01)O.sub.1.02 (Ti.sub.0.99 Yb.sub.0.01)O.sub.1.995, of the major ingredient. We prepared the following start materials for the first component of the major ingredient:
Barium carbonate (BaCO.sub.3): 1041.96 grams (0.96 mole part)
Magnesium oxide (MgO): 11.09 grams (0.05 mole part)
Zinc oxide (ZnO) 4.48 grams (0.01 mole part)
Titanium oxide (TiO.sub.2): 435.06 grams (0.99 mole part)
Yttrebium oxide (Yb.sub.2 O.sub.3) 10.84 grams (0.005 mole part)
These start materials had all purities of not less than 99.0 percent. The above specified weights of the start materials do not include those of the impurities contained.
We charged the start materials into a pot mill together with alumina balls and 2.5 liters of water and intimately intermingled them by stirring the pot mill for 15 hours. Then we introduced the mixture into a stainless steel pot and dried it by air heated to 150 degrees C. for four hours. Then we crushed the dried mixture into relatively coarse particles and then fired the particles in air within a tunnel furnace at 1200 degrees C. for two hours. There was thus obtained the first component of the major ingredient in finely divided form.
Then we proceeded to the preparation of the second component, CaZrO.sub.3, of the major ingredient of Tset No. 1. We intermingled 448.96 grams of calcium carbonate (CaCO.sub.3) and 551.04 grams of zirconium oxide (ZrO.sub.2). Then we dried and pulverized the mixture and fired the resulting particles in air at 1250 degrees C. for two hours.
Then, in order to obtain the major ingredient of Test No. 1 in the required molar ratio (0.98:0.02) of the first and second components, we intermingled 984.34 grams (98 mole parts) of (Ba.sub.0.96 Mg.sub.0.05 Zn.sub.0.01)O.sub.1.02 (Ti.sub.0.99 Yb.sub.0.01) O.sub.1.995 and 15.66 grams (two mole parts) of CaZrO.sub.3. One thousand grams of the major ingredient was thus obtained in finely divided form.
Then, in order to obtain the additive ingredients of Test No. 1 we first prepared the following substances in the following amounts:
Li.sub.2 O: 0.44 grams (1.0 mole part)
SiO.sub.2 : 70.99 grams (80.0 mole parts)
BaCO.sub.3 : 11.10 grams (3.8 mole parts)
CaCO.sub.3 : 14.70 grams (9.5 mole parts)
MgO: 3.40 grams (5.7 mole parts)
To these substances we added 300 cubic centimeters of alcohol and stirred the resulting slurry for 10 hours in a polyethylene pot with alumina balls. Then we air fired the mixture at 1000 degrees C. for two hours. Then we charged the fired mixture into an alumina pot together with 300 cubic centimeters of water and pulverized it with alumina balls over a period of 15 hours. Then we dried the pulverized mixture at 150 degrees C. for four hours.
Thus we obtained in finely divided form the desired additive mixture of one mole percent Li.sub.2 O, 80 mole percent SiO.sub.2 and 19 mole percent MO, with the MO consisting of 3.8 mole percent BaO, 9.5 mole percent CaO, and 5.7 mole percent MgO. The relative proportions of BaO, CaO, and MgO were 20, 50 and 30 mole percent.
Then, we added 20 grams (two weight parts) of the second additive ingredient to 1000 grams (100 weight parts) of the major ingredient. Further, to this mixture, we added 15 percent by weight of an organic binder and 50 percent by weight of water with respect to the total weight of the major ingredient and additives. The organic binder was an aqueous solution of acrylic ester polymer, glycerine, and condensed phosphate. Then we ball milled the mixture into a slurry and then defoamed it in vacuum.
Then we charged the defoamed slurry into a reverse roll coater and shaped it into a thin, continuous strip on an elongate backing strip of polyester film. Then we dried the strip by heating it to 100 degrees C. on the backing film. There was thus obtained a green ceramic strip with a thickness of approximately 25 micrometers. We subsequently punched it into "squares" sized 10 by 10 centimeters. These green ceramic squares were to become the ceramic layers 12, FIG. 1, in the completed test capacitors 10.
For the fabrication of the base metal film electrodes 14 on the ceramic layers 12, we prepared 10 grams of nickel in finely divided form, with an average particle size of 1.5 micrometers, and a solution of 0.9 grams of ethyl cellulose in 9.1 grams of butyl "Carbitol" (trademark for diethylene glycol monobutyl ether). We intimately intermingled them in an agitator for 10 hours, thereby providing an electroconductive paste. Then we "printed" the paste on one surface of each green ceramic square, which had been prepared as above stated, through a screen having an array of 50 perforations of rectangular shape, each sized seven by 14 millimeters.
After having allowed the printed paste to dry, we stacked two green squares, with the printings thereon directed upwardly, and with the printings on the two squares offset from each other to an extent approximately half the pitch of the paste pattern in the longitudinal direction. Then we placed the stack of two printed squares between two separate stacks of four unprinted squares each with a thickness of 60 micrometers. Then we exerted a pressure of 39.2 MPa on the resulting stack of printed and unprinted squares in their thickness direction at 50 degrees C., thereby firmly bonding them together. Then we cut the bonded squares in a latticed pattern into 50 laminate chips of identical construction.
We employed a furnace capable of atmosphere control for cofiring the above prepared green dielectric bodies and, buried therein, the conductive layers which were to become the film electrodes 14 in the completed capacitors 10. We first air heated the chips to 600 degrees C. at a rate of 100 degrees C. per hour, thereby driving off the organic binder that had been used for providing the slurry of the powdered major ingredient and additives. Then we changed the furnace atmosphere from air to a reductive (nonoxidative) atmosphere consisting of two percent by volume of molecular hydroge and 98 percent by volume of molecular nitrogen. Then, in this furnace atmosphere, we raised the furnace temperature from 600 degrees C. to 1150 degrees C. at a rate of 100 degrees C. per hour. We maintained for three hours the maximum furnace temperature of 1150 degrees C., at which the ceramic bodies formulated in accordance with our invention were to be sintered to maturity. Then we lowered the furnace temperature to 600 degrees C. at a rate of 100 degrees C. per hour. Then, with the furnace atmosphere again changed to air (oxidative atmosphere), we maintained the temperature of 600 degrees C. for 30 minutes for the oxidizing heat treatment of the sintered chips. Then we allowed the furnace temperature to drop to room temperature.
Thus we obtained the dielectric ceramic bodies 15 cosintered with the film electrodes 14 buried therein.
We proceeded to the production of the pair of conductive terminations 16 on both sides of each ceramic body 15 at which were exposed the film electrodes 14. First, for the production of the inmost zinc layers 18, we coated both sides of each ceramic body 15 with an electroconductive paste composed of zinc, glass frit and vehicle. Then, after having allowed the coatings to dry, we heated them to 550 degrees C. in air and held the temperature for 15 minutes, thereby completing the zinc layers 18 each in direct contact with one of the two film electrodes 14. Then we formed the intermediate copper layers 20 over the zinc layers 18 by electroless plating, and then the outermost solder layers 22 over the copper layers 20 by electroplating an alloy of lead and tin.
We have thus completed the fabrication of the monolithic, multilayered ceramic test capacitors 10, each constructed as in FIG. 1, in accordance with the ceramic composition of Test No. 1 of Tables 1, 2 and 3. The composition of the ceramic bodies 15 of the thus completed capacitors 10 proved substantially akin to that before sintering.
As for the other ceramic compositions of Tables 1, 2 and 3 designated Tests Nos. 2-162, we made similar capacitors through the same procedure as set forth in the foregoing in connection with the Test No. 1 composition, except for the temperature of sintering in the reductive atmosphere, to which we will presently refer in more detail.
Then we tested all the capacitors of Tests Nos. 1-162 as to their specific dielectric constants, dielectric losses, resistivities, and capacitance-temperature characteristics. We measured these electrical properties of the test capacitors by the following methods:
SPECIFIC DIELECTRIC CONSTANT
The capacitance of each test capacitor was first measured at a temperature of 20 degrees C., a frequency of one kilohertz, and an effective voltage of 1.0 volt. Then the specific dielectric constant was computed from the measured value of capacitance, and the area (25 square millimeters) of each of the opposed parts of the film electrodes 14, and the thickness (0.02 millimeter) of that ceramic layer 12 which intervenes between the film electrodes.
DIELECTRIC LOSS
The dielectric loss was measured under the same conditions as the specific constant.
RESISTIVITY
Resistance between the pair of conductive terminations 16 of each test capacitor was measured after the application of a direct voltage of 100 volts for one minute. Then the resistivity was computed from the measured resistance value and the size of each test capacitor.
TEMPERATURE DEPENDENCE OF CAPACITANCE
The test capacitors were introduced into a thermostatic oven, and their capacitances at various preselected temperatures were measured at a frequency of one kilohertz and an effective voltage of 1.0 volt. Then the percent changes of the capacitances at -55 degrees and +125 degrees C. from those at 25 degrees C., and at -25 degrees and +85 degrees C. from those at 20 degrees C., were computed.
Table 4 gives the properties of the test capacitors as measured by the above described methods, as well as the maximum temperatures at which the test capacitors were sintered in the reductive atmosphere during their manufacture.
TABLE 4__________________________________________________________________________Firing Temperature & Capacitor Characteristics Capacitor Characteristics Firing Specific DielectricTest Temp. Dielectric Loss Resistivity Capacitance Variations (%)No. (.degree.C.) Constant (%) (megohm-cm) At -55.degree. C. At 125.degree. C. At -25.degree. C. At 85.degree. C.__________________________________________________________________________ 1 1150 3930 1.1 6.5 .times. 10.sup.6 -10.2 3.1 -5.5 -6.0 2 1160 3870 1.0 7.5 .times. 10.sup.6 -9.0 1.6 -4.2 -7.2 3 1140 3900 1.1 6.1 .times. 10.sup.6 -9.5 4.4 -5.3 -5.0 4 1140 3940 1.3 4.9 .times. 10.sup.6 -10.7 5.1 -5.9 -4.7 5 1140 3880 1.3 4.7 .times. 10.sup.6 -11.0 5.6 -6.1 -4.0 6 1140 3920 1.2 5.4 .times. 10.sup.6 -9.8 2.7 -5.6 -5.7 7 1140 3940 1.1 4.9 .times. 10.sup.6 -10.3 4.0 -5.8 -6.1 8 1130 3870 1.1 6.1 .times. 10.sup.6 -10.7 5.4 -6.0 -5.1 9 1150 3970 1.1 4.7 .times. 10.sup.6 -11.2 5.0 -6.3 -3.910 1160 3840 1.1 5.1 .times. 10.sup.6 -10.3 3.6 -5.9 -6.011 1250 Not coherently bonded on firing12 1250 "13 1250 "14 1250 "15 1250 "16 1250 "17 1140 3880 1.1 6.5 .times. 10.sup.6 -10.9 5.2 -6.0 -5.218 1140 3870 1.0 5.6 .times. 10.sup.6 -10.2 3.1 -6.7 -5.619 1140 3900 1.1 6.5 .times. 10.sup.6 -10.9 4.7 -6.0 -5.220 1140 3900 1.2 6.7 .times. 10.sup.6 -10.7 4.8 -6.0 -5.221 1140 3880 1.1 5.6 .times. 10.sup.6 -10.8 3.6 -5.9 -5.422 1140 3880 1.0 6.1 .times. 10.sup.6 -10.7 5.2 -6.0 -5.223 1140 3900 1.2 6.1 .times. 10.sup.6 -10.7 4.7 -5.9 -5.124 1140 3930 1.1 6.1 .times. 10.sup.6 -10.2 3.1 -5.5 -6.325 1140 3920 1.2 4.7 .times. 10.sup.6 -9.5 4.2 -6.1 -5.126 1140 3940 1.1 7.5 .times. 10.sup.6 -9.8 5.4 -4.1 -6.127 1140 3890 1.0 6.0 .times. 10.sup.6 -10.0 3.0 -5.4 -4.828 1140 3880 1.1 4.7 .times. 10.sup.6 -10.2 1.6 -5.0 -5.229 1140 3910 1.2 5.1 .times. 10.sup.6 -9.6 4.2 -6.0 -6.030 1140 3890 1.0 6.0 .times. 10.sup.6 -10.0 3.0 -5.3 -4.831 1140 3880 1.1 4.4 .times. 10.sup.6 -10.3 1.7 -5.2 -5.532 1140 3910 1.2 5.1 .times. 10.sup.6 -9.6 4.2 -5.8 -6.033 1140 3970 1.1 6.3 .times. 10.sup.6 -9.9 5.4 -5.1 -5.034 1140 3880 1.1 7.2 .times. 10.sup.6 -10.0 2.9 -4.8 -5.435 1140 3940 1.2 4.9 .times. 10.sup.6 -10.0 1.6 -6.1 -4.736 1140 3880 1.1 6.1 .times. 10.sup.6 - 10.6 4.2 -5.7 -5.337 1140 3890 1.0 5.6 .times. 10.sup.6 -11.0 1.3 -4.4 -4.838 1140 3910 1.1 4.9 .times. 10.sup.6 -10.0 3.1 -5.4 -4.839 1140 3970 1.1 6.0 .times. 10.sup.6 -10.7 1.5 -4.2 -5.140 1140 3900 1.2 5.4 .times. 10.sup.6 -10.8 4.2 -4.1 -4.841 1140 3900 1.0 4.9 .times. 10.sup.6 -11.0 2.8 -4.2 -5.442 1250 Not coherently bonded on firing43 1190 4520 1.4 2.1 .times. 10.sup.6 -10.4 2.5 -6.0 -5.144 1170 4160 1.3 3.5 .times. 10.sup.6 -10.2 3.0 -5.9 -4.945 1120 3510 1.1 6.0 .times. 10.sup.6 -11.6 0.1 -6.6 -6.946 1090 3230 1.6 3.2 .times. 10.sup.6 -12.7 -2.4 -7.7 -9.047 1060 2820 1.8 1.9 .times. 10.sup.6 -16.8 -5.0 -9.7 -12.348 1250 Not coherently bonded on firing49 1180 4470 1.1 4.0 .times. 10.sup.6 -12.2 6.1 -8.5 -2.350 1160 4210 1.1 6.7 .times. 10.sup.6 -12.4 6.9 -8.4 -1.251 1140 3720 1.3 7.4 .times. 10.sup.6 -13.0 4.1 -8.7 -3.552 1100 3130 1.7 3.7 .times. 10.sup.6 -14.3 1.2 -9.6 -6.153 1080 2840 1.9 2.1 .times. 10.sup.6 -18.6 -2.2 -10.0 -7.054 1170 4060 1.3 1.8 .times. 10.sup.6 -10.5 3.1 -6.0 -5.255 1150 4130 1.2 2.8 .times. 10.sup.6 -9.9 3.1 -5.4 -4.256 1130 4220 1.1 5.3 .times. 10.sup.6 -9.6 3.1 -4.1 -3.957 1090 4280 1.2 5.8 .times. 10.sup.6 -8.1 3.3 -4.9 -3.058 1150 3970 1.3 1.9 .times. 10.sup.6 -9.4 3.2 -5.5 -4.259 1250 Not coherently bonded on firing60 1130 4140 1.2 2.6 .times. 10.sup.6 -9.7 3.3 -4.9 -4.261 1160 3980 1.2 2.5 .times. 10.sup.6 -9.4 3.6 -5.2 -3.962 1250 Not coherently bonded on firing63 1130 4090 1.1 3.2 .times. 10.sup.6 -9.4 3.3 -4.7 -4.164 1160 4030 1.2 2.5 .times. 10.sup.6 -9.7 3.5 -4.9 -4.365 1250 Not coherently bonded on firing66 1130 4080 1.1 3.1 .times. 10.sup.6 -9.2 3.3 -4.5 -4.167 1160 4030 1.2 2.5 .times. 10.sup.6 -9.7 3.3 -4.9 -5.168 1250 Not coherently bonded on firing69 1120 4070 1.2 4.1 .times. 10.sup.6 -9.6 3.4 -5.0 -3.970 1150 4100 1.1 2.0 .times. 10.sup.6 -9.3 3.3 -5.0 -4.371 1250 Not coherently bonded on firing72 1150 4080 1.2 3.4 .times. 10.sup.6 -8.8 6.9 -4.8 -4.473 1160 4020 1.1 2.8 .times. 10.sup.6 -9.2 7.0 -5.3 -4.574 1250 Not coherently bonded on firing75 1150 4080 1.1 3.7 .times. 10.sup.6 -9.1 2.0 -5.2 -4.276 1140 4020 1.2 2.3 .times. 10.sup.6 -9.3 3.6 -4.9 -3.977 1250 Not coherently bonded on firing78 1150 3840 1.2 7.8 .times. 10.sup.6 -19.3 9.7 -12.0 4.079 1120 3870 1.1 8.0 .times. 10.sup.6 -13.3 4.9 -8.6 -2.780 1120 3900 1.2 7.8 .times. 10.sup.6 -11.0 2.5 -1.9 -6.081 1120 4020 1.1 7.0 .times. 10.sup.6 -4.3 -3.5 -2.0 -8.882 1120 3890 1.1 7.3 .times. 10.sup.6 1.4 -8.2 -0.6 -13.083 1180 4060 1.2 7.0 .times. 10.sup.6 -16.9 7.2 -11.8 3.884 1160 4170 1.2 6.5 .times. 10.sup.6 -14.3 3.6 - 9.2 -2.285 1160 4110 1.2 6.9 .times. 10.sup.6 -8.5 -1.2 -2.0 -5.186 1160 4080 1.1 5.9 .times. 10.sup.6 -2.1 -7.2 -1.0 -8.287 1160 4170 1.2 6.3 .times. 10.sup.6 4.2 -12.7 0.8 -11.988 1160 3850 1.7 4.0 .times. 10.sup.6 -16.3 6.9 -11.0 -6.289 1150 4170 1.2 7.8 .times. 10.sup.6 -12.4 7.8 -7.8 -5.390 1150 4220 1.6 4.0 .times. 10.sup.6 -13.0 5.0 -8.4 -5.491 1160 4030 1.1 8.5 .times. 10.sup.6 -12.0 4.9 -5.9 -3.792 1160 4010 1.5 4.3 .times. 10.sup.6 -10.7 3.9 -5.6 -5.193 1160 3900 1.1 9.3 .times. 10.sup.6 -10.5 2.5 -5.8 -7.094 1190 3840 1.0 9.3 .times. 10.sup.6 -10.6 1.2 -6.0 -8.495 1190 3650 1.6 7.3 .times. 10.sup.6 -12.3 1.5 -7.5 -8.296 1190 3860 1.1 9.8 .times. 10.sup.6 -11.0 -2.5 -5.8 -11.697 1180 3550 1.8 2.5 .times. 10.sup.6 -12.5 -3.2 -8.2 -11.498 1140 3670 1.8 1.3 .times. 10.sup.6 -17.3 -12.6 -11.9 -6.399 1130 3440 1.2 2.1 .times. 10.sup.6 -12.1 6.1 -9.0 2.6100 1130 3620 1.7 1.5 .times. 10.sup.6 -12.3 4.2 -9.2 4.3101 1140 3730 1.3 3.2 .times. 10.sup.6 -4.1 2.6 -2.1 -7.1102 1170 3460 1.1 3.8 .times. 10.sup.6 -3.6 1.8 -1.3 -8.2103 1180 3380 1.0 4.2 .times. 10.sup.6 -3.4 -2.1 -1.2 -9.4104 1170 3250 1.2 3.5 .times. 10.sup.6 -3.6 -4.2 -1.5 -11.2105 1120 3190 2.6 5.2 .times. 10.sup.6 -20.9 -12.4 -15.1 -8.0106 1150 3820 1.1 3.7 .times. 10.sup.6 -12.3 7.0 -7.0 -4.5107 1160 3760 1.0 4.3 .times. 10.sup.6 -11.2 6.1 -6.9 -4.2108 1180 3620 1.2 6.2 .times. 10.sup.6 -9.8 2.6 -5.7 - 5.1109 1250 Not coherently bonded on firing110 1120 3190 3.8 4.8 .times. 10.sup.6 -22.0 -10.0 -15.4 -9.2111 1140 3750 1.2 6.5 .times. 10.sup.6 -12.5 6.1 -7.9 -3.4112 1150 3800 1.1 7.8 .times. 10.sup.6 -12.2 3.0 -7.4 -4.0113 1180 3640 1.2 8.8 .times. 10.sup.6 -10.1 1.3 -7.3 -3.6114 1250 Not coherently bonded on firing115 1160 3810 1.1 1.4 .times. 10.sup.6 -10.4 -1.0 -5.4 -6.9116 1130 3960 1.0 4.4 .times. 10.sup.6 -10.1 -1.1 -4.9 -6.3117 1120 4110 1.1 4.8 .times. 10.sup.6 -9.3 -0.5 -4.1 -5.7118 1150 3850 1.0 3.2 .times. 10.sup.6 -10.0 -1.1 -5.0 -6.5119 1250 Not coherently bonded on firing120 1150 3860 1.2 3.9 .times. 10.sup.6 -3.9 -2.8 -1.0 -7.0121 1120 4130 1.1 7.0 .times. 10.sup.6 -3.6 -2.5 -1.1 -7.1122 1120 4120 1.1 4.5 .times. 10.sup.6 -3.4 -2.4 -1.3 -7.0123 1150 3860 1.1 4.2 .times. 10.sup.6 -4.1 -3.5 -2.0 -8.6124 1150 3840 1.1 3.3 .times. 10.sup.6 -3.9 -3.6 -2.0 -8.3125 1140 3990 1.0 4.7 .times. 10.sup.6 -3.6 -2.8 -1.5 -7.7126 1150 3870 1.2 2.3 .times. 10.sup.6 -4.4 -3.7 -2.0 -8.3127 1150 3840 1.2 3.3 .times. 10.sup.6 -4.3 -3.2 -1.9 -8.1128 1150 3850 1.1 1.9 .times. 10.sup.6 -4.3 -3.8 -1.8 -8.7129 1130 4150 1.0 3.2 .times. 10.sup.6 -3.7 -2.6 -1.4 -7.7130 1140 3980 1.1 5.8 .times. 10.sup.6 -3.9 -2.9 -1.5 -8.0131 1250 Not coherently bonded on firing132 1130 3710 1.1 4.8 .times. 10.sup.6 -11.1 4.6 -6.5 -3.6133 1140 3690 1.1 5.1 .times. 10.sup.6 -10.5 3.4 -5.2 -4.7134 1120 3640 1.1 4.6 .times. 10.sup.6 -9.6 3.1 -5.1 -3.3135 1100 3580 1.2 4.1 .times. 10.sup.6 -11.9 5.8 -5.9 -2.6136 1100 3580 1.1 3.8 .times. 10.sup.6 -11.7 5.9 -6.5 -2.0137 1120 3650 1.1 1.9 .times. 10.sup.6 -10.5 4.1 -5.1 -2.5138 1130 3780 1.2 3.8 .times. 10.sup.6 -10.5 2.8 -5.4 -5.8139 1100 3710 1.0 3.5 .times. 10.sup.6 -10.4 2.6 -5.3 -5.5140 1120 3660 1.0 3.9 .times. 10.sup.6 -10.6 3.5 -5.3 -4.8141 1120 3690 0.9 3.8 .times. 10.sup.6 -11.0 4.0 -6.5 -2.4142 1250 Not coherently bonded on firing143 1250 "144 1250 "145 1130 3690 1.0 4.8 .times. 10.sup.6 -9.5 3.5 -4.1 -4.7146 1130 3660 1.0 5.3 .times. 10.sup.6 -9.4 2.3 -4.8 -5.4147 1130 3760 1.2 4.4 .times. 10.sup.6 -10.3 2.2 -5.3 -5.8148 1130 3780 1.1 6.4 .times. 10.sup.6 -8.5 1.9 -5.5 -5.8149 1130 3660 1.2 4.1 .times. 10.sup.6 -10.6 3.6 -6.2 -6.6150 1130 3840 0.3 5.3 .times. 10.sup.6 -9.9 4.1 -5.1 -6.5151 1250 Not coherently bonded on firing152 1170 4420 1.4 1.9 .times. 10.sup.6 -8.8 2.4 -4.2 -4.3153 1150 4140 1.0 2.6 .times. 10.sup.6 -6.9 4.0 -3.1 -4.8154 1120 3700 1.0 3.5 .times. 10.sup.6 -8.1 -0.3 -3.5 -7.7155 1080 3420 0.2 2.4 .times. 10.sup.6 -10.6 -2.1 -6.3 -8.8156 1050 2890 1.4 1.8 .times. 10.sup.6 -13.8 -6.8 -8.4 -11.0157 1250 Not coherently bonded on firing158 1170 4230 1.4 5.0 .times. 10.sup.6 1.6 4.5 -5.8 -0.8159 1150 4010 1.0 4.8 .times. 10.sup.6 -10.3 6.4 -5.6 -0.5160 1100 3740 1.0 4.8 .times. 10.sup.6 -10.2 2.6 -6.6 -3.4161 1080 3360 1.2 3.3 .times. 10.sup.6 -12.0 0.1 -8.7 -6.1162 1040 2990 1.5 2.5 .times. 10.sup.6 -16.1 -5.1 -9.8 -6.4__________________________________________________________________________
It will be noted from Table 4 that the specific dielectric constants of the Test No. 1 capacitors, for instance, averaged 3930, their dielectric losses 1.1 percent, their resistivities 6.5.times.10.sup.6 megohm-centimeters, and their percent variations of capacitances from those at 25 degrees C. to those at -55 degrees and +125 degrees C., -10.2 and +3.1 percent, and from those at 20 degrees C. to those at -25 degrees and +85 degrees C., -5.5 and -6.0 percent, respectively.
Before proceeding further with the examination of Table 4, we will determine the criteria of acceptability for the four electrical properties in question of the capacitors as follows:
Specific dielectric constant, at least 3000.
Dielectric loss, not more than 2.5 percent.
Resistivity, at least 1.times.10.sup.6 megohm-centimeters.
Temperature dependence of capacitance, within plus and minus 15 percent at -55 degrees and +125 degrees C., and within plus and minus 10 percent at -25 degrees and +85 degrees C.
A reconsideration of Table 4 in light of the above established criteria of favorable capacitor characteristics will reveal that the capacitors of Tests Nos. 11-16, 42, 47, 48, 53, 59, 62, 65, 68, 71, 74, 77, 78, 82, 83, 87, 88, 96-98, 104, 105, 109, 110, 114, 119, 131, 142-144, 151, 156, 157 and 162 do not meet these criteria. Accordingly, the corresponding ceramic compositions of Tables 1, 2 and 3 fall outside the scope of our invention. All the other test capacitors come up to these criteria even though they were sintered at temperatures of less than 1200 degrees C. in a reductive atmosphere.
Although Table 4 gives the percent variations of capacitances only at -55 degrees, +125 degrees, -25 degrees and +85 degrees C., we actually measured the capacitances at additional temperatures of 0 degrees, +20 degrees, +25 degrees, +40 degrees, +60 degrees and +105 degrees C. The capacitance variations of all the test capacitors in accordance with our invention were within plus and minus 10 percent in the temperature range of -25 degrees to +85 degrees C. and within plus and minus 15 percent in the temperature range of -55 degrees to +125 degrees C.
Now, let us study the ceramic compositions of Tables 1, 2 and 3, and the corresponding capacitor characteristics of Table 4 in more detail.
As for the major ingredient (1-.alpha.) {(Ba.sub.k-x M.sub.x) O.sub.k (Ti.sub.1-y R.sub.y)O.sub.2-(y/2) }+.alpha.CaZrO.sub.3, we tested various values for .alpha., k, x, z and y in order to determine desirable ranges of such values. First of all, the value of the x was set at zero in Tests Nos. 88 and 98. In the resulting capacitors the capacitance variation at -25 degrees C. was outside the desired range of plus and minas 10 percent, and the capacitance variation at -55 degrees C. was outside the desired range of plus and minus 15 percent. However, all the desired electrical characteristics were obtained when the value of the x was set at 0.01 as in Tests Nos. 89 and 99. Thus we set the lowest possible value of the x at 0.01.
The tests Nos. 96, 97, and 104 compositions had the value of the x set at 0.12. The capacitance variation of the resulting capacitors at +85 degrees C. fell outside the desired range of plus and minus 10 percent. All the desired electrical characteristics were obtained when the value of the x was set at 0.10 as in Tests Nos. 94, 95 and 103. The highest possible value of the x is therefore 0.10.
The capital M in the formula of the major ingredient represents either or both of Mg and Zn as aforesaid. The Tests indicate that the use of either or both of Mg and Zn does not substantially affect the characteristics of the resulting capacitors, and that the value of X can be in the range of 0.01 to 0.10 in either case.
The Tests Nos. 59, 62, 65, 68, 71, 74 and 77 compositions had the value of y set at 0.06. The dielectric bodies formulated accordingly were not coherently bonded on firing. All the desired electrical characteristics were obtained when the value of y was set at 0.04 as in Tests Nos. 58, 61, 64, 67, 70, 73, and 76. The highest possible value of y is therefor 0.04.
The capital R in the formula of the major ingredient represents at least one rare earth element selected from Sc, Y, Gd, Dy, Ho, Er, Yb, Tb, Tm and Lu as aforesaid. The Tests indicate that the use of one or plural of the rare earth elements does not substantially affect the characteristics of the resulting capacitors, and that the value of y can be in the range zero to 0.04.
The addition of the rare earth elements to the major ingredient improves the temperature dependence of capacitance. The rare earth elements serve to make the capacitors that the capacitance variation is from -15 percent to +15 percent in a temperature range of -55 degrees to +125 degrees C., and form -10 percent to +10 percent in a temperature range of -25 degrees to +85 degrees C. Also, the rare earth elements serve to make the dielectric bodies with a high resistivity. Furthermore, the rare earth elements serve to make the ceramic bodies having higher coherency.
The value of .alpha. in the formula of the major ingredient was set at zero in Tests Nos. 78 and 83. The capacitance variations of the resulting capacitors fell outside the desired range of plus and minus 10 percent at -25 degrees C. and the desired range of plus and minus 15 percent at -55 degrees C. All the desired characteristics were met when the value of .alpha. was set at 0.005 as in Tests Nos. 79 and 84. The lowest possible value of .alpha. is therefore 0.005.
The value 0.05 chosen for .alpha. in Tests 82 and 87 was too high because the capacitance variations of the resulting capacitors at 85 degrees C. fell outside the desired range of plus and minus 10 percent. All the desired characteristics were achieved when the value of .alpha. was set at 0.04 as in Tests Nos. 81 and 86. The highest possible value of .alpha. is therefor 0.04.
When the value of K was set at 0.98 as in Test Nos. 105 and 110, the resistivities of the resulting capacitors were both less than 1.times.10.sup.6 megohm-centimeters. The capacitor characteristics were all satisfactory when the value of K was set at 1.00 at in Tests Nos. 106, and 111. The lowest possible value of K is therefore 1.00.
When the value of K was set at 1.07 as in Tests Nos. 109 and 114, the resulting dielectric bodies were not coherently bonded on firing. Coherently bonded ceramic bodies were obtained, and the capacitor characteristics were all satisfactory, when the value of K was set at 1.05 as in Tests Nos. 99-103, 108 and 113. The upper limit of the possible values of K is therefore 1.05.
The ceramic compositions of Tests Nos. 42 and 48 contained no the additive ingredient specified by our invention. The dielectric bodies formulated accordingly were not coherently bonded on firing at a temperature as high as 1250 degrees C. For comparision the ceramic compositions of Tests Nos. 43 and 49 contained 0.2 part by weight of the additive ingredient with respect to 100 parts by weight of the major ingredient. Even though the firing temperatures for these test capacitors were as low as 1190 and 1180 degrees C., they possessed the desired electrical characteristics. We set, therefore, the lower limit of the possible proportions of the additive ingredient at 0.2 part by weight with respect to 100 parts by weight of the major ingredient.
The tests Nos. 47 and 53 ceramic compositions contained 7 parts by weight of the additive ingredient with respect to 100 parts by weight of the major ingredient. The specific dielectric constants of the resulting capacitors were less than the above established criterion of 3000. Also, their capacitance variations were outside the range of plus and minus 15 percent at -55 degrees C. However, when the proportion of the additive ingredient was reduced to five parts by weight as in Tests Nos. 46 and 52, the resulting capacitors had all the desired electrical characteristics. Accordingly, the upper limit of the possible proportions of the additive ingredient is set at five parts by weight with respect to 100 parts by weight of the major ingredient.
We have ascertained from the results of the Tests Nos. 1-16 that the acceptable range of the relative proportions of Li.sub.2 O, SiO.sub.2 and MO, the additive ingredient of the ceramic compositions in accordance with our invention, can be definitely stated in reference to the ternary diagram of FIG. 2. The point A in the ternary diagram indicates the Test No. 1 additive composition of one mole percent Li.sub.2 O, 80 mole percent SiO.sub.2, and 19 mole percent MO. The point B indicates the Test No. 2 additive composition of one mole percent Li.sub.2 O, 39 mole percent SiO.sub.2, and 60 mole percent MO. The point C indicates the Test No. 3 additive composition of 30 mole percent Li.sub.2 O, 30 mole percent SiO.sub.2, and 40 mole percent MO. The point D indicates the Test No. 4 additive composition of 50 mole percent Li.sub.2 O, 50 mole percent SiO.sub.2, and 0 mole percent MO. The point E indecates the Test No. 5 additive composition of 20 mole percent Li.sub.2 O, 80 mole percent SiO.sub.2, and 0 mole percent MO.
The relative proportions of the additives Li.sub.2 O, SiO.sub.2, and MO of the ceramic compositions in accordance with our invention are within the region bounded by the lines sequentially connecting the above defined points A, B, C, D and E in the ternary diagram of FIG. 2.
Tables 1, 2, 3 and 4 prove that the additive compositions within the above defined region makes possible the provision of capacitors of the desired characteristics. The additive compositions of Tests Nos. 11-16 all fall outside that region, and the corresponding dielectric bodies were not coherently bonded on firing at a temperature of as high as 1250 degrees C. The above specified acceptable range of the relative proportions of the additives holds true regardless of whether only one of BaO, MgO, ZnO, SrO and CaO is employed as MO, as in Tests Nos. 17-21, or two or more or all of them are employed as in the other Tests.
Also, we have ascertained from the results of the Tests Nos. 132-162 that the acceptable range of the relative proportions of B.sub.2 O.sub.3, SiO.sub.2 and MO, the additive ingredient of the ceramic compositions in accordance with our invention, can be definitely stated in reference to the ternary diagram of FIG. 3. The point A in the ternary diagram indicates the Test No. 132 additive composition of one mole percent B.sub.2 O.sub.3, 80 mole percent SiO.sub.2, and 19 mole percent MO. The point B indicates the Tests No. 133 additive composition of one mole percent B.sub.2 O.sub.3, 39 mole percent SiO.sub.2, and 60 mole percent MO. The point C indicates the Test No. 134 additive composition of 30 mole percent B.sub.2 O.sub.3, 0 mole percent SiO.sub.2, and 70 mole percent MO. The point D indicates the Test No. 135 additive composition of 90 mole percent B.sub.2 O.sub.3, 0 mole percent SiO.sub.2 , and 10 mole percent MO. The point E indicates the Test No. 136 additive composition of 90 mole percent B.sub.2 O.sub.3, 10 mole percent SiO.sub.2, and 0 mole percent MO. The point F indicates the Test No. 137 additive composition of 20 mole percent B.sub.2 O.sub.3, 80 mole percent SiO.sub.2, and 0 mole percent MO.
The relative proportions of the additives B.sub.2 O.sub.3, SiO.sub.2 and MO of the ceramic compositions in accordance with our invention are within the region bounded by the lines sequentially connecting the above defined points A, B, C, D, E and F in the ternary diagram of FIG. 3.
Tables 1, 2, 3 and 4 prove that the additive compositions within the above defined region makes possible the provision of capacitors of the desired characteristics. The additive compositions of Tests Nos. 142-144 all fall outside that region, and the corresponding dielectric bodies were not coherently bonded on firing at a temperature of as high as 1250 degrees C. The above specified acceptable range of the relative proportions of the additives holds true regardless of whether only one of BaO, MgO, ZnO, SrO and CaO is employed as MO, as in Tests Nos. 145-149, or two or more or all of them are employed as in the other Tests.
Although we have disclosed our invention in terms of specific Examples thereof, we understand that our invention is not to be limited by the exact details of such disclosure but admits of a variety of modifications or alterations within the usual knowledge of the ceramists, chemists or electricians without departing from the scope of the invention. The following, then, is a brief list of such possible modifications or alterations:
1. The low temperature sinterable ceramic compositions of our invention may contain various additives other than those disclosed herein. An example is a mineralizer such as manganese dioxide. Used in a proportion (preferably from 0.05 to 0.10 percent by weight) not adversely affecting the desired characteristics of the resulting capacitors, the mineralizer will serve to improve the sinterability of the ceramic compositions.
2. The start materials of the ceramic compositions in accordance with our invention may be substances such as oxides or hydroxides other than those employed in the foregoing Examples.
3. The temperature of the oxidizing heat treatment need not necessarily be 600 degrees C. but can be variously determined in a range (from 500 degrees to 1000 degrees C. for the best results) not exceeding the temperature of the preceding sintering in a nonoxidative atmosphere, the oxidizing temperature being dependent upon factors such as the particular base metal electrode material in use and the degree of oxidation required for each ceramic material to be produced.
4. The temperature of cosintering in a nonoxidative atmosphere may also be changed in consideration of the particular electrode material in use. We recommend a range of 1050 degrees to 1200 degrees C. if the electrode material is nickel, as we have ascertained by experiment that little or no flocculation of the nickel particles takes place in that temperature range.
5. The dielectric bodies formulated in accordance with our invention, with or without electrodes buried therein or otherwise attached thereto, may be sintered in a neutral, instead of reductive, atmosphere.
6. The principles of our invention may be applied to capacitors other than those of the monolithic, multilayered configuration disclosed herein.

Number	Date	Country	Kind
1-311094	Nov 1989	JPX
1-311095	Nov 1989	JPX

Number	Name	Date
4054532	Hanke et al.	Oct 1977
4610968	Wada et al.	Sep 1986
4610969	Wada et al.	Sep 1986
4610970	Wada et al.	Sep 1986
4610971	Wada et al.	Sep 1986
4642732	Ikeda et al.	Feb 1987
4866017	Okawa	Sep 1989

Solid dielectric capacitor and method of manufacture

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