Abstract:
A ceramic capacitor having excellent electric characteristics which includes internal electrodes essentially comprising a base metal such as Ni, and a method for fabricating the capacitor includes the step of firing under a non-oxidation atmosphere. A dielectric layer of the ceramic capacitor comprises basic and additional components. The basic component comprises a material represented by the following formula: 
     
       (Ba.sub.k-(x+y) M.sub.x L.sub.y)O.sub.k (Ti.sub.1-z R.sub.z)O.sub.2-l z/2 
     
     where, M is Mg and/or Zn, L is Ca and/or Sr, R is a rare earth element, and k, x, z and y are numerals fulfilling the conditions of 1.00≦k≦1.05, 0&lt;x&lt;0.10, 0&lt;y≦0.05, 0.01≦x+y&lt;0.10, and 0.002&lt;z≦0.06. The additional component consists comprises Li 2  O )or B 2  O 3 ), SiO 2  and MO (MO is at least one metal oxide selected from the group consisting of BaO, SrO, CaO, MgO and ZnO).

Description:
FIELD OF THE INVENTION 
     The invention relates to a ceramic capacitor having a one-layer structure or a laminated structure in which one or more than one dielectric ceramic layer is (are) sandwiched between internal electrodes, and a method for fabricating the same. 
     BACKGROUND OF THE INVENTION 
     In a conventional method for fabricating a laminated ceramic capacitor, a desired pattern of conductive paste consisting mainly of noble metal such as platinum (Pt) or palladium (Pd) is printed on a non-sintered ceramic sheet (green sheet) consisting of dielectric ceramic material powder. Then, a plural number of the green sheets are laminated and attached each other, and the laminated green sheets are fired at a temperature in the range of 1300° C. to 1600° C. under an oxidation atmosphere. 
     The non-sintered ceramic sheets consisting of dielectric ceramic sheets consisting of dielectric ceramic material powder become dielectric ceramic layers by firing the sheets, and the conductive paste consisting mainly of noble metal such as platinum or palladium become internal electrodes. 
     As described above, by adopting the conductive paste consisting mainly of noble metal such as platinum or palladium, a desired internal electrode can be obtained without oxidation thereof even if the material thereof is fired at a high temperature in the range of 1300° C. to 1600° C. under an oxidation atmosphere. 
     However, noble metals such as platinum or palladium are expensive, so that the laminated ceramic capacitors become essentially costly. 
     In order to resolve the problem described above, the applicant of the present invention has proposed in Japanese Patent Publication No. 61-14607, in which dielectric ceramic compositions including basic components consisting of (Ba k-x  M x )O k  TiO 2  (M is Mg and/or Zn) and additional components consisting of Li 2  O and SiO 2  are disclosed. 
     Japanese Patent Publication No. 61-14608 has disclosed dielectric ceramic compositions including additional components consisting of Li 2  O, SiO 2  and MO (MO is one or more than one kind of metal oxides selected from a group consisting of BaO, CaO and SrO) instead of Li 2  O and SiO 2  in the cited reference No. 61-14607. 
     Japanese Patent Publication No. 61-14609 has disclosed dielectric ceramic compositions consisting of basic components consisting of (Ba k-x-y  M x  L y ) O k  TiO 2  (M is Mg and/or Zn, and L is Sr and/or Ca) and additional components consisting of Li 2  O and SiO 2 . 
     Japanese Patent Publication No. 61-14610 has disclosed dielectric ceramic compositions including additional components consisting of Li 2  O, SiO 2  and MO (MO is one or more than one kind of metal oxides selected from a group consisting of BaO, CaO and SrO) instead of Li 2  O and SiO 2  in the cited reference No. 61-14609. 
     Japanese Patent Publication No. 61-14611 has disclosed dielectric ceramic compositions consisting of basic components consisting of (Ba k-x  M x )O k  TiO 2  (M is one or more than one kind of metals selected from a group consisting of Mg, Zn, Sr and Ca) and additional components consisting of B 2  O 3  and SiO 2 . 
     Japanese Patent Publication No. 62-1595 has disclosed dielectric ceramic compositions consisting of basic components consisting of (Ba k-x  M x )O k  TiO 2  (M is one or more than one kind of metals selected from a group consisting of Mg, Zn, Sr and Ca) and additional components consisting of B 2  O 3  and MO (MO is one or more than one kind of metal oxides selected from a group consisting of BaO, MgO, ZnO, SrO and CaO). 
     Japanese Patent Publication No. 62-1596 has disclosed dielectric ceramic compositions including additional components consisting of B 2  O 3 , SiO 2  and MO (MO is one or more than one kind of metal oxides selected from a group consisting of BaO, MgO, ZnO, SrO and CaO) instead of B 2  O 3  and MO in the cited reference No. 62-1595. 
     By using one of the dielectric ceramic compositions disclosed in the cited references as a dielectric layer, a dielectric ceramic capacitor can be obtained by firing at a temperature up to 1200° C. under a reducible atmosphere, in which a dielectric constant is at least 2000 and a dielectric constant change rate by temperature changes is in the range of -10% to +10% at a temperature in the range of -25° C. to +85° C. 
     Recently, electric circuits become high densed, which requires intensely miniaturization of ceramic capacitors, so that it has been expected to develop a ceramic capacitor including a dielectric ceramic composition which has a dielectric constant still larger than that of the dielectric ceramic compositions disclosed in the cited references shown above. 
     It has been also expected to develop a ceramic capacitor including a dielectric ceramic composition which has a relatively small capacitance change rate by temperature changes at a temperature in the range wider than that in the dielectric ceramic compositions disclosed in the cited references shown above. 
     Accordingly, it is an object of the invention to provide a ceramic capacitor including a dielectric ceramic composition which has a dielectric constant at least 3000, a dielectric loss tan (δ) up to 2.5%, a resistivity ρ at least 1×10 6  M Ω·cm, and a dielectric constant change rate by temperature changes in the range of -15% to +15% at a temperature in the range of -55° C. to 125° C. (the standard is set at 25° C.) and in the range of -10% to +10% at a temperature in the range of -25° C. to 85° C. (the standard is set at 20° C.) by firing the composition even at a temperature up to 1200° C. in a non-oxidation atmosphere, and a method for fabricating the same. 
     DISCLOSURE OF THE INVENTION 
     The first invention of the application will be described. 
     According to the first invention, a ceramic capacitor includes at least one dielectric ceramic layer consisting of a dielectric ceramic composition and internal electrodes sandwiching the dielectric ceramic composition. 
     The dielectric ceramic composition consists of a fired mixture of a basic component of 100 weight portions and an additional component of 0.2 to 5 weight portions. 
     The basic component consists of a material represented by the following formula: 
     
         (Ba.sub.k-(x+y) M.sub.x L.sub.y)O.sub.k (Ti.sub.1-z R.sub.z)O.sub.2-z/2 
    
     where, M is Mg and/or Zm, L is Ca and/or Sr, R is one or more metal elements selected from a group consisting of Sc, Y, Gd, Dy, Ho, Er and Yb. And, k, x, y and z are numerals fulfilling the following conditions: 
     
         1.00≦k≦1.05 
    
     
         0&lt;x&lt;0.10 
    
     
         0&lt;y≦0.05 
    
     
         0.01≦x+y≦0.10 
    
     
         0.002≦z≦0.06 
    
     A dielectric ceramic composition having desired electric characteristics can be obtained on the condition of 1.00≦k≦1.05, however, the resistivity ρ becomes considerably small, that is smaller than 1×10 6  MΩ·cm, the capacitance change rates ΔC -55  and ΔC 125  by temperature changes become out of the range of -15% to +15%, and ΔC -25  and ΔC 85  become out of the range of -10% to +10%, if k is smaller than 1.00. On the other hand, a dense sintered material can not be obtained if k is larger than 1.05. 
     A dielectric ceramic composition having desired electric characteristics can be obtained on the condition of 0.01≦x+y≦0.10, however, the capacitance change rate ΔC -55  by temperature changes becomes out of the range of -15% to +15% if x+y is smaller than 0.01. On the other hand, the capacitance change rate ΔC 85  becomes out of the range of -10% to +10% if x+y is larger than 0.10. 
     However, a condition of y≦0.05 should be fulfilled even if x+y≦0.10. , because the capacitance change rate ΔC 85  becomes out of the range of -10% to +10% if y is larger than 0.05. 
     Mg and Zn of the M component and Ca and Sr of the L component work for almost the same function, so that either of Mg and Zn or both thereof can be used on the condition of 0&lt;x&lt;0.10, and either of Ca and Sr or both thereof can be used on the condition of 0&lt;y≦0.05. 
     A dielectric ceramic composition having desired electric characteristics can be obtained on the condition of 0.002≦z≦0.06, however, the capacitance change rate ΔC -55  becomes out of the range of -15% to +15% and ΔC -25  becomes out of the range of -10% to +10% if z is smaller than 0.002. On the other hand, a dense sintered material can not be obtained if y is larger than 0.06. 
     Sc, Y, Dy, Ho, Er and Yb of the R component work for almost the same function, so that any one or more than one of them can be used. However, it is desirable that a value of z is in the range of 0.002 to 0.06 in any case. 
     The R component contributes an improvement of temperature characteristic of the capacitance of the dielectric ceramic composition. By adding the R component into the dielectric ceramic composition the capacitance change rates ΔC -55  to ΔC 125  by temperature changes at a temperature in the range of -55° C. to 125° C. become within the range of -15% to +15%, the capacitance change rates ΔC -25  to ΔC 85  by temperature changes at a temperature in the range of -25° C. to 85° C. become within a range of -10% to +10%, and each capacitance change rates at each temperature range becomes small. 
     Additionally, the R component has functions of increasing the resistivity ρ and improving the sintering characteristic of the dielectric ceramic composition. 
     In the composition formula representing the basic component, x, z and k represent numerals of atoms of the elements, respectively. 
     A small amount (desirably in the range of 0.05 to 0.1 weight %) of mineralizers such as MnO 2  may be added to the basic component to improve the sintering characteristic thereof so long as the addition does not obstruct objects of the invention. Other materials may be also added if necessary. 
     The starting material for obtaining the basic component may be oxides such as BaO, SrO or CaO, hydroxides or other compounds, in addition to the compounds shown in the embodiments. 
     Next, an additional component consists of of Li 2  O, SiO 2  and MO (MO is at least one metal oxide selected from a group consisting of BaO, SrO, CaO, MgO and ZnO). 
     A dielectric ceramic composition having desired electric characteristics can be obtained if the amount of the additional component added is in the range of 0.2 to 5 weight portions in 100 weight portions of the basic component, however, a dense sintered material can not be obtained if the amount of the additional component is smaller than 0.2 weight portions, on the other hand, the dielectric constant ε s  becomes smaller than 3000 and the capacitance change rate ΔC -55  by temperature changes becomes out of the range of -15% to +15% if the amount of the additional component is larger than 5 weight portions. 
     The range of a ratio among the amounts of Li 2  O, SiO 2  and MO in the additional component is represented by an area having five vertexes in the ternary system diagram of mol %, as follows: 
     the first vertex A where the amounts of Li 2  O is 1 mol %, SiO 2  is 80 mol % and MO is 19 mol %; 
     the second vertex B where the amounts of Li 2  O is 1 mol %, SiO 2  is 39 mol % and MO is 60 mol %; 
     the third vertex C where the amounts of Li 2  O is 30 mol %, SiO 2  is 30 mol % and MO is 40 mol %; 
     the fourth vertex D where the amounts of Li 2  O is 50 mol %, SiO 2  is 50 mol % and MO is 0 mol %; and 
     the fifth vertex E where the amounts of Li 2  O is 20 mol %, SiO 2  is 80 mol % and MO is 0 mol %. 
     A dielectric ceramic composition having desired electric characteristics can be obtained if the ratio among the amounts of Li 2  O, SiO 2  and MO in the additional component is within the area in the ternary system diagram of mol % described above, however, a dense sintered material can not be obtained if the ratio is out of the area. 
     The starting material of the additional component may be oxides or hydroxides or other compounds, in addition to ones shown in the embodiments. 
     The second invention of the application will be described. The second invention is the same as the first invention except of the additional component. 
     The additional component in the second invention consists of B 2  O 3 , SiO 2  and MO (MO is at least one metal oxide selected from a group consisting of BaO, SrO, CaO, MgO and ZnO). 
     A dielectric ceramic composition having desired electric characteristics can be obtained if the amount of the additional component added is in the range of 0.2 to 5 weight portions in 100 weight portions of the basic component, however, a dense sintered material can not be obtained if the amount of the additional component is smaller than 0.2 weight portions even if the temperature is at 1250° C., on the other hand, the dielectric constant ε s  becomes smaller than 3000 and the capacitance change rate ΔC -55  by temperature changes becomes out of the range of -15% to +15% if the additional component is larger than 5 weight portions. 
     The range of the ratio among the amounts of B 2  O 3 , SiO 2  and MO in the additional component is represented by an area having six vertexes in the ternary system diagram of mol %, as follows: 
     the first vertex F where the amounts of B 2  O 3  is 1 mol %, SiO 2  is 80 mol % and MO is 19 mol %; 
     the second vertex G where the amounts of B 2  O 3  is 1 mol %, SiO 2  is 39 mol % and MO is 70 mol %; 
     the third vertex H where the amounts of B 2  O 3  is 29 mol %, SiO 2  is 1 mol % and MO is 70 mol %; 
     the fourth vertex I where the amounts of B 2  O 3  is 90 mol %, SiO 2  is 1 mol % and MO is 9 mol %; 
     the fifth vertex J where the amounts of B 2  O 3  is 90 mol %, SiO 2  is 9 mol % and MO is 1 mol %; and 
     the sixth vertex K where the amounts of B 2  O 3  is 19 mol %, SiO 2  is 80 mol % and MO is 1 mol %. 
     A dielectric ceramic composition having desired electric characteristics can be obtained if the ratio among the amounts of Li 2  O, SiO 2  and MO in the additional component is within the area in the ternary system diagram of mol % described above, however, a dense sintered material can not be obtained if the ratio is out of the area. 
     The starting material for obtaining the additional component may be hydroxides or other compounds in addition to oxides. 
     The structure of the ceramic capacitor, the range of the ratio in the basic component of the dielectric ceramic composition, and the reasons of the limitations of the range in the second invention are the same as those in the first invention. 
     Next, the third invention of the application will be described. 
     According to the third invention, a method for fabricating a ceramic capacitor includes the steps of providing a mixture of non-sintered ceramic powder consisting essentially of basic and additional components, forming a non-sintered ceramic sheet consisting of the mixture, fabricating a laminated structure in which the non-sintered ceramic sheet is sandwiched between at least two conductive paste layers, firing the laminated structure under a non-oxidation atmosphere, and heating the fired laminated structure under an oxidation atmosphere. 
     The basic component composing the mixture of the non-sintered ceramic powder has the same features of the range of the composition ratio and the reasons of the limitation thereof as those in the first invention. 
     The additional component composing the mixture of the non-sintered ceramic powder has the same features of the range of the composition ratio, and the reasons of the limitations thereof as those in the first invention. 
     The weight ratio between the basic component and the additional component is of 0.2 to 5 weight portions of the additional component in 100 weight portions of the basic component. The reason of the limitation is the same as that in the first invention. 
     The temperature in the firing of a laminated structure under a non-oxidation atmosphere may be changed in accordance with materials composing the inner electrodes. If Ni is adopted as the material of the inner electrode, cohesion of Ni particles may scarcely occur at a temperature in the range of 1050° C. to 1200° C. 
     The non-oxidation atmosphere may be a neutral atmosphere such as in N 2  or Ar, in addition to a reducible atmosphere such as in H 2  or CO. 
     The temperature of heating the fired laminated structure under an oxidation atmosphere may be changed in consideration of oxidation of the electrode materials such as Ni and the ceramic materials. 
     The temperature of heating the fired laminated structure is set at 600° C. in the embodiments as described after, however, the temperature is not limited to be such a temperature, and the temperature may be any so long as it is below the sintering temperature, and it is more preferred to be in the range of 500° C. to 1000° C. 
     Next, the fourth invention of the application will be described. 
     A method for fabricating a ceramic capacitor in the fourth invention is the same as that in the third invention except of the additional component. 
     The additional component in the fourth invention is the same as the additional component (B 2  O 3  -SiO 2  -MO) in the second invention, and the range of the composition ratio and the reasons of the limitation are the same as those in the second invention. 
     In the embodiments described after, ceramic capacitors having laminated structures are described, however, the present inventions may be applied to general ceramic capacitors having one-layer structure. 
     According to the inventions, as the composition ratio of the dielectric ceramic composition is such that described above, it is enable to provide a ceramic capacitor including a dielectric ceramic composition which has features in which the dielectric constant is at least 3000, the dielectric loss tan δ is up to 2.5%, the resistivity ρ is at least 1×10 6  MΩ·cm, and the dielectric constant change rate by temperature changes is in the range of -15% to +15% at a temperature in the range of -55° C. to 125° C. (the standard is set at 25° C.) and -10% to +10% at a temperature in the range of -25° C. to 85° C. (the standard is set at 20° C.). 
     According to the invention, it is enable to fabricate a ceramic capacitor by firing the conductive paste, consisting mainly of base metal such as Ni and the green sheet, simultaneously, at a temperature under 1200° C. under a non-oxidation atmosphere, so that the fabrication cost thereof may be reduced. 
    
    
     BRIEF DESCRIPTION OF DRAWINGS 
     FIG. 1 is a cross sectional view illustrating a laminated ceramic capacitor in a preferred embodiment according to the invention; 
     FIG. 2 is a ternary-system diagram showing the composition ratio in the additional component according to the first invention; and 
     FIG. 3 is a ternary-system diagram showing the composition ratio in the additional component according to the second invention. 
    
    
     DESCRIPTION OF PREFERRED EMBODIMENTS 
     First, a method for making Sample No. 1 in Table 1 and electric characteristics thereof will be described. 
     MAKING THE BASIC COMPONENT 
     Compounds in the combination 1 are weighed, poured into a pot mill with alumina ball and 2.5 l of water, and stirred and mixed for 15 hours to obtain a material mixture. 
     
         ______________________________________The combination 1compounds      weight (g)                    mol portion______________________________________BaCO.sub.3     1029.33   0.96MgO              6.57    0.03ZnO              4.42    0.01CaCO.sub.3       5.43    0.01SrCO.sub.3       8.02    0.01TiO.sub.2       425.44   0.98Er.sub.2 O.sub.3           20.78    0.01______________________________________ 
    
     Here, values of the weight (g) and the mol portion of the compounds in the combination 1 are calculated so as that the composition formula of the basic component: 
     
         (Ba.sub.k- (x+y)M.sub.x L.sub.y)O.sub.k (Ti.sub.1-z R.sub.z)O.sub.2-z/2(1) 
    
     becomes: 
     
         (Ba.sub.0.96 Mg.sub.0.03 Zn.sub.0.01 Ca.sub.0.01 Sr.sub.0.01)O.sub.1.02 (Ti.sub.0.98 Er.sub.0.02)O.sub.1.99 
    
     Next, the material mixture is poured into a stainless pot and dried for 4 hours at 150° C. with using a hot blast drier. The dried material mixture is grinded roughly. The grinded material mixture is baked for 2 hours at 1200° C. in the air with using a tunnel furnace, and the powder of the first basic component in the composition formula (1) of the basic component can be obtained. 
     MAKING THE ADDITIONAL COMPONENT 
     Compounds in the combination 2 are weighed, added with 300 cc of alcohol, and stirred for 10 hours in a polyethylene pot with using aluminum balls. Then, the mixture is baked for 2 hours at 1000° C. in the air. 
     
         ______________________________________The combination 2compounds      weight (g)                    mol portion______________________________________Li.sub.2 O     0.43      1SiO.sub.2      68.77     80BaCO.sub.3     10.73     3.8CaCO.sub.3     5.44      3.8SrCO.sub.3     8.03      3.8MgO            2.19      3.8ZnO            4.42      3.8______________________________________ 
    
     Here, values of the weight (g) and the mol portions of the compounds in the combination 2 are calculated so as that the Li 2  O is 1 mol %, SiO 2  is 80 mol %, and MO is 19 mol % {BaO (3.8 mol %)+CaO (3.8 mol %)+SrO (3.8 mol %)+MgO (3.8 mol %)+ZnO (3.8 mol %)}. 
     Next, the baked mixture is poured into an alumina pot with 300 cc of water and grinded for 15 hours with using alumina balls. Then, the grinded mixture is dried for 4 hours at 150° C., and the powder of the additional component is obtained. 
     The ratio among BaO, CaO, SrO, MgO and ZnO is that of 20 mol % each, as shown in Table 1. 
     MAKING SLURRY 
     2 weight portions (20 g) of the additional component is added to 100 weight portions (1000 g) of the basic component. Then, the mixture of the basic and additional components are added with 15 weight % of organic binder consisting of an aqueous solution of acrylic acid ester polymer, glycerin and condensed phosphate and 50 weight % of water. Thus obtained mixture is poured into a ball mill, grinded and mixed to obtain slurry as ceramic material. 
     MAKING NON-SINTERED CERAMIC SHEET 
     The slurry is poured into a vacuum foam remover to remove foam thereof, and then is poured into a reverse roll coater to form a molded thin sheet which is continuously laid on a long polyester film. The molded thin sheet is heated to 100° C. on the polyester film to dry, and a non-sintered ceramic sheet having a thickness of approximately 25 μm is obtained. The non-sintered ceramic sheet having a large length is cut to be a 10 cm square each to be used. 
     MAKING AND PRINTING CONDUCTIVE PASTE 
     A mixture of 10 g of Ni powder having an average particle diameter of 1.5 μm and 0.9 g of ethylcellulose dissolved in 9.1 g of butylcarbitol is put in a stirrer and stirred for 10 hours, and the conductive paste for internal electrodes is obtained. Then, the conductive paste is printed on one surface of the non-sintered ceramic sheet through a screen having 50 patterns each of which is 14 mm in length and 7 mm in width, and is dried. 
     LAMINATING THE NON-SINTERED CERAMIC SHEET 
     Two of the non-sintered ceramic sheets are laminated with facing the printed surfaces thereof upward so that the printed patterns of the upper sheet and those of the lower sheet are shifted each other by a half length of the longer side of one pattern. Then, four of the non-sintered sheets having a total thickness of 60 μm is laminated on each surface of the laminated sheets thus obtained by laminating the two single sheets. 
     PRESSURE WELDING AND CUTTING THE LAMINATED SHEETS 
     The laminated sheets are pressure welded by applying a pressure of approximately 40 tons in the direction of the thickness at approximately 50° C. Then, the laminated sheets are cut to be lattices to obtain fifty laminated chips. 
     FIRING THE LAMINATED CHIP 
     The laminated chip is put into a furnace in which an atmosphere firing can be carried out, and the temperature is increased by 100° C./h to 600° C. in the atmosphere of the air to burn the organic binder of the laminated chip. 
     Then, the atmosphere of the furnace is changed from the atmosphere of the air to the reducible atmosphere of H 2  (2 volume %)+N 2  (98 volume %). The temperature is increased by 100° C./h from 600° C. to 1150° C. with keeping the reducible atmosphere, and the highest temperature of 1150° C. is kept for 3 hours. After that, the temperature is decreased by 100° C./h to 600° C., and the reducible atmosphere is changed to the atmosphere of the air (the acidic atmosphere), and the temperature of 600° C. is kept for 30 minutes to oxidate the laminated chip. Finally, the temperature is decreased to the room temperature, and a laminated fired chip is obtained. 
     FABRICATING EXTERNAL ELECTRODES 
     The conductive paste consisting of zinc, glass frit and vehicle is coated on the side surfaces of the laminated fired chip in which the internal electrodes are exposed to the outside, and is dried. Then, the chip is burned for 15 minutes at 550° C. in the air to form a zinc electrode. Copper layer is formed on the zinc electrode by non-electrolytic plating, and Pb-Sn solder layer is formed on the copper layer by electric plating. Thus, a pair of external electrodes are fabricated. 
     Thus, as shown in FIG. 1, the laminated ceramic capacitor 10 consists of a laminated fired chip 15 consisting of a 3-layer dielectric ceramic layer 12 and a 2-layer internal electrode 14 on which a pair of external electrodes 16 are formed. 
     The external electrode 16 consists of the zinc electrode layer 18, the copper layer 20 formed on the zinc electrode layer 18, and the Pb-Sn solder layer 22 formed on the copper layer 20. 
     A thickness of the dielectric ceramic layer 12 in the laminated ceramic capacitor 10 is 0.02 mm, and a facing area of a pair of the internal electrodes 14 is 5 mm×5 mm=25 mm 2 . And, the composition of the dielectric ceramic layer 12 after being sintered is substantially the same as the mixed composition of the basic and additional component before experiencing a sintering. 
     MEASUREMENTS OF ELECTRIC CHARACTERISTICS 
     The measurements of electric characteristics of the laminated ceramic capacitor 10 were carried out. The results of the measurement are that a dielectric constant ε s  is 3530, tan δ is 1.2%, a resistivity ρ is 4.7×10 6  MΩ·cm, and an capacitance change rate by temperature changes is -11.6% (ΔC -55 ) at -55° C. and +6.6% (ΔC 125 ) at 125° C. (the standard is set at 25° C.), and -6.8% (ΔC -25 ) at -25° C. and -4.9% (ΔC 85 ) at +85° C. (the standard is set at 20° C.). 
     The measurements of the electric characteristics are carried out in accordance with the process as shown below. 
     (A) The dielectric constant ε s  is calculated by values of the capacitance measured on conditions of a temperature at 20° C., a frequency 1 kHz, a voltage (effective value) 1.0 v, a facing area 25 mm 2  of the pair of the internal electrodes 14, and a thickness 0.02 mm of the dielectric ceramic layer 12 between the pair of the internal electrodes 14. 
     (B) The dielectric loss tan δ (%) is measured on the same conditions as in the measurement of the dielectric constant as shown above. 
     (C) The resistivity ρ (M Ω·cm) is calculated by values of resistance between the pair of the external electrodes 16 measured after applying DC 100 V at 20° C. for 1 minute, and the size thereof. 
     (D) The temperature characteristics of the capacitance is obtained by measuring the capacitance of the sample which is put in a constant temperature bath on conditions of a frequency 1 kHz and a voltage (effective value) 1.0 v at various temperatures of -55° C., -25° C., 0° C., ++20° C., 25° C., +40° C., +60° C., +85° C., +105° C. and +125° C. and calculating the change rates of the capacitances at each temperature from the temperatures 20° C. and 25° C. 
     The method for making Sample No. 1 and the characteristics thereof have been described as shown above. As for Samples No. 2 to No. 111, laminated ceramic capacitors are fabricated by the same method as that of Sample No. 1, except that the compositions of the basic component are varied as shown in (1) to (5) of Table 1, the compositions of the additional component are varied as shown in (1) to (5) of Table 2, and the temperatures of firing in the reducible atmosphere are varied as shown in (1) to (5) of Table 3. Then, the electric characteristics are measured on the same conditions as those in the measurement of Sample No. 1. The results are shown in (1) to (5) of Table 3. 
     The x, z and k in the column of the basic component in (1) to (5) of Table. 1 show the ratio of numerals of atoms of the elements in the composition formula (1) of the basic component as shown before, in other words, the ratio of numerals of atoms of the elements when the numerals of atoms of (Ti+R) is determined to be 1. 
     Mg and Zn of the column x are the contents of M in the composition formula (1) of the basic component. Ca and Sr of the column y are the contents of L in the composition formula (1) of the basic component. Sc, Y, Gd, Dy, Ho, Er and Yb of the column z are the contents of R in the composition formula (1) of the basic component. The values in these columns represent the numeral of atoms thereof, and the values in the column of the total represent the total numeral of the atoms (x+y) which is the total value of Mg, Zn, Ca and Sr. 
     In (1) to (5) of Table 2, the additional component is Li 2  O-SiO 2  -MO in Samples No. 1 to 86 and B 2  O 3  -SiO 2  -MO in Samples No. 87 to 111. 
     The added amount of the additional component in (1) to (5) of Table 2 is represented by weight portions in the 100 weight portions of the basic component. The contents of the column MO of the additional component represent the ratio among BaO, MgO, ZnO, SrO and CaO by mol %. 
     In (1) to (5) of Table 3, the temperature characteristics of the capacitance are described as ΔC -55  (%) and ΔC 125  (%) which are the change rates of the capacitance at -55° C. and 125° C., respectively (the standard is set at 25° C.), and ΔC -25  (%) and ΔC 85  (%) which are the change rates of the capacitance at -25° C. and at +85° C., respectively (the standard is set at 20° C.). 
     
                                           TABLE 1__________________________________________________________________________Basic Component (100 weight portions)Sample    x         y         x, y                       zNo  Mg  Zn     Total         Ca Sr Total                   Total                       Sc Y  Gd Dy Ho Er Yb Total                                                k__________________________________________________________________________ 1  0.03  0.01     0.04         0.01            0.01               0.02                   0.06                       0  0  0  0  0  0.02                                         0  0.02                                                1.02 2  0.03  0.01     0.04         0.01            0.01               0.02                   0.06                       0  0  0  0  0  0.02                                         0  0.02                                                1.02 3  0.03  0.01     0.04         0.01            0.01               0.02                   0.06                       0  0  0  0  0  0.02                                         0  0.02                                                1.02 4  0.03  0.01     0.04         0.01            0.01               0.02                   0.06                       0  0  0  0  0  0.02                                         0  0.02                                                1.02 5  0.03  0.01     0.04         0.01            0.01               0.02                   0.06                       0  0  0  0  0  0.02                                         0  0.02                                                1.02 6  0.03  0.01     0.04         0.01            0.01               0.02                   0.06                       0  0  0  0  0  0.02                                         0  0.02                                                1.02 7  0.03  0.01     0.04         0.01            0.01               0.02                   0.06                       0  0  0  0  0  0.02                                         0  0.02                                                1.02 8  0.03  0.01     0.04         0.01            0.01               0.02                   0.06                       0  0  0  0  0  0.02                                         0  0.02                                                1.02 9  0.03  0.01     0.04         0.01            0.01               0.02                   0.06                       0  0  0  0  0  0.02                                         0  0.02                                                1.0210  0.03  0.01     0.04         0.01            0.01               0.02                   0.06                       0  0  0  0  0  0.02                                         0  0.02                                                1.02*11 0.03  0.01     0.04         0.01            0.01               0.02                   0.06                       0  0  0  0  0  0.02                                         0  0.02                                                1.02*12 0.03  0.01     0.04         0.01            0.01               0.02                   0.06                       0  0  0  0  0  0.02                                         0  0.02                                                1.02*13 0.03  0.01     0.04         0.01            0.01               0.02                   0.06                       0  0  0  0  0  0.02                                         0  0.02                                                1.02*14 0.03  0.01     0.04         0.01            0.01               0.02                   0.06                       0  0  0  0  0  0.02                                         0  0.02                                                1.02*15 0.03  0.01     0.04         0.01            0.01               0.02                   0.06                       0  0  0  0  0  0.02                                         0  0.02                                                1.02*16 0.03  0.01     0.04         0.01            0.01               0.02                   0.06                       0  0  0  0  0  0.02                                         0  0.02                                                1.0217  0.03  0.01     0.04         0.01            0.01               0.02                   0.06                       0.02                          0  0  0  0  0  0  0.02                                                1.0218  0.03  0.01     0.04         0.01            0.01               0.02                   0.06                       0  0.02                             0  0  0  0  0  0.02                                                1.0219  0.03  0.01     0.04         0.01            0.01               0.02                   0.06                       0  0  0  0.02                                   0  0  0  0.02                                                1.0220  0.03  0.01     0.04         0.01            0.01               0.02                   0.06                       0  0  0  0  0  0  0.02                                            0.02                                                1.0221  0.03  0.01     0.04         0.01            0.01               0.02                   0.06                       0  0  0  0  0.02                                      0  0  0.02                                                1.0222  0.03  0.01     0.04         0.01            0.01               0.02                   0.06                       0  0  0  0  0.02                                      0  0  0.02                                                1.0223  0.03  0.01     0.04         0.01            0.01               0.02                   0.06                       0  0  0  0  0.02                                      0  0  0.02                                                1.0224  0.03  0.01     0.04         0.01            0.01               0.02                   0.06                       0  0  0  0  0.02                                      0  0  0.02                                                1.0225  0.03  0.01     0.04         0.01            0.01               0.02                   0.06                       0  0  0  0  0.02                                      0  0  0.02                                                1.02*26 0.02  0.02     0.04         0.02            0.02               0.04                   0.08                       0  0  0  0  0.01                                      0  0  0.01                                                1.0427  0.02  0.02     0.04         0.02            0.02               0.04                   0.08                       0  0  0  0  0.01                                      0  0  0.01                                                1.0428  0.02  0.02     0.04         0.02            0.02               0.04                   0.08                       0  0  0  0  0.01                                      0  0  0.01                                                1.0429  0.02  0.02     0.04         0.02            0.02               0.04                   0.08                       0  0  0  0  0.01                                      0  0  0.01                                                1.0430  0.02  0.02     0.04         0.02            0.02               0.04                   0.08                       0  0  0  0  0.01                                      0  0  0.01                                                1.04*31 0.02  0.02     0.04         0.02            0.02               0.04                   0.08                       0  0  0  0  0.01                                      0  0  0.01                                                1.04*32 0  0  0   0  0  0   0   0  0  0  0  0  0.02                                         0  0.02                                                1.0033  0.005  0  0.005         0.005            0  0.005                   0.01                       0  0  0  0  0  0.02                                         0  0.02                                                1.0034  0  0.005     0.005         0  0.005               0.005                   0.01                       0  0  0  0  0  0.02                                         0  0.02                                                1.0035  0.005  0  0.005         0  0.005               0.005                   0.01                       0  0  0  0  0  0.02                                         0  0.02                                                1.0036  0.01  0.01     0.02         0.01            0  0.01                   0.03                       0  0  0  0  0  0.02                                         0  0.02                                                1.0037  0.15  0.015     0.03         0.005            0.025               0.03                   0.06                       0  0  0  0  0  0.02                                         0  0.02                                                1.0038  0.02  0.02     0.04         0.02            0.02               0.04                   0.08                       0  0  0  0  0  0.02                                         0  0.02                                                1.0039  0  0.05     0.05         0.05            0  0.05                   0.1 0  0  0  0  0  0.02                                         0  0.02                                                1.00*40 0.03  0.01     0.04         0.03            0.03               0.06                   0.1 0  0  0  0  0  0.02                                         0  0.02                                                1.00*41 0.07  0  0.07         0.05            0  0.05                   0.12                       0  0  0  0  0  0.02                                         0  0.02                                                1.00*42 0  0.1     0.1 0  0.02               0.02                   0.12                       0  0  0  0  0  0.02                                         0  0.02                                                1.00*43 0.05  0.05     0.1 0.01            0.01               0.02                   0.12                       0  0  0  0  0  0.02                                         0  0.02                                                1.00*44 0.02  0.02     0.04         0.06            0  0.06                   0.1 0  0  0  0  0  0.02                                         0  0.02                                                1.0045  0.01  0  0.01         0.005            0  0.005                   0.015                       0  0.02                             0  0  0  0  0  0.02                                                1.0546  0  0.01     0.01         0  0.005               0.005                   0.015                       0  0.02                             0  0  0  0  0  0.02                                                1.0547  0.02  0.02     0.04         0.015            0.01               0.025                   0.065                       0  0.02                             0  0  0  0  0  0.02                                                1.0548  0.01  0.01     0.02         0.03            0.01               0.04                   0.06                       0  0.02                             0  0  0  0  0  0.02                                                1.0549  0.02  0.03     0.05         0.02            0.03               0.05                   0.1 0  0.02                             0  0  0  0  0  0.02                                                1.05*50 0.02  0.02     0.04         0.02            0.01               0.03                   0.07                       0  0  0  0  0  0  0.02                                            0.02                                                0.9851  0.02  0.02     0.04         0.02            0.01               0.03                   0.07                       0  0  0  0  0  0  0.02                                            0.02                                                1.0052  0.02  0.02     0.04         0.02            0.01               0.03                   0.07                       0  0  0  0  0  0  0.02                                            0.02                                                1.0353  0.02  0.02     0.04         0.02            0.01               0.03                   0.07                       0  0  0  0  0  0  0.02                                            0.02                                                1.05*54 0.02  0.02     0.04         0.02            0.01               0.03                   0.07                       0  0  0  0  0  0  0.02                                            0.02                                                1.07*55 0.02  0.03     0.05         0.02            0.01               0.03                   0.08                       0  0  0  0  0  0  0  0   1.0456  0.02  0.03     0.05         0.02            0.01               0.03                   0.08                       0  0  0  0  0  0.002                                         0  0.002                                                1.0457  0.02  0.03     0.05         0.02            0.01               0.03                   0.08                       0  0  0  0  0  0.01                                         0  0.01                                                1.0458  0.02  0.03     0.05         0.02            0.01               0.03                   0.08                       0  0  0  0  0  0.05                                         0  0.05                                                1.0459  0.02  0.03     0.05         0.02            0.01               0.03                   0.08                       0  0  0  0  0  0.06                                         0  0.06                                                1.04*60 0.02  0.03     0.05         0.02            0.01               0.03                   0.08                       0  0  0  0  0  0.07                                         0  0.07                                                1.04*61 0.03  0  0.03         0.03            0.01               0.04                   0.07                       0  0  0  0  0  0  0  0   1.0362  0.03  0  0.03         0.03            0.01               0.04                   0.07                       0  0  0  0  0.002                                      0  0  0.002                                                1.0363  0.03  0  0.03         0.03            0.01               0.04                   0.07                       0  0  0  0  0.02                                      0  0  0.02                                                1.0364  0.03  0  0.03         0.03            0.01               0.04                   0.07                       0  0  0  0  0.03                                      0  0  0.03                                                1.0365  0.03  0  0.03         0.03            0.01               0.04                   0.07                       0  0  0  0  0.05                                      0  0  0.05                                                1.0366  0.03  0  0.03         0.03            0.01               0.04                   0.07                       0  0  0  0  0.06                                      0  0  0.06                                                1.03*67 0.03  0  0.03         0.03            0.01               0.04                   0.07                       0  0  0  0  0.07                                      0  0  0.07                                                1.03*68 0.02  0.02     0.04         0.01            0.01               0.02                   0.06                       0  0  0  0  0  0  0  0   1.0269  0.02  0.02     0.04         0.01            0.01               0.02                   0.06                       0  0  0  0.001                                   0.001                                      0  0  0.002                                                1.0270  0.02  0.02     0.04         0.01            0.01               0.02                   0.06                       0  0  0  0.01                                   0.01                                      0  0  0.02                                                1.0271  0.02  0.02     0.04         0.01            0.01               0.02                   0.06                       0  0  0  0.02                                   0.01                                      0  0  0.03                                                1.0272  0.02  0.02     0.04         0.01            0.01               0.02                   0.06                       0  0  0  0.01                                   0.04                                      0  0  0.05                                                1.0273  0.02  0.02     0.04         0.01            0.01               0.02                   0.06                       0  0  0  0.02                                   0.04                                      0  0  0.06                                                1.02*74 0.02  0.02     0.04         0.01            0.01               0.02                   0.06                       0  0  0  0.04                                   0.03                                      0  0  0.07                                                1.0275  0.03  0.03     0.06         0.02            0.02               0.04                   0.1 0  0  0  0.01                                   0.01                                      0  0  0.02                                                1.0476  0.03  0.03     0.06         0.02            0.02               0.04                   0.1 0  0  0.01                                0  0  0  0.01                                            0.02                                                1.0477  0.03  0.03     0.06         0.02            0.02               0.04                   0.1 0.01                          0  0  0  0.01                                      0  0  0.02                                                1.0478  0.03  0.03     0.06         0.02            0.02               0.04                   0.1 0.01                          0.01                             0  0.01                                   0  0  0  0.03                                                1.0479  0.03  0.03     0.06         0.02            0.02               0.04                   0.1 0  0.01                             0.01                                0  0  0.01                                         0.01                                            0.04                                                1.0480  0.03  0.03     0.06         0.02            0.02               0.04                   0.1 0  0.01                             0  0.01                                   0.01                                      0  0.01                                            0.04                                                1.0481  0.03  0.03     0.06         0.02            0.02               0.04                   0.1 0.01                          0  0  0.02                                   0  0  0.01                                            0.04                                                1.0482  0.03  0.03     0.06         0.02            0.02               0.04                   0.1 0.01                          0.01                             0  0.01                                   0.01                                      0.01                                         0  0.05                                                1.0483  0.03  0.03     0.06         0.02            0.02               0.04                   0.1 0  0.01                             0.01                                0.01                                   0.01                                      0.01                                         0.01                                            0.06                                                1.0484  0.03  0.03     0.06         0.02            0.02               0.04                   0.1 0.005                          0.01                             0.02                                0.005                                   0.01                                      0.005                                         0.005                                            0.06                                                1.04*85 0.03  0.03     0.06         0.02            0.02               0.04                   0.1 0.005                          0.015                             0.005                                0.005                                   0.005                                      0.03                                         0.005                                            0.07                                                1.04*86 0.03  0.03     0.06         0.02            0.02               0.04                   0.1 0.01                          0.005                             0.005                                0.01                                   0.01                                      0.01                                         0.02                                            0.07                                                1.0487  0.03  0.01     0.04         0.01            0.01               0.02                   0.06                       0  0  0  0  0  0.02                                         0  0.02                                                1.0288  0.03  0.01     0.04         0.01            0.01               0.02                   0.06                       0  0  0  0  0  0.02                                         0  0.02                                                1.0289  0.03  0.01     0.04         0.01            0.01               0.02                   0.06                       0  0  0  0  0  0.02                                         0  0.02                                                1.0290  0.03  0.01     0.04         0.01            0.01               0.02                   0.06                       0  0  0  0  0  0.02                                         0  0.02                                                1.0291  0.03  0.01     0.04         0.01            0.01               0.02                   0.06                       0  0  0  0  0  0.02                                         0  0.02                                                1.0292  0.03  0.01     0.04         0.01            0.01               0.02                   0.06                       0  0  0  0  0  0.02                                         0  0.02                                                1.0293  0.03  0.01     0.04         0.01            0.01               0.02                   0.06                       0  0  0  0  0  0.02                                         0  0.02                                                1.0294  0.03  0.01     0.04         0.01            0.01               0.02                   0.06                       0  0  0  0  0  0.02                                         0  0.02                                                1.0295  0.03  0.01     0.04         0.01            0.01               0.02                   0.06                       0  0  0  0  0  0.02                                         0  0.02                                                1.0296  0.03  0.01     0.04         0.01            0.01               0.02                   0.06                       0  0  0  0  0  0.02                                         0  0.02                                                1.02*97 0.03  0.01     0.04         0.01            0.01               0.02                   0.06                       0  0  0  0  0  0.02                                         0  0.02                                                1.02*98 0.03  0.01     0.04         0.01            0.01               0.02                   0.06                       0  0  0  0  0  0.02                                         0  0.02                                                1.02*99 0.03  0.01     0.04         0.01            0.01               0.02                   0.06                       0  0  0  0  0  0.02                                         0  0.02                                                1.02100 0.03  0.01     0.04         0.01            0.01               0.02                   0.06                       0  0  0  0  0  0.02                                         0  0.02                                                1.02101 0.03  0.01     0.04         0.01            0.01               0.02                   0.06                       0  0  0  0  0  0.02                                         0  0.02                                                1.02102 0.03  0.01     0.04         0.01            0.01               0.02                   0.06                       0  0  0  0  0  0.02                                         0  0.02                                                1.02103 0.03  0.01     0.04         0.01            0.01               0.02                   0.06                       0  0  0  0  0  0.02                                         0  0.02                                                1.02104 0.03  0.01     0.04         0.01            0.01               0.02                   0.06                       0  0  0  0  0  0.02                                         0  0.02                                                1.02105 0.03  0.01     0.04         0.01            0.01               0.02                   0.06                       0  0  0  0  0  0.02                                         0  0.02                                                1.02*106    0.02  0.02     0.04         0.02            0.02               0.04                   0.08                       0  0  0  0  0.01                                      0  0  0.01                                                1.04107 0.02  0.02     0.04         0.02            0.02               0.04                   0.08                       0  0  0  0  0.01                                      0  0  0.01                                                1.04108 0.02  0.02     0.04         0.02            0.02               0.04                   0.08                       0  0  0  0  0.01                                      0  0  0.01                                                1.04109 0.02  0.02     0.04         0.02            0.02               0.04                   0.08                       0  0  0  0  0.01                                      0  0  0.01                                                1.04110 0.02  0.02     0.04         0.02            0.02               0.04                   0.08                       0  0  0  0  0.01                                      0  0  0.01                                                1.04*111    0.02  0.02     0.04         0.02            0.02               0.04                   0.08                       0  0  0  0  0.01                                      0  0  0.01                                                1.04__________________________________________________________________________ *marks show compared samples 
    
     
                                           TABLE 2__________________________________________________________________________Additional Component    AmountSample    weight    Composition (mol %)               Content of MO (mol %)No  portions    Li.sub.2 O        SiO.sub.2           MO  BaO                  SrO CaO                         MgO ZnO__________________________________________________________________________ 1  2.00 1   80 19  20 20  20 20  20 2  2.00 1   39 60  20 20  20 20  20 3  2.00 30  30 40  20 20  20 20  20 4  2.00 50  50 0   0  0   0  0   0 5  2.00 20  80 0   0  0   0  0   0 6  2.00 10  70 20  20 20  20 20  20 7  2.00 5   55 40  20 20  20 20  20 8  2.00 15  40 45  20 20  20 20  20 9  2.00 30  35 35  20 20  20 20  2010  2.00 40  55 5   20 20  20 20  20*11 2.00 10  85 5   20 20  20 20  20*12 2.00 0   90 10  20 20  20 20  20*13 2.00 5   25 70  20 20  20 20  20*14 2.00 30  5  65  20 20  20 20  20*15 2.00 40  25 35  20 20  20 20  20*16 2.00 60  30 10  20 20  20 20  2017  2.00 25  65 10  20 30  10 0   4018  2.00 25  65 10  30 0   30 20  2019  2.00 25  65 10  10 20  50 10  1020  2.00 25  65 10  0  40  40 20  021  2.00 30  45 25  100                  0   0  0   022  2.00 30  45 25  0  100 0  0   023  2.00 30  45 25  0  0   100                         0   024  2.00 30  45 25  0  0   0  100 025  2.00 30  45 25  0  0   0  0   100*26 0    0   0  0   0  0   0  0   027  0.20 15  60 25  20 20  20 20  2028  1.00 15  60 25  20 20  20 20  2029  3.00 15  60 25  20 20  20 20  2030  5.00 15  60 25  20 20  20 20  20*31 7.00 15  60 25  20 20  20 20  20*32 0.50 15  50 35  20 20  20 20  2033  0.50 15  50 35  20 20  20 20  2034  0.50 15  50 35  20 20  20 20  2035  0.50 15  50 35  20 20  20 20  2036  0.50 15  50 35  20 20  20 20  2037  0.50 15  50 35  20 20  20 20  2038  0.50 15  50 35  20 20  20 20  2039  0.50 15  50 35  20 20  20 20  20*40 0.50 15  50 35  20 20  20 20  20*41 0.50 15  50 35  20 20  20 20  20*42 0.50 15  50 35  20 20  20 20  20*43 0.50 15  50 35  20 20  20 20  20*44 0.50 15  50 35  20 20  20 20  2045  3.00 30  55 15  20 20  20 20  2046  3.00 30  55 15  20 20  20 20  2047  3.00 30  55 15  20 20  20 20  2048  3.00 30  55 15  20 20  20 20  2049  3.00 30  55 15  20 20  20 20  20*50 1.00 20  55 25  20 20  20 20  2051  1.00 20  55 25  20 20  20 20  2052  1.00 20  55 25  20 20  20 20  2053  1.00 20  55 25  20 20  20 20  20*54 1.00 20  55 25  20 20  20 20  20*55 0.50 25  60 15  20 20  20 20  2056  0.50 25  60 15  20 20  20 20  2057  0.50 25  60 15  20 20  20 20  2058  0.50 25  60 15  20 20  20 20  2059  0.50 25  60 15  20 20  20 20  20*60 0.50 25  60 15  20 20  20 20  20*61 0.2  40  45 15  20 20  20 20  2062  0.2  40  45 15  20 20  20 20  2063  0.2  40  45 15  20 20  20 20  2064  0.2  40  45 15  20 20  20 20  2065  0.2  40  45 15  20 20  20 20  2066  0.2  40  45 15  20 20  20 20  20*67 0.2  40  45 15  20 20  20 20  20*68 2.00 20  40 40  20 20  20 20  2069  2.00 20  40 40  20 20  20 20  2070  2.00 20  40 40  20 20  20 20  2071  2.00 20  40 40  20 20  20 20  2072  2.00 20  40 40  20 20  20 20  2073  2.00 20  40 40  20 20  20 20  20*74 2.00 20  40 40  20 20  20 20  2075  2.00 20  70 10  20 20  20 20  2076  2.00 20  70 10  20 20  20 20  2077  2.00 20  70 10  20 20  20 20  2078  2.00 20  70 10  20 20  20 20  2079  2.00 20  70 10  20 20  20 20  2080  2.00 20  70 10  20 20  20 20  2081  2.00 20  70 10  20 20  20 20  2082  2.00 20  70 10  20 20  20 20  2083  2.00 20  70 10  20 20  20 20  2084  2.00 20  70 10  20 20  20 20  20*85 2.00 20  70 10  20 20  20 20  20*86 2.00 20  70 10  20 20  20 20  2087  2.00 1   80 19  20 20  20 20  2088  2.00 1   39 60  20 20  20 20  2089  2.00 29  1  70  20 20  20 20  2090  2.00 90  1  9   20 20  20 20  2091  2.00 90  9  1   20 20  20 20  2092  2.00 19  80 1   20 20  20 20  2093  2.00 15  30 55  20 20  20 20  2094  2.00 45  15 40  10 30  20 30  1095  2.00 20  50 30  0  20  40 10  3096  2.00 50  30 20  40 0   30 30  0*97 2.00 10  20 70  50 0   10 40  0*98 2.00 95  5  0   0  0   0  0   0*99 2.00 10  85 5   10 20  0  30  40100 2.00 20  70 10  100                  0   0  0   0101 2.00 20  70 10  0  100 0  0   0102 2.00 20  70 10  0  0   100                         0   0103 2.00 20  70 10  0  0   0  100 0104 2.00 20  70 10  0  0   0  0   100105 2.00 40  50 10  20 20  20 20  20*106    0    0   0  0   0  0   0  0   0107 0.20 15  75 10  20 20  20 20  20108 1.00 15  75 10  20 20  20 20  20109 3.00 15  75 10  20 20  20 20  20110 5.00 15  75 10  20 20  20 20  20*111    7.00 15  75 10  20 20  20 20  20__________________________________________________________________________ *marks show compared samples 
    
     
                                           TABLE 3__________________________________________________________________________      Electric Characteristics    Temperature  ResistivitySample    of firing tan δ            ρ Change rates by temperature changes ΔC (%)No  (°C.)      εs         (%)            (MΩ.cm)                  ΔC.sub.-55                      ΔC.sub.125                          ΔC.sub.-25                              ΔC.sub.85__________________________________________________________________________ 1  1150   3530         1.2            4.7 × 10.sup.6                  -11.6                      6.6 -6.8                              -4.9 2  1150   3510         1.1            5.9 × 10.sup.6                  -12.2                      3.0 -5.9                              -5.2 3  1150   3480         1.1            5.3 × 10.sup.6                  -11.9                      2.4 -5.6                              -3.5 4  1150   3410         1.2            4.5 × 10.sup.6                  -12.3                      6.9 -5.9                              -3.7 5  1150   3380         1.1            3.6 × 10.sup.6                  -14.2                      6.8 -6.9                              -1.7 6  1150   3480         1.1            1.9 × 10.sup.6                  -12.9                      4.1 -5.0                              -2.3 7  1150   3640         1.2            3.2 × 10.sup.6                  -11.1                      2.2 -5.4                              -7.8 8  1150   3550         1.1            3.9 × 10.sup.6                  -13.2                      3.5 -6.9                              -6.2 9  1150   3490         1.1            3.2 × 10.sup.6                  -11.0                      3.3 -5.6                              -4.510  1150   3550         1.2            3.5 × 10.sup.6                  -12.3                      5.0 -7.9                              -3.1*11 1250   A dense sintered material can not be obtained*12 1250   A dense sintered material can not be obtained*13 1250   A dense sintered material can not be obtained*14 1250   A dense sintered material can not be obtained*15 1250   A dense sintered material can not be obtained*16 1250   A dense sintered material can not be obtained17  1150   3590         1.1            5.6 × 10.sup.6                   -9.3                      1.2 -6.4                              -7.118  1150   3460         1.3            4.1 × 10.sup.6                  -12.7                      3.6 -6.6                              -8.119  1150   3660         1.1            4.2 × 10.sup.6                  -11.7                      3.9 -5.1                              -7.820  1150   3490         1.0            3.9 × 10.sup.6                  -11.7                      3.4 -5.7                              -5.721  1150   3490         1.2            1.9 × 10.sup.6                  - 11.1                      5.8 -5.7                              -2.022  1150   3540         1.1            3.4 × 10.sup.6                  -10.6                      3.0 -5.5                              -5.723  1150   3470         1.1            3.2 × 10.sup.6                  -11.6                      3.6 -5.2                              -5.524  1150   3470         1.1            1.9 × 10.sup.6                  -13.1                      4.9 -5.3                              -2.125  1150   3560         1.0            3.1 × 10.sup.6                  -11.5                      2.6 -5.7                              -6.7*26 1250   A dense sintered material can not be obtained27  1190   4040         1.4            1.9 × 10.sup.6                   -9.9                      2.5 -4.0                              -4.528  1140   3950         1.0            2.4 × 10.sup.6                   -7.3                      3.8 -3.2                              -6.229  1110   3510         0.8            4.1 × 10.sup.6                   -8.8                      -1.4                          -3.5                              -9.030  1090   3240         1.0            2.1 × 10.sup.6                  -12.7                      -1.5                          -7.1                              -9.3*31 1050   2740         2.4            1.8 × 10.sup.6                  -19.2                      -14.1                          -9.7                              -7.2*32 1140   3870         1.8            2.0 × 10.sup.6                  -19.2                      9.0 -9.6                                4.533  1140   4020         1.3            1.6 × 10.sup.6                  -14.3                      10.0                          -6.7                               5.034  1140   3940         1.6            2.9 × 10.sup.6                  -13.0                      6.7 -9.2                               4.035  1150   3890         1.3            1.3 × 10.sup.7                  -12.7                      5.7 -7.0                               3.636  1150   3990         1.2            5.8 × 10.sup.6                  -12.3                      5.0 -5.8                              -4.037  1160   3970         1.6            2.8 × 10.sup.6                  -11.6                      4.0 -5.8                              -5.038  1160   3880         1.2            5.4 × 10.sup.6                  -10.9                      3.9 -4.2                              -7.339  1170   3630         1.1            4.7 × 10.sup.6                  -11.1                      0.9 -4.7                              -9.6*40 1190   3800         1.7            1.6 × 10.sup.6                  -12.4                      1.4 -7.0                              -12.7*41 1190   3450         1.1            5.5 × 10.sup.6                  -13.0                      -3.7                          -5.9                              -12.4*42 1190   3530         1.3            4.6 × 10.sup.6                  -13.7                      -4.4                          -8.5                              -12.5*43 1190   3690         1.5            2.1 × 10.sup.6                  -13.9                      0.4 -7.4                              -12.1*44 1190   3870         2.0            1.6 × 10.sup.6                  -14.2                      0.8 -7.6                              -12.645  1120   3610         1.2            3.1 × 10.sup.6                  -12.7                      7.9 -7.6                               4.546  1120   3780         1.8            2.2 × 10.sup.6                  -12.8                      5.2 -9.0                               5.047  1130   3870         1.4            2.6 × 10.sup.6                   -2.7                      3.6  0.4                              -7.748  1160   3580         1.1            6.0 × 10.sup.6                   -3.4                      1.7 -0.8                              -8.549  1160   3560         1.1            6.3 × 10.sup.6                   -3.3                      -2.9                           0.1                              -8.9*50 1140   3230         2.2            9.0 × 10.sup.4                  -22.9                      -14.2                          -14.7                              -10.451  1140   3580         1.1            4.8 × 10.sup.6                  -13.6                      4.3 -6.7                              -8.452  1140   3540         1.1            4.4 × 10.sup.6                  -10.2                      2.4 -6.2                              -8.853  1170   3540         1.0            6.7 × 10.sup.6                   -9.5                      -2.6                          -4.0                              -9.1*54 1250   A dense sintered material can not be obtained*55 1120   3590         1.4            1.4 × 10.sup.6                  -19.4                      7.0 -11.6                              - 2.856  1120   3750         1.3            3.1 × 10.sup.6                  -12.7                      4.7 -7.2                              -7.057  1120   3680         1.2            2.3 × 10.sup.6                  -11.3                      4.1 -5.4                              -5.958  1140   3650         1.3            1.8 × 10.sup.6                  -10.7                      3.8 -4.6                              -4.959  1170   3630         1.3            1.7 × 10.sup.6                  -12.2                      2.2 -6.1                              -3.9*60 1250   A dense sintered material can not be obtained*61 1120   3590         1.4            1.7 × 10.sup.6                  -19.0                      8.1 -12.1                              -2.262  1120   3630         1.3            2.0 × 10.sup.6                  -13.8                      5.6 -7.0                              -6.463  1120   3640         1.3            2.5 × 10.sup.6                  -13.2                      3.6 -6.0                              -5.664  1150   3610         1.2            3.3 × 10.sup.6                  -10.9                      2.3 -5.5                              -4.865  1150   3530         1.4            3.0 × 10.sup.6                   -9.9                      2.1 -4.8                              -3.666  1170   3430         1.6            2.0 × 10.sup.6                  -12.0                      0.9 -5.9                              -3.1*67 1250   A dense sintered material can not be obtained*68 1120   3720         1.4            2.3 × 10.sup.6                  -20.2                      6.9 -11.3                              -2.669  1120   3670         1.2            2.7 × 10.sup.6                  -14.5                      4.7 -7.0                              -8.070  1120   3590         1.2            2.5 × 10.sup.6                  -11.7                      4.3 -5.5                              -6.871  1130   3640         1.3            2.6 × 10.sup.6                  -10.0                      3.8 -4.6                              -6.372  1150   3640         1.3            2.7 × 10.sup.6                   -8.5                      2.8 -3.7                              -5.073  1180   3540         1.5            2.1 × 10.sup.6                   -8.6                      2.0 -3.9                              -3.8*74 1250   A dense sintered material can not be obtained75  1150   3680         1.3            4.8 × 10.sup.6                  -10.3                      -5.0                          -5.4                              -7.176  1150   3610         1.1            4.0 × 10.sup.6                   -9.8                      -3.0                          -6.6                              -6.077  1150   3670         1.2            5.7 × 10.sup.6                  -10.8                      -3.3                          -5.1                              -6.478  1150   3650         1.1            3.9 × 10.sup.6                  -10.4                      -6.2                          -5.8                              -9.179  1150   3660         1.3            3.0 × 10.sup.6                  -10.2                      -5.0                          -4.0                              -9.380  1150   3720         1.0            6.7 × 10.sup.6                  -10.7                      -4.3                          -5.7                              -8.581  1170   3670         1.2            2.5 × 10.sup.6                  -10.9                      -5.1                          -7.9                              -9.082  1170   3690         1.3            3.0 × 10.sup.6                   -9.9                      -4.8                          -6.1                              -8.583  1170   3660         1.1            1.5 × 10.sup.6                   -9.6                      -6.7                          -6.1                              -9.784  1180   3900         1.1            3.9 × 10.sup.6                  -10.6                      -2.6                          -4.5                              -9.2*85 1250   A dense sintered material can not be obtained*86 1250   A dense sintered material can not be obtained87  1150   3530         1.2            4.5 × 10.sup.6                  -11.4                      6.3 -6.9                              -5.088  1150   3540         1.1            6.1 × 10.sup.6                  -12.3                      3.0 -5.8                              -5.489  1150   3480         1.2            5.0 × 10.sup.6                  -12.0                      2.5 -5.5                              -3.490  1150   3420         1.2            4.6 × 10.sup.6                  -12.9                      6.7 -6.1                              -3.791  1150   3390         1.1            3.5 × 10.sup.6                  -14.3                      6.7 -6.5                              -1.792  1150   3460         1.2            1.9 × 10.sup.6                  -11.9                      4.2 -5.1                              -2.393  1150   3610         1.2            3.3 × 10.sup.6                  -11.3                      2.2 -5.5                              -7.794  1150   3550         1.1            3.7 × 10.sup.6                  -13.2                      3.6 -6.8                              -6.295  1150   3500         1.1            3.2 × 10.sup.6                  -11.6                      3.3 -5.6                              -4.696  1150   3520         0.9            3.5 × 10.sup.6                  -12.5                      5.4 -7.9                              -2.9*97 1250   A dense sintered material can not be obtained*98 1250   A dense sintered material can not be obtained*99 1250   A dense sintered material can not be obtained100 1150   3510         1.0            3.8 × 10.sup.6                  -10.2                      3.2 -4.4                              -4.3101 1150   3500         1.2            5.2 × 10.sup.6                  -10.7                      3.2 -6.4                              -7.1102 1150   3550         1.3            5.1 × 10.sup.6                  -12.7                      3.6 -5.6                              -7.5103 1150   3580         1.1            5.3 × 10.sup.6                   -9.5                      1.3 -6.3                              -6.9104 1150   3440         1.2            4.0 × 10.sup.6                  -12.0                      3.5 -6.8                              -7.7105 1150   3660         0.3            4.4 × 10.sup.6                  -11.5                      3.9 -5.1                              -8.2*106    1250   A dense sintered material can not be obtained107 1190   4020         1.4            1.8 × 10.sup.6                   -9.6                      2.6 -3.8                              -4.4108 1140   3970         1.0            2.2 × 10.sup.6                   -7.0                      3.9 -3.2                              -6.2109 1110   3490         0.8            4.1 × 10.sup.6                  -8.2                      -1.2                          -3.6                              -9.0110 1090   3230         1.1            2.1 × 10.sup.6                  -12.6                      -1.4                          -7.7                              -9.3*111    1050   2730         2.4            1.8 × 10.sup.6                  -19.4                      -14.3                          -9.8                              -7.0__________________________________________________________________________ *marks show compared samples 
    
     It is clear by Tables 1 to 3 that, in the samples which is within the range of the component according to the invention, by firing the samples in a non-oxidation atmosphere at a temperature up to 1200° C., the ceramic capacitor having desired electric characteristics can be obtained, in which a dielectric constant at least 3000, a dielectric loss tan (δ) up to 2.5%, a resistivity ρ at least 1×10 6  M Ω·cm, and capacitance change rates ΔC -55  and ΔC 125  by temperature changes in the range of -15% to +15% and ΔC -25  and ΔC 85  in the range of -10% of +10%. 
     On the other hand, the ceramic capacitor achieving the object of the invention can not be obtained by Samples No. 11 to 16, 26, 31, 32, 40 to 44, 50, 54, 55, 60, 61, 67, 68, 74, 85, 86, 97 to 99, 106, 111. Accordingly, the Samples mentioned above are out of the range of the invention. 
     The capacitance changes by temperature changes are shown only about ΔC -55 , ΔC 125 , ΔC -25  and ΔC 85  in Table 3, however, the capacitance change rates by temperature changes ΔC at a temperature in the whole range of -25° C. to +85° C. are within the range of -10% to +10%, and the cpacitance change rates ΔC at a temperature in the whole range of -55° C. to +125° C. are within the range of -15% to +15%. 
     Next, the composition range of the basic component according to the invention will be described in conjunction with the composition range and the electric characteristics etc. of the Samples. 
     A dielectric ceramic composition having desired electric characteristics can be obtained if (x+y) is 0.01 as shown in Samples No. 33 to 35, however, ΔC -55  becomes out of the range of -15% to +15% if (x+y) is 0 as shown in Sample No. 32. Therefore, the lower limit of (x+y) is 0.01. 
     A dielectric ceramic composition having desired electric characteristics can be obtained if (x+y) is 0.10 as shown in Samples No. 39 and 49, however, ΔC 85  becomes out of the range of -10% to +10% if (x+y) is 0.12 as shown in Samples No. 41 to 43. However, ΔC 85  becomes out of the range of -10% to +10% if y is over 0.05 even if (x+y) is 0.10 as shown in Samples No. 40 and 44. Therefore, the upper limit of y is 0.05 and the upper limit of (x+y) is 0.10, simultaneously. 
     Mg and Zn of the M component and Ca and Sr of the L component work for almost the same function, so that either of Mg and Zn or both thereof can be used on the condition of 0&lt;x&lt;0.10, and either of Ca and Sr or both thereof can be used on the condition of 0&lt;y≦0.05. It is desirable that the value of x+y is within the range of 0.01 to 0.10 in any case of one or more than one of M components and L components. 
     A dielectric ceramic composition having desired electric characteristics can be obtained if k is 1.00 as shown in Sample No. 51, however, the resistivity ρ becomes considerably small as 1×10 6  M Ω·cm, and ΔC -55  becomes much lower than -15% and both ΔC -25  and ΔC 85  become much lower than -10%, if k is 0.98 as shown in Sample No. 50. Therefore, the lower limit of k is 1.00 
     A dielectric ceramic composition having desired electric characteristics can be obtained if k is 1.05 as shown in Sample No. 53, however, a dense sintered material can not be obtained if k is 1.07 as shown in Sample No. 54. Therefore, the upper limit of k is 1.05. 
     A dielectric ceramic composition having desired electric characteristics can be obtained if z is 0.002 as shown in Samples No. 56, 62 and 69, however, ΔC -55  and ΔC -25  do not fulfil the lower limits of -15% and -10% respectively if z is 0 as shown in Samples No. 55, 61 and 68. Therefore, the lower limit of y is 0.002. 
     A dielectric ceramic composition having desired electric characteristics can be obtained if z is 0.06 as shown in Samples No. 59, 66, 73, 83 and 84, however, a dense sintered material can not be obtained if z is 0.07 as shown in Samples No. 60, 67, 74, 85 and 86, even if fired at 1250° C. Therefore, the upper limit of z is 0.06. 
     Sc, Y, Gd, Dy, Ho, Er and Yb of the R component work for almost the same function, so that any one or more than one of them can be used. 
     It is desirable that the value of y is in the range of 0.02 to 0.06 in any case of R component. 
     The R component contributes an improvement of the temperature characteristic of capacitance of a dielectric ceramic composition. By adding the R component into the dielectric ceramic composition, the capacitance change rates ΔC -55  to ΔC 125  at a temperature in the range of -55° C. to 125° C. become within the range of -15% to +15%, the capacitance change rates ΔC -25  to ΔC 85  at a temperature in the range of -25° C. to 85° C. become within a range from -10% to +10%, and each capacitance change rate at each temperature range becomes small. 
     Additionally, the R component has a function of increasing the resistivity ρ and improving the sintering characteristic of the dielectric ceramic composition. 
     Next, the amount and the composition range of the additional component including Li 2  O-SiO 2  -MO according to the first and the third inventions will be described in conjunction with the composition range and the electric characteristics etc. of the Samples. 
     A dielectric ceramic composition having desired electric characteristics can be obtained if the amount of the additional component added is 0.2 weight portions in 100 weight portions of the basic component by firing at 1190° C. as shown in Sample No. 27, however, a dense sintered material can not be obtained if the amount of the additional component is 0 even if the firing temperature is 1250° C. as shown in Sample No. 26. Therefore, the lower limit of the amount of the additional component is 0.2 weight portions. 
     A dielectric ceramic composition having desired electric characteristics can be obtained if the amount of the additional component added is 5.0 weight portions in 100 weight portions of the basic component as shown in Sample No. 30, however, the dielectric constant ε s  becomes smaller than 3000 and the capacitance change rate ΔC -55  by temperature changes becomes out of the range of -15% to +15% if the amount of the additional component is 7.0 as shown in Sample No. 31. Therefore, the upper limit of the amount of the additional component is 5.0 weight portions. 
     The composition ratio in the additional component is desired to be within the area profiled by a polygonal line connecting the first to fifth vertexes of A to E in turn in FIG. 2 showing the ratio of the components of Li 2  O-SiO 2  -MO. 
     In FIG. 2 of the ternary system diagram, the first vertex A represents the composition of Sample No. 1 in which Li 2  O is 1 mol %, SiO 2  is 80 mol % and MO is 19 mol %, the second vertex B represents the composition Sample No. 2 in which Li 2  O is 1 mol %, SiO 2  is 39 mol % and MO is 60 mol %, the third vertex C represents the composition of Sample No. 3 in which Li 2  O is 30 mol %, SiO 2  is 30 mol % and MO is 40 mol %, the fourth vertex D represents the composition of Sample No. 4 in which Li 2  O is 50 mol %, SiO 2  is 50 mol % and MO is 0 mol %, and the fifth vertex E represents the composition of Sample No. 5 in which Li 2  O is 20 mol %, SiO 2  is 80 mol % and MO is 0 mol %. 
     A dielectric ceramic composition having desired electric characteristics can be obtained if the composition ratio of the additional component is within the area described above as shown in Samples No. 1 to 10, however, a dense sintered material can not be obtained if the composition ratio is out of the area as shown in Samples No. 11 to 16. 
     MO component may be one of metal oxides selected from a group consisting of BaO, MgO, ZnO, SrO and CaO as like in Samples No. 21 to 25, or more than one of them blended in adequate ratio as like in other samples. 
     Next, the amount and the composition range of the additional component including B 2  O 3  -SiO 2  -MO according to the second or fourth invention will be described in conjunction with the composition range and the electric characteristics etc. of the Samples. 
     A dielectric ceramic composition having desired electric characteristics can be obtained if the amount of the additional component added is 0.2 weight portions in 100 weight portions of the basic component by firing at 1190° C. as shown in Sample No. 107, however, a dense sintered material can not be obtained if the additional component is 0.2 weight portions even if fired at 1250° C. as shown in Sample No. 106. Therefore, the lower limit of the amount of the additional component is 0.2 weight portions. 
     A dielectric ceramic composition having desired electric characteristics can be obtained if the amount of the additional component added is 5.0 weight portions in 100 weight portions of the basic component as shown in Sample 110, however, the dielectric constant ε s  becomes below 3000 and the capacitance change rate ΔC -55  by temperature changes becomes out of the range of -15% to +15%, if the additional component is 7.0 weight portions as shown in Sample No. 111. 
     The composition ratio in the additional component is desired to be within the area profiled by a polygonal line connecting the first to sixth vertexes of F to K in turn in FIG. 3 showing the ratio of the components of Ba 2  O 3  -SiO 2  -MO. 
     In FIG. 3 of the ternary system diagram, the first vertex F represents the composition of Sample No. 87 in which the amounts of B 2  O 3  is 1 mol %, SiO 2  is 80 mol % and MO is 19 mol %, the second vertex G represents the composition of Sample No. 88 in which the amounts of B 2  O 3  is 1 mol %, SiO 2  is 39 mol % and MO is 60 mol %, the third vertex H represents the composition of Sample No. 89 in which the amounts of B 2  O 3  is 29 mol %, SiO 2  is 1 mol % and MO is 70 mol %, the fourth vertex I represents the composition of Sample No. 90 in which the amounts of B 2  O 3  is 90 mol %, SiO 2  is 1 mol % and MO is 9 mol %, the fifth vertex J represents the composition of Sample No. 91 in which the amounts of B 2  O 3  is 90 mol %, SiO 2  is 9 mol % and MO is 1 mol %, and the sixth vertex K represents the composition of Sample No. 92 in which the amounts of B 2  O 3  is 19 mol %, SiO 2  is 80 mol % and MO is 1 mol %. 
     A dielectric ceramic composition having desired electric characteristics can be obtained if the composition of the additional component is within the area described above as shown in Samples No. 87 to 96, however, a dense sintered material can not be obtained if the composition ratio is out of the area as shown in Samples No. 97 to 99. 
     MO component may be one of metal oxides selected from a group consisting of BaO, MgO, ZnO, SrO and CaO as like in Samples No. 100 to 104, or more than one of them blended in adequate ratio as like in other samples.