Semiconductive ceramic composition having negative temperature coefficient of resistance

Abstract: The present invention provides a semiconductive ceramic composition comprising a lanthanum cobalt oxide and having a negative resistance-temperature characteristic, characterised in that the semiconductive ceramic composition comprises a chromium oxide in an amount of from 0.005 to 30 mol% in terms of chromium as the side component, and also provides use of the semiconductive ceramic composition for a semiconductive ceramic device. The device is usable for rush current inhibition, for motor start-up retardation and for halogen lamp protection, and is also usable in temperature-compensated crystal oscillators.

Description: FIELD OF THE INVENTION The present invention relates to a semiconductive ceramic composition comprising a lanthanum cobalt oxide and having a negative resistance-temperature characteristic, and use of the semiconductive ceramic composition for devices having a negative resistance-temperature characteristic to be used for rush-current inhibition, motor start-up retardation, or halogen lamp protection, or those to be used in temperature-compensated crystal oscillators, and so on. BACKGROUND OF THE INVENTION Heretofore are known semiconductive ceramic devices having a negative resistance-temperature characteristic (hereinafter referred to as a negative characteristic) i.e., they have a high resistance value at room temperature and their resistance value is lowered with the elevation of the ambient temperature (such devices are hereinafter referred to as NTC devices). The NTC devices of that type are used variously, for example, in temperature-compensated crystal oscillators or for rush-current inhibition, motor start-up retardation or halogen lamp protection. For example, temperature-compensated crystal oscillators (hereinafter referred to as TCXO) comprising NTC devices are used as frequency sources in electronic instruments such as those for communication systems. TCXO is grouped into a direct TCXO which comprises a temperature-compensating circuit and a crystal oscillator and in which the temperature-compensating circuit is directly connected with the crystal oscillator inside the oscillation loop, and an indirect TCXO in which the temperature-compensating circuit is indirectly connected with the crystal oscillator outside the oscillation loop. The direct TCXO comprises at least two NTC devices with which the oscillation frequency from the crystal oscillator is subjected to temperature compensation. In this, one NTC device has a low resistance value of about 30 Ω at room temperature (25°C) for attaining the intended temperature compensation at room temperature or lower, while the other has a high resistance value of about 3000 Ω at room temperature (25°C) for attaining the intended temperature compensation at temperatures higher than room temperature. NTC devices for rush-current inhibition are those for absorbing initial rush currents in electronic instruments. At the switching instant, overcurrents are applied to electronic instruments from a switching power source at the switching instant. NTC devices for rush-current inhibition act to prevent the overcurrent from breaking the other semiconductive devices such as IC and diodes and also halogen lamps, or from shortening the life of such devices and halogen lamps. After having been switched on, the NTC device of this type absorbs the initial rush current to thereby prevent any overcurrent from running through the circuit in an electronic instrument, and thereafter this is self-heated to be hot, thus having a lowered resistance value. In this self-heated condition at the steady state, the NTC device then acts to reduce the power consumption. NTC devices for motor start-up retardation are those for retarding the starting-up time for motors being started up, for a predetermined period of time. In gear motors which are so constructed that a lubricant oil is fed to the gearbox after the start of the motor, if the gear is directly rotated at a high speed immediately after the application of an electric current to the motor, the gear is often damaged due to the insufficient supply of a lubricant oil to the gear. In order to prevent the gear from being damaged in this case, the starting-up motion of the driving motor is retarded for a predetermined period of time by the use of an NTC device. On the other hand, in motors for driving lapping machines in which a grinder is rotated to polish the surface of a ceramic part, if the lapping disc is rotated at a high speed just after the start of the driving motor, the ceramic part is often cracked. In order to prevent the ceramic part from being cracked in this case, the starting-up motion of the driving motor is retarded for a predetermined period of time by the use of an NTC device. For these, the NTC device acts to lower the voltage to be applied to the terminals of the motor being started up, and thereafter it is self-heated to be hot, thus having a lowered resistance value. At the steady state, the motor shall be rotated at a desired speed. The conventional semiconductive ceramics with such a negative resistance-temperature characteristic that have heretofore been used for constructing the NTC devices such as those mentioned above comprise spinel oxides of transition metal elements such as manganese, cobalt, nickel, copper, etc. To attain accurate temperature compensation for the oscillation frequency in TCXO, it is desirable that the NTC device therein has a large degree of resistance-temperature dependence (hereinafter referred to as "constant B"). In general, the spinel oxides of transition metal elements has a positive relationship between the specific resistance at room temperature and the constant B. Therefore, those having a small specific resistance at room temperature shall have a small constant B. On the other hand, the spinel oxides of transition metal elements having a large specific resistance at room temperature shall have a large constant B. Therefore, laminate structures of NTC devices may have a lowered resistance value even though each constitutive NTC device has a high specific resistance. In that manner, therefore, it may be possible to obtain laminated NTC devices having a large constant B. However, the laminated NTC devices are problematic in that their capacitance is enlarged, resulting in that the accuracy in the temperature-compensating circuit comprising the NTC laminate is lowered. Where NTC devices are used for rush current inhibition, they must be self-heated to have a lowered resistance value at elevated temperatures. However, the conventional NTC devices comprising spinel oxides tend to have a smaller constant B, if their specific resistance is lowered. Therefore, the conventional NTC devices are problematic in that they could not have a sufficiently lowered resistance value at elevated temperatures and therefore their power consumption at the steady state could not be reduced. For example, to satisfactorily reduce the resistance value of tabular NTC devices at high temperatures, their surface area may be enlarged or their thickness may be reduced. However, the increase in the surface area of NTC devices is contradictory to the reduction in their size; and the reduction in the thickness of NTC devices will not be acceptable in view of their strength. In order to overcome these problems, there has been proposed a monolithic NTC device comprising a plurality of ceramic layers and a plurality of inner electrodes each sandwiched between the adjacent ceramic layers, in which are formed a pair of outer electrodes at the both sides of the laminate of such ceramic layers and inner electrodes. In this, the pair of outer electrodes are electrically and alternately connected with the inner electrodes. In this, however, the space between the facing inner electrodes is too narrow. Therefore, the monolithic NTC device is still problematic in that, if an overcurrent (of several A or higher) is run therethrough at the start of switch-on, it is often broken. Another NTC device has been proposed, which comprises BaTiO 3 and 20 % by weight of Li 2 CO 3 added thereto, and which may have a rapidly enlarged constant B at the phase transition point (see Japanese Patent Publication No. 48-6352). However, since this NTC device has a large specific resistance of 10 5 Ω · cm or more at 140 °C, it is problematic in that its power consumption at the steady state is large. An NTC device comprising VO 2 exhibits a rapidly-varying resistance characteristic i.e., its specific resistance is lowered from 10 Ω · cm to 0.01 Ω · cm at 80 °C. Therefore, this may be advantageously used for rush-current inhibition or for motor start-up retardation. However, this VO 2 -containing NTC device is unstable. In addition, since this must be produced by reductive baking followed by rapid cooling, its shape is limited to only beads. Moreover, since the acceptable current value for this is small to be up to several tens mA, the NTC device of this type cannot be used in switching power sources or driving motors where a large current of several A is run. V. G. Bhide and D. S. Rajoria say that rare earth-transition element oxides exhibit a negative resistance-temperature characteristic, as having a low resistance value at elevated temperatures, while having a small constant B at room temperature and having a large constant B at high temperatures (see Phys. Rev. B6, [3], 1021, 1972). For example, the electric characteristics of devices comprising LaCrO 3 are disclosed by N. Umeda and T. Awa (see Electronic Ceramics, Vol. 7, No. 1, 1976, p. 34, Figs. 4 and 5). As in this literature, the devices are known to exhibit a negative resistance-temperature characteristic. To use for rush-current inhibition, these LaCrO 3 -containing NTC devices may be good as having a specific resistance of about 10 Ω · cm at room temperature. However, as having a constant B of smaller than 2000 K, these LaCrO 3 -containing NTC devices are still problematic in that, if their resistance value is controlled in order to use them for rush-current inhibition, their power consumption at the steady state is too large with the result that they are heated too highly and are broken. Tolochko, et al. say that the substitution of a part of Co in LaCoO 3 with Cr is effective for gradually increasing the specific resistance of the thus-substituted LaCo/CrO 3 , as in Izv. Akad. Nauk. SSSR, Neorg. Mater., Vol. 23, No. 5, 1987, page 832, Fig. 3 and lines 38 to 43. In this report, however, they measured the specific resistance of the materials only at 20 °C, and they did not clarify the characteristics of the materials comprising Cr of less than 5 mol%. Given the situation, we, the present inventors have assiduously made various experiments for producing various semiconductive ceramic compositions and for using them under practical conditions, while specifically noting oxides of rare earth elements and Co-type elements, especially LaCoO 3 . The characteristics of LaCoO 3 -containing NTC devices are disclosed by A. H. Wlacov and O. O. Shikerowa in 32, [9], 1990, page 2588, Fig. 2, and page 2587, lines 36 to 42. Thus, it is known that LaCoO 3 have a lower resistance value than GdCoO 3 . However, as compared with the conventional spinel-structured transition metal oxides, such oxides of rare earth elements and Co-type elements have a small constant B, though having a low resistance value at high temperatures, and therefore have not been put to practical use in the art. In Koc et al. "Electrical conductivity and Seebeck coefficient of (La, Ca) (Cr, Co)O 3 " Journal of materials Science, 15 Oct. 1992, UK, Vol. 27, No. 20, Pages 5477-5482 La 1-x Ca x Cr y Co 1-y O 3 and LaCr 1-y Co y O 3 are described. The molar ratio of the sum of lanthanum and calcium, or lanthanum on the one hand and the sum of chromium and cobalt on the other hand is 1. SUMMARY OF THE INVENTION One object of the present invention is to provide a semiconductive ceramic composition having a low specific resistance at room temperature and a large constant B at high temperatures, and also to provide a semiconductive ceramic device which comprises the composition and which can be used for rush-current inhibition for motor start-up retardation, for halogen lamp protection and even in instruments through which large currents shall run. Another object of the present invention is to provide a semiconductive ceramic composition having a low specific resistance and a large constant B at room temperature while still having a large constant B even at temperatures lower than room temperature and also to provide a semiconductive ceramic device usable in temperature compensated crystal oscillators. The object of the present invention is achieved with a semiconductive ceramic composition having the features of claim 1. The subclaims are directed to preferable embodiments. Preferable uses of the inventive semiconductive ceramic composition form the subject matter of claims 5 to 10. The invention will now be described by way of example and with reference to the accompanying drawings in which: Fig. 1 shows the resistance-temperature characteristic of the samples of Example 1 of the present invention and the conventional Example 1. Fig. 2 shows the relationship between the chromium content of the samples of Example 2 of the present invention and the constant B thereof. The chromium content of the semiconductive ceramic composition of the present invention is defined to fall between 0.005 mol% and 30 mol% in terms of chromium. This is because, if the chromium content is smaller than 0.005 mol%, the chromium oxide added is not satisfactorily effective, resulting in the failure in enlarging the constant B of the device made of the composition. If, however, it is larger than 30 mol%, not only the constant B of the device made of the composition is smaller than that of the devices made of chromium-free compositions or conventional compositions having a negative resistance-temperature characteristic but also the specific resistance of the former is merely the same as that of the latter. The chromium content is preferably within the range between 0.1 mol% and 30 mol% in terms of chromium, because in this case the constant B becomes sufficiently large (higher than 3000K). In particular, the chromium content is preferably within the range between 0.1 mol% and 10 mol%, since the device comprising the composition that has a chromium content falling within the range may have a constant B of 4000 K or higher at high temperatures and therefore the device is the most suitable for the inhibition of initial rush currents. In particular, the chromium content is preferably within the range between 0.5 mol% and 10 mol%, since the variation in the specific resistance and the constant B at room temperature of the device that may depend on its chromium content may be small thereby resulting in the success in stable production of temperature-compensating devices having the most desirable resistance-temperature characteristic with which the oscillation frequency from crystal oscillators can be well compensated relative to the ambient temperature. In the composition of the present invention, the molar ratio of lanthanum to the sum of cobalt and chromium is preferably from 0.50/1 to 0.999/1. This is because, if the molar ratio is larger than 0.999/1, the non-reacted lanthanum oxide (La 2 O 3 ) in the sintered ceramic of the composition reacts with water in air to be broken and can no more be used as the intended device. If, however, the molar ratio is smaller than 0.50/1, the device made of the composition is to have a small constant B though having an enlarged specific resistance. Now, the present invention is described in more detail with reference to the following examples, which, however, are not intended to restrict the scope of the invention. Example 1: A cobalt compound of CoCO 3 , Co 3 O 4 or CoO and a lanthanum compound of La 2 O 3 or La(OH) 3 were weighed and ground, to which a chromium compound of Cr 2 O 3 or CrO 3 was added from 0 to 31 mol% in such a manner that the molar ratio of lanthanum to the sum of cobalt and chromium in the resulting mixture might be 0.95/1. The mixture was wet-milled in a ball mill for 24 hours together with pure water and zirconia balls, then dried, and thereafter calcined at from 900 to 1200°C for 2 hours. A binder was added to the thus-calcined powder, which was further wet-milled in a ball mill for 24 hours together with zirconia balls. Then, this was filtered, dried and shaped under pressure into discs, which were baked at from 1200 to 1600°C in air for 2 hours to obtain sintered discs. The both surfaces of these discs were coated with a silver-palladium alloy paste, and baked at from 900 to 1400°C in air for 5 hours, thereby forming outer electrodes on these discs. Thus were formed herein semiconductive ceramic device samples. The specific resistance and the constant B of each sample formed herein were measured, and the data thus measured are shown in Table 1. In Table 1, the samples with the mark "*" are outside the scope of the present invention, and the other samples are within the scope of the invention. The specific resistance (ρ) is obtained from the following equation: ρ(T) = R(T) x S/t where R(T) is the resistance value at T°C, S is the surface area of the outer electrode, and t is the thickness of the semiconductive ceramic device sample. The specific resistance of each sample as prepared in Example 1, that is obtained from the resistance value thereof at -10°C, 25°C and 140°C, may be represented by the following equations: ρ(-10) = R(-10) x S/t ρ(25) = R(25) x S/t ρ(140) = R(140) x S/t The constant B is a constant that indicates the variation in the resistance depending on the variation in temperature. This may be defined as follows: Constant B (T1, T2) = {log ρ(T2)- log ρ(T1)}/(1/T2 - 1/T1) where ρ(T1) and ρ(T2) are the specific resistance at T1°C and T2°C, respectively, and log is a common logarithm. The larger the constant B, the smaller the reduction in the resistance value with the elevation of temperature. On the basis of the above, the constant B of each sample as prepared in Example 1 to be obtained from the specific resistance thereof at -10°C, 25°C and 140°C may be as follows: B (-10, 25) = {log ρ(-10)- log ρ(25)}/{1/(-10 + 273.15) - 1/(25 + 273.15)} B (25, 140) = {log ρ(140)- log ρ(25)}/{1/(140 + 273.15) - 1/(25 + 273.15)} B (-10, 25) is the constant B within the temperature range between -10°C and +25°C; and B (25, 140) is the constant B within the temperature range between 25°C and 140°C. (1) Sample No. (2) Chromium Content (mol%) (3) Constant B (K) (4) Conventional Sample 1 (1) No. (2) mol% ρ (Ω · cm) A/B B (3) (K) D/C 25 140 -10 -10.25 25.140 A B C D 1 * 0 1.9 0.20 2.5 9.5 800 2410 3.0 2 0.005 2.5 0.22 4.7 11.4 1420 2600 1.8 3 0.010 3.6 0.18 7.1 20.0 1510 3190 2.1 4 0.020 5.0 0.19 12.6 26.3 2050 3500 1.7 5 0.050 6.7 0.19 20.6 35.3 2530 3800 1.5 6 0.10 9.5 0.21 37.4 45.2 3080 4100 1.3 7 0.20 12.5 0.19 60.5 66.3 3510 4400 1.3 8 0.50 18.5 0.23 108.1 80.4 3960 4650 1.2 9 1.0 16.1 0.23 101.1 70.0 4120 4530 1.1 10 2.0 14.8 0.22 85.1 67.3 3730 4490 1.2 11 5.0 12.9 0.22 65.7 58.6 3640 4240 1.2 12 10.0 10.9 0.21 51.2 51.3 3470 4020 1.2 13 20.0 12.4 0.56 39.3 22.1 2580 3320 1.3 14 30.0 14.0 1.29 42.9 10.9 2510 2550 1.0 15* 31.0 15.0 2.01 45.5 7.5 2490 2150 0.9 (4) 0.0 10.0 0.97 38.0 10.3 3000 2500 0.8 As in Table 1, both the specific resistance and the constant B of the samples increase with the increase in the chromium content thereof. However, when the chromium content is higher than 0.5 mol%, the specific resistance and the constant B lower; when the chromium content is higher than 20 mol%, the specific resistance increase while the constant B lowers; and when the chromium content is 31 mol%, the constant B (25, 140) is smaller than the constant B (-10, 25). When the chromium content falls between 0.005 mol% and 30 mol%, the constant B (25, 140) is higher than 2500 K. In particular, when the chromium content falls between 0.1 mol% and 10.0 mol%, both the constant B (-10, 25) and the constant B (25, 140) are high, the former being higher than 3000 K and the latter being higher than 4000 K. Fig. 1 is a characteristic graph showing the dependence on temperature of the specific resistance of semiconductive ceramic device samples, in which the vertical axis indicates the specific resistance (Ω · cm) and the horizontal axis indicates the temperature (°C) and in which each curve indicate the difference in the chromium content in each sample. The full lines indicate the samples falling within the scope of the present invention, while the dotted lines indicate those falling outside the invention. As in Fig. 1, the semiconductive ceramic device samples of the present invention have a small specific resistance at 25°C of being not higher than 20 Ω · cm, and still have a small specific resistance even at high temperatures of being not higher than 10 Ω · cm. When a current of 20 A was applied to the semiconductive ceramic device samples as prepared herein, those falling within the scope of the present invention were not broken. Since the samples of the present invention have a large constant B (25, 140), they inhibit the initial overcurrent while consuming a reduced power amount at the steady state. Thus, these are excellent as devices for rush current inhibition, for motor start-up retardation and for halogen lamp protection. Conventional Example 1: Mn 3 O 4 , NiO and Co 3 O 4 were weighed in a ratio by weight of 6:3:1, and wet-milled in a ball mill for 5 hours along with pure water, a binder and zirconia balls. Then, the thus-milled mixture was filtered and dried. Next, in the same manner as in Example 1, the resulting dry powder was shaped under compression into discs, which were baked at 1200°C in air for 2 hours to obtain sintered discs. The both surfaces of these discs were coated with a silver-palladium alloy paste and baked at from 900 to 1100°C for 5 hours in air, to thereby form outer electrodes on the discs. Thus were prepared herein semiconductive ceramic device samples. The electric characteristics of the sample prepared herein were determined in the same manner as in Example 1. Of these, the specific resistance (ρ) and the constant B at the predetermined temperatures are shown in Table 1. The resistance-temperature characteristic is shown in Fig. 1. As in Table 1, the constant B (25, 140) of the semiconductive ceramic device sample of Conventional Example 1 is smaller than the constant B (-10, 25) thereof. Thus, it is known that the energy consumption of this conventional sample is large at the steady state. Comparing the sample of Conventional Example 1 with the samples of Example 1 of the present invention having the same degree of specific resistance as the former, it is known that the samples of Example 1 of the invention have a higher constant B (25, 140). In general, the reduction in the specific resistance results in the reduction in the constant B. As opposed to this, however, it is known that the semiconductive ceramic composition of the present invention which comprises LaCoO 3 and from 0.005 to 30 mol% of chromium added thereto has a higher constant B than the sample of Conventional Example 1. Example 2: A powdery lanthanum compound of La 2 O 3 or La(OH) 3 and a powdery cobalt compound of CoCO 3 , Co 3 O 4 or CoO were weighed in a molar ratio of - lanthanum to cobalt of 0.95/1, to which was added from 0.01 to 40 mol% of a chromium compound of Cr 2 O 3 or CrO 3 . The mixture was wet-milled in a ball mill for 16 hours together with pure water and nylon balls, then dried, and thereafter calcined at from 900 to 1200 °C for 2 hours. The resulting mixture was further ground in a jet mill, to which was added 5 % by weight of a vinyl acetate binder along with pure water. This was again wet-milled, then dried and granulated. The resulting granules were shaped under pressure into discs, which were baked at from 1200 to 1600°C in air for 2 hours to obtain sintered discs. The both surfaces of these discs were screen-printed with a silver-palladium alloy paste, and baked at from 900 to 1200°C in air for 5 hours, thereby forming outer electrodes on these discs. Thus were formed herein semiconductive ceramic device samples. The specific resistance and the constant B of each sample formed herein were measured in the same manner as in Example 1, and the data thus measured are shown in Table 2. In Table 2, the samples with the mark "*" did not have the intended characteristics applicable to the use of the samples as semiconductive ceramic devices for TCXO. The specific resistance was derived from the resistance value at 25 °C according to the equation employed in Example 1. To obtain the constant B, used herein were the same equations as those in Example 1. Thus, of the samples of Example 2, the constant B was derived from the specific resistance thereof at -30°C, 25°C, 50°C and 140°C to be as follows: B (-30, 25) = {log ρ(-30)- log ρ(25)}/{1/(-30 + 273.15) - 1/(25 + 273.15)} B (25, 50) = {log ρ(50)- log ρ(25)}/{1/(50 + 273.15) - 1/(25 + 273.15)} B (25, 140) = {log ρ(140)- log ρ(25)}/{1/(140 + 273.15) - 1/(25 + 273.15)} B (-30, 25) is the constant B within the temperature range between -30°C and +25°C; B (25, 50) is the constant B within the temperature range between 25°C and 50°C; and B (25, 140) is the constant B within the temperature range between 25°C and 140°C. (1) Sample No. (2) Chromium Content (mol%) (3) Specific Resistance, ρ (25), Ω · cm (4) Constant B (K) (5) Conventional Sample 2 (1) No. (2) mol% (3) ρ(25) Ω · cm B (4) (K) -30.25 25.50 25.140 1 * 0.01 2.0 1160 2200 3150 2 * 0.05 3.9 1380 2510 3200 3 0.1 9.1 3010 3040 3390 4 0.5 14.6 3310 3700 4010 5 1.0 18.7 3760 4080 4430 6 1.5 18.6 3930 4170 4560 7 2.0 17.7 3990 4140 4620 8 2.5 17.2 4040 4200 4620 9 3.0 16.8 4040 4190 4610 10 3.5 16.4 4030 4180 4610 11 4.0 15.9 4040 4130 4600 12 4.5 15.9 4020 4160 4590 13 5.0 16.2 3980 4130 4590 14 6.0 16.1 4010 4130 4570 15 7.0 17.5 3940 4110 4550 16 8.0 19.3 3890 4070 4520 17 9.0 21.0 3840 4060 4500 18 10.0 23.5 3810 4030 4470 19 15.0 31.4 3670 3900 4380 20 20.0 37.6 3480 3760 4190 21 25.0 42.8 3340 3650 4100 22 30.0 48.9 3200 3510 4010 23* 35.0 55.1 3020 3250 3620 24* 40.0 59.3 2890 3010 3230 (5) 0.0 16.2 2760 2750 2750 As in Table 2, the specific resistance of the samples increases and the constant B thereof increases to be higher than 3000 K with the increase in the chromium content of the samples. When the chromium content is not higher than 0.05 mol%, the constant B (-30, 25), (25, 50) is lower than 3000 K, and when the chromium content is higher than 30.0 mol%, the specific resistance is above 50 Ω · cm. Both are not suitable for temperature compensation. As opposed to these, the samples falling within the scope of the present invention have low specific resistance. Using these, therefore, the surface area of the electrode of the devices having a predetermined resistance value may be reduced and the capacitance of the devices may be small. Accordingly, the accuracy of the devices of the present invention, when used in temperature-compensating circuits for temperature compensation in TCXO, is high. With the increase in the constant B (-30, 25), the variation in the resistance value, relative to temperature, increases, resulting in that the devices in temperature-compensating circuits in TCXO can compensate low temperatures falling within a broad range. It is known from Table 2 that the constant B (25, 50) and the constant B (25, 140) of the samples of the present invention are both higher than the constant B (-30, 25) thereof. When the chromium content of the samples fall between 0.1 mol% and 30 mol%, all the constant B (-30, 25), the constant B (25, 50) and the constant B (25, 140) are higher than 3000 K. In particular, when the chromium content of the samples fall between 0.5 mol% and 10.0 mol%, the variation in the resistance-temperature characteristic, relative to the chromium content, is stably small. Thus, the samples of the present invention having a chromium content of from 0.5 mol% to 10.0 mol% are the most suitable as NTC devices to be in temperature-compensating circuits in TCXO. Fig. 2 shows the relationship between the chromium content of the semiconductive ceramic device samples prepared in Example 2 and the constant B thereof, in which the vertical axis indicates the constant B (K) and the horizontal axis indicates the chromium content (mol%). In Fig. 2,  (filled circle) indicates the constant B (-30, 25); ▪ (filled rectangle) indicates the constant B (25, 50), and Δ indicates the constant B (25, 140). As in Fig. 2, the samples having a chromium content of 0.1 mol% or higher all have a constant B of higher than 3000 K. Conventional Example 2: A semiconductive ceramic device sample was prepared herein in the same manner as in Example 2, except that Mn 3 O 4 , NiO and Co 3 O 4 as weighed in a ratio by weight of 6:3:1 were used herein. The characteristics of the sample prepared herein were determined in the same manner as in Example 2. The data are shown in Table 2. As in Table 2, the constant B (25, 50) at higher temperatures of the semiconductive ceramic device sample of Conventional Example 2 is smaller than the constant B (-30, 25) thereof at lower temperatures. In addition, the both constants B are smaller than 3000 K. In the composition of the present invention, the molar ratio of lanthanum to the sum of cobalt and chromium is not limited to only 0.95/1 but may be within the scope between 0.50/1 and 0.999/1. If the molar ratio of lanthanum to me sum of cobalt and chromium is larger than 0.999/1, the non-reacted La 2 O 3 in the sintered ceramic reacts with water in air to be broken and can no more be used as the intended device. If, however, the molar ratio is smaller than 0.50/1, the sintered ceramic is to have a small constant B though having an enlarged specific resistance. If so, its constant B is smaller than the constant B of conventional semiconductive ceramic devices, and the device comprising the sintered ceramic thus having such a small constant B is not suitable to the use to which the present invention is directed. In the above-mentioned examples, produced were semiconductive ceramic discs. However, the semiconductive ceramic device of the present invention is not limited to only the shape of such discs but may be in any other form of laminated devices, cylindrical devices, square chips, etc. In the above-mentioned examples, a silver palladium alloy or platinum was used to form the outer electrodes on the semiconductive ceramic devices. However, such is not limitative, but any other electrode material of, for example, silver, palladium, nickel, copper, chromium or their alloys may also be employed to obtain similar characteristics. As has been described in detail hereinabove, since the semiconductive ceramic composition of the present invention comprises a lanthanum cobalt oxide as a component, it has a small specific resistance at room temperature while having a higher constant B at high temperatures than at low temperatures. And, according to the present invention, when the semiconductive ceramic composition comprises chromium oxide in an amount of from 0.005 to 30 mol% in terms of chromium as the second component, the composition may have a small specific resistivity at the steady state, while having a high constant B of higher than 3000 K at high temperatures. Further, when the semiconductive ceramic composition of the present invention consists of, as the essential component, a lanthanum cobalt oxide and, as the side component, a chromium oxide in an amount of from 0.1 to 30 mol% in terms of chromium, it has a small specific resistance at the steady state and has a high constant B of higher than 3000 K. In particular, the composition having a chromium content of from 0.5 to 10 mol% may have a high constant B of higher than 3500 K at high temperatures. In particular, the composition having a chromium content of from 0.1 to 10 mol% may have a much higher constant B of higher than 4000 K at high temperatures. As having the above-mentioned characteristics, the semiconductive ceramic composition of the present invention can be used for forming devices to be usable in temperature-compensated crystal oscillators and those to be usable for rush current inhibition, for motor start-up retardation and for halogen lamp protection. In addition, since the semiconductive ceramic composition of the present invention comprises a lanthanum cobalt oxide while containing a chromium oxide in an amount of from 0.005 to 30 mol% in terms of chromium, it has a low specific resistance at the steady state while having a high B constant of higher than 2500 K at high temperatures. Thus, being different from that of conventional semiconductive ceramic devices, the devices using the composition of the present invention have large difference in the resistance between the electrification thereof at room temperature and that at high temperatures (140°C or so). Moreover, since the semiconductive ceramic device using the composition of the present invention comprises a lanthanum cobalt oxide, it has a small constant B at room temperature while having a large constant B at high temperatures. Therefore, the device consumes a reduced amount of energy at the steady state, and therefore can be used in instruments through which large currents shall run. In addition, the semiconductive ceramic device using the compostition of the present invention which consists of, as the essential component, a lanthanum cobalt oxide and , as the side component, a chromium oxide in an amount of from 0.1 to 30 mol% in terms of chromium, has a low specific resistance at room temperature while having a high constant B of higher than 3000 K. As having such improved characteristics, the semiconductive ceramic device using the composition of the present invention can be used for rush current inhibition, for motor start-up retardation and for halogen lamp protection, and can be used in temperature-compensated crystal oscillators. Temperature-compensated crystal oscillators have been specifically referred to herein, in which the device of the present invention is usable. Apart from these, the device is usable in any other temperature-compensating circuits to be in other instruments.

Claims: A semiconductive ceramic composition having a negative resistance-temperature characteristic and a composition La p (Cr z Co 1-z ) q O 3 with 0.5 ≤ p / q ≤ 0,999 and 0.00005 ≤ z ≤ 0.3. A semiconductive ceramic composition according to claim 1, wherein 0.001 ≤ z ≤ 0.3. A semiconductive ceramic composition according to claim 2, wherein 0.001 ≤ z ≤ 0.1. A semiconductive ceramic composition according to claim 3, wherein 0.005 ≤ z ≤ 0.1. Use of the semiconductive ceramic composition according to one of claims 1 to 4 for a device having a negative resistance-temperature characteristic. Use of the semiconductive ceramic composition according to one of claims 1 to 4 for a device for rush-current inhibition, or motor start-up retardation, or halogen lamp protection. Use of the semiconductive ceramic composition according to one of claims 2 to 4 for a device in temperature-compensated crystal oscillators. Use of the semiconductive ceramic composition according to one of claims 1 to 4 for a semiconductive ceramic device having an electrode provided on the surface of said semiconductive ceramic device. Use of the semiconductive ceramic composition according to one of claims 1 to 4 for a semiconductive ceramic device for rush-current inhibition, or motor start-up retardation, or halogen lamp protection, and said semiconductive ceramic device has an electrode provided on the surface thereof. Use of the semiconductive ceramic composition according to one of claims 2 to 4 for a semiconductive ceramic device in temperature-compensated crystal oscillators, and said semiconductive ceramic device has an electrode provided on the surface thereof.

Inventors: ISHIKAWA TERUNOBI, NAKAYAMA AKINORI, SAKABE YUKIO, TAKAGI HIROSHI, ISHIKAWA, TERUNOBI, NAKAYAMA, AKINORI, SAKABE, YUKIO, TAKAGI, HIROSHI
Applicants: MURATA MANUFACTURING CO, MURATA MANUFACTURING CO., LTD.
Application year: 1997
Main classification: H01C7
IPC codes: C04B35, H01C7