Dielectric ceramic composition for high frequencies

Information

  • Patent Grant
  • 4102696
  • Patent Number
    4,102,696
  • Date Filed
    Wednesday, July 28, 1976
    47 years ago
  • Date Issued
    Tuesday, July 25, 1978
    45 years ago
Abstract
A dielectric ceramic composition for high frequencies consisting essentially of 83 to 99.8 wt% of a basic composition composed of 22 to 43 wt% of titanium dioxide, 38 to 58 wt% of zirconium dioxide and 9 to 26 wt% of stannic oxide, and 0.2 to 17 wt% of one or two addditives selected from the group consisting of lanthanum oxide, cobaltic oxide and zinc oxide. The dielectric ceramic composition has high permittivity and high Q and is suitable for use as dielectric resonators in microwave bandpass filters, or as antennas employed at microwave frequencies, or as substrates for microwave circuits.
Description

BACKGROUND AND SUMMARY OF THE INVENTION
This invention relates to a dielectric ceramic composition for high frequencies. More particularly, the invention relates to a dielectric ceramic composition for microwave devices designed to operate at frequencies of 300 MHz to 30 GHz, having high permittivity and high Q and being stable in temperature characteristics.
Recently, it has been attempted to miniaturize microwave circuits with the advance of technology in high frequency circuits designed to operate at microwave and millimeter wave frequencies having a wave length of not more than several ten centimeters.
In such high frequency circuits, there have been used cavity resonators and antennas. However, such conventional elements must have the sizes corresponding to the wave lengths of microwaves so that the use of such elements is an obstacle to miniaturize the circuits. In order to overcome such a disadvantage, it has been proposed to use dielectric ceramic materials in place of conventional metal materials. Many of the dielectric ceramic materials commonly used consist essentially of compositions of the titanate system, such as CaTiO.sub.3 -MgTiO.sub.3 -La.sub.2 O.sub.3.sup.. 2TiO.sub.2 or MgTiO.sub.3 -CaTiO.sub.3. It is, however, impossible with such compositions to produce dielectric elements having adequate characteristics required for the application to the microwave devices. Although the dielectric materials are required to have low dielectric loss, high permittivity and small temperature coefficient of permittivity, none of said compositions have sufficient characteristics which satisfy the above requirements, simultaneously.
It is therefore an object of the present invention to provide a dielectric ceramic composition for high frequencies having high permittivity and high Q (i.e., low dielectric loss).
Another object of the present invention is to provide a dielectric ceramic composition for high frequencies having small temperature coefficient of resonant frequency.
A further object of the present invention is to provide a dielectric ceramic composition for high frequencies which makes it possible to obtain dielectric ceramic elements having an optional temperature coefficient of resonant frequency in the range of from - 20 .times. 10.sup.-6 /.degree. C. to + 56 .times. 10.sup.-6 /.degree. C. by the variation of the compositional proportions.
According to the present invention, there is provided a dielectric ceramic composition for high frequencies consisting essentially of 83 to 99.8 wt% of a basic composition composed of 22 to 43 wt% of titanium dioxide (TiO.sub.2), 38 to 58 wt% of zirconium dioxide (ZrO.sub.2) and 9 to 26 wt% of stannic oxide (SnO.sub.2), and 0.2 to 17 wt% of one or two additive selected from the group consisting of lanthanum oxide (La.sub.2 O.sub.3), cobaltic oxide (Co.sub.2 O.sub.3) and zinc oxide (ZnO).
When lanthanum oxide is used alone as the additive, the content thereof is preferably from 0.5 to 10 wt%. However, when lanthanum oxide is used together with zinc oxide as the additive, the content thereof is preferably not more than 2 wt%. When cobaltic oxide is used alone or together with zinc oxide as the additive, the content thereof is preferably not more than 10 wt%. When zinc oxide is used alone or together with lanthanum oxide or cobaltic oxide as the additive, the content thereof is preferably not more than 7 wt%. However, when zinc oxide is used alone, the content thereof is preferably not less than 1.2 wt%.
The above-mentioned limitation on the proportion of the constituents is required for the following reasons.
If titanium dioxide is less than 22 wt%, the permittivity of the products becomes small while on the other hand larger amount than 43 wt% causes the great increase of the temperature coefficient of resonant frequency. If zirconium dioxide is present in an amount less than 38 wt% or more than 58 wt%, the temperature coefficient of resonant frequency becomes too large. If stannic oxide is present in an amount smaller than 9 wt%, Q becomes small, and larger amount than 26 wt% causes the increase of the temperature coefficient of resonant frequency.
In cases where lanthanum oxide is used alone as the additive, if lanthanum oxide present is smaller than 0.5 wt%, the sintering of the product becomes insufficient, resulting in the deterioration of the permittivity and Q while on the other hand larger amount than 10 wt% causes the deterioration of Q. In cases where lanthanum oxide is used together with zinc oxide as the additive, if lanthanum oxide present is larger than 2 wt%, it causes the deterioration of Q.
In cases where cobaltic oxide is used alone or together with zinc oxide as the additive, if cobaltic oxide present is larger than 10 wt%, it causes the deterioration of the permittivity and Q. In cases where cobaltic oxide is used alone, if cobaltic oxide present is samller than 0.2 wt%, it is impossible to obtain a sufficiently sintered ceramic body.
In cases where zinc oxide is used alone or together with lanthanum oxide or cobaltic oxide as the additive, if zinc oxide present is larger than 7 wt%, it causes the deterioration of the permittivity and Q. In cases where zinc oxide is used alone, if zinc oxide present is smaller than 1.2 wt%, it is impossible to obtain a sufficiently sintered ceramic body.
The dielectric ceramic compositions of the present invention may be prepared by technique conventionally employed for the production of dielectric ceramic compositions. A preferred method, however, hereinafter described, consists in the use of highly purified oxides.
The highly purified oxides, viz, TiO.sub.2, ZrO.sub.2, SnO.sub.2, La.sub.2 O.sub.3, ZnO are used as starting materials for the preparation of the dielectric ceramic materials of the examples shown in Tables 1 and 2. In each example, the mixture of powdered starting materials having the compositional proportion shown in Tables 1 and 2 was ball milled with water for 16 hours, then the resulting mixture was dehydrated, dried and molded into a disk having a diameter of 12 mm and a thickness of 5.5 mm under a pressure of 2500 kg/cm.sup.2. The disk was sintered in natural atmosphere at 1320.degree. C. for 4 hours to convert it to a dielectric ceramic body.
The measurements of the electrical properties were made for each ceramic body of the examples. The results obtained are shown in Tables 1 and 2. The properties given in the tables are the permittivity, Q and temperature coefficient of resonant frequency at a microwave frequency of 7 GHz and at 25.degree. C. In the tables, the asterisks (*) designate compositions beyond the scope of the present invention.
The permittivity and Q at microwave frequency were measured by the well-known dielectric resonant method. The temperature coefficient of resonant frequency, TC(fo), represents the change rate of the resonant frequency (fo) over the temperature range of from +25.degree. to +85.degree. C. The change rate of resonant frequency, TC(fo), on temperature was derived from the temperature coefficient of permittivity, TC(.epsilon.), and the temperature coefficient of expansion, .alpha., of the ceramic body. Thus, the relationship between the temperature coefficient of resonant frequency, TC(fo), and the temperature coefficient of permittivity, TC(.epsilon.), is given by the equation:
TC(fo)=- 1/2 TC(.epsilon.) - .alpha.
it will be seen from the results shown in Tables 1 and 2 that according to the present invention it is possible to obtain dielectric ceramic compositions having high permittivity in the range of 29.3 to 44.2 and high Q in the range of 4100 to 9500 at microwave frequencies and at 25.degree. C. In addition, the dielectric ceramic compositions of the present invention have small temperature coefficients of resonant frequency. Furthermore, according to the present invention it is possible to prepare a dielectric ceramic composition having an optional temperature coefficient of resonant frequency in the range of from - 20 .times. 10.sup.-6 /.degree. C. to + 56 .times. 10.sup.-6 /.degree. C. by the variation of the compositional proportions, thus making it possible to provide dielectric ceramic elements with the temperature compensating function for the other electrical elements in the high frequency circuits in which said ceramic elements are incorporated. Thus, the dielectric ceramic compositions according to the invention are suitable for use as dielectric resonators in microwave bandpass filters, or as antennas employed at microwave frequencies, or as substrates for microwave circuits.
Table 1__________________________________________________________________________Basic Additivecomposition (wt %) (wt %) TCEx. TiO.sub.2 ZrO.sub.2 SnO.sub.2 La.sub.2 O.sub.3 .epsilon. Q (.times. 10.sup.-6 /.degree. C.)__________________________________________________________________________1* 20 56 24 4.0 32.7 5800 -102 22 52 26 " 32.9 5700 -123 22 58 20 " 33.0 6000 +394 24 52 24 " 33.4 6500 - 85 24 56 20 " 33.5 5900 + 26 28 48 24 " 33.5 6000 - 97 28 52 20 " 34.2 6600 - 48 28 56 16 " 34.7 5300 +229 32 44 24 " 34.5 6800 -1610 32 48 20 " 34.6 6800 - 411 32 52 16 " 35.6 5100 + 112 32 56 12 " 36.7 4700 +2513 33 58 9 " 37.8 4100 +3614 36 38 26 " 35.6 6000 + 415 36 44 20 " 36.2 6800 - 716 36 48 16 " 36.9 6100 - 117 36 52 12 " 37.8 4900 +1118* 40 36 24 " 42.2 6200 +7619 40 40 20 " 39.6 6000 +2420 40 44 16 " 39.0 6000 + 421 40 48 12 " 39.0 5000 + 922 43 38 19 " 39.2 5700 +5623 43 48 9 " 42.1 4900 +2424* 46 42 12 " 45.6 5000 +7625 22 52 26 0.5 29.3 350026 " " " 1 33.1 520027 " " " 4 32.9 5700 -12.+-.528 " " " 10 32.9 490029* " " " 20 32.8 250030 32 52 16 0.5 32.4 300031 " " " 4 35.6 5100 + 1.+-.532 " " " 10 35.5 430033* " " " 20 35.5 200034 36 38 26 0.5 31.8 400035 " " " 1 35.7 540036 " " " 4 35.6 6000 + 4.+-.537 " " " 10 35.6 420038* " " " 20 35.6 290039 40 48 12 0.5 36.1 310040 " " " 1 39.1 440041 " " " 4 39.0 5000 + 9.+-.542 " " " 10 39.0 420043* " " " 20 38.9 200044* 20 56 24 0.5 33.6 8200 -1045 22 52 26 " 33.7 9000 -1146 22 58 20 " 33.8 8400 +4047 24 52 24 " 34.0 8900 - 948 24 56 20 " 34.2 8400 049 28 48 24 " 34.5 8300 -1050 28 52 20 " 35.0 9000 - 551 28 56 16 " 35.5 7800 +2052 32 44 24 " 35.3 9200 -1553 32 48 20 " 35.5 9500 - 554 32 52 16 " 36.3 8400 + 155 32 56 12 " 37.4 7100 +2156 33 58 9 " 38.6 6500 +3557 36 38 26 " 36.5 8600 + 458 36 44 20 " 37.0 9200 - 859 36 48 16 " 37.7 8500 - 160 36 52 12 " 38.6 7400 +1061* 40 36 24 " 43.1 8600 +7562 40 40 20 " 40.4 8600 +2063 40 44 16 " 39.7 8400 + 464 40 48 12 " 39.9 7500 + 865 43 38 19 " 44.0 8100 +5166 43 48 9 " 42.9 7400 +2367* 46 42 12 " 46.3 7600 +7368 22 52 26 0.2 33.4 820069 " " " 0.5 33.7 900070 " " " 1 33.0 880071 " " " 3 31.5 7600 -11.+-.772 " " " 5 30.9 720073 " " " 10 29.5 600074* " " " 20 28.4 420075 32 52 16 0.5 36.3 840076 " " " 1 35.7 7600 +1.+-.777 " " " 10 32.1 550078* " " " 20 31.0 410079 36 38 26 0.2 36.4 800080 " " " 0.5 36.5 860081 " " " 1 35.9 8300 +4.+-.782 " " " 3 34.5 720083 " " " 10 32.2 580084* " " " 20 31.1 410085 40 48 12 0.5 39.9 750086 " " " 1 39.2 6600 +8.+-.787 " " " 5 36.9 550088* " " " 20 34.4 340089* 28 58 14 1.5 35.0 5100 +3290 30 46 24 " 33.0 7600 -2091 30 30 12 " 36.0 4800 +3792 31 51 18 " 34.3 6100 - 193 31 54 15 " 35.4 5900 +1394* 32 42 26 " 33.0 7500 -5295 33 58 9 " 37.5 4500 +3896 34 45 21 " 35.0 7800 -1097 34 48 18 " 35.5 7400 - 398 34 51 15 " 36.1 6400 + 199 34 54 12 " 37.5 5400 +12100 36 40 24 " 35.0 7000 -33101 37 42 21 " 36.2 7000 - 9102 37 45 18 " 36.6 7400 - 7103 37 48 15 " 37.7 6300 + 1104 37 51 12 " 37.7 5500 + 8105 40 42 18 " 39.0 7000 + 7106 40 45 15 " 38.5 6300 + 4107 40 48 12 " 38.9 5900 + 5108 43 40 17 " 42.5 6500 +32109 43 48 9 " 41.9 5600 +23110* 46 42 12 " 46.6 6000 +75__________________________________________________________________________
Table 2__________________________________________________________________________Basic Additivecomposition (wt %) (wt %) TCExample TiO.sub.2 ZrO.sub.2 SnO.sub.2 ZnO La.sub.2 O.sub.3 .epsilon. Q (.times. 10.sup.-6 /.degree. C.)__________________________________________________________________________111* 20 56 24 1.0 0.5 33.8 6500 - 9112 22 52 26 " " 33.9 6400 -12113 22 58 20 " " 33.9 6700 +43114 24 52 24 " " 34.2 7300 - 9115 24 56 20 " " 34.4 6500 0116 28 48 24 " " 34.7 6800 -11117 28 52 20 " " 35.2 7200 - 5118 28 56 16 " " 35.7 5900 +21119 32 44 24 " " 35.6 7400 -16120 32 48 20 " " 35.7 7500 - 4121 32 52 16 " " 36.5 5800 + 1122 32 56 12 " " 37.5 6400 +20123 33 58 9 " " 38.8 4800 +38124 36 38 26 " " 36.7 6900 + 4125 36 44 20 " " 37.2 7700 - 7126 36 48 16 " " 37.9 6800 - 1127 36 52 12 " " 38.8 5500 +12 128* 40 36 24 " " 43.3 6900 +79129 40 40 20 " " 40.6 6700 +21130 40 44 16 " " 39.9 6600 + 4131 40 48 12 " " 40.2 5700 + 7132 43 38 19 " " 44.2 6400 +55123 43 48 9 " " 43.1 5700 +25 134* 46 42 12 " " 46.5 5600 +75135 22 52 26 0.5 0.2 34.3 6800136 " " " " 1 34.3 5000 137* " " " " 3 34.2 500138 " " " 1 0.5 33.9 6400 -12.+-.5139 " " " 3 2 33.0 5000140 " " " 7 0.2 31.9 4900 141* " " " " 3 31.9 300 142* " " " 10 2 30.7 500143 32 52 116 0.5 0.2 36.7 6200 144* " " " " 3 36.6 200145 " " " 1 0.5 36.5 5800146 " " " " 1 36.4 4900147 " " " 3 " 35.6 5500 + 1.+-.5148 " " " " 2 35.5 4300 149* " " " " 3 35.5 300150 " " " 7 0.2 34.3 4200 151* " " " " 3 34.2 200 152* " " " 10 2 33.1 300153 36 38 26 0.5 0.5 36.7 6900154 " " " " 2 36.9 4900 155* " " " " 3 36.8 300 + 4.+-.5156 " " " 1 2 36.7 4500157 " " " 7 0.5 34.8 4500 158* " " " " 3 34.6 200159 43 38 19 0.5 0.2 40.5 6100 160* " " " " 3 40.4 500161 " " " 1 0.5 40.2 5700162 " " " 3 1 39.3 5400 + 7.+-.6163 " " " " 2 39.2 4800 164* " " " 7 3 38.1 200 165* " " " 10 1 36.8 1900 166* 20 56 24 1.5 0.25 32.5 6800 -12167 22 52 26 " " 32.7 6600 - 8168 22 58 20 " " 32.8 6900 +39169 24 52 24 " " 33.1 7500 - 9170 24 56 20 " " 33.3 6900 - 1171 28 48 24 " " 33.5 6900 -11172 28 52 20 " " 34.0 7500 - 4173 28 56 16 " " 34.6 6200 +21174 32 44 24 " " 34.3 7700 -16175 32 48 20 " " 34.5 7800 - 5176 32 52 16 " " 35.4 6000 0177 32 56 12 " " 36.5 5600 +23178 33 58 9 " " 37.6 5100 +36179 36 38 26 " ` 35.4 7000 + 7180 36 44 20 " " 36.0 7700 - 9181 36 48 16 " " 36.7 7000 - 1182 36 52 12 " " 37.7 5800 + 9 183* 40 36 24 " " 42.0 7100 +78184 40 40 20 " " 39.4 7000 +18185 40 44 16 " " 38.8 6900 + 3186 40 48 12 " " 38.9 5900 + 9187 43 38 19 " " 39.0 6600 +52188 43 48 9 " " 42.0 5800 +26 189* 46 42 12 " " 45.4 6000 +78190 22 52 26 0.5 0.5 32.9 7300191 " " " " 1 32.6 7600192 " " " " 10 30.5 6100 193* " " " " 20 29.7 5000194 " " " 1.5 1 32.3 7100195 " " " " 3 31.6 7200196 " " " " 10 30.5 6400 197* " " " " 20 29.9 5500 -8.+-.4198 " " " 3.0 1 31.6 6500199 " " " " 3 30.6 6400 200* " " " " 20 28.6 4400201 " " " 7.0 0.5 30.5 5200202 " " " " 3 29.3 5000 203* " " " " 20 27.4 3000 204* " " " 10.0 3 28.4 4500 205* " " " " 10 27.2 3600206 32 " 16 0.5 1 35.4 6900207 " " " " 10 34.3 5400 208* " " " " 20 33.2 4300 +1.+-.5209 " " " 3.0 3 33.5 5800210 " " " 7.0 0.5 33.2 4500 211* " " " 10.0 3 31.1 3900212 36 38 26 0.5 1 35.5 7800 213* " " " " 20 32.6 5500214 " " " 1.5 3 34.4 7500215 " " " " 10 33.3 6800 -7.+-.4216 " " " 3 3 33.4 6800217 " " " 7 10 31.1 4500 218* " " " " 20 30.2 3400 219* " " " 10 10 30.0 4000220 40 48 12 0.5 10 36.8 5300221 " " " 1.5 3 37.8 6400222 " " ` 3 1 37.9 5800 +9.+-.4 223* " " " 7 20 33.7 2300 224* " " " 10 3 34.7 3800__________________________________________________________________________The invention being thus described, it will be obvious that the same maybe varied in many ways. Such variations are not to be regarded as adeparture from the spirit and scope of the invention, and all suchmodifications as would be obvious to one skilled in the art are intendedto be included within the scope of the following claims.
Claims
  • 1. A dielectric ceramic composition for high frequencies consisting essentially of 83 to 99.8 wt% of a basic composition composed of 22 to 43 wt% of titanium dioxide dioxide, 38 to 58 wt% of zirconium and 9 to 26 wt% of stannic oxide, and 0.2 to 17 wt% of one or two additives selected from the group consisting of lanthanum oxide and cobaltic oxide.
  • 2. A dielectric ceramic composition according to claim 1 wherein said additive is lanthanum oxide and wherein said lanthanum oxide is present in an amount of from 0.5 to 10 wt%.
  • 3. A dielectric ceramic composition according to claim 1 wherein said additive is cobaltic oxide and wherein said cobaltic oxide is present in an amount of from 0.2 to 10 wt%.
  • 4. A dielectric ceramic composition according to claim 1 wherein said additive is lanthanum oxide and further containing zinc oxide, said lanthanum oxide being present in an amount of not more than 2 wt%, said zinc oxide being present in an amount of not more than 7 wt%.
  • 5. A dielectric ceramic composition according to claim 1 wherein said additive is cobaltic oxide and further containing zinc oxide, said cobaltic oxide being present in an amount of 0.2 to 10 wt%, said zinc oxide being present in an amount of not more than 7 wt%.
Priority Claims (4)
Number Date Country Kind
50-93983 Jul 1975 JP
50-93984 Jul 1975 JP
50-93985 Jul 1975 JP
50-93986 Jul 1975 JP
US Referenced Citations (2)
Number Name Date Kind
2668118 Jonker Feb 1954
2962452 Counts et al. Nov 1960
Foreign Referenced Citations (1)
Number Date Country
1,386,509 Mar 1975 GB