JPH0775206B2 - Microwave / millimeter wave magnetic composition - Google Patents

Microwave / millimeter wave magnetic composition

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Publication number
JPH0775206B2
JPH0775206B2 JP1153129A JP15312989A JPH0775206B2 JP H0775206 B2 JPH0775206 B2 JP H0775206B2 JP 1153129 A JP1153129 A JP 1153129A JP 15312989 A JP15312989 A JP 15312989A JP H0775206 B2 JPH0775206 B2 JP H0775206B2
Authority
JP
Japan
Prior art keywords
microwave
4πms
millimeter wave
present
composition
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired - Lifetime
Application number
JP1153129A
Other languages
Japanese (ja)
Other versions
JPH0319204A (en
Inventor
健弘 鴻池
博 田村
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Murata Manufacturing Co Ltd
Original Assignee
Murata Manufacturing Co Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Murata Manufacturing Co Ltd filed Critical Murata Manufacturing Co Ltd
Priority to JP1153129A priority Critical patent/JPH0775206B2/en
Publication of JPH0319204A publication Critical patent/JPH0319204A/en
Publication of JPH0775206B2 publication Critical patent/JPH0775206B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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  • Magnetic Ceramics (AREA)
  • Soft Magnetic Materials (AREA)

Description

【発明の詳細な説明】 <産業上の利用分野> この発明は、マイクロ波やミリ波などの高周波領域にお
いて使用される磁性体組成物に関するものである。
DETAILED DESCRIPTION OF THE INVENTION <Industrial field of application> The present invention relates to a magnetic material composition used in a high frequency region such as a microwave and a millimeter wave.

<従来の技術> 従来、高周波用磁性体材料としては、Mn−Mgフェライ
ト、Ni−Znフェライト、YIGフェライト、リチウムフェ
ライトなどが用いられている。
<Prior Art> Conventionally, Mn-Mg ferrite, Ni-Zn ferrite, YIG ferrite, lithium ferrite and the like have been used as high frequency magnetic material.

これらは、飽和磁化(4πMs)の値が500〜4000ガウス
を有する優れた材料である。
These are excellent materials with saturation magnetization (4πMs) values of 500-4000 Gauss.

これらの中でも特にリチウムフェライトは4πMsが3700
ガウス程度と大きく、かつキュリー点(Tc)が650℃付
近の高い温度にあるため、4πMsの室温付近における温
度変化率が小さいので、高安定なアイソレータやサーキ
ュレータなどの回路素子に応用可能な材料である。
Among them, especially lithium ferrite has 4πMs of 3700
Since it is as large as Gaussian and has a high Curie point (Tc) near 650 ° C, the temperature change rate near room temperature of 4πMs is small, so it is a material that can be applied to circuit elements such as highly stable isolators and circulators. is there.

<発明が解決しようとする課題> しかしながら、リチウムフェライトは、強磁性共鳴吸収
半値幅(ΔH)や誘電損失(tan δe)等の損失が他の
マイクロ波・ミリ波用フェライトに比べて大きいという
欠点を有している。
<Problems to be Solved by the Invention> However, lithium ferrite has a drawback that losses such as ferromagnetic resonance absorption half-value width (ΔH) and dielectric loss (tan δe) are larger than those of other ferrites for microwaves and millimeter waves. have.

例えば、純粋なリチウムフェライトLi0.5Fe2.5O4はΔH
とtan δeが周波数10GHzで、それぞれ500エルステッド
以上、0.01以上と大きく、実際のマイクロ波・ミリ波用
回路素子には使用できない場合が多い。
For example, pure lithium ferrite Li 0.5 Fe 2.5 O 4 has ΔH
And tan δe at a frequency of 10 GHz are as large as 500 Oersted or more and 0.01 or more, respectively, and often cannot be used for actual microwave / millimeter wave circuit elements.

この発明は上記のような問題点に鑑みてなされたもの
で、Li0.5Fe2.5O4の一部をZnで置換して4πMsを高め
て、高い周波数帯で使用できるようにし、かつZnの量を
適宜変化させることにより、4πMsを任意の値に設定で
きるようにすると共に、PbOを添加含有させてΔHとtan
δeについて改善されたマイクロ波・ミリ波用磁性体
材料を提供することを目的としている。
The present invention has been made in view of the above problems, and a part of Li 0.5 Fe 2.5 O 4 is replaced with Zn to increase 4πMs so that it can be used in a high frequency band, and the amount of Zn 4πMs can be set to an arbitrary value by appropriately changing the value, and PbO is added to contain ΔH and tan.
It is an object of the present invention to provide a microwave / millimeter wave magnetic material material having an improved δe.

<課題を解決するための手段> 上記目的を達成するために、この発明のマイクロ波・ミ
リ波用磁性体組成物はLixFeyZnzO0.5+y+0.5z(但
し、x+y+z )で表わされる組成において、x、y、
zがそれぞれ0.10≦x≦0.21、0.77≦y≦0.88、0.02≦
z≦0.13の範囲にある組成を主成分とし、これにPbOの
形で表わした酸化鉛を0.01モル%以上、0.5モル%以下
添加したことを特徴としている。
<Means for Solving the Problems> In order to achieve the above-mentioned object, the magnetic substance composition for microwave / millimeter wave of the present invention is Li x Fe y Zn z O 0.5 + y + 0.5z (where x + y + z = 1 ), x, y,
z is 0.10 ≦ x ≦ 0.21, 0.77 ≦ y ≦ 0.88, 0.02 ≦
It is characterized in that the main component is a composition in the range of z ≦ 0.13, and 0.01 mol% or more and 0.5 mol% or less of lead oxide represented by the form of PbO is added thereto.

<作用> この発明によれば、4πMsを3900〜5100ガウスの範囲で
任意に設定でき、従って、その使用する周波数に最も適
した4πMsの値を有する材料を選択できる。
<Operation> According to the present invention, 4πMs can be arbitrarily set within the range of 3900 to 5100 gauss, and therefore, a material having a value of 4πMs most suitable for the frequency used can be selected.

この発明によると、4πMsの値が他のマイクロ波・ミリ
波用フェライトに比べて高い材料が得られるので、特に
30GHz以上の超高周波帯で使用するのに好適である。
According to the present invention, a material having a higher value of 4πMs than other ferrites for microwave and millimeter waves can be obtained.
It is suitable for use in 30GH z or ultra high frequency band.

また、この発明によると、Tcが高いゆえに室温付近での
4πMsの温度変化率が小さく、更に、ΔHおよびtan δ
eが十分に小さい、マイクロ波・ミリ波特性の良好な磁
性体を得ることができる。
Further, according to the present invention, since Tc is high, the temperature change rate of 4πMs near room temperature is small, and further, ΔH and tan δ
It is possible to obtain a magnetic material having a sufficiently small e and good microwave / millimeter wave characteristics.

上述したこの発明の目的、特徴、および利点について、
以下図面を参照して実施例により説明する。
Regarding the above-mentioned objects, features, and advantages of the present invention,
Examples will be described below with reference to the drawings.

<実施例> 先ず、原料として、高純度のLi2CO3、Fe2O3、ZnOおよび
PbOを準備した。これらの原料を第1表に示す組成が得
られる用に秤量し、エチルアルコールを分散媒に用いて
ボールミルで16時間湿式混合した。この混合物を乾燥し
た後、850℃で2時間仮焼し、仮焼物を得た。この仮焼
物をエチルアルコールおよび有機バインダと共に、ボー
ルミルに入れ、16時間湿式粉砕した。この粉砕物を乾燥
した後、50メッシュの網を通して造粒し、得られた粉末
を2000kg/cm2の圧力で3mm×3mm×20mmの角柱に成形し
た。この成形物を1050〜1200℃で2時間焼成した後、機
械加工により直径1.3mmの球および直径1.3mm、長さ16mm
の円柱のサンプルを得た。
Example First, as raw materials, high-purity Li 2 CO 3 , Fe 2 O 3 , ZnO, and
Prepared PbO. These raw materials were weighed so that the composition shown in Table 1 was obtained, and wet mixed with a ball mill for 16 hours using ethyl alcohol as a dispersion medium. After this mixture was dried, it was calcined at 850 ° C. for 2 hours to obtain a calcined product. This calcined product was put into a ball mill together with ethyl alcohol and an organic binder, and wet-milled for 16 hours. The pulverized product was dried and then granulated through a 50-mesh net, and the obtained powder was molded into a 3 mm × 3 mm × 20 mm prism at a pressure of 2000 kg / cm 2 . After this molded product was fired at 1050-1200 ℃ for 2 hours, it was machined to form a sphere with a diameter of 1.3 mm and a diameter of 1.3 mm and a length of 16 mm
A cylindrical sample of was obtained.

得られた球形サンプルについて、振動形磁力計を用いて
4πMsおよびTcを測定し、TE106空胴共振器中で10GHzに
おけるΔHを測定した。
For the obtained spherical sample, 4πMs and Tc were measured using a vibrating magnetometer, and ΔH at 10 GHz was measured in a TE106 cavity resonator.

また、円柱形サンプルについて、TM010空胴共振器中で
攝動法を用いて10GHzにおけるε、tan δeを測定し
た。それらの結果を第1表に示す。
Further, ε and tan δe at 10 GHz were measured for the cylindrical sample in the TM010 cavity resonator by using the displacement method. The results are shown in Table 1.

尚、第1表中※印はこの発明の範囲外であり、それ以外
はすべてこの発明の範囲内のものである。
Incidentally, the * mark in Table 1 is out of the scope of the present invention, and all other items are within the scope of the present invention.

更に、第1表に示した実験例の結果を、LixFeyZnzO
0.5+y+0.5zの組成比を表わす3成分組成図中に示し
た。この図面中の番号は、各試料番号を表わす。尚、こ
の図面において、発明の範囲内にある組成比を示す領域
は、頂点A、BおよびCを有する三角形で示されてい
る。
Furthermore, the results of the experimental examples shown in Table 1 are shown as Li x Fe y Zn z O
It is shown in the three-component composition diagram showing the composition ratio of 0.5 + y + 0.5z . The numbers in this figure represent the sample numbers. In this drawing, a region showing a composition ratio within the scope of the invention is shown by a triangle having vertices A, B and C.

次に、この発明の組成範囲を限定した理由について説明
する。
Next, the reason why the composition range of the present invention is limited will be described.

試料番号1、6、11、16、21および26のように、PbOの
添加量が0.01モル%以下のものは、ΔHおよびtan δe
が大きくなり、実用に適さない。
Samples Nos. 1, 6, 11, 16, 21 and 26, in which the amount of PbO added is 0.01 mol% or less, have ΔH and tan δe.
Is not suitable for practical use.

また、試料番号5、10、15、20、25および30のようにPb
Oの添加量が0.5モル%を越えるものはtan δeが大きく
なり好ましくない。
In addition, as in sample numbers 5, 10, 15, 20, 25 and 30, Pb
If the amount of O added exceeds 0.5 mol%, tan δe becomes large, which is not preferable.

試料番号31および32のように、zが0.02以下のものは、
Znによる4πMsの向上の効果がなく、この発明の範囲か
ら除外される。
For samples with z of 0.02 or less, such as sample numbers 31 and 32,
This is excluded from the scope of the present invention because it has no effect of improving 4πMs by Zn.

試料番号33および34のように、xが0.10以下のものは、
ΔHが大きく、かつTcが低くなり、従って4πMsの温度
変化率が大きくなり好ましくない。
If x is 0.10 or less, like sample numbers 33 and 34,
ΔH is large and Tc is low, so that the temperature change rate of 4πMs is large, which is not preferable.

試料番号35及び36のように、yが0.77以下のものは、Δ
Hおよびtan δeが大きくなり好ましくない。
If y is 0.77 or less like sample numbers 35 and 36, Δ
H and tan δe increase, which is not preferable.

これに対して、この発明の磁性体組成物では十分に小さ
いΔHとtan δeを有し、かつ高いTcを有している。
又、この発明の磁性体組成物は4πMsの値が他のマイク
ロ波・ミリ波用磁性体に比べて大きいため、それらの磁
性体よりも高い周波数帯で使用することが可能である。
On the other hand, the magnetic composition of the present invention has sufficiently small ΔH and tan δe, and has a high Tc.
Further, the magnetic material composition of the present invention has a larger value of 4πMs than other magnetic materials for microwaves and millimeter waves, and thus can be used in a frequency band higher than those magnetic materials.

更に、LixFeyZnzO0.5+y+0.5zの化学式で表わされる
x、yおよびzをこの発明の範囲内で適宜変化させるこ
とによって、4πMsの値を3900〜5100ガウスの間で自由
に選択することができ、従って、使用する周波数に最も
適した4πMsの値を得ることができるのである。
Further, by appropriately changing x, y and z represented by the chemical formula of Li x Fe y Zn z O 0.5 + y + 0.5z within the scope of the present invention, the value of 4πMs can be freely selected from 3900 to 5100 gauss. Therefore, it is possible to obtain the value of 4πMs most suitable for the frequency used.

【図面の簡単な説明】[Brief description of drawings]

図面はこの発明に係るマイクロ波・ミリ波用磁性体組成
物のLixFeyZnzO0.5+y+0.5zの組成比を表わす3成分
組成図である。
The drawing is a three-component composition diagram showing the composition ratio of Li x Fe y Zn z O 0.5 + y + 0.5z in the microwave / millimeter wave magnetic material composition according to the present invention.

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】LixFeyZnzO0.5+y+0.5z(但し、x+y+z
)で表わされる組成において、x、y、zがそれぞれ
0.10≦x≦0.21、0.77≦y≦0.88、0.02≦z≦0.13の範
囲にある組成を主成分とし、これにPbOの形で表わした
酸化鉛を0.01モル%以上、0.5モル%以下添加含有して
なるマイクロ波・ミリ波用磁性体組成物。
1. Li x Fe y Zn z O 0.5 + y + 0.5z (where x + y + z =
In the composition represented by 1 ), x, y and z are respectively
0.10 ≤ x ≤ 0.21, 0.77 ≤ y ≤ 0.88, 0.02 ≤ z ≤ 0.13 is the main component, and lead oxide expressed in the form of PbO is added by 0.01 mol% or more and 0.5 mol% or less. A magnetic substance composition for microwaves and millimeter waves.
JP1153129A 1989-06-15 1989-06-15 Microwave / millimeter wave magnetic composition Expired - Lifetime JPH0775206B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1153129A JPH0775206B2 (en) 1989-06-15 1989-06-15 Microwave / millimeter wave magnetic composition

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1153129A JPH0775206B2 (en) 1989-06-15 1989-06-15 Microwave / millimeter wave magnetic composition

Publications (2)

Publication Number Publication Date
JPH0319204A JPH0319204A (en) 1991-01-28
JPH0775206B2 true JPH0775206B2 (en) 1995-08-09

Family

ID=15555620

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1153129A Expired - Lifetime JPH0775206B2 (en) 1989-06-15 1989-06-15 Microwave / millimeter wave magnetic composition

Country Status (1)

Country Link
JP (1) JPH0775206B2 (en)

Also Published As

Publication number Publication date
JPH0319204A (en) 1991-01-28

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