JPH081843B2 - Microwave / millimeter wave magnetic composition - Google Patents
Microwave / millimeter wave magnetic compositionInfo
- Publication number
- JPH081843B2 JPH081843B2 JP1153128A JP15312889A JPH081843B2 JP H081843 B2 JPH081843 B2 JP H081843B2 JP 1153128 A JP1153128 A JP 1153128A JP 15312889 A JP15312889 A JP 15312889A JP H081843 B2 JPH081843 B2 JP H081843B2
- Authority
- JP
- Japan
- Prior art keywords
- microwave
- millimeter wave
- 4πms
- tan
- 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 - Fee Related
Links
Landscapes
- Magnetic Ceramics (AREA)
- Soft Magnetic Materials (AREA)
- Compounds Of Iron (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 Application Field> 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37
00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。Of these, lithium ferrite has 37% 4πMs.
It is as large as about 00 gauss and has a Curie point (Tc) of 650 ° C.
It is a material that can be applied to circuit elements such as highly stable isolators and circulators because it has a high temperature near it and has a small rate of temperature change near room temperature of 4πMs.
〈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)の誘電損失(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 loss such as dielectric loss (tan δe) of ferromagnetic resonance absorption half width (ΔH) is larger than that 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Δ
Hとtan δeが周波数10GH2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 is Δ
H and tan δe are large at 500 Oersted and 0.01 or more, respectively, at a frequency of 10 GH 2 and 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Tiで置換して4πMsを任意の
値に設定できるようにすると共に、B2O3、SiO2の何れか
1種以上を添加含有させて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, in which a portion of Li 0.5 Fe 2.5 O 4 is replaced with Ti so that 4πMs can be set to an arbitrary value, and B 2 O 3 , It is an object of the present invention to provide a magnetic material for microwave / millimeter wave in which ΔH and tan δe are improved by adding and containing any one or more kinds of SiO 2 .
〈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LixFeyTizO0.5+y+1.5z(但し、
x+y+z=1)で表わされる組成において、x、y、
zがれぞれ0.15≦x≦0.30、0.55≦y<0.85、0<z≦
0.30の範囲にある組成を主成分とし、これにB2O3、SiO2
の何れか1種類以上を合計0.02モル%以上、1.0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 object, the microwave of the present invention
The magnetic composition for millimeter waves is Li x Fe y Ti z O 0.5 + y + 1.5z (however,
x + y + z = 1), x, y,
z is 0.15 ≦ x ≦ 0.30, 0.55 ≦ y <0.85, 0 <z ≦
The main component is a composition in the range of 0.30, and B 2 O 3 , SiO 2
Any one or more of 0.02 mol% or more, 1.0 mol%
The feature is that it is added below. .
〈作用〉 この発明によれば、4πMsを600〜3700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、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及びtan δe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。<Operation> According to the present invention, 4πMs can be arbitrarily set in the range of 600 to 3700 gauss, and therefore, a material having a value of 4πMs most suitable for the frequency to be used can be selected, and Tc is high, so that the material can be used near room temperature. The temperature change rate of 4πMs is small, and
It is possible to obtain a magnetic body having a sufficiently small ΔH and tan δe 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。The above-mentioned objects, features, and advantages of the present invention will be described below by way of embodiments with reference to the drawings.
〈実施例〉 先ず、原料として、高純度のLi2CO3、Fe2O3、TiO2、B
2O3およびSiO2を準備した。これらの原料を第1表に示
す組成が得られるように秤量し、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1.3m
m、長さ16mmの円柱のサンプルを得た。<Example> First, as a raw material, high purity Li 2 CO 3, Fe 2 O 3, TiO 2, B
2 O 3 and SiO 2 were prepared. These raw materials were weighed so as to obtain the composition shown in Table 1, and wet-mixed in 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. After drying this crushed product, granulate through a 50 mesh net,
The obtained powder was molded into a 3 mm × 3 mm × 20 mm prism with a pressure of 2000 kg / cm 2 . After this molded product was fired at 1050-1200 ℃ for 2 hours, it was machined to a ball with a diameter of 1.3mm and a diameter of 1.3m.
A cylindrical sample of m and 16 mm in length 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 10 GHz was measured in the TE106 cavity resonator.
ΔH at was measured.
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表中試料番号1〜7、12、13、18〜25、30、
31、36〜42はこの発明の範囲外であり、そのうち※印の
付されたものはΔHおよびtanδeの値が大きくなり実
用に適さないものを示している。In addition, in Table 1, sample numbers 1 to 7, 12, 13, 18 to 25, 30,
31 and 36 to 42 are out of the scope of the present invention, and those marked with * indicate those which are not suitable for practical use because the values of ΔH and tan δe are large.
又、試料番号1〜6及び19〜24は、Tiを添加しない比
較例であり、Tiを添加した他の試料との比較により、Ti
の添加やその添加量によって4πMsの値を任意に設定で
きるのがわかる。In addition, sample numbers 1 to 6 and 19 to 24 are comparative examples in which Ti is not added, and by comparing with other samples to which Ti is added,
It can be seen that the value of 4πMs can be set arbitrarily depending on the addition and the addition amount.
更に、第1表に示した実験例の結果を、LixFeyTizO
0.5+y+1.5z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、CおよびDを有する四角形(但し、z=0
の部分は含まず)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 Ti z O
It is shown in the three-component composition diagram showing the composition ratio of 0.5 + y + 1.5z .
The numbers in this figure represent the sample numbers. In this drawing, the region showing the composition ratio within the scope of the invention is
A quadrangle with vertices A, B, C and D, where z = 0
Is not included).
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、7、13、19、25および31のように、B
2O3、SiO2の何れか1種以上の添加量が合計0.02モル%
未満のものは、ΔH およびtan δeが大きくなり、実
用に適さない。B as in sample numbers 1, 7, 13, 19, 25 and 31
Addition amount of at least one of 2 O 3 and SiO 2 is 0.02 mol% in total
If it is less than 1, the ΔH and tan δe are large, and are not suitable for practical use.
また、試料番号6、12、18、24、30および36のようにB2
O3、SiO2の何れか1種以上の添加量が合計1.0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, B 2 as in sample numbers 6, 12, 18, 24, 30 and 36
If the total amount of one or more of O 3 and SiO 2 exceeds 1.0 mol%, tan δe becomes large, which is not preferable.
試料番号37および38のように、xが0.15未満になる
と、ΔHおよびtan δeが大きくなり好ましくない。When x is less than 0.15 as in sample numbers 37 and 38, ΔH and tan δe increase, which is not preferable.
試料番号39および40のように、yが0.55未満になる
と、ΔHおよびtan δe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。As in sample numbers 39 and 40, when y is less than 0.55, ΔH and tan δe are large, and Tc is low,
Therefore, the temperature change rate of 4πMs becomes large, which is not preferable.
試料番号41および42のように、xが0.3を越えると、
ΔHおよびtan δeが大きくなり好ましくない。When x exceeds 0.3, as in sample numbers 41 and 42,
ΔH 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。
更に、LixFeyTizO0.5+y+1.5z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600〜3700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。On the other hand, the magnetic composition of the present invention has sufficiently small ΔH and tan δe, and has a high Tc.
Furthermore, x represented by the chemical formula of Li x Fe y Ti z O 0.5 + y + 1.5z ,
By appropriately changing y and z within the scope of the present invention, it is possible to freely select the value of 4πMs between 600 and 3700 gauss, and thus to obtain the value of 4πMs most suitable for the frequency to be used. Can be done.
図面はこの発明にかかるマイクロ波・ミリ波用磁性体組
成物のLixFeyTizO0.5+y+1.5z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 Ti z O 0.5 + y + 1.5z in the microwave / millimeter wave magnetic material composition according to the present invention.
Claims (1)
=1)で表される組成において、x、y、zがそれぞれ
0.15≦x≦0.30、 0.55≦y<0.85、0<z≦0.30の範囲にある組成を主成
分とし、これにB2O3、SiO2の何れか1種類以上を合計0.
02モル%以上、1.0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 Ti z O 0.5 + y + 1.5z (where x + y + z
= 1), x, y and z are respectively
0.15 ≤ x ≤ 0.30, 0.55 ≤ y <0.85, 0 <z ≤ 0.30 as the main component, and at least one of B 2 O 3 and SiO 2 in total of 0.
A magnetic material composition for microwaves and millimeter waves, which contains 02 mol% or more and 1.0 mol% or less.
Priority Applications (2)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1153128A JPH081843B2 (en) | 1989-06-15 | 1989-06-15 | Microwave / millimeter wave magnetic composition |
| US07/452,704 US5028348A (en) | 1988-12-19 | 1989-12-19 | Magnetic material for high frequencies |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1153128A JPH081843B2 (en) | 1989-06-15 | 1989-06-15 | Microwave / millimeter wave magnetic composition |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH0319203A JPH0319203A (en) | 1991-01-28 |
| JPH081843B2 true JPH081843B2 (en) | 1996-01-10 |
Family
ID=15555598
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP1153128A Expired - Fee Related JPH081843B2 (en) | 1988-12-19 | 1989-06-15 | Microwave / millimeter wave magnetic composition |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH081843B2 (en) |
Family Cites Families (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5815923B2 (en) * | 1974-10-04 | 1983-03-28 | 日本電気株式会社 | Microha Millihayo Ferrite |
| JPS5853496B2 (en) * | 1975-08-27 | 1983-11-29 | 株式会社東芝 | Micro flywheel |
-
1989
- 1989-06-15 JP JP1153128A patent/JPH081843B2/en not_active Expired - Fee Related
Also Published As
| Publication number | Publication date |
|---|---|
| JPH0319203A (en) | 1991-01-28 |
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Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| LAPS | Cancellation because of no payment of annual fees |