JP3796682B2 - Electromagnetic wave absorber - Google Patents
Electromagnetic wave absorber Download PDFInfo
- Publication number
- JP3796682B2 JP3796682B2 JP18366299A JP18366299A JP3796682B2 JP 3796682 B2 JP3796682 B2 JP 3796682B2 JP 18366299 A JP18366299 A JP 18366299A JP 18366299 A JP18366299 A JP 18366299A JP 3796682 B2 JP3796682 B2 JP 3796682B2
- Authority
- JP
- Japan
- Prior art keywords
- electromagnetic wave
- wave absorber
- weight
- titanium
- iron
- 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
- 239000006096 absorbing agent Substances 0.000 title claims description 17
- XEEYBQQBJWHFJM-UHFFFAOYSA-N Iron Chemical compound [Fe] XEEYBQQBJWHFJM-UHFFFAOYSA-N 0.000 claims description 25
- RTAQQCXQSZGOHL-UHFFFAOYSA-N Titanium Chemical compound [Ti] RTAQQCXQSZGOHL-UHFFFAOYSA-N 0.000 claims description 23
- 239000010936 titanium Substances 0.000 claims description 23
- 229910052719 titanium Inorganic materials 0.000 claims description 23
- 239000002893 slag Substances 0.000 claims description 17
- 239000011230 binding agent Substances 0.000 claims description 12
- 239000000203 mixture Substances 0.000 claims description 10
- 229910052751 metal Inorganic materials 0.000 claims description 6
- 239000002184 metal Substances 0.000 claims description 6
- 238000000465 moulding Methods 0.000 claims description 6
- 229910010413 TiO 2 Inorganic materials 0.000 claims description 5
- SVMGVNXXUVNGRK-UHFFFAOYSA-N oxomethylideneiron Chemical compound O=C=[Fe] SVMGVNXXUVNGRK-UHFFFAOYSA-N 0.000 claims 2
- 238000010521 absorption reaction Methods 0.000 description 9
- 230000000052 comparative effect Effects 0.000 description 9
- 239000000843 powder Substances 0.000 description 9
- 239000010410 layer Substances 0.000 description 6
- 239000011347 resin Substances 0.000 description 5
- 229920005989 resin Polymers 0.000 description 5
- 229920001187 thermosetting polymer Polymers 0.000 description 5
- 239000000463 material Substances 0.000 description 4
- 238000000034 method Methods 0.000 description 4
- JRPBQTZRNDNNOP-UHFFFAOYSA-N barium titanate Chemical compound [Ba+2].[Ba+2].[O-][Ti]([O-])([O-])[O-] JRPBQTZRNDNNOP-UHFFFAOYSA-N 0.000 description 3
- 229910002113 barium titanate Inorganic materials 0.000 description 3
- 238000005259 measurement Methods 0.000 description 3
- 239000002245 particle Substances 0.000 description 3
- 239000011358 absorbing material Substances 0.000 description 2
- 229910052742 iron Inorganic materials 0.000 description 2
- 239000002356 single layer Substances 0.000 description 2
- 229910000805 Pig iron Inorganic materials 0.000 description 1
- 238000003723 Smelting Methods 0.000 description 1
- 229910001035 Soft ferrite Inorganic materials 0.000 description 1
- 230000002745 absorbent Effects 0.000 description 1
- 239000002250 absorbent Substances 0.000 description 1
- PNEYBMLMFCGWSK-UHFFFAOYSA-N aluminium oxide Inorganic materials [O-2].[O-2].[O-2].[Al+3].[Al+3] PNEYBMLMFCGWSK-UHFFFAOYSA-N 0.000 description 1
- RHZUVFJBSILHOK-UHFFFAOYSA-N anthracen-1-ylmethanolate Chemical compound C1=CC=C2C=C3C(C[O-])=CC=CC3=CC2=C1 RHZUVFJBSILHOK-UHFFFAOYSA-N 0.000 description 1
- 239000003830 anthracite Substances 0.000 description 1
- 230000006835 compression Effects 0.000 description 1
- 238000007906 compression Methods 0.000 description 1
- 238000001816 cooling Methods 0.000 description 1
- 238000006477 desulfuration reaction Methods 0.000 description 1
- 230000023556 desulfurization Effects 0.000 description 1
- YDZQQRWRVYGNER-UHFFFAOYSA-N iron;titanium;trihydrate Chemical compound O.O.O.[Ti].[Fe] YDZQQRWRVYGNER-UHFFFAOYSA-N 0.000 description 1
- 238000010030 laminating Methods 0.000 description 1
- 238000004519 manufacturing process Methods 0.000 description 1
- 238000000691 measurement method Methods 0.000 description 1
- QMQXDJATSGGYDR-UHFFFAOYSA-N methylidyneiron Chemical compound [C].[Fe] QMQXDJATSGGYDR-UHFFFAOYSA-N 0.000 description 1
- 239000011812 mixed powder Substances 0.000 description 1
- 238000002156 mixing Methods 0.000 description 1
- 239000004570 mortar (masonry) Substances 0.000 description 1
- 238000002360 preparation method Methods 0.000 description 1
- 238000010298 pulverizing process Methods 0.000 description 1
- 238000000926 separation method Methods 0.000 description 1
- 239000002002 slurry Substances 0.000 description 1
- 229910001220 stainless steel Inorganic materials 0.000 description 1
- 239000010935 stainless steel Substances 0.000 description 1
- 239000000126 substance Substances 0.000 description 1
- XLYOFNOQVPJJNP-UHFFFAOYSA-N water Substances O XLYOFNOQVPJJNP-UHFFFAOYSA-N 0.000 description 1
- 229910000859 α-Fe Inorganic materials 0.000 description 1
Images
Landscapes
- Shielding Devices Or Components To Electric Or Magnetic Fields (AREA)
Description
【0001】
【発明の属する技術分野】
本発明は、電磁波吸収体、詳しくはサブGHz帯を含む広い周波数範囲(106 Hz〜1010Hz)の電磁波の吸収に使用することができる電磁波吸収体に関する。
【0002】
【従来の技術】
ソフトフェライトやカーボニル鉄、純鉄などが電磁波吸収材料として使用し得ることは知られている。これらの材料を建造物の電磁波吸収に使用するためにはシート状に加工しなければならない。そのためこれら材料はその粉体をバインダーを用いてシート状に加工して用いられる。
【0003】
ところがこれら材料が主として吸収する周波数帯は数GHzの域にあり、より低周波すなわちサブGHz帯の電磁波を吸収するためにはシートの厚みを実用に供し得ない程厚くしなければならない。
【0004】
特開平10−308596は、電磁波の入射側から順にチタン酸バリウム等の強誘電層、カーボニル鉄系の軟磁性体層、短絡層として金属板を積層してなる電波吸収体を開示し、厚さ1.5mmのカーボニル鉄シートと厚さ0.5mmのチタン酸バリウム焼結体を使って900MHzにおいて20dBの反射減衰量を示す合計2mmの厚みの電波吸収体を得ている。しかしながらこの電波吸収体も実用化にはいくつかの難点がある。例えば広い面積の薄いチタン酸バリウムの焼結体を得るのは困難であり、限られた面積のものしか得られないなどである。また短絡のための金属板を除いた本体は材料の異なる二層構造であるため、製作上および使用上様々の問題を抱えている。
【0005】
【問題を解決するための手段】
そこで本発明は、単層構造(金属板を除く)であり、サブGHz帯の電磁波の吸収にも使用できる新しい電磁波吸収体を提供する。
この電磁波吸収体は、TiO2 重量換算でチタン分を70〜90%含有するチタンスラッグ5〜30重量%およびカーボニル鉄または鉄粉95〜70%の混合物をバインダーを用いて成形してなる。
【0006】
この電磁波吸収体は、短絡層として金属板に積層することができる。しかしながら短絡層として金属板を用いなくても例えば約3mmの厚みにおいてサブGHz帯の電磁波を高い吸収度をもって吸収し、その性能は厚み約6mmのフェライト系吸収体に匹敵する。
【0007】
このように単層で使用可能であり、かつバインダーを用いて成形加工するので比較的厚みの小さい広い面積の吸収体を容易に製造できる利益を有する。
【0008】
【実施態様】
チタンスラグは、イルメナイト鉱を脱硫処理後、無煙炭を加えて電気炉で精錬し、銑鉄を分離後のスラグを水冷、破砕、粉砕して得られ、そのチタン含量はTiO2 として一般に70〜90%である。
【0009】
本発明者が特願平10−107007において明らかにしたように、チタンスラグは単独で4.3GHzを中心にGHz帯の電磁波を吸収する電磁波吸収材料である。しかしながらサブGHzの電磁波は殆ど吸収しない。
【0010】
しかるにチタンスラグへ、同様に単独ではサブGHz帯域の電磁波を殆ど吸収しないカーボニル鉄または鉄粉をある割合で配合し、バインダーを用いて成形する時、前記したようにサブGHz帯域の電磁波を有意義に吸収する電磁波吸収体が得られる。
【0011】
ここに用いられるチタンスラグは粉末状のものであり、一般には4〜100μmの粒径が好ましい。カルボニル鉄および鉄粉も同程度の粒径の粉末が好ましく、市販品をそのまま使用することができる。
【0012】
成形体は、70〜95重量%がカーボニル鉄または鉄粉で残余をチタンスラグが占めるブレンドをバインダーを用いて成形することによって製造される。ブレンド中のチタンスラグの割合は10重量%以上が好ましい。
【0013】
バインダーとしては粉末状の熱硬化性樹脂が好ましい。乾式法によって三成分の均一な混合が容易であり、混合物の圧縮成形が可能であるからである。勿論成形方法によっては他の無機および有機バインダーも使用可能である。
【0014】
バインダーの使用量は成形体に満足な機械的な強度が得られる限り少ない方が好ましく、熱硬化樹脂の場合全体の5〜60重量%である。
【0015】
熱硬化樹脂をバインダーとする成形はプレスを使用して加熱加圧し、必要あればアフターキュアにより実質上完全に硬化させる。
【0016】
【実施例】
以下に限定を意図しない実施例および比較例によって本発明を例証する。これらにおいて「%」は重量基準による。
【0017】
1.測定サンプルの調製法
RTZ Iron & Titanium Inc.社製チタンスラグ粉末(TiO2 分90%、平均粒子径1000μm)1kgをステンレス製ボールミルに入れ、48時間湿式粉砕した後、そのスラリーをバットに移し、105℃で24時間乾燥した。この乾燥粉末200gをアルミナ製乳鉢にとり、30分間擂潰した。
【0018】
このように調製したチタンスラグ粉末と、カーボニル鉄(BASF製EW)(実施例1)または鉄粉(300M−200)(実施例2)と、熱硬化性樹脂粉末(大日本インキ化学工業社製ファインディックA−56−1024−Y)の所定量をミキサー中で1分間混合した。
【0019】
比較例サンプルには、チタンスラグ粉末のみ、カーボニル鉄または鉄粉のみを熱硬化樹脂と混合して用いた。
【0020】
次にこの混合粉末を加圧成形用治具に所定量採り、3.3トン/cm2 で圧縮成型後、180℃において30分間加熱して熱硬化させ、次にネットワークアナライザーにセット出来るように、再度、内径8.66mm、外径19.94mmのトロイダルコア状に成型加工して測定用サンプルとした。
【0021】
2.測定方法
電磁波吸収測定はWILTRON社製37269A型ネットワークアナライザによる短絡解放法により測定した。
【0022】
実施例1および比較例1〜2
表1に示す組成を用いた。
【0023】
結果:
実施例1、比較例1および2のサンプルについて電磁波吸収曲線をそれぞれ図1〜3に示す。図1には図2〜3に見られない低周波での電磁波吸収が顕著に表れている。
【0024】
実施例2および比較例3〜4
実施例2においてはチタンスラグ10%および鉄粉90%の混合物を用い、比較例3および4においてはチタンスラグ単独および鉄粉単独をそれぞれ使用した。これへバインダー粉末が成形体全体のそれぞれ20%,30%および40%となるようにミキサー中で混合し、前記した方法によって測定サンプルを調製し、試験した。結果を以下の表2〜4に示す。
【0025】
【0026】
【0027】
【0028】
表2に示す実施例2のサンプルの吸収ピークは、表3および4に示す比較例3および4のサンプルの吸収ピークに比較して、匹敵する各サンプル厚みにおいて吸収ピーク周波数が低い側へ移動しており、チタンスラブと鉄粉のブレンドが低周波帯の電磁波の吸収に効果があることが明らかである。
【図面の簡単な説明】
【図1】本発明の電磁波吸収体(実施例1)の電磁波吸収曲線のグラフである。
【図2】チタンスラグ単独(比較例1)を用いた電磁波吸収体の図1と同様なグラフである。
【図3】カーボニル鉄単独(比較例2)を用いた電磁波吸収体の図1と同様なグラフである。[0001]
BACKGROUND OF THE INVENTION
The present invention relates to an electromagnetic wave absorber, and more particularly to an electromagnetic wave absorber that can be used to absorb electromagnetic waves in a wide frequency range (10 6 Hz to 10 10 Hz) including a sub-GHz band.
[0002]
[Prior art]
It is known that soft ferrite, carbonyl iron, pure iron, and the like can be used as an electromagnetic wave absorbing material. In order to use these materials for electromagnetic wave absorption of buildings, they must be processed into sheets. Therefore, these materials are used by processing the powder into a sheet using a binder.
[0003]
However, the frequency band mainly absorbed by these materials is in the range of several GHz. In order to absorb electromagnetic waves of a lower frequency, that is, a sub-GHz band, the thickness of the sheet must be increased so that it cannot be practically used.
[0004]
Japanese Patent Laid-Open No. 10-308596 discloses a radio wave absorber formed by laminating a ferroelectric layer such as barium titanate, a carbonyl iron-based soft magnetic layer, and a metal plate as a short-circuit layer in order from the electromagnetic wave incident side. Using a 1.5 mm carbonyl iron sheet and a 0.5 mm thick barium titanate sintered body, an electromagnetic wave absorber having a total thickness of 2 mm showing a return loss of 20 dB at 900 MHz is obtained. However, this radio wave absorber also has some difficulties in practical use. For example, it is difficult to obtain a thin sintered body of barium titanate having a large area, and only a limited area can be obtained. Moreover, since the main body excluding the metal plate for short circuit has a two-layer structure made of different materials, it has various problems in production and use.
[0005]
[Means for solving problems]
Therefore, the present invention provides a new electromagnetic wave absorber that has a single-layer structure (excluding a metal plate) and can also be used to absorb sub-GHz band electromagnetic waves.
This electromagnetic wave absorber is formed by molding a mixture of
[0006]
This electromagnetic wave absorber can be laminated on a metal plate as a short-circuit layer. However, even if a metal plate is not used as the short-circuit layer, for example, a sub-GHz band electromagnetic wave is absorbed with a high absorption at a thickness of about 3 mm, and the performance is comparable to a ferrite-based absorber having a thickness of about 6 mm.
[0007]
Thus, since it can be used in a single layer and is molded using a binder, it has an advantage that an absorbent body having a relatively small thickness and a large area can be easily produced.
[0008]
Embodiment
Titanium slag, after the desulfurization treatment of ilmenite, and smelting in an electric furnace by adding anthracite, water cooling the slag after separation of the pig iron, crushing, obtained by pulverizing, generally 70% to 90% the titanium content as TiO 2 It is.
[0009]
As clarified in Japanese Patent Application No. 10-107007 by the present inventor, titanium slag is an electromagnetic wave absorbing material that absorbs electromagnetic waves in the GHz band around 4.3 GHz alone. However, it hardly absorbs sub-GHz electromagnetic waves.
[0010]
However, when titanium slag is mixed with a certain proportion of carbonyl iron or iron powder that hardly absorbs electromagnetic waves in the sub-GHz band alone and is molded using a binder, the electromagnetic waves in the sub-GHz band are significant as described above. An absorbing electromagnetic wave absorber is obtained.
[0011]
The titanium slag used here is in a powder form, and generally a particle size of 4 to 100 μm is preferable. Carbonyl iron and iron powder are also preferably powders having similar particle sizes, and commercially available products can be used as they are.
[0012]
The molded body is produced by molding a blend in which 70 to 95% by weight is carbonyl iron or iron powder and the remainder is occupied by titanium slag using a binder. The proportion of titanium slag in the blend is preferably 10% by weight or more.
[0013]
As the binder, a powdery thermosetting resin is preferable. This is because the three-component uniform mixing is easy by the dry method, and the mixture can be compression-molded. Of course, other inorganic and organic binders can be used depending on the molding method.
[0014]
The amount of the binder used is preferably as small as possible to obtain satisfactory mechanical strength for the molded body, and is 5 to 60% by weight in the case of a thermosetting resin.
[0015]
The molding using a thermosetting resin as a binder is heated and pressurized using a press, and if necessary, is cured substantially completely by after-curing.
[0016]
【Example】
The invention is illustrated by the following non-limiting examples and comparative examples. In these, “%” is based on weight.
[0017]
1. Preparation method of measurement sample RTZ Iron & Titanium Inc. 1 kg of Titanium slag powder (TiO 2 min 90%, average particle size 1000 μm) manufactured by the company was put into a stainless steel ball mill and wet-ground for 48 hours, and then the slurry was transferred to a vat and dried at 105 ° C. for 24 hours. 200 g of this dry powder was placed in an alumina mortar and crushed for 30 minutes.
[0018]
The titanium slag powder thus prepared, carbonyl iron (EW made by BASF) (Example 1) or iron powder (300M-200) (Example 2), and thermosetting resin powder (Dainippon Ink & Chemicals, Inc.) A predetermined amount of fine dic A-56-1024-Y) was mixed in a mixer for 1 minute.
[0019]
For the comparative sample, only titanium slag powder, only carbonyl iron or iron powder was mixed with a thermosetting resin.
[0020]
Next, a predetermined amount of this mixed powder is taken in a pressure molding jig, compression molded at 3.3 ton / cm 2 , heated at 180 ° C. for 30 minutes to be thermally cured, and then set in a network analyzer. The sample was again molded into a toroidal core shape having an inner diameter of 8.66 mm and an outer diameter of 19.94 mm.
[0021]
2. Measurement Method The electromagnetic wave absorption measurement was performed by a short circuit release method using a 37269A type network analyzer manufactured by WILTRON.
[0022]
Example 1 and Comparative Examples 1-2
The composition shown in Table 1 was used.
[0023]
result:
The electromagnetic wave absorption curves for the samples of Example 1 and Comparative Examples 1 and 2 are shown in FIGS. In FIG. 1, electromagnetic wave absorption at a low frequency not seen in FIGS.
[0024]
Example 2 and Comparative Examples 3-4
In Example 2, a mixture of 10% titanium slag and 90% iron powder was used, and in Comparative Examples 3 and 4, titanium slag alone and iron powder alone were used. This was mixed in a mixer so that the binder powder would be 20%, 30% and 40% of the whole compact, and a measurement sample was prepared and tested by the method described above. The results are shown in Tables 2 to 4 below.
[0025]
[0026]
[0027]
[0028]
The absorption peak of the sample of Example 2 shown in Table 2 moves to the side where the absorption peak frequency is lower at each comparable sample thickness compared to the absorption peaks of the samples of Comparative Examples 3 and 4 shown in Tables 3 and 4. It is clear that a blend of titanium slab and iron powder is effective in absorbing low frequency electromagnetic waves.
[Brief description of the drawings]
FIG. 1 is a graph of an electromagnetic wave absorption curve of an electromagnetic wave absorber (Example 1) of the present invention.
FIG. 2 is a graph similar to FIG. 1 of an electromagnetic wave absorber using titanium slag alone (Comparative Example 1).
FIG. 3 is a graph similar to FIG. 1 of an electromagnetic wave absorber using carbonyl iron alone (Comparative Example 2).
Claims (3)
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP18366299A JP3796682B2 (en) | 1999-06-29 | 1999-06-29 | Electromagnetic wave absorber |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP18366299A JP3796682B2 (en) | 1999-06-29 | 1999-06-29 | Electromagnetic wave absorber |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JP2001015979A JP2001015979A (en) | 2001-01-19 |
| JP3796682B2 true JP3796682B2 (en) | 2006-07-12 |
Family
ID=16139746
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP18366299A Expired - Fee Related JP3796682B2 (en) | 1999-06-29 | 1999-06-29 | Electromagnetic wave absorber |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JP3796682B2 (en) |
Families Citing this family (6)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| KR100505856B1 (en) * | 2002-05-29 | 2005-08-03 | 학교법인 호서학원 | Electromagnetic Interference(EMI) Shielding Composites and Manufacturing Processes thereof |
| JP2005012103A (en) * | 2003-06-20 | 2005-01-13 | Yokohama Rubber Co Ltd:The | Radio wave absorption housing and its manufacturing method |
| CN107286907B (en) * | 2017-07-07 | 2020-04-10 | 中国人民解放军国防科学技术大学 | Molybdenum disulfide/carbonyl iron composite microwave absorbent with core-shell structure and preparation method thereof |
| CN108342230B (en) * | 2018-03-05 | 2020-09-11 | 重庆工商大学 | A kind of removal process of acid gas in blast furnace gas |
| CN112812612B (en) * | 2021-02-08 | 2022-05-13 | 大连理工大学 | A kind of building wave absorbing paint based on magnesium oxide excited steel slag and preparation method |
| CN116251679B (en) * | 2022-12-09 | 2026-02-17 | 攀钢集团攀枝花钢铁研究院有限公司 | Low-sulfur ilmenite beneficiation process and method for preparing high-purity iron by using ilmenite |
-
1999
- 1999-06-29 JP JP18366299A patent/JP3796682B2/en not_active Expired - Fee Related
Also Published As
| Publication number | Publication date |
|---|---|
| JP2001015979A (en) | 2001-01-19 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| CN107578877A (en) | A kind of iron based nano crystal powder core of magnetic permeability μ=90 and preparation method thereof | |
| CN109273185B (en) | Method for preparing magnetic powder core by using iron-based nanocrystalline alloy powder | |
| KR100503133B1 (en) | Complex magnetic material and electron interference suppressor | |
| JPS64802B2 (en) | ||
| JP2006077264A (en) | METHOD FOR RECYCLING RARE-EARTH SINTERED MAGNET AND TRANSITION-METAL BASED SCRAP, AND METHOD FOR MANUFACTURING MAGNETIC-MATERIAL POWDER FOR GHz BAND WAVE ABSORBER AND METHOD FOR MANUFACTURING WAVE ABSORBER | |
| CN104078183A (en) | Electric wave absorption sheet for near-field and manufacturing method thereof | |
| JP3796682B2 (en) | Electromagnetic wave absorber | |
| Miura et al. | Microwave absorption properties of the nano-composite powders recovered from Nd–Fe–B bonded magnet scraps | |
| CN108865062A (en) | Electromagnetic wave absorbent and preparation method thereof | |
| Bantsis et al. | Electromagnetic absorption, reflection and interference shielding in X-band frequency range of low cost ceramic building bricks and sandwich type ceramic tiles using mill scale waste as an admixture | |
| CN111995385A (en) | Permanent magnetic ferrite material with high radial and axial shrinkage consistency and preparation method thereof | |
| JP4643137B2 (en) | Method of manufacturing electromagnetic wave absorbing magnetic powder, electromagnetic wave absorbing magnetic powder and radio wave absorber using the same | |
| KR100298685B1 (en) | Lump cokes used to Electric furnace or steel-making furnace | |
| US6369150B1 (en) | Electromagnetic radiation absorption composition | |
| JPH0516679B2 (en) | ||
| CN114899618A (en) | Wave-absorbing patch for 700MHz5G base station in P wave band and preparation method thereof | |
| JP3796680B2 (en) | Electromagnetic wave absorbing material | |
| CN106252014A (en) | A kind of jamproof ferrite core material | |
| JP2001093719A (en) | Partial carbonized ferrite and method for manufacturing thereof | |
| JP3279701B2 (en) | Molding method of ferrite raw material powder | |
| CN118812255B (en) | High-frequency high-Bs high-DC superimposed low-loss manganese zinc ferrite and preparation method thereof | |
| JPH0750645B2 (en) | Electromagnetic shield material | |
| JP2001057307A (en) | Composite magnetic material | |
| JPS61205627A (en) | Production of powder for electric wave absorber | |
| JP3438231B2 (en) | Low loss magnetic material |
Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| A61 | First payment of annual fees (during grant procedure) |
Free format text: JAPANESE INTERMEDIATE CODE: A61 Effective date: 20060405 |
|
| R150 | Certificate of patent or registration of utility model |
Free format text: JAPANESE INTERMEDIATE CODE: R150 |
|
| FPAY | Renewal fee payment (event date is renewal date of database) |
Free format text: PAYMENT UNTIL: 20100428 Year of fee payment: 4 |
|
| FPAY | Renewal fee payment (event date is renewal date of database) |
Free format text: PAYMENT UNTIL: 20110428 Year of fee payment: 5 |
|
| FPAY | Renewal fee payment (event date is renewal date of database) |
Free format text: PAYMENT UNTIL: 20120428 Year of fee payment: 6 |
|
| LAPS | Cancellation because of no payment of annual fees |