JPH046243Y2 - - Google Patents
Info
- Publication number
- JPH046243Y2 JPH046243Y2 JP1983183758U JP18375883U JPH046243Y2 JP H046243 Y2 JPH046243 Y2 JP H046243Y2 JP 1983183758 U JP1983183758 U JP 1983183758U JP 18375883 U JP18375883 U JP 18375883U JP H046243 Y2 JPH046243 Y2 JP H046243Y2
- Authority
- JP
- Japan
- Prior art keywords
- waveguide
- cut
- resonator
- standard
- housing
- 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
Links
- 125000006850 spacer group Chemical group 0.000 claims description 9
- 230000000694 effects Effects 0.000 claims description 6
- 230000008878 coupling Effects 0.000 description 4
- 238000010168 coupling process Methods 0.000 description 4
- 238000005859 coupling reaction Methods 0.000 description 4
- 230000000903 blocking effect Effects 0.000 description 3
- 230000005684 electric field Effects 0.000 description 3
- 238000012360 testing method Methods 0.000 description 3
- 230000002411 adverse Effects 0.000 description 2
- 238000010586 diagram Methods 0.000 description 2
- 239000003989 dielectric material Substances 0.000 description 2
- 238000009434 installation Methods 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 230000013011 mating Effects 0.000 description 1
- 239000002184 metal Substances 0.000 description 1
- 230000000149 penetrating effect Effects 0.000 description 1
- 238000000926 separation method Methods 0.000 description 1
Landscapes
- Control Of Motors That Do Not Use Commutators (AREA)
Description
【考案の詳細な説明】
考案の技術分野
本考案は導波管形波器(フイルタ)に関し、
特に誘電体共振器を利用して構成された導波管形
波器の分割構造に関するものである。[Detailed description of the invention] Technical field of the invention This invention relates to a waveguide type filter.
In particular, the present invention relates to a divided structure of a waveguide waveform constructed using a dielectric resonator.
従来の背景
従来一般の導波管形波器は、金属製容器を用
いた空胴共振器や同軸共振器を利用して構成した
ものであり、これらの共振器は調整が比較的容易
にできるという長所がある反面、形状が大形で重
量も大きくなるという短所がある。Conventional Background Conventional general waveguide waveforms are constructed using a cavity resonator using a metal container or a coaxial resonator, and these resonators can be adjusted relatively easily. On the other hand, it has the disadvantage of being large in size and heavy in weight.
一方、誘電体共振器は形状が小形であり、取扱
いも簡単である。また誘電体共振器は従来は損失
が若干大きいという欠点があつたが、最近では材
料の開発が盛んに行なわれ、マイクロ波からミリ
波に及ぶ高周波帯においても損失が少なく、また
温度特性の良好なものが得られるようになつてき
た。 On the other hand, a dielectric resonator is small in size and easy to handle. In addition, dielectric resonators traditionally had the disadvantage of slightly high loss, but recently materials have been actively developed, and they have low loss even in high frequency bands ranging from microwaves to millimeter waves, and have good temperature characteristics. I've started getting things.
かかる小形、軽量で特性の良好な誘電体共振器
の開発を背景として、近年、誘電体共振器を利用
して導波管形波器を構成することが提案されて
いる。この導波管形波器は、標準導波管の一部
に内法が使用周波数域において遮断作用をなす遮
断導波管部が形成され、該遮断導波管部内に1個
以上のTE01〓あるいはTE11〓共振モードを利用し
た誘電体共振器が配列された構成のものである。
誘電体共振器は、これら共振器の誘電率よりも低
い低誘電率誘電体材料から成るスペーサを介して
遮断導波管部の内壁面に固定支持される。 Against the background of the development of such small, lightweight dielectric resonators with good characteristics, in recent years, it has been proposed to construct a waveguide waveform using dielectric resonators. This waveguide type waveguide has a cut-off waveguide section formed in a part of a standard waveguide, and has one or more TE 01 in the cut-off waveguide section. 〓 Or TE 11 〓 This is a structure in which dielectric resonators using resonance mode are arranged.
The dielectric resonators are fixedly supported on the inner wall surface of the cut-off waveguide section via spacers made of a dielectric material with a low dielectric constant lower than the dielectric constant of these resonators.
しかるに、かかる誘電体共振器を用いた導波管
形波器においては、誘電体共振器の配列及び固
定のために遮断導波管部が分割可能であることが
望ましい。しかし遮断導波管部の分割は、波器
の組立や分解作業および特性に重大な影響があ
り、重要な問題である。 However, in a waveguide type waveguide using such dielectric resonators, it is desirable that the cut-off waveguide section is separable for arranging and fixing the dielectric resonators. However, the division of the cut-off waveguide section is an important problem because it has a serious effect on the assembly and disassembly operations and characteristics of the wave device.
考案の目的
本考案はかかる点に鑑み、上記のような誘電体
共振器を用いて構成した導波管形波器におけ
る、組立や分解作業が簡単に行なえ、しかも波
器の特性に対する悪影響を生じないような分割構
造を提供することを目的とするものである。Purpose of the invention In view of these points, the present invention has been developed to enable easy assembly and disassembly of a waveguide type wave device constructed using a dielectric resonator as described above, and to avoid any adverse effects on the characteristics of the wave device. The purpose of this is to provide a division structure that would otherwise exist.
考案の構成
本考案は、前記の如き導波管形波器におい
て、前記遮断導波管部は標準導波管に対し分離可
能に接続される筐体から構成され、また該筐体は
誘電体共振器の電界面(E面)と平行で且つ該筐
体の誘電体共振器固定内壁面から前記スペーサの
厚さより小さな距離だけ離れた平面に沿つて分割
可能な構造としたことを特徴とするものである。Structure of the Invention The present invention provides a waveguide waveguide as described above, in which the cut-off waveguide section is constructed of a casing separably connected to the standard waveguide, and the casing is made of a dielectric material. It is characterized by having a structure that can be divided along a plane that is parallel to the electric surface (E-plane) of the resonator and that is separated from the dielectric resonator fixing inner wall surface of the housing by a distance smaller than the thickness of the spacer. It is something.
考案の実施例
以下、本考案の実施例につき図面を参照して詳
細に説明する。Embodiments of the invention Hereinafter, embodiments of the invention will be described in detail with reference to the drawings.
まず、誘電体共振器(以下単に「共振器」とも
略記)を用いて構成した導波管波器(以下単に
「波器」とも略記)の基本的な構成及び作用に
つき第1図から第4図を参照して説明する。 First, we will explain the basic structure and operation of a waveguide wave device (hereinafter also simply abbreviated as a "wave device") constructed using a dielectric resonator (hereinafter simply abbreviated as a "resonator") in Figures 1 to 4. This will be explained with reference to the figures.
第1図は波器の導波管に沿つた縦断面図であ
り、第2図は第1図の矢印−に沿つた横断面
図である。図中、符号1は標準導波管を示し、こ
れは横幅a、縦幅b(一般にa:b=2:1)の
内法を有している。この標準導波管1の一部に遮
断導波管部2が形成されている。遮断導波管部2
の内法は横幅a′(<a)、縦幅bであり、標準導波
管1に対し使用周波数域において遮断(カツトオ
フ)作用をする。そしてこの遮断導波管部2の内
部には、1個以上(図示例は3個)の誘電体共振
器3が、遮断導波管部2の内壁面にスペーサ4を
介し固定された状態で設けられる。 FIG. 1 is a longitudinal cross-sectional view along the waveguide of the wave device, and FIG. 2 is a cross-sectional view along the arrow - in FIG. In the figure, reference numeral 1 indicates a standard waveguide, which has a width a and a width b (generally a:b=2:1). A cut-off waveguide section 2 is formed in a part of this standard waveguide 1 . Cutoff waveguide section 2
The width is a'(<a) and the length is b, which acts as a cut-off for the standard waveguide 1 in the frequency range used. Inside this cut-off waveguide section 2, one or more (three in the illustrated example) dielectric resonators 3 are fixed to the inner wall surface of the cut-off waveguide section 2 via spacers 4. provided.
第3図及び第4図は誘電体共振器3の2つの異
なる例を示し、各図の(イ)、(ロ)、(ハ)はそれぞれ共振
器の斜視図、平面図、側面図である。第3図に示
す共振器3Aは直径D、高さhの円筒形状を有す
るTE01〓共振モードのものであり、電界E及び磁
界Hは図示の如く分布する。また、第4図に示す
共振器3Bは縦A,横B,高さhの角柱形状を有
するTE11〓共振モードのものであり、電界E及び
磁界Hは図示の如く分布する。尚、第2図から第
10図において、矢印EPは共振器3,3A,3
Bの電界面(E面)を示す。 3 and 4 show two different examples of the dielectric resonator 3, and (A), (B), and (C) in each figure are a perspective view, a top view, and a side view of the resonator, respectively. . The resonator 3A shown in FIG. 3 has a cylindrical shape with a diameter D and a height h and is in the TE 01 resonance mode, and the electric field E and magnetic field H are distributed as shown. The resonator 3B shown in FIG. 4 has a prismatic shape with a length A, a width B, and a height h and is in the TE 11 resonance mode, and the electric field E and magnetic field H are distributed as shown. In addition, in FIGS. 2 to 10, arrows EP indicate resonators 3, 3A, and 3.
The electric surface (E plane) of B is shown.
上記のようなTE01〓またはTE11〓共振モードの
共振器3を第1図及び第2図に示すように遮断導
波管部2内に共振器相互の間隔及び共振器と入出
力導波管(標準導波管)との距離を適宜設定して
配列すれば、共振器相互間ならびに共振器と入出
力導波管との間の磁界結合によつて所望の特性の
波器が得られる。 The resonator 3 in the above-mentioned TE 01 〓 or TE 11 〓 resonance mode is installed in the cut-off waveguide section 2 as shown in Figs. If the distance between the resonators and the waveguides (standard waveguides) is appropriately set and arranged, a waveguide with the desired characteristics can be obtained through magnetic field coupling between the resonators and between the resonators and the input/output waveguide. .
このような波器においては、遮断導波管部2
への共振器3の配列及び固定のために遮断導波管
部2が分割可能であることが望ましい。 In such a wave device, the cut-off waveguide section 2
It is desirable that the cut-off waveguide section 2 is divisible for arranging and fixing the resonators 3 to the waveguide.
第5図から第10図は本考案による波器の一
実施例を示す。第5図は遮断導波管部の斜視図で
あり、また第6図は第5図の矢印−に沿つた
遮断導波管部の横断面図である。第5図から明ら
かなように、本考案による遮断導波管部は、後述
する如くその両端に取り付けられるフランジ6を
介して入出力導波管(標準導波管)に分離可能に
接続される筐体5によつて構成されている。 5 to 10 show an embodiment of the wave device according to the present invention. FIG. 5 is a perspective view of the cut-off waveguide section, and FIG. 6 is a cross-sectional view of the cut-off waveguide section taken along the arrow - in FIG. As is clear from FIG. 5, the cut-off waveguide section according to the present invention is separably connected to the input/output waveguide (standard waveguide) via flanges 6 attached to both ends, as will be described later. It is constituted by a housing 5.
筐体5は第5図及び第6図に明示するように、
平面Dに沿つて2つの部分、つまり共振器3が固
定される基部5A及び蓋部5B、に分割されてい
る。この分割平面Dは、共振器3の電界面EPに
平行で且つ基部5Aの内壁面51から距離Cだけ
離れた平面である。距離Cは共振器固定用のスペ
ーサ4の厚さよりも小さく設定される。 As clearly shown in FIGS. 5 and 6, the housing 5 is
It is divided into two parts along plane D: a base part 5A to which the resonator 3 is fixed, and a lid part 5B. This dividing plane D is a plane parallel to the electric surface EP of the resonator 3 and spaced a distance C from the inner wall surface 51 of the base 5A. The distance C is set smaller than the thickness of the spacer 4 for fixing the resonator.
第7図は筐体5の分割状態の斜視図であり、ま
た第8図及び第9図は筐体基部5Aの平面図及び
端面図である。これらの図に示すように筐体基部
5Aの分割面にはネジ穴7が形成され、また筐体
蓋部5Bには外面から分割面に貫通するボルト穴
8が形成され、ボルト9を螺入することにより蓋
部5Bを基部5Aに固定することができる。 FIG. 7 is a perspective view of the housing 5 in a divided state, and FIGS. 8 and 9 are a plan view and an end view of the housing base 5A. As shown in these figures, a screw hole 7 is formed in the divided surface of the housing base 5A, and a bolt hole 8 is formed in the housing cover 5B, penetrating from the outer surface to the divided surface, into which a bolt 9 is screwed. By doing so, the lid portion 5B can be fixed to the base portion 5A.
共振器3は、第8図及び第9図に示すように、
蓋部5Bを取り付ける前に基部5Aにスペーサ4
を介して取り付けられる。この場合、基部5Aの
内壁面51及びこれと直角な段部内壁面52を基
準面として共振器3の位置を正確に決定すること
ができ、取付作業が容易である。 The resonator 3, as shown in FIGS. 8 and 9,
Spacer 4 is attached to the base 5A before attaching the lid 5B.
Attached via. In this case, the position of the resonator 3 can be accurately determined using the inner wall surface 51 of the base portion 5A and the step inner wall surface 52 perpendicular thereto as reference planes, and the installation work is easy.
共振器3を筐体基部5Aに取り付け、更に筐体
蓋部5Bを組み付けた後、第5図に示すように筐
体5の両端部にフランジ6が取り付けられる。フ
ランジ6には標準導波管と同寸法の開口10が形
成されており、ボルト穴11から皿頭ボルト12
(第10図参照)を挿入し、筐体2の端面に形成
したネジ穴13に螺入することにより筐体2に固
定される。更にフランジ6にはネジ穴14が形成
され、これを用いて入出力導波管(標準導波管)
のフランジ(図示せず)をフランジ6に接続す
る。これにより筐体5で構成される遮断導波管部
が波器を構成することになる。 After the resonator 3 is attached to the casing base 5A and the casing lid 5B is assembled, flanges 6 are attached to both ends of the casing 5 as shown in FIG. The flange 6 is formed with an opening 10 having the same dimensions as the standard waveguide, and a countersunk bolt 12 is inserted through the bolt hole 11.
(see FIG. 10) and is fixed to the casing 2 by screwing into the screw hole 13 formed on the end surface of the casing 2. Furthermore, a screw hole 14 is formed in the flange 6, and this is used to connect the input/output waveguide (standard waveguide).
flange (not shown) is connected to flange 6. As a result, the cut-off waveguide section constituted by the housing 5 constitutes a wave device.
尚、図示してないが、筐体蓋部5Bの共振器上
側の壁に共振周波数調整ビスや結合度調整ビスが
設けられ、これらを用いて共振器の共振周波数な
らびに結合度を適宜調整することができるように
なつている。 Although not shown, resonant frequency adjusting screws and coupling degree adjusting screws are provided on the upper wall of the resonator of the housing cover 5B, and these can be used to adjust the resonant frequency and degree of coupling as appropriate. It is becoming possible to do this.
上記のような本考案による遮断導波管部の構造
には以下のような長所がある。 The structure of the blocking waveguide section according to the present invention as described above has the following advantages.
(1) まず、遮断導波管部を構成する筐体が入出力
導波管(標準導波管)と分離可能であり且つ共
振器固定部である基部とその蓋の役目をする蓋
部とに分割可能であるから、共振器の配列及び
固定が非常に容易である。特に、筐体の分割面
を共振器固定内壁面から離して筐体基部にわず
かな高さの段部を形成してあるため、この段部
内壁面を利用して共振器の位置決めを正確に行
なうことが可能である。(1) First, the casing that constitutes the cut-off waveguide section is separable from the input/output waveguide (standard waveguide), and has a base section that is the resonator fixing section and a lid section that serves as the lid. Since the resonators can be divided into two, it is very easy to arrange and fix the resonators. In particular, since the splitting surface of the housing is separated from the resonator fixing inner wall surface and a slightly high stepped section is formed at the housing base, this stepped inner wall surface can be used to accurately position the resonator. Is possible.
(2) また筐体の分割面は共振器の電界面(E面)
と平行で且つ共振器固定平面からの離間距離は
共振器固定用スペーサの厚さよりも小さいの
で、筐体の分割面は共振器の磁界結合に重大な
影響を及ぼす領域外に位置することになり、分
割構造に伴う波器特性への悪影響を最小限あ
るいはほぼ無視できる程度に抑えることがで
き、良好な特性を得ることが可能である。また
かかる分割面位置は前記の周波数調整ネジの取
付けにも何んら支障がなく、好都合である。(2) Also, the dividing surface of the housing is the electric surface (E surface) of the resonator.
and the separation distance from the resonator fixing plane is smaller than the thickness of the resonator fixing spacer, so the dividing plane of the housing is located outside the area that has a significant effect on the magnetic field coupling of the resonator. In this case, it is possible to minimize or almost ignore the adverse effects of the divided structure on the waveform characteristics, and it is possible to obtain good characteristics. Further, such a position of the dividing plane does not pose any problem in attaching the frequency adjustment screw, which is convenient.
更に図示実施例の如く筐体5の両端に標準導
波管開口を有するフランジ6を設けた構造では
次のような付加長所がある。まず、インターフ
エイスを全て標準導波管で行なうことができ
る。また、第10図に示すように、フランジ6
を筐体基部5Aにネジ12で固定したままと
し、筐体蓋部5Bはネジ9及び12を外して取
り外し自在にしておけば、波器の試験調整が
非常に簡便なものとなる。 Furthermore, the structure in which flanges 6 having standard waveguide openings are provided at both ends of the housing 5 as in the illustrated embodiment has the following additional advantages. First, all interfaces can be performed using standard waveguides. In addition, as shown in FIG. 10, the flange 6
If the housing cover 5B is left fixed to the housing base 5A with the screws 12, and the housing cover 5B is made removable by removing the screws 9 and 12, testing and adjustment of the corrugator becomes very simple.
尚、図示実施例のフランジ6は外形寸法が筐
体5とほぼ同じであり、入出力導波管側フラン
ジ固定用のボルトはネジ穴14(第5図)に螺
入される構造であるが、相手フランジが大形の
ものであればこれに合わせてフランジ6を大形
のものに交換することによりボルト及びナツト
を用いて取付けが可能である。また、図示例の
寸法のフランジの場合でも、図示してないが筐
体5のフランジネジ穴14に対応する隅角部を
切除することによつてボルト及びナツトによる
取付けが可能である。 The flange 6 in the illustrated embodiment has almost the same external dimensions as the housing 5, and the bolts for fixing the flange on the input/output waveguide side are screwed into the screw holes 14 (FIG. 5). If the mating flange is large in size, the flange 6 can be replaced with a larger one to accommodate the larger flange, allowing for attachment using bolts and nuts. Further, even in the case of a flange having the dimensions shown in the illustrated example, it is possible to attach the flange with bolts and nuts by cutting out the corner portion corresponding to the flange screw hole 14 of the housing 5 (not shown).
考案の効果
以上のように本考案によれば、軽量且つ小形、
組立や分解作業ならびに試験調整作業が非常に容
易、しかも特性の良好な、誘電体共振器を用いて
構成したすぐれた導波管形波器を実現可能であ
る。Effects of the invention As described above, according to the invention, it is lightweight, small,
It is possible to realize an excellent waveguide waveform using a dielectric resonator, which is very easy to assemble, disassemble, and test and adjust, and has good characteristics.
第1図から第4図は誘電体共振器を用いて構成
した導波管形波器の基本的な構成及び作用を示
す図で第1図が波器の縦断面図、第2図が第1
図の矢印−に沿つた横断面図、第3図及び第
4図が誘電体共振器の2つの異なる例を示す図で
あり、第5図から第10図は本考案による波器
の一実施例を示す図で第5図が遮断導波管部を構
成する筐体の斜視図、第6図が第5図の矢印−
に沿つた筐体の横断面図、第7図が筐体の分割
状態の斜視図、第8図及び第9図が筐体基部のそ
れぞれ平面図及び端面図、第10図が波器の試
験調整時に筐体蓋部を取り外した状態の斜視図で
ある。
1……標準導波管、2……遮断導波管部、3、
3A,3B……誘電体共振器、4……スペーサ、
5……筐体(遮断導波管部)、5A……筐体基部、
5B……筐体蓋部、6……フランジ、7……ネジ
穴、8……ボルト穴、9……ボルト、10……フ
ランジの標準導波管開口、11……ボルト穴、1
2……ボルト、13……ネジ穴、14……ネジ
穴、D……筐体の分割平面、E……電界、H……
磁界、EP……誘電体共振器の電界面(E面)。
Figures 1 to 4 are diagrams showing the basic structure and operation of a waveguide type wave device constructed using a dielectric resonator. 1
3 and 4 are diagrams showing two different examples of dielectric resonators, and FIGS. 5 to 10 are cross-sectional views taken along the arrow - in the figure, and FIGS. Figure 5 is a perspective view of the casing constituting the cut-off waveguide section, and Figure 6 is the arrow shown in Figure 5.
Figure 7 is a perspective view of the housing in a divided state, Figures 8 and 9 are a plan view and end view of the base of the housing, respectively, and Figure 10 is a test of the corrugated device. FIG. 3 is a perspective view with the housing lid removed during adjustment. 1...Standard waveguide, 2...Blocking waveguide section, 3,
3A, 3B...dielectric resonator, 4...spacer,
5... Housing (blocking waveguide part), 5A... Housing base,
5B... Housing cover, 6... Flange, 7... Screw hole, 8... Bolt hole, 9... Bolt, 10... Standard waveguide opening of flange, 11... Bolt hole, 1
2... Bolt, 13... Screw hole, 14... Screw hole, D... Housing dividing plane, E... Electric field, H...
Magnetic field, EP...Electric surface (E plane) of a dielectric resonator.
Claims (1)
いて遮断作用をなす遮断導波管部が形成され、
該遮断導波管部内に1個以上のTE01〓あるいは
TE11〓共振モードを利用した誘電体共振器が該
遮断導波管部内壁面にスペーサを介し固定して
配列される導波管形波器において、前記遮断
導波管部は標準導波管に対し分離可能に接続さ
れる筐体から構成され、また該筐体は誘電体共
振器の電界面(E面)に平行で且つ該筐体の誘
電体共振器固定内壁面から前記スペーサの厚さ
より小さな距離だけ離れた平面に沿つて分割可
能な構造としたことを特徴とする導波管形波
器。 2 実用新案登録請求の範囲第1項記載の導波管
形波器において、前記遮断導波管部を構成す
る筐体の両端部に標準導波管開口を有するフラ
ンジが着脱自在に取り付けられ、該フランジを
介して標準導波管に接続されるように構成され
ていることを特徴とする導波管形波器。[Claims for Utility Model Registration] 1. A cut-off waveguide part is formed in a part of the standard waveguide, the inner diameter of which has a cut-off effect in the frequency range used,
One or more TE 01 〓 or
TE 11 〓In a waveguide type waveguide in which dielectric resonators using a resonance mode are fixedly arranged on the inner wall surface of the cut-off waveguide section via a spacer, the cut-off waveguide section is arranged in a standard waveguide. The casing is parallel to the electric surface (E-plane) of the dielectric resonator and is more than the thickness of the spacer from the inner wall surface of the casing where the dielectric resonator is fixed. A waveguide waveform device characterized by having a structure that can be divided along a plane separated by a small distance. 2 Utility Model Registration Scope of Claims 1. The waveguide type wave device according to claim 1, wherein flanges having standard waveguide openings are removably attached to both ends of the casing constituting the cut-off waveguide section, A waveguide-shaped waveguide configured to be connected to a standard waveguide via the flange.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP18375883U JPS6093301U (en) | 1983-11-30 | 1983-11-30 | waveguide filter |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP18375883U JPS6093301U (en) | 1983-11-30 | 1983-11-30 | waveguide filter |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS6093301U JPS6093301U (en) | 1985-06-26 |
JPH046243Y2 true JPH046243Y2 (en) | 1992-02-20 |
Family
ID=30397619
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP18375883U Granted JPS6093301U (en) | 1983-11-30 | 1983-11-30 | waveguide filter |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS6093301U (en) |
Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5522961A (en) * | 1978-08-07 | 1980-02-19 | Fuji Photo Film Co Ltd | Thermal recording material |
Family Cites Families (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5494137U (en) * | 1977-12-16 | 1979-07-03 |
-
1983
- 1983-11-30 JP JP18375883U patent/JPS6093301U/en active Granted
Patent Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5522961A (en) * | 1978-08-07 | 1980-02-19 | Fuji Photo Film Co Ltd | Thermal recording material |
Also Published As
Publication number | Publication date |
---|---|
JPS6093301U (en) | 1985-06-26 |
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