JPH0632208B2 - Non-volatile high recording density random access memory - Google Patents
Non-volatile high recording density random access memoryInfo
- Publication number
- JPH0632208B2 JPH0632208B2 JP59001255A JP125584A JPH0632208B2 JP H0632208 B2 JPH0632208 B2 JP H0632208B2 JP 59001255 A JP59001255 A JP 59001255A JP 125584 A JP125584 A JP 125584A JP H0632208 B2 JPH0632208 B2 JP H0632208B2
- Authority
- JP
- Japan
- Prior art keywords
- random access
- access memory
- high recording
- recording density
- lattice points
- 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
Links
Classifications
-
- G—PHYSICS
- G11—INFORMATION STORAGE
- G11C—STATIC STORES
- G11C11/00—Digital stores characterised by the use of particular electric or magnetic storage elements; Storage elements therefor
Landscapes
- Engineering & Computer Science (AREA)
- Computer Hardware Design (AREA)
- Magnetic Record Carriers (AREA)
- Semiconductor Memories (AREA)
- Mram Or Spin Memory Techniques (AREA)
Description
【発明の詳細な説明】 本発明は強磁性体を用いた不揮発性高記録密度ランダム
アクセスメモリーに関する。The present invention relates to a nonvolatile high recording density random access memory using a ferromagnetic material.
本発明は、従来の磁気記録装置あるいは半導体を用いた
記録装置に対して、前者に比べては記録密度の点で、後
者に比べては不揮発性と言う点で、それぞれ優位に立つ
記録装置を提供することを目的とする。The present invention provides a recording device that is superior to a conventional magnetic recording device or a recording device using a semiconductor in terms of recording density as compared with the former and in non-volatility as compared with the latter. The purpose is to provide.
以上の様な目的を達成するために、本発明によって、強
磁性体超微粒子を非磁性体中の定められた格子点上に規
則的正しく着床・固定し、この格子点を通る随時書き込
み・読み出し用の線を設けた不揮発性高記録密度ランダ
ムアクセスメモリーが提供される。In order to achieve the above object, according to the present invention, ferromagnetic ultrafine particles are regularly and correctly landed / fixed on a predetermined lattice point in a non-magnetic substance, and writing is performed at any time through the lattice point. A nonvolatile high recording density random access memory provided with a read line is provided.
望ましくは、非磁性体は基板状のものであり、格子点は
この基板の平面上の格子点である。そして、強磁性体超
微粒子は基板平面上の格子点に規則的にあけられた穴に
着床・固定する。格子点は例えば正方格子の格子点であ
る。また、強磁性体超微粒子はSi又はSiO2等の第1の
絶縁体膜によって固定する。随時書き込み・読み出し用
の線は相互にSi又はSiO2等の第2の絶縁体膜を介して
第1の絶縁体膜上に設ける。随時書き込み線は格子点に
おいて相互に接触しないで交叉する2群の線からなって
いる。随時読み出し線は1本のラインからなっている。
そして、書き込みたい格子点を通る相互に交叉する2本
の随時書き込み線には、強磁性体超微粒子の磁化の反転
に必要な臨界電流以下の電流を送り込むように構成す
る。また、読み出したい格子点を通る随時書き込み線に
は、読み出し時及び読み出し後にも電流を送り込むよう
に構成する。さらに、強磁性体超微粒子は非磁性体基板
平面上の格子点に規則的にあけられた穴に着床・固定
し、この格子点を通る随時書き込み・読み出し用の線を
設け、このように構成したものを複数枚重ね合わせて一
体とする。Desirably, the non-magnetic material is a substrate, and the lattice points are lattice points on the plane of the substrate. Then, the ultrafine particles of the ferromagnetic material are set in and fixed in the holes regularly formed at the lattice points on the plane of the substrate. The grid points are, for example, grid points of a square grid. Further, the ferromagnetic ultrafine particles are fixed by a first insulating film such as Si or SiO 2 . Writing / reading lines are provided on the first insulator film via the second insulator film such as Si or SiO 2 mutually as needed. The writing line is composed of two groups of lines which intersect each other without touching each other at the lattice points. The read line from time to time consists of one line.
Then, a current below the critical current necessary for reversing the magnetization of the ferromagnetic ultrafine particles is fed to the two writing lines that intersect each other and pass through the lattice points to be written. In addition, a current is sent to a write line that passes through a grid point to be read at any time during and after reading. Furthermore, the ferromagnetic ultrafine particles are implanted and fixed in holes that are regularly formed at lattice points on the plane of the non-magnetic substrate, and lines for writing and reading that pass through the lattice points at any time are provided. A plurality of the constructed ones are superposed and integrated.
次に、本発明の1実施例を第1図から第4図を参照にし
ながら説明する。Next, one embodiment of the present invention will be described with reference to FIGS. 1 to 4.
第1図は、この実施例の不揮発性高記録密度ランダムア
クセスメモリーの分解斜視図を示すもので、この図にお
いて符号1はSi又はSiO2の非磁性体基板である。符号1
bはこの基板1上にあけられた、強磁性体超微粒子たと
えば鉄、ニツケル、コバルトなどを着床させるための穴
であり、光、電子線あるいはX線を用いた通常のリソグ
ララフィーの技術によつて、基板1上に予め決められた
形状、深さ、位置でこの穴1bは形成される。第1図に
おいては、立体的に見えるようにするために穴1bの断
面1aを示したある。穴1bは定まつた格子点上に規則
的にあけられており、その格子点の配置の対称性は正方
格子を例として示してあるが、他の対称性の場合も可能
である。穴1bをあけた後、基板1に垂直に強い磁場を
かけながら強磁性体超微粒子をキヤリアーガス(N2又は
H2)に乗せて吹きつけ、穴1bにこの超微粒子を着床さ
せる。その際、穴1b以外の基板1の表面はレジスト膜
でおおつておき、超微粒子の着床後このレジスト膜を除
去する。その後、基板1の表面に符号2で示すSi又はSi
O2等の絶縁性膜を蒸着して、着床した超微粒子を固定す
る膜を作る。その上に読み出し用の線2aを、やはり前
記したリソグラフィーの技術を用いて作成する。読み出
し線2aの配置は、第2図に示すように例えば正方格子
の対角線を通る平行な線の群であり、点線2bで示すよ
うにそれらは1本のラインに連結されている。読み出し
線2aは必ずしも正方格子の対角線を通る必要はなく、
種々の変形が可能である。また、当然のことながら穴1
bの格子点の対称性によつても異なる。なお、第2図中
にSi又はSiO2膜2の下面に接する穴1bの上面の形を点
線で示してある。読み出し線2aを作製した後、その上
にSi又はSiO2等の絶縁体膜3を蒸着し、その上に第1の
書き込み線3aを同様に作製する(第3図)。更に、そ
の上に別のSi又はSiO2等の絶縁体膜4を蒸着し、第2の
書き込み線4aを同様に作製する(第4図)。第1の書
き込み線3aは正方格子の場合横方向に平行に伸びてお
り、第2の書き込み線4aはこれと交叉する縦方向に平
行に伸びている。そして、第1及び第2の書き込み線の
交叉点は各格子点に一致している。以上の実施例におい
ては、読み出し線2aの上に書き込み線3a、4aが配
置されているが、基板1の上にまず書き込み線3a、4
aを配置し、その上に読み出し線2aを設ける等の変形
が可能であることは明らかであろう。なお、穴あけの寸
法、線の幅等は現リソグラフィー技術で到達可能な限り
微細なものとする。FIG. 1 is an exploded perspective view of the nonvolatile high recording density random access memory of this embodiment, in which reference numeral 1 is a non-magnetic substrate of Si or SiO 2 . Code 1
Reference numeral b is a hole formed on the substrate 1 for implanting ferromagnetic ultrafine particles such as iron, nickel, and cobalt, which is a normal lithographic technique using light, electron beams or X-rays. Thus, the hole 1b is formed on the substrate 1 in a predetermined shape, depth and position. In FIG. 1, the cross section 1a of the hole 1b is shown in order to make it appear three-dimensional. The holes 1b are regularly formed on fixed grid points, and the symmetry of the arrangement of the grid points is shown as an example of a square grid, but other symmetry is also possible. After forming the hole 1b, the ferromagnetic ultrafine particles are applied to the carrier gas (N 2 or N 2 while applying a strong magnetic field perpendicular to the substrate 1).
H 2 ), and spraying, the ultrafine particles are implanted in the hole 1 b. At that time, the surface of the substrate 1 other than the holes 1b is covered with a resist film, and the resist film is removed after the implantation of the ultrafine particles. After that, Si or Si shown by reference numeral 2 on the surface of the substrate 1
An insulating film such as O 2 is vapor-deposited to form a film for fixing the implanted ultrafine particles. The read line 2a is formed thereon by using the above-mentioned lithographic technique. The arrangement of the read lines 2a is, for example, a group of parallel lines passing through diagonal lines of a square lattice as shown in FIG. 2, and they are connected to one line as shown by a dotted line 2b. The readout line 2a does not necessarily have to pass through the diagonal of the square lattice,
Various modifications are possible. Also, of course, hole 1
It also depends on the symmetry of the lattice points of b. In FIG. 2, the shape of the upper surface of the hole 1b in contact with the lower surface of the Si or SiO 2 film 2 is shown by a dotted line. After the read line 2a is formed, an insulating film 3 such as Si or SiO 2 is vapor-deposited on the read line 2a, and the first write line 3a is similarly formed thereon (FIG. 3). Further, another insulating film 4 such as Si or SiO 2 is vapor-deposited thereon, and the second write line 4a is similarly prepared (FIG. 4). In the case of a square lattice, the first write line 3a extends in parallel to the horizontal direction, and the second write line 4a extends in parallel to the vertical direction intersecting with this. The intersections of the first and second writing lines coincide with the lattice points. In the above embodiment, the write lines 3a and 4a are arranged on the read line 2a, but the write lines 3a and 4a are first formed on the substrate 1.
It will be apparent that modifications such as arranging a and providing the read line 2a thereon can be made. The size of the holes and the width of the lines should be as fine as possible with current lithography technology.
以上の実施例のメモリーは次のように動作する。まず、
書き込む前には全ての超微粒子は各格子点で例えば上向
きの磁化方向を持つていたとする。このとき第1の書き
込み線3a及び第2の書き込み線4aのうち、書き込み
たい格子点を通るラインを決めて、それらに同時に、強
磁性体超微粒子の磁化の反転に必要な臨界海電流以下の
電流を送り込むと、他の格子点を通る電流は全て臨界電
流以下であるため磁化は反転しないが、選ばれたライン
3aと4aの交叉する点の格子点のみ、両者の電流の和
が臨界電流以上に達し、その格子点の超微粒子のみの磁
化が反転する。すなわち、反転前が0、反転後が1に対
応する記録ができる。読み出しは、書き込み線3a、4
aに全く同様な操作を行つた時に、その選ばれた格子点
が0の状態にあるか、又は1の状態にあるかによつて、
磁化の反転が起るか、又は起らないかであり、読み出し
線2aに誘起される電流が異なることになるので、その
格子点の超微粒子の記憶内容(0か1か)を知ることが
できることによる。ただし、その時に読んだことによつ
て起きた磁化の反転は再びもとに戻しておくことが必要
であり、これは書き込み線3a、4aに必要な電流を送
り込むことによつて行う。The memory of the above embodiment operates as follows. First,
Before writing, it is assumed that all the ultrafine particles have, for example, an upward magnetization direction at each lattice point. At this time, of the first write line 3a and the second write line 4a, the line passing through the lattice point to be written is determined, and at the same time, the line below the critical sea current required for reversing the magnetization of the ferromagnetic ultrafine particles is determined. When a current is sent, the magnetization does not reverse because all the currents passing through the other lattice points are below the critical current, but the sum of the two currents is the critical current only at the lattice point at the intersection of the selected lines 3a and 4a. After reaching the above, the magnetization of only the ultrafine particles at the lattice point is reversed. That is, it is possible to perform recording corresponding to 0 before inversion and 1 after inversion. For reading, write lines 3a, 4
Depending on whether the selected lattice point is in the state of 0 or in the state of 1 when performing the same operation on a,
Since the reversal of magnetization occurs or does not occur and the current induced in the read line 2a is different, it is possible to know the stored content (0 or 1) of the ultrafine particles at the lattice point. It depends on what you can do. However, the reversal of the magnetization caused by the reading at that time needs to be restored again, and this is performed by sending a necessary current to the write lines 3a and 4a.
本発明の効果は、この発明により、従来半導体のLSI
に用いられて来た技術をそのまま利用することによつて
比較的簡単に製作することができ、従来のテープあるい
はディスク等のメモリーより1桁以上大きな記録密度を
得ることができることにある。また、微細加工の技術が
発展するのに伴い、本発明のメモリーの記録密度は必然
的に増大することが見込まれる。さらに、半導体を用い
たRAMに比べて、本発明のメモリーは不揮発性であ
り、メモリー内容の保存ができることが、半導体メモリ
ーに比べての著しい利点である。According to the present invention, the effect of the present invention is to provide a conventional semiconductor LSI.
It is possible to manufacture relatively easily by directly using the technology used in the above, and it is possible to obtain a recording density larger by one digit or more than the memory such as the conventional tape or disk. Further, it is expected that the recording density of the memory of the present invention will inevitably increase with the development of fine processing technology. Further, the memory of the present invention is non-volatile as compared with a RAM using a semiconductor, and the memory content can be stored, which is a significant advantage over a semiconductor memory.
なお、以上のようにして構成された単層のメモリーを複
数枚重ね合わせて一体として、立体構造のメモリーを構
成することができる等の変形が可能であることは明らか
であろう。その場合、書き込み線は、方向の異なる3群
以上の線で構成することも可能である。It will be apparent that modifications such as a three-dimensional memory can be configured by superimposing a plurality of single-layer memories configured as described above and integrating them. In that case, the write line can be formed by three or more groups of lines having different directions.
第1図は本発明の1実施例の不揮発性高記録密度ランダ
ムアクセスメモリーの分解斜視図、第2図は第1図のメ
モリーの読み出し線に関する部分の詳細図、第3図及び
第4図は第1図のメモリーの第1及び第2の書き込み線
に関する部分の詳細図である。 1:非磁性体基板、1b:穴、2、3、4:絶縁体膜、
2a:読み出し線、3a、4a:書き込み線FIG. 1 is an exploded perspective view of a nonvolatile high recording density random access memory according to an embodiment of the present invention, FIG. 2 is a detailed view of a portion related to a read line of the memory of FIG. 1, and FIGS. 3 is a detailed view of a portion of the memory of FIG. 1 relating to first and second write lines. FIG. 1: non-magnetic substrate, 1b: hole, 2, 3, 4: insulating film,
2a: read line, 3a, 4a: write line
Claims (13)
点上に穴を有する非磁性体基板、前述格子点上の穴に埋
設された強磁性体の超微粒子、およびリソグラフィー技
術によって作られ、前記格子点を通る随時書き込みおよ
び読み出し用の互いに絶縁された配線を備えたことを特
徴とする不揮発性高記録密度ランダムアクセスメモリー1. A non-magnetic substrate made by a lithographic technique and having holes on lattice points, ultrafine particles of a ferromagnetic material embedded in the holes on said lattice points, and said lattice points made by a lithographic technique. Non-volatile high recording density random access memory characterized by having mutually insulated wiring for occasional writing and reading through
とリソグラフィー技術を用いて作られたことを特徴とす
る特許請求の範囲第1項記載の不揮発性高記録密度ラン
ダムアクセスメモリー2. The nonvolatile high recording density random access memory according to claim 1, wherein the ferromagnetic ultrafine particles are produced by using a gas evaporation method and a lithography technique.
法によって作る際に、磁場を加えることを特徴とする特
許請求の範囲第2項記載の不揮発性高記録密度ランダム
アクセスメモリー3. A nonvolatile high recording density random access memory according to claim 2, wherein a magnetic field is applied when the ultrafine particles of the ferromagnetic material are produced by the gas evaporation method.
平面上の格子点であることを特徴とする特許請求の範囲
第1項記載の不揮発性高記録密度ランダムアクセスメモ
リー4. The non-volatile high recording density random access memory according to claim 1, wherein the lattice points on the non-magnetic substrate are lattice points on a plane of the substrate.
子点に規則的にあけられた穴に着床・固定されることを
特徴とする特許請求の範囲第4項記載の不揮発性高記録
密度ランダムアクセスメモリー5. Nonvolatile according to claim 4, wherein the ultrafine ferromagnetic particles are landed and fixed in holes regularly formed at lattice points on the plane of the substrate. High recording density random access memory
の巣状又は三角格子状の格子点であることを特徴とする
特許請求の範囲第4項又は第5項記載の不揮発性高記録
密度ランダムアクセスメモリー6. The nonvolatile high recording density according to claim 4 or 5, wherein the lattice points are square lattices, parallelograms, honeycombs or triangular lattices. Random access memory
1の絶縁体膜によって固定されることを特徴とする特許
請求の範囲第4項から第6項の何れかの不揮発性高記録
密度ランダムアクセスメモリー7. The nonvolatile high recording according to any one of claims 4 to 6, wherein the ferromagnetic fine particles are fixed by a first insulating film such as Si or SiO 2. Density random access memory
Si又はSiO2等の第2の絶縁体膜を介して第1の絶
縁体膜の上に設けることを特徴とする特許請求の範囲第
7項記載の不揮発性高記録密度ランダムアクセスメモリ
ー8. A line for writing / reading at any time is provided on the first insulator film via a second insulator film such as Si or SiO 2 with respect to each other. Nonvolatile high recording density random access memory according to item 7.
触しないで交差する2群の線からなることを特徴とする
特許請求の範囲第4項から第8項の何れかの不揮発性高
記録密度ランダムアクセスメモリー9. The non-volatile high recording density according to any one of claims 4 to 8, characterized in that the write line at any time is composed of two groups of lines which intersect without touching each other at lattice points. Random access memory
ことを特徴とする特許請求の範囲第4項から第9項の何
れかの不揮発性高記録密度ランダムアクセスメモリー10. The non-volatile high recording density random access memory according to claim 4, wherein the read line at any time comprises one line.
る2本の随時書き込み線には、それぞれ強磁性体超微粒
子の磁化の反転に必要な臨界電流以下の電流を送りこむ
ように構成したことを特徴とする特許請求の範囲第8項
または第9項の何れかの不揮発性高記録密度ランダムア
クセスメモリー11. A configuration is such that a current below a critical current required for reversing the magnetization of ferromagnetic ultrafine particles is sent to each of two write lines that intersect each other and pass through a lattice point to be written. Non-volatile high recording density random access memory according to any one of claims 8 and 9 characterized by
線には、読み出し時および読み出し後にも電流を送りこ
むように構成したことを特徴とする特許請求の範囲第8
項、第9項又は第11項の何れかの不揮発性高記録密度
ランダムアクセスメモリー12. The present invention according to claim 8, characterized in that a current is sent to the write line passing through the grid point to be read at any time during and after reading.
Non-volatile high recording density random access memory according to any one of items 9 and 11
の格子点に規則的にあけられた穴に着床・固定し、この
格子点を通る随時書き込み・読み出し用の線を設け、こ
のように構成したものを複数枚重ね合わせて一体とする
ことを特徴とする特許請求の範囲第1項記載の不揮発性
高記録密度ランダムアクセスメモリー13. Ferromagnetic ultrafine particles are landed and fixed in holes regularly formed at lattice points on the surface of a non-magnetic substrate, and lines for writing and reading are provided at any time passing through the lattice points. A nonvolatile high recording density random access memory according to claim 1, characterized in that a plurality of the thus constituted ones are superposed and integrated.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP59001255A JPH0632208B2 (en) | 1984-01-10 | 1984-01-10 | Non-volatile high recording density random access memory |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP59001255A JPH0632208B2 (en) | 1984-01-10 | 1984-01-10 | Non-volatile high recording density random access memory |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS60145589A JPS60145589A (en) | 1985-08-01 |
| JPH0632208B2 true JPH0632208B2 (en) | 1994-04-27 |
Family
ID=11496344
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP59001255A Expired - Lifetime JPH0632208B2 (en) | 1984-01-10 | 1984-01-10 | Non-volatile high recording density random access memory |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0632208B2 (en) |
-
1984
- 1984-01-10 JP JP59001255A patent/JPH0632208B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPS60145589A (en) | 1985-08-01 |
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