JPH067435B2 - Magnetic bubble memory device - Google Patents
Magnetic bubble memory deviceInfo
- Publication number
- JPH067435B2 JPH067435B2 JP190584A JP190584A JPH067435B2 JP H067435 B2 JPH067435 B2 JP H067435B2 JP 190584 A JP190584 A JP 190584A JP 190584 A JP190584 A JP 190584A JP H067435 B2 JPH067435 B2 JP H067435B2
- Authority
- JP
- Japan
- Prior art keywords
- magnetic field
- current
- rotating magnetic
- coil
- memory device
- 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
- G11C11/02—Digital stores characterised by the use of particular electric or magnetic storage elements; Storage elements therefor using magnetic elements
- G11C11/14—Digital stores characterised by the use of particular electric or magnetic storage elements; Storage elements therefor using magnetic elements using thin-film elements
Landscapes
- Engineering & Computer Science (AREA)
- Computer Hardware Design (AREA)
Description
【発明の詳細な説明】 〔発明の利用分野〕 本発明は磁気バブルメモリ装置、特に磁気バブルを転送
するために用いられる回転磁界発生用電流駆動回路に係
わるものであり、さらに詳しくは駆動電流波形を一定に
保つための駆動タイミングパルスに関するものである。Description: FIELD OF THE INVENTION The present invention relates to a magnetic bubble memory device, and more particularly to a rotating magnetic field generating current drive circuit used for transferring magnetic bubbles. More specifically, the present invention relates to a drive current waveform. Is related to the drive timing pulse for keeping constant.
一般に、磁気バブルメモリデバイスにおいて、磁気バブ
ルを転送するために、磁気バブルの存在する磁性薄膜面
内で回転する磁界(以下回転磁界と称する)を加えるこ
とが必要である。そして、この回転磁界を発生するには
第1図aに示すように互いに直交して巻設された2組の
回転磁界発生用コイル(以下コイルと称する)に90°
位相の異なる正弦波電流,三角波電流または台形波電流
を流す方法が用いられている。三角波による駆動の場合
を例にとって説明すると、第1図aのXコイル10およ
びYコイル20に同図bに示すようなX電流IXをY電
流IYに対して90°進んだ位相で流すと、反時計方向
に回転する回転磁界を発生することができる。Generally, in a magnetic bubble memory device, in order to transfer a magnetic bubble, it is necessary to apply a magnetic field rotating in the plane of the magnetic thin film in which the magnetic bubble exists (hereinafter referred to as a rotating magnetic field). In order to generate this rotating magnetic field, 90 ° is applied to two sets of rotating magnetic field generating coils (hereinafter referred to as coils) wound orthogonally to each other as shown in FIG. 1a.
A method of flowing sine wave current, triangular wave current or trapezoidal wave current with different phases is used. The case of driving by a triangular wave will be described as an example. An X current I X as shown in FIG. 1B is passed through the X coil 10 and the Y coil 20 in FIG. 1A at a phase advanced by 90 ° with respect to the Y current I Y. Then, a rotating magnetic field rotating counterclockwise can be generated.
通常、磁気バブルは、常時回転磁界によって転送されて
いるだけでなく、磁気バブルを使用しないときは回転磁
界を停止して磁気バブルを停止させておくことがある。
このような場合、磁気バブルを停止させて再スタートさ
せることになるが、従来の磁気バブルメモリ装置におい
ては、この際も回転磁界駆動タイミングパルスは、定常
状態におけると同様のものが印加されていた。しかしな
がら、このような従来の磁気バブルメモリ装置において
は再スタート時回転磁界電流が小さくなってしまい安定
な動作が得られないという問題点があった。Usually, the magnetic bubble is not always transferred by the rotating magnetic field, but when the magnetic bubble is not used, the rotating magnetic field may be stopped to stop the magnetic bubble.
In such a case, the magnetic bubble is stopped and then restarted. In the conventional magnetic bubble memory device, the rotating magnetic field driving timing pulse is the same as that in the steady state in this case as well. . However, such a conventional magnetic bubble memory device has a problem that the rotating magnetic field current at the time of restart becomes small and stable operation cannot be obtained.
第2図は三角波駆動回路の一例、第3図は従来方法によ
るその回路への入力信号パルスと出力波形の関係を示す
ものである。先ずコイル5に図示の+方向に電流を流す
にはコイルプリドライバ(CPD)8に+ON信号を入
力すると、コイルドプリドライバ8からMOSFET1
およびMOSFET2をONにするに必要な信号が出力
されて、電流は電源VRからMOSFET1→コイル5
→MOSFET2の方向に流れる。この時流れる電流は
ほぼ直線的に電流値が増え、電流値ILは、 ここで、VR:電源電圧 L:コイル5のインダクタンス t:時間 で表わされる。ついで+ON信号が0に戻るとコイル5
のインダクタンスのため、まだ電流が流れ続けようとす
るため、MOSFET3およびMOSFET4の寄生サ
ブストレートダイオードを通してコイル5に蓄積されて
いたエネルギーを放出するのでMOSFET4(ダイオ
ード)→コイル5→MOSFET3(ダイオード)の経
路で電流は流れ、かつその値は次第に減少してゆき、つ
いには0に戻る。同様にコイル5に−方向に電流を流す
にはコイルプリドライバ8に−ON信号を入力すること
により行われる。FIG. 2 shows an example of a triangular wave drive circuit, and FIG. 3 shows the relationship between the input signal pulse and the output waveform to the circuit by the conventional method. First, in order to pass a current in the + direction shown in the coil 5, a + ON signal is input to the coil pre-driver (CPD) 8, and the coiled pre-driver 8 causes the MOSFET 1
And MOSFET2 are output signals required to ON, current MOSFET 1 → coil 5 from the power source V R
→ Flows in the direction of MOSFET 2. The current value flowing at this time increases almost linearly, and the current value I L is Here, V R : power supply voltage L: inductance of coil 5 t: time Then, when the + ON signal returns to 0, the coil 5
Due to the inductance of, the current tends to continue to flow, and the energy stored in the coil 5 is released through the parasitic substrate diode of the MOSFET 3 and the MOSFET 4, so that the path of MOSFET 4 (diode) → coil 5 → MOSFET 3 (diode) At, the current flows, and its value gradually decreases until it finally returns to zero. Similarly, in order to pass a current through the coil 5 in the-direction, a -ON signal is input to the coil pre-driver 8.
ここでコイル5の電流が定常状態で流れている場合に
は、浮遊容量Cs16およびCs27においては、電流の流
れる方向により+ON信号、−ON信号の直前で各々そ
の電位,電荷は常に一定の状態となっている。しかしス
タートサイクルではコイル端の電圧は回路のインピーダ
ンスにより定まる電位となる(通常は0電位)。この状
態では回転磁界電流を流し始めると浮遊容量Cs16およ
びCs27をチャージアップする分だけ、電流を流す力が
弱くなりスタート時のコイル5の電流すなわち回転磁界
用電流が少なくなってしまう。すなわち第3図におい
て、スタート時の回転磁界電流のピーク値IPSは定常状
態で動作時の回転磁界電流のピーク値IPよりも小さく
なって、スタート時の動作マージンが低下してしまうと
いう問題点があった。Here, when the current of the coil 5 is flowing in a steady state, in the stray capacitances Cs 1 6 and Cs 2 7, the potential and the charge are always constant immediately before the + ON signal and the -ON signal depending on the direction of the current flow. It is in a constant state. However, in the start cycle, the voltage at the coil end becomes a potential determined by the impedance of the circuit (normally 0 potential). In this state, when the rotating magnetic field current is started to flow, the stray capacitances Cs 1 6 and Cs 2 7 are charged up, so that the current flowing force is weakened and the current of the coil 5 at the start, that is, the rotating magnetic field current is reduced. . That is, in FIG. 3, the peak value I PS of the rotating magnetic field current at the time of start becomes smaller than the peak value I P of the rotating magnetic field current at the time of operation in the steady state, and the operation margin at the time of start decreases. There was a point.
本発明は従来のこのような問題点を解消するためになさ
れたもので、その目的とするところは、回転磁界発生電
流波形を常に一定にし、安定で動作マージンの広い磁気
バブルメモリ装置を提供することにある。The present invention has been made in order to solve such a conventional problem, and an object of the present invention is to provide a magnetic bubble memory device which is stable and has a wide operation margin, in which the rotating magnetic field generation current waveform is always constant. Especially.
本発明はこのような目的を達成するために、磁気バブル
メモリ装置の回転磁界用電流回路の浮遊容量によるスタ
ート時の回転磁界電流値の減少を、駆動タイミングパル
ス幅により補償し、回転磁界発生用電流波形を一定に保
つものである。In order to achieve such an object, the present invention compensates for the decrease in the rotating magnetic field current value at the start due to the stray capacitance of the rotating magnetic field current circuit of the magnetic bubble memory device by the drive timing pulse width to generate the rotating magnetic field. It keeps the current waveform constant.
以下、実施例にもとづいて本発明を詳細に説明する。 Hereinafter, the present invention will be described in detail based on Examples.
第2図の三角波駆動回路において、コイルプリドライバ
8に入力する+ON信号の波形を第4図に示す如く、ス
タート時のみ、定常状態動作時のパルスよりも△Tだけ
パルス幅が広く、しかも定常動作時のパルスに比し、そ
の位相も△Tだけ早い動作パルスとすることにより、時
間△Tの間に浮遊容量Cs16およびCs27がチャージア
ップされるので、スタート時においてもその回転磁界電
流のピーク値は、定常動作時の回転磁界電流のピーク値
と同じにすることができる。In the triangular wave drive circuit of FIG. 2, as shown in FIG. 4, the waveform of the + ON signal input to the coil pre-driver 8 has a wider pulse width by ΔT than the pulse in the steady state operation only at the start, and the steady state. Since the stray capacitances Cs 1 6 and Cs 2 7 are charged up during the time ΔT by making the operation pulse whose phase is ΔT earlier than that of the pulse at the time of operation, the rotation thereof at the time of start as well. The peak value of the magnetic field current can be the same as the peak value of the rotating magnetic field current during steady operation.
ここでスタート時の+ON信号パルスのパルス幅の増加
分△Tは、各々の回転例における浮遊容量値Cs1,Cs2
を勘案して適宜決定すればよいことは勿論である。Here, the increment ΔT of the pulse width of the + ON signal pulse at the start is the stray capacitance values Cs 1 and Cs 2 in each rotation example.
Needless to say, it may be appropriately determined in consideration of the above.
このように、本発明においては、磁気バブル転送のため
の回転磁界発生用電流回路のための動作パルスを、スタ
ート時においては、そのパルス幅およびタイミングを定
常動作時のそれと変えることにより、回転磁界発生用電
流波形を常に一定にすることができる。As described above, according to the present invention, the operating pulse for the rotating magnetic field generating current circuit for transferring the magnetic bubbles is changed at the start from the pulse width and the timing thereof during the steady operation, so that the rotating magnetic field is changed. The current waveform for generation can be kept constant.
なお本実施例においては、回転磁界発生用電流回路のス
イッチ素子にMOSFETを、電流波形を三角波電流と
したが、本発明はこれらに限定されることなく、スイッ
チ素子はバイポーラトランジスタ(+逆方向電流用ダイ
オード)、電流波形は台形波電流,正弦波電流としても
上記同様の本発明の効果が得られることは殊に説明する
までもなく明らかである。In this embodiment, a MOSFET is used as the switch element of the rotating magnetic field generating current circuit and a triangular wave current is used as the current waveform. However, the present invention is not limited to these, and the switch element is a bipolar transistor (+ reverse current). It is obvious, of course, that the same effects of the present invention can be obtained even if the current waveform is a trapezoidal wave current or a sine wave current.
また上記パルス幅およびタイミングによる浮遊容量の補
償は、回転磁界発生用コイルのうち、Xコイル,Yコイ
ルの一方あるいはXコイル,Yコイル双方に、その磁気
バブルメモリ装置の目的,用途に応じて使い分け適用す
ればよい。Further, the compensation of the stray capacitance by the pulse width and the timing is selectively applied to one of the X coil and the Y coil or both the X coil and the Y coil of the rotating magnetic field generating coils according to the purpose and use of the magnetic bubble memory device. You can apply.
このように本発明に係る磁気バブルメモリ装置による
と、回転磁界発生用電流の波形をスタート時,定常動作
時の如何に拘らず常に一定にできるので、回転磁界のス
タート時においても、磁気バブルメモリ装置の動作マー
ジンの低下を防止でき安定な動作領域が広くなる効果が
ある。As described above, according to the magnetic bubble memory device of the present invention, the waveform of the rotating magnetic field generating current can be always constant regardless of whether the rotating magnetic field is generated at the start or during the steady operation. This has the effect of preventing a decrease in the operating margin of the device and widening the stable operating area.
第1図a,bは磁気バブルメモリ装置に用いられるXコ
イルおよびYコイルの要部斜視図およびその電流波形
図、第2図は回転磁界用電流回路の一例を示す要部回路
図、第3図は従来の回転磁界駆動パルス,回転磁界発生
用電流およびコイル端電圧を示す図、第4図は本発明に
よる回転磁界駆動パルス,回転磁界発生用電流およびコ
イル端電圧を示す図である。 1,2,3,4……MOSFET、5……回転磁界発生
用コイル、6,7……浮遊容量、8……コイルプリドラ
イバ、10,20……回転磁界発生用コイル。1a and 1b are perspective views and main current waveform diagrams of main parts of an X coil and a Y coil used in a magnetic bubble memory device, and FIG. 2 is a main part circuit diagram showing an example of a rotating magnetic field current circuit. FIG. 4 is a diagram showing a conventional rotating magnetic field driving pulse, a rotating magnetic field generating current and a coil end voltage, and FIG. 4 is a diagram showing a rotating magnetic field driving pulse, a rotating magnetic field generating current and a coil end voltage according to the present invention. 1, 2, 3, 4 ... MOSFET, 5 ... Rotating magnetic field generating coil, 6, 7 ... Stray capacitance, 8 ... Coil pre-driver, 10, 20 ... Rotating magnetic field generating coil.
Claims (1)
用コイルおよび該コイルをブリッジ形式で駆動するため
の4個のMOSFETを含む電流回路を備える磁気バブ
ルメモリ装置において、上記MOSFETの浮遊容量の
影響を補償するため、上記MOSFETの駆動パルスの
前縁を、回転磁界定常動作時よりも回転磁界スタート時
において時間的に早く位置させることにより、前記駆動
パルスの幅を、回転磁界定常動作時よりも回転磁界スタ
ート時において広くしたことを特徴とする磁気バブルメ
モリ装置。1. A magnetic bubble memory device comprising a rotating magnetic field generating coil for transferring a magnetic bubble and a current circuit including four MOSFETs for driving the coil in a bridge form. In order to compensate the influence, the leading edge of the drive pulse of the MOSFET is positioned earlier in time when the rotating magnetic field is started than when in the rotating magnetic field steady operation, so that the width of the drive pulse is made wider than that in the rotating magnetic field steady operation. The magnetic bubble memory device is also characterized in that it is widened when the rotating magnetic field is started.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP190584A JPH067435B2 (en) | 1984-01-11 | 1984-01-11 | Magnetic bubble memory device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP190584A JPH067435B2 (en) | 1984-01-11 | 1984-01-11 | Magnetic bubble memory device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS60147994A JPS60147994A (en) | 1985-08-05 |
| JPH067435B2 true JPH067435B2 (en) | 1994-01-26 |
Family
ID=11514590
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP190584A Expired - Lifetime JPH067435B2 (en) | 1984-01-11 | 1984-01-11 | Magnetic bubble memory device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH067435B2 (en) |
-
1984
- 1984-01-11 JP JP190584A patent/JPH067435B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPS60147994A (en) | 1985-08-05 |
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