JPS63108587A - Magnetic storing element - Google Patents

Abstract

PURPOSE:To enhance the stability and the reliability of a domain arrangement by deleting a part of a ferromagnetic film surface, disposing fine lines having a vertical magnetization in the corresponding part of the area and generating a bubble and a local magnetic field. CONSTITUTION:A plateau 4 is formed by an etching in an area desired to hold the domain of the surface of a stripe domain holding layer 1 on a substrate 2. On an area between adjacent plateauss 4, a fine line pattern 5 formed by the magnetic film having the vertical magnetization is disposed and a bubble generator and a magnetic field generating means 7 in a local plane are disposed at one end of the pattern 5 and a local magnetic field generating means 8 at the other end. According to a necessity, a bubble generating conductor pattern 9 is disposed at the intermediate part of both the ends. The respective bubbles are extended along the pattern 5 to form the stripe domain. Then, a single domain having the respective plateaus at the center is formed according to a magnetic field operation, a domain magnetic wall in the plateau is contacted with the periphery 6 of the plateau and a ring shape domain 12 is stabilized in the outside thereof.

Description

DETAILED DESCRIPTION OF THE INVENTION (Field of Industrial Application) The present invention relates to a nonvolatile ultra-high density solid state magnetic memory element.

(Prior art) This magnetic memory element includes an information reading means, an information writing means, and an information storage means, and exists in a ferromagnetic material (including a ferrimagnetic film) whose easy magnetization direction is perpendicular to the film surface. Adjacent vertical Bloch lines (hereinafter referred to as VBL) created in Bloch domain walls around the striped domain
It has a means to hold and transfer them as a pair within the Bloch domain wall. For example, when the element configuration is a major line and a minor loop configuration, in the major line, bubbles are used as information carriers, the minor loop is composed of striped domains, and the VBL pairs existing in the Bloch domain wall around the bubbles are used as information carriers. shall be. To show the overall flow of information, first, information written by the bubble generator (the presence or absence of bubbles) moves along the write major line. In order to sequentially store one page's worth of information in the minor loop, the minor loop is constructed with a Bloch domain wall that can hold VBL pairs so that the information on the major line indicated by the presence or absence of bubbles can be transferred to the minor loop in the form of VBL pairs. This is a feature of the present invention, and is an important key to dramatically improving storage capacity. The information transferred to the minor loop (VBL pair) by the write line transfer gate can move the striped domain domain wall soil forming the minor loop. Reading from the minor loop and transferring information to the major line involves converting VBL pairs to bubbles.

Read the converted bubble presence/absence column with the bubble generator. In this way, by configuring the minor loop with striped domains existing in the bubble material and using VBL pairs instead of bubbles as information carriers on the minor loop, it is possible to improve the storage density by about two orders of magnitude compared to bubble elements. It can be achieved. As a method for retaining the stripe domain/minor loop of a magnetic memory element (Bloch line memory element) that uses such VBL pairs as information carriers, trenches are selectively dug in the film surface over the region where the stripe domains are desired to be stabilized. It is known to stabilize the striped domains in the form of ring-shaped striped domains in the grooves (Japanese Patent Application No. 60-079659).

FIG. 7 is a configuration diagram of the main part of the striped domain holding layer in the minor loop portion. A striped domain holding layer 1 is provided on a substrate 2 shown in FIG. 7(a). Grooves 23 are formed by selectively digging grooves on the surface only in areas where it is desired to hold the striped domains in a ring shape.

This width is larger than the natural width wO (width in the absence of a magnetic field) of the stripe domain, and is about 2wO or less.

The reason for this can be understood by considering the role of the film thickness step at the groove boundary. Among the boundaries of the groove, the boundary 6 has a convex portion inside thereof having a boundary of 6, so it serves to attract the inner domain wall of the ring-shaped domain 12 to 6, and the boundary 24 initializes the ring-shaped domain 12. At this time, it acts as a guide to prevent the inner domain wall from being too far away from 6. Furthermore, the width of the convex portion having a border of 6 must be greater than or equal to wO.

If this is not done, when the domain 12 is held in a ring shape in the groove, the repulsive interaction between the linear domains on both sides of the convex portion having the boundary 6 will be strong, and the inner domain wall of the ring-shaped domain will be held at the boundary 6. It will no longer be firmly fixed directly underneath. When the grooves 23 are formed so as to satisfy the above conditions, the striped domains are fixed in a ring shape having the groove boundary 6 as the inner diameter as shown in FIG. 7(b).

When the stripe domains are maintained in this way, the profile in the normal direction of the domain wall surface of the potential well in the outer domain wall (domain wall existing away from the boundary 6) portion 13 of the ring-shaped domain is mainly determined by the demagnetizing field effect determined by the stripe domain width. It is determined by , and is not affected by minute irregularities in the finish at the boundary of the grooved part.

When an externally applied pulsed bias magnetic field is applied to such a domain wall, the domain wall is driven uniformly over the entire domain wall 13.

Therefore, by applying a pulse bias magnetic field applied in a direction parallel to the static bias magnetic field 11 for maintaining the domain, the information stored in the domain wall in the form of the presence or absence of VBL pairs is applied to the VBL pair.
When moving using the gyro force generated in the L pair, the amount of movement can be easily controlled by the shape of the pulse bias magnetic field. In the figure, 18 and 19 are the directions of magnetization inside and outside the domain, respectively.

Figure 8 shows the process of forming a striped domain into a ring shape, and the process of converting information stored in VBL pairs within the striped domain domain wall, which is a necessary condition for this device, into bubbles when reading out, or converting the information A specific example of the groove pattern shape including the gate portion 32 for performing the function of storing data expressed in the form of the presence or absence of bubbles on the major line 31 in the form of the presence or absence of VBL pairs within the stripe domain domain wall during writing will be explained in detail. Shows the operating process. Grooving section 2
A bubble generator consisting of a conductive pattern 26 is placed on the tip 25 of the 3. A bias magnetic field 11 is applied to the entire effective chip area in advance.
By applying a magnetic field in the same direction as 11, the entire body is tilted in the direction 11 (.And, with an appropriate bias magnetic field Hz applied, a pulse current 27 of the shape shown in the figure is applied to this bubble generator.
When given, a bubble is generated in 25, and the bubble is in groove 2.
It becomes a striped domain extending along 3.23',
U whose tips are each inserted into the introduction guide 28.28”
It becomes a letter shape. For such a stripe domain, a pulse current 30 is applied to the conductor pattern 29 in the direction of the arrow to generate a portion of the stripe domain extending into 28 and 28' in the region between the two conductor patterns. and the other parts. The joined striped domains try to minimize the sum of the Zeeman energy due to the bias magnetic field Hz and the surface energy of the domain wall. Finally, Figure 7 (
This results in a ring-shaped striped domain with the groove boundary 6 as the inner edge as shown in b). Another method is to move the grooved portion boundary layer to the outside of the film thickness step portion, which is a striped domain domain wall (Japanese Patent Application No. 60°079658). The reason for this is that when a stripe domain is set to include the trench and the outside of its boundary, the film thickness step at the trench boundary generates a demagnetizing field that prevents the domain wall outside the boundary from approaching the film thickness step. □On the other hand, when striped domains are confined within the grooved portion, the difference in film thickness generates a demagnetizing field that strongly suppresses the striped domains from moving outside the grooved boundary. Therefore, in order to generate a demagnetizing field that prevents the domain wall from approaching the groove boundary step, the stripe domain is initially set so that the stripe domain domain wall is outside the groove boundary layer thickness step. There is a need to.

FIG. 9 shows a method of arranging striped domains in the minor loop portion according to the present invention. Reference numeral 14 denotes a grooved region whose width W is set close to the stripe domain natural width WO (stripe domain width when the external bias magnetic field 11 is zero) determined by the material properties of the stripe domain holding layer. A bubble generator 33 made of a conductive pattern is built into this grooved portion. The bubbles generated by this bubble generator are designed to include not only the inside of the trench but also the surrounding area. In reality, the relative ratio between the width W of the grooved portion and the conductor spacing wG of the bubble generator, and the distance d between the bottom end of the generator and the tip of the grooved portion are important parameters. d is wO/2
It is necessary to keep it above. As described above, a pulse current Is is applied to the striped domain extension conductive pattern 34 arranged to surround the grooved portion of the generated bubble so that the domain wall around the striped domain is placed outside the grooved portion. Once the striped domains are arranged in this manner, the trench boundary step 15 produces a demagnetizing field effect that prevents the striped domain domain wall from approaching the boundary step. As a result, the striped domain domain wall is stably held at a position away from the trench boundary step, and a structure is achieved in which the domain wall does not directly contact the trench boundary step. The situation is shown in FIG. The domain wall 17 of the striped domain 16 is stabilized outside the boundary of the grooved portion 14. Once such a state is obtained, a repulsive interaction occurs between the striped domain domain wall and the trench boundary, and the domain wall is prevented from coming into direct contact with the trench boundary. 18 is the direction of magnetization within the stripe domain.

FIG. 11 three-dimensionally shows the relative relationship between the striped domain domain wall 17 and the grooved portion 14 in the striped domain retention layer.

(Problems to be solved by the invention) These methods are difficult to operate in order to stably arrange a large number of magnetic domains, and it is quite difficult to control the external application conditions, which is a practical problem. . An object of the present invention is to provide an ultra-high-density solid-state magnetic memory element that eliminates the drawbacks of the conventional method and simplifies external application conditions for stably arranging striped domains, which are minor loops. It is in.

(Means for solving the interpolation point) The present invention is based on two adjacent VBLs created in the Bloch domain wall at the stripe domain boundary existing in a ferromagnetic film whose easy magnetization direction is perpendicular to the film surface. In a magnetic memory element using a VBL pair as a storage carrier, (1) a part of the plateau is selectively left on the surface of the stripe domain holding layer over a region where the stripe domain is desired to be stabilized, and a ring-shaped ring is formed around the plateau. In the configuration that stabilizes the domain, and (2) in the method of carving out the retention layer only in that part (creating a hollowed out part and stabilizing the domain domain wall around the hollowed out part, part of the adjacent plateau Alternatively, a fine line pattern is arranged on the striped domain holding layer in the middle region of the groove, parallel to the longitudinal direction of the plateau or groove, with the direction perpendicular to the film surface being the easy magnetization direction, and a bubble generator and local magnetic field applied at both ends. A means is provided to facilitate the formation of a required domain.The configuration will be described in detail below.

The relationship between the thin line pattern and the domain immediately below it is shown in FIGS. 5 and 6. 1 is a domain holding layer, 2 is a substrate, 5 is a thin line pattern formed of a material with perpendicular magnetization, 1
8 is magnetization outside the domain, and 19 is magnetization inside the domain. HD is a magnetic field generated from a thin wire pattern. FIG. 1 is a diagram showing an example of the structure of the main part of the minor loop part of the striped domain holding layer in the present invention. Figure 1(a)
is the main part of the stripe domain holding layer when the first invention of the present invention is used.

FIG. 1(b) is a cross section of the chip taken along the dashed line in FIG. 1(a). A plateau 4 is formed on the surface of the striped domain holding layer 1 on the substrate 2 in a region where domains are desired to be held.

This can be obtained, for example, by etching the surface of the striped domain holding layer, leaving a plateau part and etching other areas. A thin line pattern 5 formed of a magnetic film having perpendicular magnetization is arranged in a region between adjacent plateaus.

A bubble generator and local in-plane magnetic field generating means 7 are disposed at one end of the fine line pattern, and a local magnetic field generating means 8 is disposed at the other end. Further, if necessary, a bubble generating conductive pattern 9 is arranged in the middle between both ends.

(Function) The first invention will be explained with reference to FIG. The magnetization of the fine line pattern 5 is saturated in the opposite direction to the magnetization in the domain stabilized around the pattern 4. Next, an external magnetic field is applied so as to saturate the magnetization in the striped domain holding layer in the same direction as the magnetization in the domain to be stabilized around 4. At this time, the thin wire pattern must have a coercive force sufficient to prevent its magnetization from being reversed. Thereafter, a bubble generator 7 generates bubbles at the ends of each thin line pattern. Thereafter, the absolute value of the external magnetic field is decreased, and each bubble is extended to the other end along the thin line pattern 5, forming a stripe domain. Thereafter, antiparallel currents are applied to the conductor wires 7.8 so that a magnetic field in the same direction as the magnetization in the stripe domain is generated above 7 and below 8 in FIG. 1(a). These magnetic fields cause each stripe domain to join together at both ends of the thin line pattern,
Conversely, a single domain is formed with each plateau at its center. Furthermore, when the absolute value of the externally applied magnetic field is reduced, the single domain shrinks and the domains around it expand. When the externally applied magnetic field becomes near zero, the bubble generator 9 is activated to generate bubbles in each platelet portion 4. This bubble then spreads from one end of the plateau to the other. When the direction of the externally applied magnetic field is reversed and the absolute value is increased, the domain domain wall inside the plateau comes into close contact with the plateau outer periphery 6, and a ring-shaped domain 12 is stabilized outside of it as shown in FIG. . FIG. 1(b) is a cross section taken along the dashed-dotted line in FIG. 1(a).

In the second invention, the main part of the structure is shown in FIGS. 3(a) and 3(b).The center part 13 of the region where the domain is to be placed is hollowed out, and a closed domain domain wall is arranged to surround it. Its method of operation is almost the same as the first structure. The difference is that there is no need to generate bubbles in the hollowed out area, so the bubble generator 9 is not required. Another idea is to groove the surface of the striped domain retention layer instead of using a thin line pattern of a material with perpendicular magnetization. However, experiments have shown that the trenching method has a strong ability to trap domains at the edges of the trench, making it difficult for the domains to separate from it. Often only the side walls moved over the edge, expanding the domain width. For this state, reduce the external magnetic field,
When the direction is further reversed, the edge 1 of the hollowed out part 14
From 5, inverted domains (domains with magnetization in the same direction as the domain initially formed in the surface trench) may momentarily expand into an irregular shape, and the closed domain wall surrounding 4 may not necessarily be expanded. There was a drawback that the domains with which they were formed were not formed stably. A technology similar to this was introduced in 1986.
It was reported at the Annual National Conference of the Institute of Electronics and Communication Engineers (1986, March 26, lecture number: 229). Where,
This method limits the grooved portions to only the areas near 7 and 8 in Figure 3, but since various adjustments are made to create the bit positions of the VBL pair along the longitudinal direction of the striped domain, the above-mentioned If there is no guide groove, the domain will not extend straight through the area between the cutouts from the 7 side to the 8 side, and the bit positioning will get caught in the pattern on the way, and the domain head will eventually reach 15. There was a chance we would collide. Once they collide, there is nothing that can be done about it anymore, making it difficult to stably form a domain with a closed domain wall surrounding 14.

The present invention eliminates these drawbacks. Regarding the first point of the above-mentioned trench digging method, by using a nonmagnetic layer as a spacer between the thin wire pattern formed of a material with perpendicular magnetization and the striped domain holding layer, the barrier for domain wall trapping at the edge of the thin wire can be made steeper. You can change the size at will. The second problem does not arise with the present invention. As described above, by using this method, it is possible to form a ring-shaped domain at a predetermined position with good controllability, or a domain having a closed domain wall surrounding a hollowed part (FIG. 4).

(Example 1) (VSmLuC
a) 4u of 3(FeGe) 5012 composition garnet film
LPE was grown to a thickness of m. The height of the plateau 4 in the structure shown in FIGS. 1 and 2 is 0.4 um, and the depth of the hollowed out part 13 is 4 um.
um, and the width is both 6 um. On top of that, a 0.2um thick amorphous GdTb film, which is a node perpendicular magnetization film, was applied by sputtering via a 0.2um 5i02 spacer, and the surface was covered with 5i02 to prevent oxidation. . Thereafter, a GdTb film was formed in the form of striped domains with a width of 0.2 um. A conductive pattern with a width of 2 um is placed at both ends of this structure, and by a series of operations starting from the bubble generation described above, a ring-shaped domain surrounding the plateau 4 is formed in the structure shown in FIG. 1, and a hollowed out portion is surrounded in the structure shown in FIG. 2. A domain with a closed domain wall could be formed.

(Example 2) In Example 1, the same effect as in Example 1 could be obtained when 5i02 was arranged as a lum spacer between the amorphous GdTb film and the garnet film. As can be seen, the striped domain domain wall trapping force of the pattern edge increased compared to Example 1, and when the external magnetic field was decreased, non-uniformity was noticeable from place to place in the distance from the external magnetic field.

(Effects of the Invention) According to the present invention, the stability and reliability of the domain arrangement, which has conventionally been interlayered, can be significantly improved.

[Brief explanation of the drawing]

Figure 1 is a diagram of the main structure for holding ring-shaped domains, Figure 2 is a diagram showing the ring-shaped domains formed by the method shown in Figure 1, and Figure 3 is a diagram of the main structure for holding hollow striped domains. Structure diagram, Figure 4 is a diagram of striped domains formed by the method shown in Figure 3, Figure 5 is a diagram showing the mechanism in which the thin line pattern with perpendicular magnetization used in the present invention traps domains, and Figure 6 is a diagram of vertical magnetization. Figure 7 shows an example of the conventional method for holding ring-shaped domains. Figure 8 shows the magnetization of domains stabilized under a thin line pattern with magnetization. A diagram showing an example of a conductor pattern for forming a domain, FIG. 9 a diagram showing an example of a conventional hollow domain stabilization method, FIG. 10 a diagram showing a hollow stripe domain viewed from above, and FIG. FIG. 3 is a three-dimensional view of a domain. In the figure: 1. domain retention layer; 2. substrate, 3. 4. surface etched portion of domain holding layer; Part of Plato, 5. 6. A thin line pattern formed of a material with perpendicular magnetization. Plato Part Edge, 7
, Bubble generator and conductor pattern for generating local in-plane magnetic field, 86 Conductor pattern for generating local in-plane magnetic field, 9. Conductive pattern for bubble generation, 10. Spacer, 11. Bias magnetic field, 12. Ring-shaped domain, 13. Ring-shaped domain domain wall, 14. Domain holding layer hollowed out part, 15 burr cut out part edge, 16. Hollow domain, 17. Domain outer domain wall, 18. Magnetization outside the domain under the fine line pattern with perpendicular magnetization, 19. Magnetization within the domain, 20. Domains attracted to the edges of fine line patterns with perpendicular magnetization, 21. Domain domain wall, 22. Sidewall of fine line pattern with perpendicular magnetization, 23.23', grooved part around plateau,
24. Outer edge of grooved portion for holding ring-shaped domain; 25. Bubble generator, 26. Conductive pattern for bubble generator, 27. Pulse current for bubble generation, 28.28”,
Stripping groove at the tip of the stripe domain, 29. Conductor pattern for striped domain sewing, 30. Pulse current for stripe domain stitching, 31.31', major line, 32-32', gate section, 33. Bubble generator, 34, conductor pattern for bubble expansion. Figure 1 Figure 2 Figure 3 Figure 4 Figure 5 Figure 6 Figure 7 (a) Figure 8 Figure 9 Figure 10

Claims (2)

[Claims] (1) The boundary of a stripe domain existing in a ferromagnetic (including ferrimagnetic) film that has information reading means, information writing means, and information storage means and whose easy magnetization direction is perpendicular to the film surface. In a magnetic memory element having a means for retaining and transferring a pair of two adjacent vertical Bloch lines formed in a Bloch domain wall within the Bloch domain wall, the ferromagnetic film surface is A part is left selectively and other areas are shaved, and a thin wire made of a material with perpendicular magnetization is placed parallel to the uncut part in the part corresponding to the shaved area, and a bubble is created at a position including the tip of the wire. What is claimed is: 1. A magnetic memory element comprising means for generating and generating a local magnetic field, and means for generating a local magnetic field provided at the other end thereof. (2) The boundary of a stripe domain existing in a ferromagnetic (including ferrimagnetic) film that has information reading means, information writing means, and information storage means and whose easy magnetization direction is perpendicular to the film surface. In a magnetic memory element having means for retaining and transferring a pair of two adjacent perpendicular Bloch lines formed in a Bloch domain wall within the Bloch domain wall, the stripe domain in the ferromagnetic film is placed in a region where the stripe domain is desired to be arranged. Hollowed out parts are provided in the striped domain holding layer, and thin wires made of a material having perpendicular magnetization are arranged parallel to these hollowed out parts in the region between the hollowed out parts and adjacent hollowed out parts. A magnetic memory element characterized in that a means for generating a bubble and a local magnetic field is provided at a position including the tip, and a means for generating a local magnetic field is provided at the other end of the thin wire.