JP3152166B2 - Anisotropic conductive sheet and method for producing the same - Google Patents

Description

DETAILED DESCRIPTION OF THE INVENTION

[0001]

BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a jig for inspecting an IC and a printed circuit board, a connector for an IC socket and a printed circuit board for mounting, or a connector for an IC card in a peripheral portion thereof. The present invention relates to a method for producing an anisotropic conductive sheet used for achieving electrical connection.

[0002] The anisotropic conductive sheet of the present invention has good conductivity and pressure conductivity in the thickness direction. The technical fields which can be suitably used for each characteristic will be described in more detail below. It seems.

(Especially in fields utilizing good conductivity) 1) Sockets for electrical connection of integrated circuits such as ICs, LSIs and MCMs, especially sockets for BGA 2) Connectors for LCD panels 3) Connectors for mounting printed circuit boards 4) PC card terminals and connectors 5) Anisotropic conductive adhesive sheet, anisotropic conductive adhesive tape,
Anisotropic conductive adhesive sheet, anisotropic conductive adhesive tape 6) Sheet-shaped probe for IC inspection and printed circuit board inspection (particularly in the field that uses pressurized conductivity) 7) Pressure-sensitive switch, limit switch, keyboard 8 ) Pressure sensitive volume, keyboard, coordinate input device, joystick 9) Tactile sensor 10) Pressure distribution measuring sensor

[0004]

2. Description of the Related Art Conventionally, anisotropic conductive sheets used in the above technical fields have conductivity only in the thickness direction, or have conductivity only in the thickness direction when pressed. It has a large number of pressurized conductive portions exhibiting properties, and various structures are disclosed in, for example, JP-B-56-489.
No. 51, JP-A-51-93393, JP-A-5-93393
JP-A-3-147772, JP-A-54-146873, JP-A-7-105741, U.S. Pat.
For example, it is known from Japanese Patent No. 292,261.

Hereinafter, an outline of a conventional anisotropic conductive sheet and a method for manufacturing the same will be described.

When the anisotropic conductive sheet is viewed from the surface, FIG.
As shown in FIG. 2, for example, a large number of conductive portions 2 are formed in an island shape or a band shape on a sheet 1 made of silicone rubber and having a thickness of about 1 mm. FIG. 3 shows an enlarged schematic cross-sectional view of the sheet. In FIG.
The conductive portion 2 is formed, for example, by collecting a plurality of particle rows in which nickel particles are continuously connected in the thickness direction of the sheet. This sheet has conductivity in the thickness direction, but has no conductivity in the plane direction, and is therefore called an anisotropic conductive sheet.

A method for manufacturing such an anisotropic conductive sheet will be described with reference to FIG. A mold 5 (composed of a pair of upper and lower) made of a ferromagnetic material is placed between the magnetic poles 3 and 4 of the pair of electromagnets. In a space (chamber; molding space) surrounded by the mold 5 and the molding spacer 6, a mixture of silicone particles of liquid silicone rubber (molding material 7) is put, and a magnetic field is applied. Are aligned in the direction of the magnetic field between the magnetic pole portions M. The space (chamber) is a flat plate having a thickness of about 1 mm, and a sheet is formed in this space. When the liquid silicone rubber is heated and cured in this state, an anisotropic conductive sheet is completed. In FIG. 4, the mold 5 includes a mold substrate 8, a magnetic pole portion M, and a non-magnetic portion N that fills the periphery of the magnetic pole portion M. The non-magnetic part N is made of, for example, a heat-resistant resin such as an epoxy resin or a phenol resin, and the surfaces of the magnetic pole part M and the non-magnetic part N usually have the same horizontal plane. When there is a non-magnetic pole portion N and a magnetic pole portion M, when a magnetic field is applied, the conductive ferromagnetic particles (eg, nickel particles) concentrate on the magnetic pole portion M. It is formed in an island shape or a band shape according to the shape of.

Even when a non-magnetic pole portion N is not used and the entire surface of the flat surface is a magnetic pole portion M, the conductive ferromagnetic particles are also aligned in the thickness direction, and are randomly and uniformly distributed in the plane direction. Since it is thinly distributed, an anisotropic conductive sheet having conductivity only in the thickness direction can be obtained. In this case, the sheet has conductivity over the entire sheet surface, but has high conduction resistance.

On the other hand, in the anisotropic conductive sheet shown in FIGS. 1 and 2, the conductive portion 2 has an island shape or a band shape, and conductive ferromagnetic particles are localized in this portion. Due to the high density, the conduction resistance is small.

The present invention relates to an anisotropic conductive sheet of the latter type (FIGS. 1 and 2) in which the conduction resistance is further reduced. In addition, the anisotropic conductive sheet includes a sheet utilizing pressure conductivity due to rubber elasticity of the sheet material and a sheet utilizing simply good conductivity, but the basic configuration is the same,
The present invention is not limited to one.

The technique for producing the anisotropic conductive sheet described above is described in Japanese Patent Application Laid-Open No. 54-146873. Patents relating to anisotropic conductive sheets have been published since then, but the basics of the manufacturing technology are disclosed in
No. 4,687,387.

In the above example, the conductive portion 2 and the insulating portion of the anisotropic conductive sheet are formed on the same horizontal plane. However, the conductive portion 2 and the insulating portion described in Japanese Patent Application Laid-Open No. 7-105741, The conductive portion of the one-sided conductive sheet may have a slightly convex shape protruding from the surface of the insulating portion. Further, the shape may be concave.

By the way, the conduction resistance of the conventional anisotropic conductive sheet is much higher than expected from the resistance value of the aggregate composed of only the conductive particles, and it is necessary to further reduce the conduction resistance. It is the present situation that is desired.

FIG. 5, FIG. 6, and FIG. 7 are schematic diagrams showing the results of observing the conductive portion of an anisotropic conductive sheet manufactured by the prior art, typically shown in JP-A-54-146873, with a microscope. Shown in FIG. 5 (a) which is an enlarged schematic view of the conductive portion as viewed from the sheet surface, and FIG. 5 (b) which is an enlarged schematic diagram of a cross section in the sheet thickness direction of the central portion of the conductive portion (also showing the magnetic pole portion).
As shown in FIG. 2, the conductive ferromagnetic particles 11 are arranged in the thickness direction of the sheet to form a conductive ferromagnetic particle row 12.
The conductivity in the sheet thickness direction is realized by these particle rows 12. However, these particle rows 12 do not exist uniformly at desired positions (portions sandwiched between the opposing magnetic pole portions M and M), that is, in the conductive portion 2, but in the vertical cross-sectional structure, as shown in FIG. As shown in FIG. 5 (a), the magnetic poles M are gathered in the shape of a drum, and the center of the magnetic pole portion M is sparse in the vicinity of the surface, that is, on the sheet surface, as shown in FIG. Further, a conventional anisotropic conductive sheet is shown in FIG.
As shown in (a), there is a configuration in which the particle rows 11 partially form a small group in the conductive portion 2 and a plurality of small groups are unevenly gathered to form the conductive portion 2. It is considered that such an aggregated state of the conductive ferromagnetic particles 11 is a cause that the conduction resistance of the conductive portion 2 cannot be further reduced in the conventional sheet. The conduction resistance of the conventional anisotropic conductive sheet 10 is insufficient for using the sheet 10 for mounting an electronic circuit such as a socket or a connector. Further, in the conventional anisotropic conductive sheet 10, as described above, the conductive portion 2 to which conductivity is to be imparted is used.
In this case, the conductive ferromagnetic particles 11 are not densely and uniformly aggregated, so to speak, are in a state of spreading around the peripheral portion thereof, and the distance between the adjacent conductive portions is short, and a short circuit may occur. Therefore, the gap between the adjacent conductive portions 2 and 2 (hereinafter, referred to as a magnetic pole pitch) cannot be further reduced, and the density of the conductive portions 2 in a predetermined area of the sheet 10 cannot be further increased. . Further, for the same reason, it is impossible to form a sheet having a thickness exceeding the magnetic pole pitch.

[0015]

SUMMARY OF THE INVENTION The present invention has been made in view of the above-mentioned circumstances, and a first object of the present invention is to provide an electronic circuit such as a socket or a connector which can be used for mounting. An object of the present invention is to provide an anisotropic conductive sheet having a small conduction resistance. A second object of the present invention is to provide an anisotropic conductive sheet in which conductive ferromagnetic particles are densely localized up to the center of the conductive part. A third problem of the present invention is that the distance between the centers (magnetic pole pitch) of adjacent conductive portions 2 is extremely small, the conductive portions are electrically insulated from each other, and the conductive portions are electrically conductive in portions other than the conductive portions. An object of the present invention is to provide an anisotropic conductive sheet substantially free of particles. A fourth object of the present invention is to provide a pressurized conductive anisotropic conductive sheet that can achieve good electrical connection from a small compressive displacement. Still another object of the present invention is to provide an anisotropic conductive sheet having a large thickness.

A further object of the present invention is to provide a method for producing the above-mentioned anisotropic conductive sheet.

[0017]

Means for Solving the Problems The inventor of the present invention has conducted intensive studies in order to solve the above problems, and has obtained the following findings.

The reason why the state of aggregation of the conductive ferromagnetic particles in the conductive portion of the conventional anisotropic conductive sheet is not uniform is that the magnetic field intensity distribution in the mold for forming the anisotropic conductive sheet is as shown in FIG. This is because, as shown in FIG. Furthermore, as a conventional anisotropic conductive sheet and a mold for manufacturing the same, FIGS.
The structure shown in FIGS. 7A and 7B was also considered. In the anisotropic conductive sheet of FIG. 6, the distribution state of the conductive ferromagnetic particles 11 in the conductive portion 2 is not localized only between the magnetic pole portions M, and the magnetic conductive particles 11 'also remain around. In the anisotropic conductive sheet of FIG. 7, when the sheet manufactured in FIG. 7B is viewed from above, the magnetic particles are non-uniformly distributed with gaps as shown in FIG. 7A. . When the sheet is viewed from below, a sparse portion is formed at the center near one surface of the sheet.

The force acting on the ferromagnetic particles in the magnetic field is proportional to the product of the magnetic field strength and the magnetic field gradient at the position where the ferromagnetic particles are present, and the magnetic field gradient changes its sign at the maximum position of the magnetic field distribution. Therefore, the ferromagnetic particles existing around the local maximum of the magnetic field distribution receive a force toward the position of the local maximum. That is, when there is a local maximum in the magnetic field intensity distribution, the ferromagnetic particles are localized at the position of the local maximum.

The drum-shaped aggregate shape of the ferromagnetic particles 11 in the conductive portion 2 shown in FIG. 5 will be described as follows. Since the magnetic field distribution on the surface near the magnetic pole surface has a maximum at the position of the magnetic pole periphery, the ferromagnetic particles 11 are localized at the position of the magnetic pole periphery. Then, when observing the conductive part 2 of the anisotropic conductive sheet 10 from the surface, a sparse part of the ferromagnetic particles 11 exists in the central part. On the other hand, on the horizontal plane at the central position between the opposed magnetic poles, the local maximum at the magnetic pole peripheral position disappears and the local maximum appears at the magnetic pole central position (see FIG. 12), so the ferromagnetic particles 11 are localized around the magnetic pole central position. Since the shape of the magnetic field distribution on the intermediate surface between the two changes continuously between the two magnetic field distribution shapes, the localization radius of the ferromagnetic particles also changes continuously, and the ferromagnetic particle distribution forming a drum shape Is configured.

The sheet shown in FIG. 6 shows a case where the diameter of the magnetic pole portion M is reduced. In the conductive portion 2, the conductive ferromagnetic particles 11 are densely provided up to the center portion, but are not provided between adjacent conductive portions. The non-localized conductive ferromagnetic particles 11 'remain. Such an aggregated shape of the particles 11 is described as follows. As in the case of FIG. 5, the magnetic field distribution on the surface close to the magnetic pole surface has a local maximum at the position of the magnetic pole periphery. However, as the magnetic pole diameter is reduced, the local maximum position of the magnetic pole periphery approaches, and Since the magnetic field intensity increases and approaches a flat surface, the force for localizing the conductive ferromagnetic particles existing between the opposing magnetic pole portions MM to the magnetic pole peripheral portion decreases, and the particles are likely to be localized on the magnetic pole peripheral edge from the outside. It is described that the conductive ferromagnetic particles 11 are pushed to the center position of the magnetic pole by the pressure of. Further, since the magnetic pole diameter is reduced, a region where the magnetic field strength and the magnetic field gradient are small between adjacent magnetic poles increases, and the force acting on the conductive ferromagnetic particles 11 existing in the region is weak, and particles that cannot be localized remain.

FIG. 7 shows an anisotropic conductive sheet in which the conductive portion 2 of the anisotropic conductive sheet 10 is formed in a convex shape, as described in JP-A-7-105741.
A molding space is formed by applying an insulating sheet P having an opening smaller than the magnetic pole portion M. In the sheet mold, the diameter of the magnetic pole portion M is larger than the convex diameter, and there is no maximum magnetic field intensity distribution at the position of the convex portion, and the magnetic field intensity distribution at a position inside the periphery of the magnetic pole is constant. , The conductive ferromagnetic particles 11 are arranged in a chain in the vertical direction to form a line. However, since the force for assembling the lines is weak, small groups are unevenly distributed. The distribution form of the conductive ferromagnetic particles 11 is similar to the distribution form of the conductive particles of the anisotropic conductive sheet formed by the mold of the magnetic pole part having a flat flat surface without the nonmagnetic part N. I have.

As described above, in the conventional anisotropic conductive sheet, the reason why the conductive ferromagnetic particles are not uniformly and densely gathered up to the center of the conductive portion is that in the conventional mold for forming the anisotropic conductive sheet. The Z-axis component of the magnetic field strength distribution is shown in FIG.
As shown in (c), the fact that the maximum value is at the periphery of the small magnetic pole, and that the main factor governing such a magnetic field intensity distribution shape is the shape of the small magnetic pole of the mold, I understand.

In order to clarify the relationship between this factor and the shape of the conductive portion, the vertical cross section of the magnetic pole portion (cross section perpendicular to the magnetic pole surface) is shown in FIG. 8 (rectangular; conventional mold) and FIG. A pair of models having four types of shapes, that is, a rectangular section with rounded corners at the tip, FIG. 10 (shape of the tip is semicircular, but the tip is cut off horizontally), and FIG. 11 (tip is semicircular). Molds (upper and lower molds) are made, and this model mold is placed in a vertical external magnetic field generated by a magnet.
The axial component (the component in the vertical direction) was measured. The dimensions of the model mold used for the measurement depend on the shape of the magnetic pole width, magnetic pole height, magnetic pole pitch, and the distance between the upper magnetic pole surface and the lower magnetic pole surface (hereinafter simply referred to as the opposing magnetic pole distance). And 10 mm, 10 mm, 20 mm, and 10 mm, respectively. The measurement position of the magnetic field intensity distribution is 5%, 15%, 25%, 45% of the distance between the opposing magnetic poles and on four surfaces separated from the lower magnetic pole surface, and scanning measurement is performed using a Hall element as a magnetic field sensor. did. FIG. 12, FIG.
This is shown in FIG. 13, FIG. 14, and FIG. Although the measurement results are not shown here, the same measurement was performed on a magnetic pole having a steeple cross section, a trapezoidal cross section, and a trapezoidal cross section having a circular tip.

From the series of measurement results, the following became clear. (1) In a magnetic pole having a rectangular cross section having the same magnetic pole shape as that of the conventional mold shown in FIG. 8, as shown in FIG. The magnetic field strength distribution of a) is sharply maximum at the periphery of the magnetic pole. On 15% of the surface (b), the local maximum at the position changes to a gentle maximum, and 25% (c) and 45%
On the plane (d), the local maximum at the position disappears and a new local maximum appears at the center of the magnetic pole. From these findings, various localized forms (FIGS. 5, 6, and 7) of the conductive ferromagnetic particles in the conductive portion of the anisotropic conductive sheet formed by the conventional mold are described. (2) As shown in FIG. 9, in the magnetic pole having a rectangular cross section with a rounded tip at the tip (horizontal linear portion 60%, rounded portion 20% on both sides), as shown in FIG. The maximum of the magnetic field strength distribution on the surface (a) 5% away from the position of the magnetic pole periphery in the case of a magnetic pole having a rectangular cross section is
As the tip angle is rounded, that is, the magnetic pole surface moves to a position where it changes from a flat surface to a curved surface, and the magnetic field gradient at the magnetic pole periphery becomes gentle. In addition, the height of the peak decreases, and the magnetic field intensity at the center increases. On the 15% surface (b), the maximum disappears and the surface is flattened. On the 25% and 45% surfaces, a new maximum appears at the center of the magnetic pole. The change in the shape of the magnetic field distribution by rounding the corners of such a rectangular magnetic pole is as follows.
When the rounded portion is further enlarged, the magnetic pole distribution of the extreme magnetic pole shape, that is, a magnetic pole having a rounded portion of 50% on both sides and no horizontal linear portion, that is, a magnetic pole having a semicircular cross section at the tip (FIG. 15). It changes continuously. (3) A part of the tip of the magnetic pole having a semicircular tip portion shown in FIG.
As shown in FIG. 14, a magnetic pole having a linear shape (30% of the maximum horizontal width) parallel to the magnetic pole surface has a magnetic field intensity distribution of 2% on the surface (a) separated from the magnetic pole surface by 5% of the distance between the opposing magnetic poles. Only two small maxima appear, the maxima disappear on 10% of the surface (b), and on the 15% surface (c), the shape is similar to the magnetic field distribution of the semicircular magnetic pole at the tip (FIG. 15). Has become.
(4) In the magnetic pole whose cross-sectional shape shown in FIG. 11 has a semicircular tip, the magnetic field strength distribution is as shown in FIG. The maximum position of the magnetic field intensity distribution is on the axis in the Z direction at the center position of the magnetic pole on any horizontal plane between the opposing magnetic poles.

The present invention has been made based on the above findings, and an anisotropic conductive sheet obtained by the method of the present invention has a sheet shape comprising an insulating portion and a plurality of conductive portions surrounded by the insulating portion. A member, wherein the conductive portion is made of conductive ferromagnetic particles arranged in the thickness direction of the sheet, and the aggregate density of the conductive ferromagnetic particles in the aggregate as viewed from the sheet surface side is uniform and dense. It is characterized by being. Here, that the aggregate density is uniform and dense means that the particles are uniformly and densely distributed as shown in FIGS. 16 and 21 when the aggregate portion is observed in an enlarged manner. That is, the dispersed state of the particles in the aggregate portion is uniform and no missing portion is observed (dense state). FIG. 5 described above.
(A), FIG. 6 (a), and FIG. 7 (a) are non-uniform examples. The minimum width of the aggregate is the diameter of the circle when the conductive part is circular (island-shaped) in the conductive part 2 of FIG.
When the conductive portion 2 is rectangular (line or band shape), it means the length of the short side of the rectangle, in other words, the thickness of the line or band.

[0027]

[0028]

[0029]

[0030]

[0031]

[0032]

[0033]

[0034]

The method of manufacturing an anisotropic conductive sheet according to claim 1 of the present invention is characterized in that a plurality of small magnetic poles made of a ferromagnetic material are provided between a pair of opposed mold magnetic poles so that a magnetic field is localized. A molding space is provided, a molding material in which conductive ferromagnetic particles are dispersed in a curable material that can flow under molding conditions is disposed in the molding space, and a conductive material in the molding material is formed by the pair of mold magnetic poles. A method in which the anisotropic conductive sheet is manufactured by localizing the conductive ferromagnetic particles and curing the molding material, wherein the distance from the magnetic pole surface of the mold pole to the distance of the opposing magnetic pole during molding is 0. % On any plane parallel to the pole face of the mold pole in the molding space within the range of not less than 25% and the component (Z-axis component) perpendicular to the pole face of the magnetic field strength distribution is Note that the maximum is shown on the axis almost at the center of the small magnetic pole. To. That is, when the shape of the small magnetic pole is as shown in FIG. 11, as shown in FIG. 15, the magnetic field intensity distribution has a maximum on the central axis of the small magnetic pole on all the planes parallel to the magnetic pole faces between the opposing small magnetic poles. Show. The shape of the small magnetic pole is shown in FIG.
In the case of FIG. 10, as shown in FIGS. 13 and 14, the magnetic field intensity distribution shows a maximum on the central axis of the small magnetic pole on a plane separated from the magnetic pole surface by 20% or 10% or more of the distance between the opposing magnetic poles. Such a space is referred to as a molding space, and a molding material is placed in the molding space and a magnetic field is applied to cure the molding material. In this claim 1,
It is preferable that the localization of the conductive ferromagnetic particles is uniform. In this case, “uniform localization” refers to the case where the conductive ferromagnetic particles are aggregated as described above. This means that the aggregate density of the particles is uniform. Also,
A method of manufacturing an anisotropic conductive sheet according to claim 2 is the manufacturing method according to claim 1, wherein the width of at least one vertical cross section of the small magnetic pole decreases toward the tip, and the base end of the width. The rate of decrease from to the tip is increasing,
The tip portion has a linear portion parallel to the pole face of 60% or less of the maximum value of the width of the cross section parallel to the pole face, and the small poles are arranged in a plane. The present invention is characterized in that a mold magnetic pole is used as the mold magnetic pole.

According to a third aspect of the present invention, there is provided the method of manufacturing an anisotropic conductive sheet according to the second aspect, wherein the linear portion parallel to the magnetic pole surface has the cross-sectional shape of the small magnetic pole. The width is not more than 50% of the maximum value of the width parallel to the pole face.

According to a fourth aspect of the present invention, there is provided the method of manufacturing an anisotropic conductive sheet according to the first aspect, wherein at least one of the vertical cross sections of the small magnetic poles has a width toward a tip. The width of the magnetic pole becomes narrower, the rate of decrease in the width from the base end to the tip end increases, and the tip end has a shape in which there is no linear portion parallel to the magnetic pole surface. It is characterized in that a mold magnetic pole arranged in a shape is used as the mold magnetic pole.

According to a fifth aspect of the present invention, there is provided the method of manufacturing an anisotropic conductive sheet according to any one of the first to fourth aspects, wherein the curable molding material is applied with a magnetic field during the manufacturing of the sheet. It is characterized by being an electrically insulating polymer material which sometimes has fluidity and then hardens.

The method of manufacturing an anisotropic conductive sheet according to claim 6 is the method of manufacturing an anisotropic conductive sheet according to claim 5, wherein the electrically insulating polymer material is silicone rubber,
Ethylene propylene rubber, urethane rubber, fluorine rubber, polyester rubber, styrene butadiene rubber, styrene butadiene block copolymer rubber, styrene isopropylene block copolymer rubber, soft epoxy resin, thermoplastic elastomer, thermoplastic soft It is selected from resins and is characterized by being liquid or fluid at the temperature during sheet production.

The method of manufacturing an anisotropic conductive sheet according to claim 7 is the method of manufacturing an anisotropic conductive sheet according to claim 5 or 6, wherein the electrically insulating polymer material has a crosslinked structure after molding. It is characterized by having.

The method for producing an anisotropically conductive sheet according to claim 8 is the method for producing anisotropically conductive sheet according to any one of claims 5 to 7, wherein the electrically insulating polymer material is solid after molding. It is characterized by having rubber elasticity.

According to a ninth aspect of the present invention, in the method for manufacturing an anisotropic conductive sheet according to any one of the first to eighth aspects, the conductive ferromagnetic particles have ferromagnetism as particles, In addition, at least the surface has conductivity.

According to a tenth aspect of the present invention, there is provided the method of manufacturing an anisotropic conductive sheet according to the ninth aspect, wherein the conductive ferromagnetic particles are single ferromagnetic metal particles,
It is one of coated particles made of an organic or inorganic material coated with a metal, and mixed particles thereof.

According to a eleventh aspect of the present invention, in the method for manufacturing an anisotropic conductive sheet according to the tenth aspect, the conductive ferromagnetic particles have a ferromagnetic property of nickel, iron, cobalt, or the like. Shown metal particles or particles of alloys containing them, whiskers of ferromagnetic metals such as iron, short-fibrous ferromagnetic metals, or these particles or short-fiber objects,
Metals selected from gold, silver, copper, tin, palladium, and rhodium coated by plating, etc., inorganic particles or polymer particles such as non-magnetic metal particles or glass beads, and conductive ferromagnetism such as iron, nickel, and cobalt It is characterized by being one of a metal plated or a mixed particle thereof.

[0045]

[0046]

[0047]

[0048]

[0049]

[0050]

[0051]

[0052]

[0053]

[0054]

That is, an anisotropic conductive sheet manufacturing apparatus suitable for use in the present invention is an opposed sheet having a plurality of small magnetic poles made of a ferromagnetic material between a pair of magnets so that a magnetic field is localized. A molding material in which a conductive ferromagnetic material is dispersed in a curable material that can be flowed under molding conditions, between the pair of mold magnetic poles. An apparatus for manufacturing an anisotropic conductive sheet in which a mold magnetic pole localizes the conductive ferromagnetic particles in the molding material and heats and cures the molding material by a heating means. The cross-sectional shape along at least one surface perpendicular to the surface of the mold magnetic pole, the width decreases toward the tip,
The decreasing rate of the width from the base end to the tip end is increasing, and the tip of the magnetic pole has a maximum width of 60% or less, preferably 50% or less of the maximum width of the cross section parallel to the pole face. It is characterized in that the shape has a straight line portion parallel to the plane. Further, another configuration of the apparatus for manufacturing an anisotropic conductive sheet suitable for use in the present invention has a cross-sectional shape along at least one surface perpendicular to the surface of the mold pole of each of the small magnetic poles, , The decreasing rate of the width from the base end to the tip is increasing, and the tip has no linear portion parallel to the pole face at the tip. .

As shown in FIG. 10, the former example of the manufacturing apparatus has a narrow cross-sectional shape with a convex curve toward the front end, and has a horizontal straight line portion at the top.
As shown in FIG. 4, when the distance from the magnetic pole surface is more than 10% of the distance between the opposed magnetic poles, the peak of the magnetic field strength distribution becomes one on the central axis of the small magnetic pole, and the invention according to claim 1 or 10 is carried out. Is preferred. The linear portion parallel to the pole face is the maximum value of the width parallel to the pole face in the cross-sectional shape (that is, the thickest portion of the small pole M, usually the bottom of the small pole, and the small pole M is For medium fat shapes,
It means the width of the thickest part. ) Of 60% or less, preferably 50% or less, more preferably 30% or less. Further, it is preferable that the connection point between the convex curve portion and the horizontal straight line portion of the cross-sectional shape is continuous (for example, an arc and a tangent). When the horizontal straight line portion is 30% of the maximum value of the width and the distance from the magnetic pole surface is 10% or more of the interval between the opposing magnetic poles, one peak of the magnetic field intensity distribution is obtained.
As shown in FIG. 0, an anisotropic conductive sheet having good localization of conductive ferromagnetic particles can be formed by interposing a spacer S of 10% or more of the distance between the opposing magnetic poles between the small magnetic pole 53a and the molding material. In the latter example of the manufacturing apparatus, the cross-sectional shape as shown in FIG. 11 is part of a circle or an ellipse (typically half).
It consists of

As can be seen from the description of the manufacturing apparatus, a mold magnetic pole suitable for use in the present invention is a mold magnetic pole for localizing ferromagnetic particles constituting the anisotropic conductive sheet, Preformed ferromagnetic small magnetic poles are arranged in a plane, and at least one vertical cross-sectional shape of the small magnetic poles decreases in width toward the distal end, and from the base end of the width. The rate of decrease toward the tip increases, and the tip has a maximum width of 6 parallel to the pole face of the cross-sectional shape.
0% or less, preferably 50% or less of a shape having a linear portion parallel to the magnetic pole surface, or a shape having no linear portion parallel to the magnetic pole surface at a tip portion thereof. I do.

The small magnetic pole preferably has a spherical top such as a hemisphere or a sphere . In this case, the small magnetic pole whose top is formed into a spherical shape is, for example, an iron ball (having a diameter of 1).
Or an iron pillar with one end in the long axis direction rounded (diameter less than 10 mm, length is one to several times the diameter)
It is. In addition to the above-mentioned spherical shape, a pillar shape with one end rounded, a pillar shape with two rounded ends (the pillar is selected from a square pillar, a cylinder, a polygonal pillar, etc.), an oval shape, and a circular or oval cross section There is a wire shape. Here, the wire-shaped thing is fixed with its long axis parallel to the mold surface. In the above description, the surface shape is generally a flat shape, but may be a part of a spherical surface. The arrangement of the small magnetic poles is arbitrarily designed according to the pattern of the aggregate of the conductive ferromagnetic particles in the anisotropic conductive sheet. When the assembly is designed to be linear, a wire-like ferromagnetic material is used as the small magnetic pole. The fixation of the small magnetic pole may be a non-magnetic material, for example, using a plate made of ceramics, aluminum, copper, brass, stainless steel, resin, or the like, or a silicon wafer, or the like. A hole for inserting a small magnetic pole is made in a plate of the above. The fixation of the small magnetic pole may be performed with a liquid curable resin, for example, a liquid epoxy resin. The fixing method is
Without being limited to these examples, known conventional means are used.

FIGS. 22 (a) and 22 (b) are schematic diagrams when the above-mentioned small spherical magnetic poles are used. In FIG. 22, reference numeral 40 denotes a magnetic pole plate (a mold substrate made of a ferromagnetic material), 41 denotes a spherical small magnetic pole, and 42 denotes a nonmagnetic material for arranging and fixing the small magnetic pole 41 to the magnetic pole plate 40. It is a board.

The fifth object of the present invention, that is, “providing an anisotropic conductive sheet having a large thickness” will be described. In the prior art, there was a limit in manufacturing an anisotropic conductive sheet having a thickness approximately equal to the pitch of the conductive portions. However, according to the method of the present invention, an anisotropic conductive sheet having a small conduction resistance can be manufactured even with a sheet thickness of about twice the conductive part pitch.

[0061]

BEST MODE FOR CARRYING OUT THE INVENTION Hereinafter, the present invention will be described in more detail with reference to embodiments of the present invention, but the present invention is not limited to these embodiments.

As shown in FIGS. 16 and 17, the anisotropic conductive sheet 30 of the present invention comprises an insulating portion 31 and a plurality of conductive portions 32 surrounded by the insulating portion 31 in the width direction. Is a sheet member having a normal thickness of 0.1 to 10 mm, preferably 0.3 to 2 mm. The conductive portion 32 is composed of an aggregate of conductive magnetic particle rows 33 arranged in the thickness direction of the sheet, and the minimum width of the aggregate is 10 μm.
mm.

As shown in FIG. 16, the distribution of the conductive ferromagnetic particle rows 33 in the aggregate viewed from the sheet surface side is such that the aggregate density is uniform and the inside has a low density portion (FIG. 5).
(A) and FIG. 7 (a) are characterized by the absence of non-uniform aggregation density.

In order to form such an anisotropic conductive sheet 30, as shown in FIG. 18, a forming material 52 in which conductive ferromagnetic particles 51 are mixed in a polymer material 50 is heated and formed. In addition, it is necessary that the magnetic field intensity distribution applied to the portion m to be formed with the conductive portion has a maximum P on a substantially central axis in the sheet thickness direction (Z-axis direction) of the portion m to be formed.

As a specific means for this, as shown in FIG. 19, a molding material 52 in which conductive ferromagnetic particles 51 are dispersed in a fluid material or a material 50 having a fluid state under molding conditions is arranged. The anisotropic conductive sheet molding die for localizing the anisotropic ferromagnetic particles 51 and curing the molding material to obtain an anisotropic conductive sheet is made of a plurality of ferromagnetic materials such that a magnetic field is localized. The small magnetic pole 53 is composed of a pair of opposed mold magnetic poles 55 and 56 provided on a mold substrate 54, and the small magnetic pole 53 extends along at least one surface perpendicular to the surfaces of the mold magnetic poles 55 and 56. It is characterized in that the cross-sectional shape is formed into a shape whose width becomes narrower toward the tip. In this case, the gap between the plurality of small magnetic poles 53 is, for example, a heat-resistant resin such as a polyimide resin, an epoxy resin, or a phenol resin, and a mixture of these resins with a non-magnetic heat-resistant filler, and It is made of a non-magnetic material 57 selected from non-magnetic metals such as copper, aluminum and stainless steel, or ceramics. further,
As shown in FIG. 20, the small magnetic pole may be a small magnetic pole 53a in which the tip of a member having a circular cross section is flattened. When such a small magnetic pole 53a is formed in a mold, a spacer S is inserted between the magnetic pole and the molding material, and the sheet 30 is manufactured,
As shown in FIGS. 20 and 21, in the conductive portion 32 of the formed sheet 30, the ferromagnetic particles 51 aggregate substantially uniformly. Therefore, a small magnetic pole 5 having a flattened tip is provided.
3a is also suitable for practical use. Further, the small magnetic pole may be provided only on one of the opposing molds, and the mold on one side may be a plane magnetic pole. In the case of this mold, it is desirable to insert a spacer between the plane magnetic pole and the molding material. When compared with a mold having both small magnetic poles, this mold is inferior in the localization performance of the conductive ferromagnetic particles, but does not require the positioning of the mold. The benefits are great.

(Material) A description will be given with reference to FIGS. The insulating portion 31 of the anisotropic conductive sheet 30 according to the present invention is made of an electrically insulating polymer material 50 having fluidity when a magnetic field is applied during the production of the sheet, and then hardening. That is,
At the time of manufacturing the sheet, the conductive ferromagnetic particles 51 have fluidity such that the conductive ferromagnetic particles 51 can be aggregated in the small magnetic poles, and then are cured to fix the conductive ferromagnetic particles 51.

As such a material, silicone rubber,
Examples include ethylene propylene rubber, urethane rubber, fluorine rubber, polyester rubber, styrene butadiene rubber, styrene butadiene block copolymer rubber, styrene isopropylene block copolymer rubber, and soft epoxy resin. These need to be liquid or fluid at the temperature at the time of sheet production. Preferably, it is a liquid at room temperature, such as a thermosetting silicone rubber, and is cured by heating to form a solid rubber. What is fluid at the time of sheet production even if it is solid at room temperature and becomes solid after sheet production, for example, a soft liquid epoxy resin, a thermoplastic elastomer, a thermoplastic soft resin and the like are also used. After the production of the sheet, those having a crosslinked structure are preferable in terms of heat resistance, durability and the like.

These are solid in a sheet state, but preferably have rubber elasticity. Depending on the use of the sheet, the sheet may have low elasticity. Also,
Depending on the use of the sheet, a material having adhesiveness or tackiness may be used. These polymer materials are not limited to the above-described examples, and are conventionally known to be used as an anisotropic conductive sheet, or materials having functions equivalent to or similar to the above materials. If there is, it is not particularly limited.

The conductive ferromagnetic particles 51 constituting the conductive portion 32 of the sheet 30 have ferromagnetism as particles and have conductivity at least on the surface. That is, it may be a single ferromagnetic metal or a composite particle, that is, a mixture particle, or a coated particle made of an organic or inorganic material coated with a metal.

As such conductive ferromagnetic particles 51,
For example, nickel, iron, particles of ferromagnetic metals such as cobalt or particles of alloys containing these, or these particles, gold, silver, copper, tin, palladium, those coated by plating or the like, Inorganic particles or polymer particles such as non-magnetic metal particles or glass beads,
Examples thereof include those plated with a conductive ferromagnetic metal such as iron, nickel, and cobalt. From the perspective of reducing manufacturing costs, especially nickel, iron, or
Particles of these alloys are preferable, and gold-plated particles can be preferably used for applications such as sockets and connectors that utilize the electrical characteristics of low conduction resistance. The conductive ferromagnetic particles 51 are not preferable, but whiskers (whiskers) such as iron, and short-fiber ferromagnetic metals can also be used.

The anisotropic conductive sheet of the present invention is mainly intended for a sheet which is manufactured as a stand-alone product and handled independently. However, the configuration of the present invention includes a circuit board and an anisotropic conductive material integrally formed on a surface of a lead electrode region of the circuit board as described in Japanese Patent Application Laid-Open No. 4-151889. The manufacturing method of the present invention can be easily applied to the circuit board device manufacturing method described in the publication.

[0072]

Embodiments of the present invention will be described below.

(Example 1) 961 (31) cylindrical conductive portions of conductive ferromagnetic particles having a diameter of about 0.4 mmφ were formed in a square lattice at a pitch of 1 mm.
× 31) A method of forming an arrayed anisotropic conductive sheet having a thickness of 1 mm.

(Forming Method of Mold) After a conventional iron plate mold having a small magnetic pole having a rectangular vertical cross section is once manufactured, the tip of the small magnetic pole is formed by using a mold electrode type electric discharge machine. Was made spherical.

As shown in FIG. 23, the thickness is 5 mm,
A pair of mold substrates 60 is made of two ferromagnetic plates, each of which is a ferromagnetic material having a width of 1 mm and a depth of 1 m.
The grooves 61 having a length of 0.4 mm and a width of 0.4 mm were formed in a grid pattern at intervals of 1 mm, each having 32 rows and columns. 4 surrounded by these grooves 61
The portion of the prism is the conventional small magnetic pole 62 having a rectangular cross section.

In order to make the tip of the small magnetic pole 62 spherical, a flat electrode material 63 is used as shown in FIG. 24, and the surface of the electrode material 63 is positioned at a position corresponding to the small magnetic pole 62. A die electrode 65 for an electric discharge machine was obtained by forming 961 hemispherical holes 64 having a tip of 0.6 mm in diameter in a square lattice arrangement at 1 mm intervals. This mold electrode 65 is attached to an electric discharge machine, and as shown in FIG. 25A, the mold electrode 60 is aligned with the mold substrate 60, and the distal end of each small magnetic pole 62 is subjected to electric discharge machining, as shown in FIG. As shown, it was made spherical.

Next, as shown in FIG. 25 (c), an epoxy resin 66 containing aluminum filler is filled in the groove 61 of the mold substrate 60 having the small magnetic pole 62 'having a spherical tip. Then, a mold 67 suitable for forming an anisotropic conductive sheet in which island-shaped conductive portions are arranged in a square lattice by flattening the mold surface was manufactured.

Also, a thickness of 1 mm, an outer shape of 50 mm, and an inner shape of 3
One square frame of non-magnetic stainless steel of 5 mm was sandwiched between a pair of molds, and used as a spacer for creating a space for forming an anisotropic conductive sheet. Two mold substrates and spacers
In order to perform accurate mutual alignment, holes having a diameter of 4 mmφ for alignment pins were prepared at four corners.

(Formation of Anisotropic Conductive Sheet) Gold-plated conductive ferromagnetic nickel particles having an average particle size of 40 μm were mixed with a thermosetting silicone rubber at a ratio of 10% by volume, uniformly dispersed, and formed into a fluid molding material. Is prepared and filled in the molding space between the pair of molds 67 made of the spacer (see FIG. 26).

As shown in FIG. 26, the molding material 100
Is placed closely between a pair of opposed flat magnetic poles 90 of the electromagnet device 93. A plate-shaped heater 91 for heating the mold is attached to the surface of each of the pair of magnetic poles 90 of the electromagnet device via a heat insulating layer 92. By arranging the mold 67 in this manner, the mold 67 becomes a part of the magnetic pole of the electromagnet 93, and the small magnetic pole 62 '(53 in FIG. 19).
) Are opposed to each other by the electromagnet 9.
3 is a pair of new magnetic pole surfaces. Hereinafter, the new magnetic pole of this electromagnet will be referred to as a mold magnetic pole, and the magnetic pole 90 of the electromagnet apparatus will be described.
To be distinguished.

Next, the electromagnet 93 is excited to generate a magnetic field having a magnetic field distribution created by the small magnetic pole 62 ′ in the molding space filled with the molding material 100 between the surfaces of the pair of mold magnetic poles. The conductive ferromagnetic particles 51 (see FIG. 17) dispersed in the material 100 are localized in a columnar shape. The excitation magnetic field strength and the excitation time are determined by the viscosity and curing time of the molding material 100, the material and shape and size of the conductive ferromagnetic particles 51, the shape and size of the small magnetic pole 62 'of the mold 67, the anisotropic conductivity to be formed. It depends on many factors, such as the thickness of the conductive sheet. Here, the average magnetic field strength between the mold magnetic poles is excited to about 5 kOe, the localization of the conductive ferromagnetic particles 51 is advanced at room temperature for 10 minutes, and then the mold is heated using a mold heating heater. The temperature was raised to 100 ° C. and kept for 30 minutes, and the molding material 100 was cured while further localizing. Next, the electromagnet 93
Was reduced to zero magnetic field, the mold 67 was removed, and when the mold temperature dropped to about 70 ° C., the mold 67 was opened, and the formed anisotropic conductive sheet was taken out. When this sheet was viewed from the front side with a microscope, the aggregation density of the particles in the particle aggregate was uniform. When the cross section of the aggregate portion was viewed, the particles were aggregated in a columnar shape. The conduction resistance of this sheet was sufficiently small.

(Example 2) A method for producing an anisotropic conductive sheet having a thickness of 1 mm in which 31 conductive strips having a width of about 0.2 mm are arranged in parallel at a pitch of 1 mm.

As shown in FIG. 27, the thickness is 5 mm,
The two flat plates made of a ferromagnetic material having a width of 50 mm and a width of 50 mm are used as a pair of mold substrates 70, and the surface of each of the surfaces is formed using a wire electric discharge machine capable of processing a function curve. 31 rows of semicircular linear small magnetic poles 72, 1 mm
The grooves 73 are processed in parallel with each other, and the groove 73 is filled with an epoxy resin (not shown) mixed with an aluminum filler. The surface of the mold is flattened to form an anisotropic conductive sheet having a strip-shaped conductive portion. A mold suitable for molding was manufactured. The vertical cross-sectional shape of the small magnetic pole 72 is 1 mm in height and 0.7 mm from the bottom.
At a height of mm, the width was constant at 0.6 mm, and the tip was semicircular with a radius of 0.3 mm.

Further, a thickness of 1 mm, an outer shape of 50 mm, and an inner shape of 3 mm
One 5 mm non-magnetic stainless steel square frame was sandwiched between a pair of molds to serve as a spacer for creating a space for forming an anisotropic conductive sheet. Holes having a diameter of 4 mmφ for alignment pins were prepared at four corners of the two mold substrates and the spacer in order to perform accurate alignment between them.

Using this mold substrate, an anisotropic conductive sheet was manufactured in the same manner as in Example 1. The surface of the obtained sheet and the cross section of the particle aggregate portion were the same as in Example 1. The conduction resistance of this sheet was sufficiently small.

Example 3 A sheet having a thickness of 0.7 mm, a diameter of a conductive portion of 0.5 mmφ, and a pitch of a conductive portion of 1.27 mm was produced in the same manner as in Example 1. As a comparative example, a sheet having the same dimensions was manufactured using a conventional mold. FIG. 28 shows the measurement results of the compressive strain dependence of the conduction resistance in the conductive portions of these sheets. The measurement was performed at room temperature for the conductive portions at six points on each sheet. The measurement results were clearly divided into two groups for the sheet manufactured by the method of the present invention and the sheet manufactured by the conventional method. The upper group shows the measurement results of the anisotropic conductive sheet according to the conventional method, and the lower group shows the measurement results of the anisotropic conductive sheet according to the present invention. As is clear from this,
It can be seen that the conduction resistance of the anisotropic conductive sheet manufactured by the method of the present invention is about one digit smaller than that of the conventional method.

(Example 4) (Preparation of a mold) 961 holes (31 mm pitch, 1 mm pitch, 0.60 mm diameter) were formed in the center of a 50 mm square, 0.60 mm thick aluminum plate. × 31) Opened for alignment. Place a 0.60 mm diameter steel ball in all these holes,
It was inserted using a press. A stainless steel sheet having a thickness of 20 μm was attached to one surface of an aluminum plate with an adhesive, and the other surface was fixed to a 50 mm square iron mold substrate having a thickness of 5 mm, thereby forming a mold magnetic pole. The mold pole is
Two sheets were prepared, and the two sheets were combined on the stainless sheet surface side so that the steel balls arranged on each surface in a square lattice form faced each other correctly. One stainless steel square frame having an outer shape of 50 mm square, a frame width of 5 mm, and a thickness of 1 mm was sandwiched between a pair of molds, and used as a spacer for forming a space for forming an anisotropic conductive sheet.

(Formation of Anisotropic Conductive Sheet) An anisotropic conductive sheet was produced in exactly the same manner as in Example 1 except that the mold produced as described above was used. The obtained sheet is an aggregate of 31 × 31 ferromagnetic particles at a pitch of 1 mm.
The dispersion state in the particle aggregate was uniform, and no missing portion was observed. That is, the aggregate density of the particles was uniform. In addition, no magnetic particles were observed between the aggregates.

This anisotropic conductive sheet was cut in the thickness direction through the center of one particle aggregate, and the aggregated state of the particles was observed. The result was almost the same as that in FIG. 17, and the shape was such that the columns of particles were slightly swelled in the middle part in the thickness direction. The conductive resistance of this sheet was sufficiently small.

[0090]

As described above, according to the present invention,
An anisotropic conductive sheet with a small conduction resistance that can be used for mounting electronic circuits such as sockets or connectors, and conductive ferromagnetic particles densely localized to the center of the conductive part. The anisotropic conductive sheet,
A pressurized conductive type anisotropic conductive sheet capable of achieving good electrical connection from a small compression displacement, an anisotropic conductive sheet having a large thickness dimension, and these anisotropic conductive sheets are manufactured. The manufacturing method suitable for the above can be provided.

[Brief description of the drawings]

FIG. 1 is an external view of a conventional anisotropic conductive sheet.

FIG. 2 is an external view of another conventional anisotropic conductive sheet.

FIG. 3 is a schematic diagram of a vertical cross section of an anisotropic conductive sheet.

FIG. 4 is a cross-sectional configuration diagram of a conventional anisotropic conductive sheet manufacturing apparatus.

FIG. 5 shows the relationship between the shape of a sheet conductive portion when the cross-sectional shape of a magnetic pole of a conventional mold is a rectangular shape, and the relationship between the magnetic pole shape of the mold and the magnetic field distribution. It is the schematic diagram seen from the sheet | seat surface, (b) is a schematic diagram which shows the perpendicular cross-sectional shape and magnetic pole shape of a conductive part, (c) is a graph which shows the magnetic field intensity distribution (Z-axis component) near the magnetic pole surface. is there.

6A and 6B are diagrams showing the relationship between the shape of a conductive portion and the shape of a magnetic pole in the case of a conventional narrow-section rectangular magnetic pole, where FIG. 6A is a schematic view of the conductive portion as viewed from the sheet surface, and FIG. It is a schematic diagram of a vertical cross section of a part.

FIG. 7 shows the relationship between the shape of a conductive portion and the shape of a magnetic pole in an anisotropic conductive sheet having a conductive portion having a convex shape (projection size <magnetic pole size) in the case of a conventional magnetic pole having a rectangular cross section. (A)
FIG. 3 is a schematic diagram of the conductive portion as viewed from the sheet surface, and FIG. 4B is a schematic diagram of a vertical cross section of the conductive portion.

FIG. 8 is a schematic cross-sectional view of a model magnetic pole mold in which a conventional magnetic pole has a rectangular cross-sectional shape.

FIG. 9 is a schematic cross-sectional view of a model magnetic pole mold in which a cross-sectional shape of a magnetic pole is a shape in which a corner of a rectangular tip is rounded.

FIG. 10 is a schematic cross-sectional view of a model magnetic pole mold in which the cross-sectional shape of a magnetic pole has a shape in which a horizontal straight line portion is provided at the tip of a semicircular tip.

FIG. 11 is a schematic cross-sectional view of a model magnetic pole mold in which the cross section of the magnetic pole is circular.

FIG. 12 is a graph showing a measurement result of a magnetic field intensity distribution between opposed magnetic poles when the magnetic poles have a rectangular cross section.

FIG. 13 is a graph showing a measurement result of a magnetic field intensity distribution between opposed magnetic poles when the cross-sectional shape of the magnetic pole is a rounded corner of a rectangular tip.

FIG. 14 is a graph showing a measurement result of a magnetic field intensity distribution between opposed magnetic poles when the cross-sectional shape of the magnetic pole is a shape in which a horizontal straight line portion is provided at the tip of a semicircular tip.

FIG. 15 is a graph showing a measurement result of a magnetic field intensity distribution between opposed magnetic poles when the magnetic poles have a circular cross section.

FIG. 16 is a schematic diagram of a particle arrangement of a conductive portion when a magnetic pole has a circular cross section, as viewed from the surface.

FIG. 17 is a schematic diagram illustrating a particle arrangement of a conductive portion when a magnetic pole has a circular cross section, viewed from a vertical cross section of the conductive portion.

FIG. 18 is a schematic diagram showing a positional relationship between a magnetic field intensity distribution between opposed magnetic poles of a mold and a portion m where a conductive portion is to be formed of a molding material layer.

FIG. 19 is a schematic view of a main part when a molding material is placed between opposed magnetic poles of a mold.

FIG. 20 is a schematic view of a particle arrangement of a conductive portion viewed from a vertical cross section when a magnetic pole has a circular section with a flattened tip.

FIG. 21 is a schematic diagram illustrating a particle arrangement of a conductive portion when the magnetic pole has a circular cross section having a flattened tip as viewed from the surface of the conductive portion.

FIGS. 22A and 22B are schematic diagrams illustrating an example of a mold magnetic pole using a small spherical magnetic pole, where FIG. 22A is a side sectional view and FIG. 22B is a plan view.

FIG. 23 is a perspective view of a conventional mold substrate. FIG. 2 is a perspective view of a mold substrate in an intermediate stage of manufacturing the mold according to the first embodiment of the present invention.

FIG. 24 is a perspective view of a mold electrode for an electric discharge machine, for explaining a first embodiment of the present invention, for forming a small magnetic pole of a mold.

FIG. 25 illustrates a first embodiment of the present invention.
(A) is a schematic cross-sectional view when a mold substrate and a mold electrode for an electric discharge machine are aligned, and (b) is a schematic cross-sectional view of the mold substrate after the tip of a small magnetic pole is curved. (C) is a schematic sectional view of the completed mold.

FIG. 26 is a schematic cross-sectional view for explaining the first embodiment of the present invention and showing a state where a sheet is being formed by a mold attached to an electromagnet device.

FIG. 27 is a perspective view of a mold substrate for explaining a second embodiment of the present invention.

FIG. 28 is a graph showing the compressive strain dependency of the conduction resistance in each conductive part of the anisotropic conductive sheet according to the present invention and the conventional anisotropic conductive sheet.

[Explanation of symbols]

 REFERENCE SIGNS LIST 30 anisotropic conductive sheet 31 insulating part 32 conductive part 33 conductive magnetic particle row 40 magnetic pole plate (mold substrate made of ferromagnetic material) 41 spherical small magnetic pole 42 plate made of non-magnetic material 50 polymer material 51 conductive strength Magnetic particles 52 Molding material 53, 53a, 62 ', 72 Small magnetic pole 54 Mold substrate 55, 56 Mold magnetic pole 60, 70 Mold substrate 61, 73 Groove 62 Small magnetic pole 63 Electrode material 64 Hemispherical hole 65 Electric discharge machining Mold electrode for machine 66 Epoxy resin containing aluminum filler 67 Mold 90 A pair of flat magnetic poles facing each other in electromagnet device 91 Plate heater for heating mold 92 Heat insulating layer 93 Electromagnet 100 Molding material

──────────────────────────────────────────────────続 き Continuation of the front page (56) References JP-A-1-100822 (JP, A) JP-A-54-146873 (JP, A) JP-A-53-147772 (JP, A) JP-A-59-1984 127810 (JP, A) JP-A-4-151889 (JP, A) JP-A-3-183974 (JP, A) JP-A-3-141506 (JP, A) JP-A-7-106380 (JP, A) JP-A-3-196416 (JP, A) JP-A-3-250609 (JP, A) JP-A-7-105741 (JP, A) JP-A-5-32755 (JP, A) (58) Fields investigated (Int.Cl. ⁷ , DB name) H01R 11/01 H01R 43/00

Claims (11)

(57) [Claims] A molding space is provided between a pair of opposed mold magnetic poles provided with a plurality of small magnetic poles made of a ferromagnetic material so that a magnetic field is localized, and the molding space is formed under molding conditions. A molding material in which conductive ferromagnetic particles are dispersed in a flowable curable material is arranged, and the pair of mold poles localizes the conductive ferromagnetic particles in the molding material, and the molding material is A method for producing an anisotropic conductive sheet by curing, wherein a distance of the mold pole from a pole surface is within a range of 0% or more and less than 25% of a distance between opposed magnetic poles during molding. A component (Z-axis component) of the magnetic field strength distribution perpendicular to the magnetic pole surface on any plane parallel to the magnetic pole surface of the type magnetic pole shows a maximum on an axis substantially at the center of each of the small magnetic poles. A method for producing an anisotropic conductive sheet, comprising: 2. The method according to claim 1, wherein the width of the at least one vertical cross section of the small magnetic pole is reduced toward the distal end, the rate of decrease in the width from the proximal end toward the distal end is increased, The maximum value of the width of the cross section parallel to the pole face of 6 is 6
2. A mold magnetic pole having a shape having a linear portion parallel to the magnetic pole surface of 0% or less and having small magnetic poles arranged in a plane is used as the mold magnetic pole. 3. The method for producing an anisotropic conductive sheet according to 1.). 3. A linear portion parallel to the magnetic pole surface has a maximum value of 50 of a width parallel to the magnetic pole surface of the cross section of the small magnetic pole.
%. The method for producing an anisotropic conductive sheet according to claim 2, wherein 4. The vertical cross-sectional shape of at least one of the small magnetic poles is such that the width decreases toward the tip, the rate of decrease of the width from the base end toward the tip increases, and 2. The mold according to claim 1, wherein the mold has a shape in which there is no linear portion parallel to the magnetic pole surface, and uses a mold magnetic pole having the small magnetic poles arranged in a plane as the mold magnetic pole. The method for producing an anisotropic conductive sheet of the above. 5. The curable molding material is an electrically insulating polymer material having a fluidity when a magnetic field is applied during the production of the sheet, and then having a property of being cured. A method for producing an anisotropic conductive sheet according to claim 1. 6. The electrically insulating polymer material may be silicone rubber, ethylene propylene rubber, urethane rubber, fluorine rubber, polyester rubber, styrene butadiene rubber, styrene butadiene block copolymer rubber, styrene iso 6. The composition according to claim 5, which is selected from a propylene block copolymer rubber, a soft epoxy resin, a thermoplastic elastomer, and a thermoplastic soft resin, and has liquid or fluidity at the temperature at the time of sheet production. A method for producing a conductive sheet. 7. The method for producing an anisotropic conductive sheet according to claim 5, wherein the electrically insulating polymer material has a crosslinked structure after molding. 8. The anisotropic conductive sheet according to claim 5, wherein the electrically insulating polymer material is solid after molding and has rubber elasticity. Production method. 9. The anisotropic conductive sheet according to claim 1, wherein the conductive ferromagnetic particles have ferromagnetism as particles and have at least a surface having conductivity. Manufacturing method. 10. The conductive ferromagnetic particles are one of a single ferromagnetic metal particle, a coated particle made of an organic or inorganic material coated with a metal, and a mixed particle thereof. Item 10. The method for producing an anisotropic conductive sheet according to item 9. 11. The conductive ferromagnetic particles include nickel,
Iron, particles of ferromagnetic metals such as cobalt or alloy particles containing them, whiskers of ferromagnetic metals such as iron,
Short fiber ferromagnetic metals, or particles or short fibers thereof, coated with a metal selected from gold, silver, copper, tin, palladium, rhodium by plating or the like, non-magnetic metal particles or glass beads, etc. 11. The anisotropically conductive material according to claim 10, wherein the inorganic particles or the polymer particles are plated with a conductive ferromagnetic metal such as iron, nickel, or cobalt, or a mixture thereof. Method for producing a functional sheet.