WO2010113641A1 - 導電性微粒子、異方性導電材料、及び、接続構造体 - Google Patents
導電性微粒子、異方性導電材料、及び、接続構造体 Download PDFInfo
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- WO2010113641A1 WO2010113641A1 PCT/JP2010/054540 JP2010054540W WO2010113641A1 WO 2010113641 A1 WO2010113641 A1 WO 2010113641A1 JP 2010054540 W JP2010054540 W JP 2010054540W WO 2010113641 A1 WO2010113641 A1 WO 2010113641A1
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- fine particles
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- point metal
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- melting point
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01B—CABLES; CONDUCTORS; INSULATORS; SELECTION OF MATERIALS FOR THEIR CONDUCTIVE, INSULATING OR DIELECTRIC PROPERTIES
- H01B1/00—Conductors or conductive bodies characterised by the conductive materials; Selection of materials as conductors
- H01B1/02—Conductors or conductive bodies characterised by the conductive materials; Selection of materials as conductors mainly consisting of metals or alloys
- H01B1/026—Alloys based on copper
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- C—CHEMISTRY; METALLURGY
- C23—COATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; CHEMICAL SURFACE TREATMENT; DIFFUSION TREATMENT OF METALLIC MATERIAL; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL; INHIBITING CORROSION OF METALLIC MATERIAL OR INCRUSTATION IN GENERAL
- C23C—COATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; SURFACE TREATMENT OF METALLIC MATERIAL BY DIFFUSION INTO THE SURFACE, BY CHEMICAL CONVERSION OR SUBSTITUTION; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL
- C23C18/00—Chemical coating by decomposition of either liquid compounds or solutions of the coating forming compounds, without leaving reaction products of surface material in the coating; Contact plating
- C23C18/16—Chemical coating by decomposition of either liquid compounds or solutions of the coating forming compounds, without leaving reaction products of surface material in the coating; Contact plating by reduction or substitution, e.g. electroless plating
- C23C18/1601—Process or apparatus
- C23C18/1633—Process of electroless plating
- C23C18/1635—Composition of the substrate
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01B—CABLES; CONDUCTORS; INSULATORS; SELECTION OF MATERIALS FOR THEIR CONDUCTIVE, INSULATING OR DIELECTRIC PROPERTIES
- H01B1/00—Conductors or conductive bodies characterised by the conductive materials; Selection of materials as conductors
- H01B1/20—Conductive material dispersed in non-conductive organic material
- H01B1/22—Conductive material dispersed in non-conductive organic material the conductive material comprising metals or alloys
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01B—CABLES; CONDUCTORS; INSULATORS; SELECTION OF MATERIALS FOR THEIR CONDUCTIVE, INSULATING OR DIELECTRIC PROPERTIES
- H01B5/00—Non-insulated conductors or conductive bodies characterised by their form
- H01B5/16—Non-insulated conductors or conductive bodies characterised by their form comprising conductive material in insulating or poorly conductive material, e.g. conductive rubber
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01R—ELECTRICALLY-CONDUCTIVE CONNECTIONS; STRUCTURAL ASSOCIATIONS OF A PLURALITY OF MUTUALLY-INSULATED ELECTRICAL CONNECTING ELEMENTS; COUPLING DEVICES; CURRENT COLLECTORS
- H01R4/00—Electrically-conductive connections between two or more conductive members in direct contact, i.e. touching one another; Means for effecting or maintaining such contact; Electrically-conductive connections having two or more spaced connecting locations for conductors and using contact members penetrating insulation
- H01R4/04—Electrically-conductive connections between two or more conductive members in direct contact, i.e. touching one another; Means for effecting or maintaining such contact; Electrically-conductive connections having two or more spaced connecting locations for conductors and using contact members penetrating insulation using electrically conductive adhesives
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- H—ELECTRICITY
- H05—ELECTRIC TECHNIQUES NOT OTHERWISE PROVIDED FOR
- H05K—PRINTED CIRCUITS; CASINGS OR CONSTRUCTIONAL DETAILS OF ELECTRIC APPARATUS; MANUFACTURE OF ASSEMBLAGES OF ELECTRICAL COMPONENTS
- H05K3/00—Apparatus or processes for manufacturing printed circuits
- H05K3/30—Assembling printed circuits with electric components, e.g. with resistor
- H05K3/32—Assembling printed circuits with electric components, e.g. with resistor electrically connecting electric components or wires to printed circuits
- H05K3/321—Assembling printed circuits with electric components, e.g. with resistor electrically connecting electric components or wires to printed circuits by conductive adhesives
- H05K3/323—Assembling printed circuits with electric components, e.g. with resistor electrically connecting electric components or wires to printed circuits by conductive adhesives by applying an anisotropic conductive adhesive layer over an array of pads
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- H—ELECTRICITY
- H05—ELECTRIC TECHNIQUES NOT OTHERWISE PROVIDED FOR
- H05K—PRINTED CIRCUITS; CASINGS OR CONSTRUCTIONAL DETAILS OF ELECTRIC APPARATUS; MANUFACTURE OF ASSEMBLAGES OF ELECTRICAL COMPONENTS
- H05K2201/00—Indexing scheme relating to printed circuits covered by H05K1/00
- H05K2201/02—Fillers; Particles; Fibers; Reinforcement materials
- H05K2201/0203—Fillers and particles
- H05K2201/0206—Materials
- H05K2201/0218—Composite particles, i.e. first metal coated with second metal
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- Y—GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
- Y10—TECHNICAL SUBJECTS COVERED BY FORMER USPC
- Y10T—TECHNICAL SUBJECTS COVERED BY FORMER US CLASSIFICATION
- Y10T428/00—Stock material or miscellaneous articles
- Y10T428/29—Coated or structually defined flake, particle, cell, strand, strand portion, rod, filament, macroscopic fiber or mass thereof
- Y10T428/2982—Particulate matter [e.g., sphere, flake, etc.]
- Y10T428/2991—Coated
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- Y—GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
- Y10—TECHNICAL SUBJECTS COVERED BY FORMER USPC
- Y10T—TECHNICAL SUBJECTS COVERED BY FORMER US CLASSIFICATION
- Y10T428/00—Stock material or miscellaneous articles
- Y10T428/29—Coated or structually defined flake, particle, cell, strand, strand portion, rod, filament, macroscopic fiber or mass thereof
- Y10T428/2982—Particulate matter [e.g., sphere, flake, etc.]
- Y10T428/2991—Coated
- Y10T428/2998—Coated including synthetic resin or polymer
Definitions
- the present invention relates to conductive fine particles capable of suppressing the occurrence of a blackening phenomenon during storage and realizing high connection reliability, an anisotropic conductive material using the conductive fine particles, and a connection structure About the body.
- soldering electrodes In an electronic circuit board, ICs and LSIs are connected by soldering electrodes to a printed circuit board.
- soldering cannot efficiently connect the printed circuit board to the IC or LSI.
- a BGA ball grid array
- solder balls In order to solve this problem, a BGA (ball grid array) has been developed in which the solder is made into a spherical shape, so-called “solder balls” that connect the IC or LSI to the substrate.
- an electronic circuit that achieves both high productivity and high connection reliability can be configured by melting a solder ball mounted on a chip or a substrate at a high temperature and connecting the substrate and the chip.
- Patent Document 1 discloses that a metal layer (conductive layer) containing a highly conductive metal is formed on the surface of resin fine particles, and further, a metal such as tin is formed on the surface of the metal layer.
- a conductive fine particle having a low melting point metal layer (solder layer) formed thereon is disclosed. If such conductive fine particles are used, the stress applied to the conductive fine particles by the flexible resin fine particles can be relaxed, and the low melting point metal layer can be formed on the outermost surface to easily conduct conductive connection between the electrodes. it can.
- Patent Document 1 describes conductive fine particles whose surface is uniformly coated with a lubricant, but when such conductive fine particles are used, There is a problem that the conductive fine particles are slightly adhered to each other by the lubricant on the surface and are easily aggregated.
- Patent Document 2 and Patent Document 3 describe a method using conductive fine particles having a metal soap molecular film or an organic film formed on the surface. In these methods, the metal soap molecular film or The generation of impurities due to the organic film has caused a new problem that the melting property of the low melting point metal is inhibited.
- the present invention relates to conductive fine particles capable of suppressing the occurrence of a blackening phenomenon during storage and realizing high connection reliability, an anisotropic conductive material using the conductive fine particles, and a connection structure
- the purpose is to provide a body.
- the present invention relates to a conductive fine particle in which a conductive layer and a low-melting point metal layer are sequentially formed on the surface of a base particle, wherein the low-melting point metal layer has an arithmetic average roughness of 50 nm or less. It is.
- the present invention is described in detail below.
- the inventors of the present invention have suppressed the blackening phenomenon that occurs when the low melting point metal is scraped off during storage by setting the arithmetic average roughness of the low melting point metal layer surface to 50 nm or less.
- the inventors have found that the connection reliability of the conductive fine particles can be greatly improved, and have completed the present invention.
- the conductive fine particles of the present invention are conductive fine particles in which a conductive layer and a low melting point metal layer are sequentially formed on the surface of the substrate fine particles, and the arithmetic average roughness of the surface of the low melting point metal layer is 50 nm or less. is there.
- the resin fine particles are not particularly limited, and include, for example, polyolefin resin, acrylic resin, polyalkylene terephthalate resin, polysulfone resin, polycarbonate resin, polyamide resin, phenol formaldehyde resin, melamine formaldehyde resin, benzoguanamine formaldehyde resin, urea formaldehyde resin, and the like.
- Resin fine particles include polyolefin resin, acrylic resin, polyalkylene terephthalate resin, polysulfone resin, polycarbonate resin, polyamide resin, phenol formaldehyde resin, melamine formaldehyde resin, benzoguanamine formaldehyde resin, urea formaldehyde resin, and the like.
- Resin fine particles include polyolefin resin, acrylic resin, polyalkylene terephthalate resin, polysulfone resin, polycarbonate resin, polyamide resin, phenol formaldehyde resin, melamine formaldehyde resin, benzoguanamine
- the method for producing the resin fine particles is not particularly limited, and examples thereof include a polymerization method, a method using a polymer protective agent, and a method using a surfactant.
- the polymerization method is not particularly limited, and examples thereof include emulsion polymerization, suspension polymerization, seed polymerization, dispersion polymerization, and dispersion seed polymerization.
- the preferred lower limit of the 10% K value of the fine resin particles is 1000 MPa, and the preferred upper limit is 15000 MPa. If the 10% K value is less than 1000 MPa, the resin fine particles may be destroyed when the resin fine particles are compressed and deformed. When the 10% K value exceeds 15000 MPa, the conductive fine particles may damage the electrode.
- the more preferable lower limit of the 10% K value is 2000 MPa, and the more preferable upper limit is 10,000 MPa.
- the 10% K value is obtained by using a micro compression tester (for example, “PCT-200” manufactured by Shimadzu Corporation), and using a smooth indenter end face of a diamond cylinder having a diameter of 50 ⁇ m and a compression speed of 2.6 mN /
- the compression displacement (mm) when compressed under conditions of seconds and a maximum test load of 10 g can be measured and determined by the following equation.
- K value (N / mm 2) ( 3 / ⁇ 2) ⁇ F ⁇ S -3/2 ⁇ R -1/2
- F Load value at 10% compression deformation of resin fine particles (N)
- S Compression displacement (mm) in 10% compression deformation of resin fine particles
- R radius of resin fine particles (mm)
- the average particle diameter of the substrate fine particles is not particularly limited, but a preferable lower limit is 1 ⁇ m and a preferable upper limit is 2000 ⁇ m.
- a preferable lower limit is 1 ⁇ m and a preferable upper limit is 2000 ⁇ m.
- the average particle diameter of the above-mentioned substrate fine particles is less than 1 ⁇ m, the substrate fine particles are likely to aggregate.
- conductive fine particles in which a low melting point metal layer is formed on the surface of the aggregated substrate fine particles are used, a gap between adjacent electrodes can be obtained. May cause a short circuit.
- the average particle diameter of the base material fine particles exceeds 2000 ⁇ m, the range suitable for connection between electrodes such as a circuit board may be exceeded.
- the more preferable lower limit of the average particle diameter of the substrate fine particles is 3 ⁇ m, and the more preferable upper limit is 1000 ⁇ m.
- the average particle size of the above-mentioned substrate fine particles is obtained by measuring the particle size of 50 randomly selected substrate fine particles using an
- a conductive layer is formed on the surface of the substrate fine particles.
- the conductive layer serves as a base metal layer.
- the metal forming the conductive layer is not particularly limited, and examples thereof include gold, silver, copper, zinc, iron, lead, tin, aluminum, cobalt, indium, nickel, chromium, antimony, bismuth, germanium, and cadmium. .
- the metal which forms the said conductive layer is gold, copper, or nickel.
- the method for forming the conductive layer on the surface of the substrate fine particles is not particularly limited, and examples thereof include an electroless plating method, an electrolytic plating method, a vacuum deposition method, an ion plating method, and an ion sputtering method.
- the thickness of the said conductive layer is not specifically limited, A preferable minimum is 0.1 micrometer and a preferable upper limit is 100 micrometers. If the thickness of the conductive layer is less than 0.1 ⁇ m, sufficient conductivity may not be obtained. When the thickness of the conductive layer exceeds 100 ⁇ m, the flexibility of the conductive fine particles may be lowered. A more preferable lower limit of the thickness of the conductive layer is 0.2 ⁇ m, and a more preferable upper limit is 50 ⁇ m.
- the thickness of the conductive layer is a thickness obtained by observing and measuring a section of 10 randomly selected conductive fine particles with a scanning electron microscope (SEM) and arithmetically averaging them.
- SEM scanning electron microscope
- the conductive fine particles of the present invention have a low melting point metal.
- the low-melting-point metal layer has a role of melting and joining the electrodes by a reflow process and conducting between the electrodes.
- the arithmetic average roughness of the surface of the low melting point metal layer is 50 nm or less. When the arithmetic average roughness exceeds 50 nm, a part of the low melting point metal is scraped off during storage, and a blackening phenomenon occurs.
- the arithmetic average roughness is preferably 45 nm or less, and more preferably 25 nm or less.
- arithmetic mean roughness (Ra) is measured by the method based on JIS B0601.
- the low-melting-point metal layer preferably contains tin having 6 or more crystal orientations having a peak intensity of 30% or more with respect to the peak intensity of the first preferential orientation.
- the conventional low melting point metal layer formed on the surface of the conductive fine particles is composed of a metal having low hardness and high ductility.
- the low melting point metal layer may be deformed by the contact, and the sphericity of the conductive fine particles may be lowered. As a result, there is a problem in that the ball mounter is attracted in the mounting process, resulting in a mounting defect.
- the conductive fine particles of the present invention contain tin having 6 or more crystal orientations having a peak intensity of 30% or more with respect to the peak intensity of the first preferred orientation when the XRD measurement is performed. Since the hardness of the low melting point metal layer increases and the ductility decreases, it is possible to prevent the low melting point metal layer from being deformed by friction between conductive fine particles during storage or contact with equipment during mounting. As a result, it is possible to reduce defects in the mounting process, such as poor mounting of the ball mounter.
- XRD measurement refers to a method for analyzing a crystal by X-ray diffraction (X-Ray Diffraction) measurement. Specifically, X-rays are incident on the crystal to be measured, and the intensity of Bragg reflection at each crystal orientation is measured. Thereby, the existence ratio of each crystal orientation is obtained from the kind of crystal orientation existing in the crystal and its intensity ratio.
- the “first preferred orientation” refers to a crystal orientation having the highest peak intensity when 2 ⁇ is in the range of 30 to 90 ° in the XRD measurement.
- the “intensity ratio” means the intensity ratio when the peak intensity of the crystal orientation defined as the first preferred orientation is 100%.
- the number of “crystal orientations having a peak intensity with an intensity ratio of 30% or more with respect to the peak intensity of the first preferential orientation” includes the first preferential orientation itself.
- the tin has 6 or more crystal orientations having a peak intensity with an intensity ratio of 30% or more with respect to the peak intensity of the first preferred orientation defined as described above. Having 6 or more crystal orientations in which the intensity ratio is 30% or more means that the tin has a large orientation.
- the hardness of the low-melting-point metal layer increases and the ductility decreases, so that the low-melting-point metal is rubbed by rubbing between conductive fine particles during storage and contact with equipment during mounting. It is possible to prevent the layer from being deformed, and as a result, it is possible to reduce inconveniences in the mounting process, such as poor adhesion of the ball mounter.
- the intensity ratio has a crystal orientation having a peak intensity of 30% or more, and more preferably 10 or less.
- the low melting point metal constituting the low melting point metal layer is not particularly limited, but is preferably tin or an alloy containing tin.
- the alloy include a tin-silver alloy, a tin-copper alloy, a tin-silver-copper alloy, a tin-bismuth alloy, and a tin-zinc alloy.
- tin, tin-silver alloy, and tin-silver-copper alloy are suitable as the low melting point metal because of excellent wettability with respect to each electrode material.
- the low-melting-point metal layer includes nickel, copper, antimony, aluminum, zinc, iron, gold, titanium, phosphorus, germanium, tellurium, cobalt, Metals such as bismuth, manganese, chromium, molybdenum, and palladium may be included.
- the said low melting metal layer since it is excellent in the effect which improves the joining strength of the said low melting metal layer and an electrode, it is suitable to make the said low melting metal layer contain nickel, copper, antimony, aluminum, and zinc.
- the content of the metal in the total of metals contained in the low melting point metal layer is not particularly limited, but a preferable lower limit is 0.0001% by weight and a preferable upper limit is 1% by weight.
- a preferable lower limit is 0.0001% by weight
- a preferable upper limit is 1% by weight.
- the content of the metal in the total of metals contained in the low melting point metal layer is in the range of 0.0001 to 1% by weight, the bonding strength between the low melting point metal layer and the electrode is further increased. Can be improved.
- the tin content in the low melting point metal layer is preferably 40% by weight or more. When the content is less than 40% by weight, the effects of the present invention cannot be sufficiently obtained, and mounting defects may be caused.
- the tin content in the low melting point metal layer means the ratio of tin to the total of the elements contained in the low melting point metal layer, and the tin content in the low melting point metal layer is the high frequency inductively coupled plasma. It can be measured using an emission spectroscopic analyzer (“ICP-AES” manufactured by Horiba, Ltd.), a fluorescent X-ray analyzer (“EDX-800HS” manufactured by Shimadzu), and the like.
- the thickness of the said low melting metal layer is not specifically limited, A preferable minimum is 0.1 micrometer and a preferable upper limit is 200 micrometers.
- a preferable minimum is 0.1 micrometer and a preferable upper limit is 200 micrometers.
- the thickness of the low-melting-point metal layer is less than 0.1 ⁇ m, it may not be able to be sufficiently bonded to the electrode even when reflowed and melted.
- the thickness of the low-melting-point metal layer exceeds 200 ⁇ m, Aggregation tends to occur when the melting point metal layer is formed, and the aggregated conductive fine particles may cause a short circuit between adjacent electrodes.
- the minimum with more preferable thickness of the said low melting metal layer is 0.2 micrometer, and a more preferable upper limit is 50 micrometers.
- the thickness of the low melting point metal layer is a thickness obtained by observing and measuring a cross section of 10 randomly selected conductive fine particles with a scanning electron microscope (SEM) and arithmetically averaging the measured values.
- the low melting point metal layer may have a close contact layer on the conductive layer side.
- the adhesion layer is preferably formed by displacement plating. As a result, the adhesion between the conductive layer and the low-melting-point metal layer is greatly improved, so that it is possible to effectively prevent the occurrence of poor bonding due to the exposure of the conductive layer after the primary mounting.
- the metal forming the adhesion layer is preferably tin, but may contain an element other than tin, or may be an alloy of tin and another metal.
- the alloy is not particularly limited, and examples thereof include a tin-copper alloy, a tin-silver alloy, a tin-bismuth alloy, a tin-zinc alloy, and a tin-indium alloy.
- the above displacement plating is a method of immersing an object to be plated in a plating solution containing a metal salt solution, and using the difference in ionization tendency between the substrate metal of the object to be plated and the metal ion in the displacement plating solution, This is a method for precipitating ions. For example, by immersing a substrate fine particle on which a conductive layer made of a metal having a high ionization tendency is formed in a plating solution containing metal ions having a low ionization tendency, the metal having a high ionization tendency is dissolved and the ionization tendency is low. An adhesion layer made of metal can be formed.
- the above displacement plating is a plating method different from electroplating in which a base metal of an object to be plated is energized as a cathode in a plating solution containing metal ions, and a metal film is deposited on the surface.
- electroless reduction plating in which metal ions in the plating solution are chemically reduced and deposited to form a metal film on the surface of the base metal.
- the substitution plating solution used in the substitution plating step is not particularly limited as long as it contains metal ions, and examples thereof include those containing tin ions and silver ions.
- concentration of metal ions is appropriately changed according to the material of the conductive layer.
- various acids, complexing agents, and other additives are added to the above replacement plating solution for the purpose of lowering the potential of the base metal and allowing precipitation of metal ions in the plating solution, which has a higher ionization tendency than the base metal.
- An agent may be added.
- various counter ions such as sulfate ions, nitrate ions, halide ions may be contained as counter ions of the metal ions.
- the upper limit of the thickness of the intermetallic diffusion layer between the conductive layer and the low melting point metal layer after heating at 150 ° C. for 300 hours is the thickness of the conductive layer and the thickness of the low melting point metal layer. It is preferable that it is 20% with respect to the sum total.
- the present inventors have found that the metal constituting the conductive layer is a factor that causes breakdown at the interface between the metal layer (conductive layer) and the low melting point metal layer in the conductive connection between the electrodes. It was found that a layer composed of an intermetallic compound (intermetallic diffusion layer) formed between the metal and the metal constituting the low melting point metal layer is involved. That is, it has been found that the formation of a fragile intermetallic diffusion layer causes the interface to break with the intermetallic diffusion layer as a starting point against external force. As a result of further intensive studies, the present inventors have determined that the thickness of the intermetallic diffusion layer between the conductive layer and the low melting point metal layer after heating at 150 ° C.
- the thickness of the conductive layer and the low melting point metal layer is the thickness of the conductive layer and the low melting point metal layer. It has been found that when the total thickness is 20% or less, breakage at the interface between the conductive layer and the low-melting-point metal layer can be suppressed and connection reliability can be greatly improved.
- the upper limit of the thickness of the intermetallic diffusion layer between the conductive layer and the low melting point metal layer after heating at 150 ° C. for 300 hours is 20% of the total thickness of the conductive layer and the low melting point metal layer.
- the phrase “is” means that there is very little contact in atomic units between the metal constituting the conductive layer and the metal constituting the low melting point metal layer when the conductive fine particles are produced. Thereby, formation of an intermetallic diffusion layer can be suppressed, destruction of the interface can be prevented, and conductive fine particles having high connection reliability can be obtained.
- the thickness of the intermetallic diffusion layer exceeds 20% with respect to the total thickness of the conductive layer and the low melting point metal layer, the interface may be broken starting from the intermetallic diffusion layer.
- the more preferable lower limit of the thickness of the intermetallic diffusion layer is 1% of the total of the thickness of the conductive layer and the low melting point metal layer, and the more preferable upper limit is 16 of the total of the thickness of the conductive layer and the thickness of the low melting point metal layer. 0.7%.
- the “intermetallic diffusion layer” refers to a layer made of an “intermetallic compound” in which a metal element constituting the conductive layer and a metal element constituting the low melting point metal layer are combined.
- the thickness of the intermetallic diffusion layer can be measured using a scanning electron microscope (FE-SEM, manufactured by HORIBA, Ltd.) by performing electron micrograph photography and element beam analysis.
- the method for producing the conductive fine particles of the present invention is not particularly limited as long as the low melting point metal layer having the shape as described above is obtained.
- the step of forming a conductive layer on the surface of the substrate fine particles A method comprising a step of forming a low-melting-point metal layer on the surface of the conductive layer by bringing the low-melting-point metal fine particles into contact with the substrate fine particles on which the conductive layer is formed and melt-softening the low-melting-point metal fine particles by shear compression.
- Such a method for producing conductive fine particles is also one aspect of the present invention.
- adherence layer containing tin etc. by displacement plating on the said conductive layer further forming the layer which consists of an alloy of tin or tin, and another metal, low melting metal A layer may be formed.
- a conventionally known method such as an electroless plating method can be used for the step of forming the conductive layer containing a metal such as copper.
- the step of forming the adhesion layer the above-described method can be used.
- the low melting point metal fine particles containing tin or an alloy of tin and another metal are brought into contact with the base material fine particles on which the conductive layer is formed, and the low melting point metal is formed by shear compression.
- a method having a step of forming a low melting point metal layer by melting the fine particles dry coating method
- conductive fine particles having an arithmetic average roughness of the surface of the low melting point metal layer of 50 nm or less are preferably produced. can do.
- Examples of the dry coating method include a method using a theta composer (manufactured by Tokuju Kogakusho Co., Ltd.).
- the theta composer includes a vessel having an elliptical cavity and a rotor that is separately rotated on the same axis as the vessel in the cavity. During mixing, the vessel and the rotor are rotated in reverse. A shear compressive force can be applied in the gap in the vicinity where the minor axis of the cavity and the major axis of the rotor coincide.
- FIG. 1 shows an example of a process for forming a low-melting-point metal layer on the surface of the substrate fine particles by bringing the low-melting-point metal fine particles into contact with the substrate fine particles and melting the low-melting-point metal fine particles by shear compression. It is drawing which shows typically.
- FIG. 1 shows a method using a theta composer (manufactured by Tokuju Kogakusha Co., Ltd.) as a method for forming a low-melting point metal layer on the surface of the substrate fine particles.
- the base particle 1 and the low melting point metal particle 2 are put between the rotating container (vessel) of the theta composer 4 and the rotating blade (rotor).
- the low melting point metal fine particles 2 are formed by shear compression in a gap in the vicinity where the minor axis of the cavity in the vessel approximately coincides with the major axis of the rotor. Is instantaneously melted (FIG. 1A) and adheres to the surface of the substrate fine particles 1 (FIG. 1B).
- conductive fine particles 3 having a low melting point metal layer formed on the surface of the substrate fine particles 1 are obtained (FIG. 1C).
- the low melting point metal layer can be formed on the substrate fine particles having a particle diameter of 200 ⁇ m or less by performing the step of forming the low melting point metal layer as shown in FIG. Moreover, a low melting point metal layer having a desired composition can be formed by selecting low melting point metal fine particles. Furthermore, it is not necessary to perform complicated steps such as preparation of a plating solution, and conductive fine particles can be produced at a low cost by a simple method. *
- a mixer such as Theta Composer (manufactured by Tokuju Kogakusho Co., Ltd.), Mechanofusion (manufactured by Hosokawa Micron) And the like.
- the theta composer includes a vessel having an elliptical cavity and a rotor that is separately rotated on the same axis as the vessel in the cavity. During mixing, the vessel and the rotor are rotated in reverse. A shear compression force is generated in the gap in the vicinity where the minor axis of the cavity and the major axis of the rotor substantially coincide.
- the average particle diameter of the low melting point metal fine particles used when forming the low melting point metal layer is not particularly limited, but the preferred lower limit is 0.1 ⁇ m and the preferred upper limit is 100 ⁇ m.
- the average particle diameter of the low melting point metal fine particles is less than 0.1 ⁇ m, the low melting point metal fine particles are likely to aggregate, and it may be difficult to form the low melting point metal layer.
- the average particle diameter of the low melting point metal fine particles exceeds 100 ⁇ m, it may be difficult to form a low melting point metal layer without being melted and softened during shear compression.
- the average particle size of the low-melting-point metal fine particles is obtained by measuring the particle sizes of 50 low-melting-point metal fine particles selected at random using an optical microscope or an electron microscope, and arithmetically averaging the measured particle sizes. Can be sought. Moreover, it is preferable that the average particle diameter of the said low melting metal fine particle is 1/10 or less of the average particle diameter of the said base particle. When the average particle size of the low-melting-point metal fine particles exceeds 1/10 of the average particle size of the substrate fine particles, the low-melting-point metal fine particles adhere to the conductive layer of the substrate fine particles and form a film during shear compression. May not be possible.
- An anisotropic conductive material can be produced by dispersing the conductive fine particles of the present invention in a binder resin. Such an anisotropic conductive material is also one aspect of the present invention.
- anisotropic conductive material of the present invention examples include anisotropic conductive paste, anisotropic conductive ink, anisotropic conductive adhesive, anisotropic conductive film, and anisotropic conductive sheet.
- the binder resin is not particularly limited, but an insulating resin is used, and examples thereof include a vinyl resin, a thermoplastic resin, a curable resin, a thermoplastic block copolymer, and an elastomer.
- the said vinyl resin is not specifically limited, For example, a vinyl acetate resin, an acrylic resin, a styrene resin etc. are mentioned.
- the thermoplastic resin is not particularly limited, and examples thereof include polyolefin resin, ethylene-vinyl acetate copolymer, polyamide resin, and the like.
- the said curable resin is not specifically limited, For example, an epoxy resin, a urethane resin, a polyimide resin, an unsaturated polyester resin etc. are mentioned.
- the curable resin may be a room temperature curable resin, a thermosetting resin, a photocurable resin, or a moisture curable resin.
- the curable resin may be used in combination with a curing agent.
- the thermoplastic block copolymer is not particularly limited. For example, styrene-butadiene-styrene block copolymer, styrene-isoprene-styrene block copolymer, hydrogenated styrene-butadiene-styrene block copolymer, styrene -Hydrogenated product of isoprene-styrene block copolymer.
- the elastomer is not particularly limited, and examples thereof include styrene-butadiene copolymer rubber and acrylonitrile-styrene block copolymer rubber. These resins may be used alone or in combination of two or more.
- the anisotropic conductive material of the present invention is, for example, an extender, a plasticizer, and improved adhesiveness within a range that does not hinder the achievement of the present invention.
- the method for producing the anisotropic conductive material of the present invention is not particularly limited.
- the conductive fine particles of the present invention are added to the binder resin, and the mixture is uniformly mixed and dispersed. Examples thereof include a method for producing an anisotropic conductive ink, an anisotropic conductive adhesive, and the like.
- the conductive fine particles of the present invention are added to the binder resin and uniformly dispersed or dissolved by heating, and a predetermined film thickness is applied to a release treatment surface of a release material such as release paper or release film.
- a method for producing an anisotropic conductive film, an anisotropic conductive sheet or the like by coating may be used.
- connection structure using the conductive fine particles of the present invention or the anisotropic conductive material of the present invention is also one aspect of the present invention.
- connection structure of the present invention is a conductive connection structure in which a pair of circuit boards are connected by filling the pair of circuit boards with the conductive fine particles of the present invention or the anisotropic conductive material of the present invention. is there.
- conductive fine particles capable of suppressing the occurrence of blackening phenomenon during storage and realizing high connection reliability, an anisotropic conductive material using the conductive fine particles, and A connection structure can be provided.
- FIG. 2 is an atomic force microscope image of the surface of conductive fine particles obtained in Example 1.
- FIG. 2 is an electron micrograph of a cross section of conductive fine particles obtained in Example 1 before heating.
- 2 is an electron micrograph of a cross section after heating of the conductive fine particles obtained in Example 1.
- FIG. 2 is a chart showing element beam analysis measurement results before heating of the conductive fine particles obtained in Example 1.
- FIG. 2 is a chart showing element beam analysis measurement results after heating the conductive fine particles obtained in Example 1.
- FIG. 3 is a chart showing XRD measurement results of conductive fine particles obtained in Example 1.
- FIG. 2 is an atomic force microscope image of the surface of conductive fine particles obtained in Comparative Example 1.
- FIG. 2 is an electron micrograph of a cross section of conductive fine particles obtained in Comparative Example 1 before heating.
- 4 is an electron micrograph of a cross section of conductive fine particles obtained in Comparative Example 1 after heating.
- 6 is a chart showing element beam analysis measurement results of conductive fine particles obtained in Comparative Example 1 before heating.
- 4 is a chart showing element beam analysis measurement results after heating the conductive fine particles obtained in Comparative Example 1.
- FIG. 4 is a chart showing XRD measurement results of conductive fine particles obtained in Comparative Example 1.
- Example 1 A copper layer having a thickness of 10 ⁇ m was formed by electroplating on the surface of resin fine particles (average particle diameter of 240 ⁇ m) made of a copolymer of tetramethylolmethane tetraacrylate and divinylbenzene to obtain substrate fine particles. Subsequently, substitution plating was performed on 90 g of the obtained copper layer forming substrate fine particles using 500 g of a tin plating solution (plating solution temperature 20 ° C.) having the following composition, and a thickness of 0. A 5 ⁇ m tin layer was formed.
- resin fine particles average particle diameter of 240 ⁇ m
- a copolymer of tetramethylolmethane tetraacrylate and divinylbenzene to obtain substrate fine particles.
- substitution plating was performed on 90 g of the obtained copper layer forming substrate fine particles using 500 g of a tin plating solution (plating solution temperature 20 ° C.) having the following composition, and a thickness
- Tin plating solution composition 15 g of tin sulfate Methanesulfonic acid 75g Thiourea 45g 365g of water
- the sphericity measured by measuring the sphericity of 50 randomly selected conductive particles using an optical microscope or an electron microscope and arithmetically averaging the measured sphericity is 99.4%. Met.
- the sphericity was calculated from the following equation by obtaining the area of the circumscribed circle in contact with the conductive fine particles and the area of the inscribed circle from a projection photograph taken using an optical microscope or an electron microscope. ⁇ 1-((area of circumscribed circle ⁇ area of inscribed circle) / area of circumscribed circle) ⁇ ⁇ 100
- Example 2 In Example 1, conductive fine particles were produced in the same manner as in Example 1 except that copper fine particles (average particle size 260 ⁇ m) were used instead of resin fine particles (average particle size 240 ⁇ m) and no copper layer was formed. .
- Example 3 In Example 1, instead of tin 96.5 silver 3.5 alloy fine particles (particle size distribution 5 to 15 ⁇ m), tin 96.5 silver 3.0 copper 0.5 alloy fine particles (particle size distribution 5 to 15 ⁇ m) were used. Conductive fine particles were produced in the same manner as in Example 1 except that they were used.
- Example 4 In Example 1, tin 42.0 bismuth 58.0 alloy fine particles (particle size distribution 5 to 15 ⁇ m) were used in place of tin 96.5 silver 3.5 alloy fine particles (particle size distribution 5 to 15 ⁇ m). Conductive fine particles were produced in the same manner as in Example 1.
- Example 1 In the same manner as in Example 1, a copper layer and a tin layer were formed on the surface of resin fine particles (average particle size 240 ⁇ m) made of a copolymer of tetramethylolmethane tetraacrylate and divinylbenzene. Next, a tin 96.5 silver 3.5 alloy layer having a thickness of 25 ⁇ m was formed by electroplating on the surface of the resin fine particles on which the obtained copper layer and tin layer were formed, and conductive fine particles were obtained.
- resin fine particles average particle size 240 ⁇ m
- a tin 96.5 silver 3.5 alloy layer having a thickness of 25 ⁇ m was formed by electroplating on the surface of the resin fine particles on which the obtained copper layer and tin layer were formed, and conductive fine particles were obtained.
- the sphericity measured by measuring the sphericity of 50 randomly selected conductive fine particles using an optical microscope or an electron microscope and arithmetically averaging the measured sphericity is 99.5%. Met.
- FIG. 9 shows an electron micrograph after heating.
- 5 shows the results of element beam analysis before heating of the conductive fine particles obtained in Example 1
- FIG. 6 shows the results of element beam analysis after heating
- FIG. 6 shows the results of the element fine particle analysis before heating of the conductive fine particles obtained in Comparative Example 1.
- FIG. 11 shows the result of element beam analysis in FIG. 11, and FIG. 12 shows the result of element beam analysis after heating.
- Example 1 X-ray-diffraction apparatus
- Table 2 shows eight peaks with high intensity.
- Sn (101) is the first priority orientation.
- conductive fine particles capable of suppressing the occurrence of blackening phenomenon during storage and realizing high connection reliability, an anisotropic conductive material using the conductive fine particles, and A connection structure can be provided.
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Abstract
Description
これを解決するためにハンダを球状にした、いわゆる「ハンダボール」でICやLSIを基板に接続するBGA(ボールグリッドアレイ)が開発された。この技術によれば、チップ又は基板上に実装されたハンダボールを高温で溶融し基板とチップとを接続することで高生産性、高接続信頼性を両立した電子回路を構成することができる。
これに対して、特許文献2及び特許文献3には、表面に金属石鹸分子膜や有機皮膜を形成した導電性微粒子を用いる方法が記載されているが、これらの方法では、金属石鹸分子膜や有機皮膜に起因する不純物が発生することで、低融点金属の溶融性が阻害されるという新たな問題が生じていた。
以下に本発明を詳述する。
上記ポリオレフィン樹脂は特に限定されず、例えば、ポリエチレン樹脂、ポリプロピレン樹脂、ポリスチレン樹脂、ポリイソブチレン樹脂、ポリブタジエン樹脂等が挙げられる。上記アクリル樹脂は特に限定されず、例えば、ポリメチルメタクリレート樹脂、ポリメチルアクリレート樹脂等が挙げられる。これらの樹脂は、単独で用いられてもよいし、2種以上が併用されてもよい。
上記重合法は特に限定されず、乳化重合、懸濁重合、シード重合、分散重合、分散シード重合等の重合法が挙げられる。
上記金属微粒子は特に限定されず、例えば、アルミニウム、銅、ニッケル、鉄、金、銀等の金属からなる微粒子が挙げられる。なかでも、銅微粒子が好ましい。上記銅微粒子は、実質的に銅金属のみで形成された銅微粒子であってもよく、銅金属を含有する銅微粒子であってもよい。なお、上記基材微粒子が銅微粒子である場合は、後述する導電層を形成しなくてもよい。
K値(N/mm2)=(3/√2)・F・S-3/2・R-1/2
F:樹脂微粒子の10%圧縮変形における荷重値(N)
S:樹脂微粒子の10%圧縮変形における圧縮変位(mm)
R:樹脂微粒子の半径(mm)
なお、上記基材微粒子の平均粒子径は、光学顕微鏡又は電子顕微鏡を用いて無作為に選んだ50個の基材微粒子の粒子径を測定し、測定した粒子径を算術平均することにより求めることができる。
上記導電層を形成する金属は特に限定されず、例えば、金、銀、銅、亜鉛、鉄、鉛、錫、アルミニウム、コバルト、インジウム、ニッケル、クロム、アンチモン、ビスマス、ゲルマニウム、カドミウム等が挙げられる。なかでも、導電性に優れることから、上記導電層を形成する金属は、金、銅又はニッケルであることが好ましい。
なお、上記導電層の厚さは、無作為に選んだ10個の導電性微粒子の断面を走査型電子顕微鏡(SEM)により観察して測定し、これらを算術平均した厚さである。
なお、本明細書において、算術平均粗さ(Ra)は、JIS B0601に準拠した方法で測定されたものである。
具体的には、被測定結晶にX線を入射し、各結晶方位でのブラッグ(Bragg)反射の強度を測定する。
これにより、該結晶中に存在する結晶方位の種類、及び、その強度比から各結晶方位の存在比率を求めるものである。
また、「第一優先配向」とは、該XRD測定にて2θを30~90°の範囲内とした場合における最もピーク強度の大きい結晶方位のことをいう。
そして、「強度比」とは、第一優先配向と規定された結晶方位のピーク強度を100%とした場合の強度比のことをいう。
なお、「第一優先配向のピーク強度に対して強度比が30%以上のピーク強度を有する結晶方位」の数には、第一優先配向自体も含めるものとする。
上記強度比が30%以上である結晶方位を6以上有するということは、上記錫の配向が多いことを意味する。
このような錫を含有することで、低融点金属層の硬度が増し、延性が低下することから、保管時における導電性微粒子同士の擦れ合いや、実装時における機器との接触によって、低融点金属層が変形することを防止することができ、その結果、ボールマウンタの吸着不良等の実装工程での不具合を低減することができる。
上記強度比が30%以上のピーク強度を有する結晶方位が6未満であると、上記低融点金属層の硬度が低く、延性が高くなるため、実装不良を招くことがある。
本発明では、上記強度比が30%以上のピーク強度を有する結晶方位を6以上有することがより好ましく、10以下有することが好ましい。
なかでも、各電極材料に対し濡れ性が優れることから、低融点金属は、錫、錫-銀合金、錫-銀-銅合金が好適である。
上記低融点金属層中に含有される金属の合計に占める上記金属の含有量は特に限定されないが、好ましい下限は0.0001重量%、好ましい上限は1重量%である。上記低融点金属層中に含有される金属の合計に占める上記金属の含有量が、0.0001~1重量%の範囲内であることにより、上記低融点金属層と電極との接合強度をより向上させることができる。
なお、上記低融点金属層の厚さは、無作為に選んだ10個の導電性微粒子の断面を走査型電子顕微鏡(SEM)により観察して測定し、測定値を算術平均した厚さである。
上記密着層は、置換めっきによって形成されていることが好ましい。これにより、導電層と低融点金属層との密着性が大幅に向上するため、一次実装後に導電層が露出することに起因する接合不良の発生を効果的に防止できる。
なお、上記置換めっきは、金属イオンを含有するめっき液中で被めっき物の素地金属を陰極として通電し、表面に金属被膜を析出させる電気めっきとは異なるめっき方法であり、また、還元補助剤を加えることで、めっき液中の金属イオンを化学的に還元析出させ、素地金属表面に金属被膜を形成する無電解還元めっきとも異なるめっき方法である。
また、上記置換めっき液には、素地金属の電位を下げ、素地金属よりイオン化傾向が高いめっき液中の金属イオンでも析出が可能となることを目的として、各種の酸や錯化剤、その他添加剤を加えてもよい。更に、上記金属イオンの対イオンとして、硫酸イオン、硝酸イオン、ハロゲン化物イオン等の各種対イオンを含有していてもよい。
そして、本発明者らは更に鋭意検討した結果、150℃で300時間加熱した後における導電層と低融点金属層との間の金属間拡散層の厚みを導電層の厚みと低融点金属層の厚みとの合計に対して20%以下とした場合に、導電層と低融点金属層との界面での破壊を抑制して、接続信頼性を大幅に改善できることを見出した。
これにより、金属間拡散層の形成を抑制し、界面の破壊を防止して、接続信頼性の高い導電性微粒子とすることができる。
上記金属間拡散層の厚みが、導電層の厚みと低融点金属層の厚みとの合計に対して20%を超えると、金属間拡散層を起点とした界面の破壊が生じることがある。
上記金属間拡散層の厚みのより好ましい下限は導電層の厚みと低融点金属層の厚みとの合計の1%、より好ましい上限は導電層の厚みと低融点金属層の厚みとの合計の16.7%である。
また、上記金属間拡散層の厚みは、走査電子顕微鏡(FE-SEM、堀場製作所社製)を用いて電子顕微鏡写真撮影と元素線分析とを行い、その結果を用いて測定することができる。
このような導電性微粒子の製造方法もまた本発明の1つである。
なお、上記導電層上に置換めっきにより錫等を含有する密着層を形成する工程を行った後、更に、錫又は錫と他の金属との合金からなる層を形成することにより、低融点金属層を形成してもよい。
また、上記低融点金属微粒子の平均粒子径は、上記基材微粒子の平均粒子径の1/10以下であることが好ましい。上記低融点金属微粒子の平均粒子径が、上記基材微粒子の平均粒子径の1/10を超えると、せん断圧縮時に上記低融点金属微粒子を上記基材微粒子の導電層に付着、皮膜化させることができないことがある。
上記ビニル樹脂は特に限定されないが、例えば、酢酸ビニル樹脂、アクリル樹脂、スチレン樹脂等が挙げられる。
上記熱可塑性樹脂は特に限定されないが、例えば、ポリオレフィン樹脂、エチレン-酢酸ビニル共重合体、ポリアミド樹脂等が挙げられる。
上記硬化性樹脂は特に限定されないが、例えば、エポキシ樹脂、ウレタン樹脂、ポリイミド樹脂、不飽和ポリエステル樹脂等が挙げられる。なお、上記硬化性樹脂は、常温硬化型樹脂、熱硬化型樹脂、光硬化型樹脂、湿気硬化型樹脂であってもよい。上記硬化性樹脂は硬化剤と併用してもよい。
上記熱可塑性ブロック共重合体は特に限定されないが、例えば、スチレン-ブタジエン-スチレンブロック共重合体、スチレン-イソプレン-スチレンブロック共重合体、スチレン-ブタジエン-スチレンブロック共重合体の水素添加物、スチレン-イソプレン-スチレンブロック共重合体の水素添加物等が挙げられる。
上記エラストマーは特に限定されないが、例えば、スチレン-ブタジエン共重合ゴム、アクリロニトリル-スチレンブロック共重合ゴム等が挙げられる。
これらの樹脂は、単独で用いられてもよいし、2種以上が併用されてもよい。
また、上記バインダー樹脂と、本発明の導電性微粒子とを混合することなく、別々に用いて異方性導電材料としてもよい。
テトラメチロールメタンテトラアクリレートとジビニルベンゼンとの共重合体からなる樹脂微粒子(平均粒子径240μm)の表面に、電気めっきにより厚さ10μmの銅層を形成し、基材微粒子を得た。
次いで、得られた銅層形成基材微粒子90gに対して、下記組成の錫めっき液(めっき液温20℃)500gを用いて置換めっきを行い、銅層形成樹脂微粒子の表面に厚さ0.5μmの錫層を形成した。
硫酸錫 15g
メタンスルホン酸 75g
チオ尿素 45g
水 365g
{1-((外接円の面積-内接円の面積)/外接円の面積)}×100
実施例1において、樹脂微粒子(平均粒子径240μm)に代えて、銅微粒子(平均粒子径260μm)を用い、銅層を形成しなかった以外は実施例1と同様にして導電性微粒子を作製した。
実施例1において、錫96.5銀3.5合金微粒子(粒子径分布5~15μm)に代えて、錫96.5銀3.0銅0.5合金微粒子(粒子径分布5~15μm)を用いた以外は実施例1と同様にして導電性微粒子を作製した。
実施例1において、錫96.5銀3.5合金微粒子(粒子径分布5~15μm)に代えて、錫42.0ビスマス58.0合金微粒子(粒子径分布5~15μm)を用いた以外は実施例1と同様にして導電性微粒子を作製した。
実施例1と同様の方法で、テトラメチロールメタンテトラアクリレートとジビニルベンゼンとの共重合体からなる樹脂微粒子(平均粒子径240μm)の表面に、銅層及び錫層を形成した。
次いで、得られた銅層及び錫層を形成した樹脂微粒子の表面に電気めっきにより厚さ25μmの錫96.5銀3.5合金層を形成し、導電性微粒子を得た。
実施例及び比較例で得られた導電性微粒子について、以下の評価を行った。結果を表1に示した。
原子間力顕微鏡(VN-8000:キーエンス社製)を用い、得られた導電性微粒子表面の算術平均粗さをJIS B0601-1994に準拠した方法で測定した。なお、測定においては、2次曲面補正(自動)を行い、断面形状についても同様の補正を行った。
なお、実施例1で得られた導電性微粒子表面の原子間力顕微鏡画像を図2、比較例1で得られた導電性微粒子表面の原子間力顕微鏡画像を図8に示した。
得られた導電性微粒子を、ガラス製容器内に入れ、振動機(シェーカー)にて1時間振動した。その後、これらの導電性微粒子を、銅電極を有するシリコンチップ上に112個搭載し、270℃に設定したリフロー炉に投入し溶融させた。次いで、走査型電子顕微鏡を用いて実装表面を観察し、銅電極上に低融点金属層が濡れ広がり、バンプ形成しているものの総数を計測した。
得られた導電性微粒子について、走査電子顕微鏡(FE-SEM、堀場製作所社製)を用いて、150℃で300時間加熱する前後における導電性微粒子の厚み方向の切断面の電子顕微鏡写真を撮影し、同時に元素線分析を行った。次いで、導電性微粒子の厚み方向の直線上における銅元素及び錫元素の混在する長さから金属間拡散層の厚みを測定した。同様の厚み測定を10回行い、厚みの平均値を求めることにより、金属間拡散層の厚みを決定した。また、銅層、錫層及び合金層の厚みの合計に対する金属間拡散層の厚みの膜厚比を表1に示した。
なお、実施例1で得られた導電性微粒子の加熱前における電子顕微鏡写真を図3、加熱後における電子顕微鏡写真を図4、比較例1で得られた導電性微粒子の加熱前における電子顕微鏡写真を図9、加熱後における電子顕微鏡写真を図10に示した。
また、実施例1で得られた導電性微粒子の加熱前における元素線分析の結果を図5、加熱後における元素線分析の結果を図6、比較例1で得られた導電性微粒子の加熱前における元素線分析の結果を図11、加熱後における元素線分析の結果を図12に示した。
得られた導電性微粒子を150℃で300時間加熱した後、銅電極を有するシリコンチップ上に112個搭載し、270℃に設定したリフロー炉に投入し溶融させた。次いで導電性微粒子を実装したシリコンチップを、銅電極を有する基板上に搭載し、270℃に設定したリフロー炉に投入し溶融させることで接続構造体を得た。
得られた接続構造体の落下強度試験をJEDEC規格JESD22-B111に従って行った。接続構造体の断線が確認されるまで落下を行い、断線が起こるまでの落下回数を求めた。落下回数が150回を超えても断線しない場合を○、150回以下で断線する場合を×と評価した。
得られた導電性微粒子について、X線回折装置(RINT1000、リガク社製)を用いて、XRD測定を行い、各結晶方位おける第一優先配向のピーク強度に対する強度比を測定した。実施例1及び比較例1で得られた結果を表2に示した。表2には強度の高いピーク8つについて記載した。
なお、実施例1で得られた導電性微粒子のXRD測定チャート結果を図7に、比較例1で得られた導電性微粒子のXRD測定チャート結果を図13に示す。図7及び図13に示すように、実施例及び比較例では、Sn(101)が第一優先配向となっている。
得られた導電性微粒子と水とを容器内に入れて混合し、超音波を印加することによって導電性微粒子同士の接触を促進させた(加速試験)。次いで、超音波印加後の導電性微粒子の真球度を求めた。
「(6)接触による変形」試験を行った後の導電性微粒子を、ボールマウンタを用いて基板上の電極部分に搭載させ、その際に発生した導電性微粒子の搭載不良の割合を求めた。
Claims (10)
- 基材微粒子の表面に、導電層及び低融点金属層が順次形成されている導電性微粒子であって、前記低融点金属層表面の算術平均粗さが50nm以下であることを特徴とする導電性微粒子。
- 低融点金属層は、XRD測定を行った場合に、第一優先配向のピーク強度に対して強度比が30%以上のピーク強度を有する結晶方位を6以上有する錫を含有することを特徴とする請求項1記載の導電性微粒子。
- 150℃で300時間加熱した後における導電層と低融点金属層との間の金属間拡散層の厚みが、導電層の厚みと低融点金属層の厚みとの合計に対して20%以下であることを特徴とする請求項1又は2記載の導電性微粒子。
- 低融点金属層は、錫又は錫と他の金属との合金からなることを特徴とする請求項1、2又は3記載の導電性微粒子。
- 導電層は、銅からなることを特徴とする請求項1、2、3又は4記載の導電性微粒子。
- 基材微粒子は、樹脂微粒子であることを特徴とする請求項1、2、3、4又は5記載の導電性微粒子。
- 基材微粒子は、銅微粒子であることを特徴とする請求項1、2、3、4又は5記載の導電性微粒子。
- 請求項1、2、3、4、5、6又は7記載の導電性微粒子がバインダー樹脂に分散されてなることを特徴とする異方性導電材料。
- 請求項1、2、3、4、5、6或いは7記載の導電性微粒子、又は、請求項7記載の異方性導電材料を用いてなることを特徴とする接続構造体。
- 請求項1、2、3、4、5、6又は7記載の導電性微粒子を製造する方法であって、
基材微粒子の表面に導電層を形成する工程、前記導電層を形成した基材微粒子に低融点金属微粒子を接触させ、せん断圧縮によって前記低融点金属微粒子を溶融軟化させることにより、前記導電層の表面に低融点金属層を形成する工程を有することを特徴とする導電性微粒子の製造方法。
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US20160012931A1 (en) * | 2014-07-11 | 2016-01-14 | Tyco Electronics Corporation | Conductive Particle |
US10476074B2 (en) * | 2017-07-27 | 2019-11-12 | GM Global Technology Operations LLC | Methods of making electroactive composite materials for an electrochemical cell |
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