solid state batteries

By incorporating graphite particles with internal voids filled with a solid electrolyte, the negative electrode layer in solid-state batteries achieves improved electronic and ionic conductivity, enhancing the battery's rate characteristics.

JP7759624B2Active Publication Date: 2025-10-24PANASONIC INTELLECTUAL PROPERTY MANAGEMENT CO LTD
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Patent Information

Application Number
JP2022528459
Authority / Receiving Office
JP · JP
Patent Type
Patents
Current Assignee / Owner
Priority Date
2020-06-02
Filing Date
2021-04-02
Publication Date
2025-10-24
Estimated Expiration
2041-04-02

AI Technical Summary

Technical Problem

Existing solid-state batteries face challenges in achieving a balance between electronic conductivity and ionic conductivity in the negative electrode layer, leading to suboptimal rate characteristics during charge and discharge.

Method used

The negative electrode active material comprises graphite particles with internal voids filled with a solid electrolyte, optimizing the balance between electronic and ionic conductivity by using graphite particles as aggregates of primary particles with controlled void sizes and compositions, such as Li6PS5X with an argyrodite-type crystal structure.

Benefits of technology

This configuration enhances the rate characteristics of solid-state batteries by improving both electronic and ionic conductivity, allowing for efficient lithium ion intercalation and deintercalation.

✦ Generated by Eureka AI based on patent content.

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Patent Text Reader

Abstract

A solid-state battery 2000 according to the present disclosure comprises: a negative electrode layer 201 having a negative electrode active substance 1000; a positive electrode layer 203; and a solid electrolyte layer 202 located between the positive electrode layer 203 and the negative electrode layer 201. The negative electrode active substance 1000 is an aggregation of a plurality of primary particles 101 containing graphite, and includes: graphite particles 100 having a void 102 therein; and a solid electrolyte 103 located in the void 102. At least a portion of the void 102 may be filled with the solid electrolyte 103. The smallest diameter of the void 102 is, for example, 1-70 nm.
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Description

[Technical Field]

[0001] The present disclosure relates to solid-state batteries. [Background technology]

[0002] In all-solid-state lithium-ion batteries, both electrons and lithium ions are required to be efficiently supplied to the active material in the electrode layer. In all-solid-state lithium-ion batteries, the active material is, for example, dispersed in the electrode layer. In a typical negative electrode layer, it is desirable to have both an electron conduction path formed by contact between active material particles and an ion conduction path formed by connecting solid electrolyte particles.

[0003] Graphite particles are sometimes used as anode active materials. Graphite has a layered structure containing carbon. High-capacity batteries are realized through reactions in which lithium ions are inserted into or extracted from the graphite layer structure. However, while graphite has electronic conductivity, it has poor ionic conductivity. To compensate for the ionic conductivity of graphite, graphite particles are sometimes composited with a solid electrolyte in a typical anode layer. Furthermore, graphite particles are sometimes composited with a binder. The binder is suitable for binding the particles together to form a membrane. [Prior art documents] [Patent documents]

[0004] [Patent Document 1] Japanese Patent Application Publication No. 8-195219 Summary of the Invention [Problem to be solved by the invention]

[0005] In the prior art, it is desirable to improve the rate characteristics of solid-state batteries. [Means for solving the problem]

[0006] The solid-state battery of the present disclosure comprises: a negative electrode layer having a negative electrode active material; a positive electrode layer; a solid electrolyte layer located between the positive electrode layer and the negative electrode layer; Equipped with The negative electrode active material is graphite particles which are aggregates of a plurality of primary particles containing graphite and have voids therein; a solid electrolyte located in the void; Includes: [Effects of the Invention]

[0007] According to the present disclosure, the rate characteristics of a solid-state battery can be improved. [Brief explanation of the drawings]

[0008] [Figure 1] FIG. 1 is a cross-sectional view showing a schematic configuration of a solid-state battery according to the first embodiment. [Figure 2] FIG. 2 is a cross-sectional view showing a schematic configuration of a negative electrode active material used to prepare a negative electrode layer. [Figure 3] FIG. 3 is a flowchart showing a method for producing a negative electrode active material. [Figure 4] FIG. 4 is a scanning electron microscope (SEM) image of a cross section of the graphite particle used in Example 1. [Figure 5] FIG. 5 is an SEM image of a cross section of the negative electrode active material prepared in Example 1. [Figure 6] FIG. 6 is an SEM image of a cross section of the negative electrode active material contained in the negative electrode layer of the solid battery of Example 1. DETAILED DESCRIPTION OF THE INVENTION

[0009] (Findings that formed the basis of this disclosure) In a negative electrode layer containing graphite particles and a solid electrolyte, the solid electrolyte has poor electronic conductivity. Therefore, increasing the amount of solid electrolyte added relative to the graphite particles reduces the volume ratio of graphite in the negative electrode layer, resulting in a decrease in the capacity of the negative electrode layer. Furthermore, the electronic conductivity of the negative electrode layer also decreases due to the prevention of contact between the graphite particles. In other words, when graphite particles are combined with a solid electrolyte in the negative electrode layer, a trade-off occurs between electronic conductivity and ionic conductivity in the negative electrode layer. In this case, it is necessary to improve the capacity of the negative electrode layer while maintaining a balance between electronic conductivity and ionic conductivity.

[0010] Patent Document 1 discloses that in order to improve the utilization rate of the active material in the electrodes of conventional all-solid-state lithium secondary batteries, the average particle size of the active material, the average particle size of the solid electrolyte, and the mixing ratio of the active material and the solid electrolyte are adjusted.

[0011] Patent Document 1 discloses adjusting the average particle diameters of the active material and solid electrolyte to a range of 0.1 μm to 50 μm. Increasing the average particle diameter of the active material within this range is considered to improve the capacity of the negative electrode layer. However, in this case, the rate characteristics of the battery during charge and discharge deteriorate due to slow ion conduction within the active material. On the other hand, decreasing the average particle diameter of the active material increases the outer surface area of ​​the active material. This increases the contact area between the active material and the solid electrolyte, reducing the electronic conductivity of the negative electrode layer. Active materials with small average particle diameters can also increase the viscosity of the coating liquid. Therefore, when preparing a negative electrode layer using a coating liquid containing this active material, process issues may arise. As such, it is difficult to prepare a battery with excellent rate characteristics during charge and discharge by adjusting the average particle diameter of the active material.

[0012] (Summary of one aspect of the present disclosure) The solid-state battery according to the first aspect of the present disclosure comprises: a negative electrode layer having a negative electrode active material; a positive electrode layer; a solid electrolyte layer located between the positive electrode layer and the negative electrode layer; Equipped with The negative electrode active material is graphite particles which are aggregates of a plurality of primary particles containing graphite and have voids therein; a solid electrolyte located in the void; Includes:

[0013] According to the first aspect, the negative electrode active material contained in the negative electrode layer has high electronic conductivity due to the graphite particles. Furthermore, the negative electrode active material efficiently intercalates and deintercalates lithium ions. The negative electrode active material can improve the rate characteristics of the solid-state battery.

[0014] In the second aspect of the present disclosure, for example, in the solid-state battery according to the first aspect, at least a portion of the voids may be filled with the solid electrolyte, and the shortest diameter of the voids may be 1 nm or more and 70 nm or less. With this configuration, the rate characteristics of the solid-state battery can be improved.

[0015] In the third aspect of the present disclosure, for example, in the solid-state battery according to the first or second aspect, the primary particles may be plate-like or scaly, and the graphite particles may be stacked. With this configuration, the negative electrode active material can be easily produced using the graphite particles.

[0016] In a fourth aspect of the present disclosure, for example, in the solid state battery according to any one of the first to third aspects, the solid electrolyte may contain lithium, phosphorus, sulfur, and a halogen. With this configuration, the negative electrode active material has high ionic conductivity.

[0017] In a fifth aspect of the present disclosure, for example, in the solid state battery according to any one of the first to fourth aspects, the solid electrolyte may be represented by the following composition formula (1): Li α PS β X γ ...Equation (1) α, β, and γ may satisfy 5.5≦α≦6.5, 4.5≦β≦5.5, and 0.5≦γ≦1.5, and X may contain at least one selected from the group consisting of F, Cl, Br, and I. With this configuration, the negative electrode active material has high ionic conductivity.

[0018] In a sixth aspect of the present disclosure, for example, in the solid state battery according to any one of the first to fifth aspects, the solid electrolyte may have an argyrodite-type crystal structure, and the negative electrode active material has high ionic conductivity.

[0019] In a seventh aspect of the present disclosure, for example, in the solid state battery according to any one of the first to sixth aspects, the ratio of the mass of the solid electrolyte to the mass of the graphite particles may be 0.3 mass % or more and 10 mass % or less. With this configuration, the negative electrode active material can have improved ionic conductivity while suppressing a decrease in capacity density.

[0020] In an eighth aspect of the present disclosure, for example, in the solid-state battery according to any one of the first to seventh aspects, the graphite particles may have a median diameter of 300 nm or more and 30 μm or less. This configuration allows the graphite particles to be easily handled. Furthermore, the solid electrolyte can be easily introduced into the graphite particles.

[0021] In a ninth aspect of the present disclosure, for example, in the solid state battery according to any one of the first to eighth aspects, the negative electrode layer may further contain a solid electrolyte having a different composition from the solid electrolyte contained in the negative electrode active material. This configuration can easily improve the ionic conductivity of the negative electrode layer.

[0022] In a tenth aspect of the present disclosure, for example, in the solid state battery according to any one of the first to ninth aspects, the solid electrolyte layer may contain a solid electrolyte having lithium ion conductivity. With this configuration, the solid state battery has high rate characteristics.

[0023] Hereinafter, embodiments of the present disclosure will be described with reference to the drawings.

[0024] (Embodiment 1) FIG. 1 is a cross-sectional view showing a schematic configuration of a solid-state battery 2000 according to the first embodiment.

[0025] The solid state battery 2000 in the first embodiment includes an anode layer 201 , a solid electrolyte layer 202 , and a cathode layer 203 .

[0026] The solid electrolyte layer 202 is located between the positive electrode layer 203 and the negative electrode layer 201 .

[0027] The negative electrode layer 201 has a negative electrode material including a negative electrode active material 1000 .

[0028] The following description will first explain the negative electrode active material 1000 used to fabricate the negative electrode layer 201. Figure 2 is a cross-sectional view showing a schematic configuration of the negative electrode active material 1000 used to fabricate the negative electrode layer 201.

[0029] The negative electrode active material 1000 includes graphite particles 100 and a solid electrolyte 103 .

[0030] The graphite particle 100 can function as an active material. The graphite particle 100 has a void 102 therein. The graphite particle 100 may have a plurality of voids 102 therein. A solid electrolyte 103 is located in the void 102. In other words, the solid electrolyte 103 fills the void 102. In this specification, the solid electrolyte 103 located in the void 102 may be referred to as a "first solid electrolyte."

[0031] The negative electrode active material 1000 contains the first solid electrolyte 103 in the voids 102 of the graphite particles 100. This tends to give the negative electrode active material 1000 high ionic conductivity and high electronic conductivity.

[0032] The graphite particle 100 is an aggregate of a plurality of primary particles 101 containing graphite. In other words, the graphite particle 100 is a secondary particle made up of a plurality of primary particles 101. In the graphite particle 100, the plurality of primary particles 101 may be in contact with each other. The primary particles 101 can form an intercalation compound containing carbon. In the graphite particle 100, for example, voids 102 are formed between the plurality of primary particles 101.

[0033] The shape of the primary particles 101 is not particularly limited and may be, for example, plate-like or scale-like. The shape of the primary particles 101 may also be needle-like, spherical, oval-spherical, or the like. In the graphite particle 100, a plurality of plate-like or scale-like primary particles 101 may be stacked. That is, the graphite particle 100 may have a layered structure made of a plurality of plate-like or scale-like primary particles 101. In this layered structure, for example, a void 102 is formed between two of the plurality of primary particles 101. The void 102 extends, for example, in a direction perpendicular to the stacking direction of the plurality of primary particles 101.

[0034] As an example, the graphite particle 100 may have a plurality of voids 102, and the plurality of voids 102 may be aligned in the stacking direction of the plurality of primary particles 101. The plurality of voids 102 may be independent of each other. However, at least one void 102 of the plurality of voids 102 may be connected to another void 102. The plurality of voids 102 may be formed three-dimensionally and continuously. At least one void 102 of the plurality of voids 102 may penetrate the graphite particle 100.

[0035] For example, the graphite particle 100 is spherical or ellipsoidal. In this case, at the center of the graphite particle 100, a plurality of plate-like or scale-like primary particles 101 are overlapped and united so that the main surfaces of the plate-like or scale-like primary particles 101 extend in the diameter direction of the graphite particle 100. At the outer periphery of the graphite particle 100, the plate-like or scale-like primary particles 101 are curved and overlapped and united. Some of the plurality of primary particles 101 are folded and overlap one another. Voids 102 are formed between the primary particles 101 and between the folded primary particles 101. The "main surface" means the surface having the largest area.

[0036] The primary particles 101 may contain graphite as a main component, for example, may consist essentially of graphite. "Main component" refers to the component that is contained in the primary particles 101 in the largest amount by mass. "Consist essentially of" means that other components that alter the essential characteristics of the referenced material are excluded. However, the primary particles 101 may contain impurities in addition to graphite.

[0037] At least a portion of the voids 102 may be filled with the first solid electrolyte 103. The inside of the voids 102 may be filled with the first solid electrolyte 103.

[0038] The shortest diameter of the voids 102 in which the first solid electrolyte 103 is located is, for example, 1 nm or more and 70 nm or less. The first solid electrolyte 103 can be easily introduced into the voids 102 whose shortest diameter is 1 nm or more. If the shortest diameter of the voids 102 is 70 nm or less, the ion conduction path is not too long, and the negative electrode active material 1000 has sufficient ion conductivity.

[0039] The shortest diameter of the voids 102 can be determined by the following method. First, the negative electrode active material 1000 is processed to expose a cross section of the negative electrode active material 1000. The processing of the negative electrode active material 1000 can be performed using, for example, a cross section polisher (registered trademark). The cross section polisher can form a smooth cross section of the negative electrode active material 1000. Next, the cross section of the negative electrode active material 1000 is observed with a scanning electron microscope (SEM). This allows an SEM image of the cross section of the negative electrode active material 1000 to be obtained.

[0040] Next, the graphite particles 100, voids 102, and first solid electrolyte 103 are identified from the obtained SEM image. These may be identified based on the contrast of the image, or may be identified based on the results of elemental analysis such as energy dispersive X-ray analysis (EDS). Next, the center of gravity of the voids 102 is identified from the SEM image. Of the diameters of the voids 102 that pass through the center of gravity, the shortest diameter can be considered to be the shortest diameter of the voids 102.

[0041] The shortest diameter of the voids 102 may be 10 nm or more, or may be 20 nm or more. The shortest diameter of the voids 102 may be 65 nm or less. Furthermore, the average shortest diameter of the voids 102 may be 1 nm or more and 70 nm or less. The average shortest diameter of the voids 102 can be determined by the following method. First, a cross section of the negative electrode active material 1000 is observed using an SEM. From the obtained SEM image, the shortest diameters of any number of voids 102 (for example, five voids 102) are calculated. The average of the calculated values ​​is regarded as the average shortest diameter of the voids 102. When multiple voids 102 are displayed in the SEM image, the largest shortest diameter of the respective shortest diameters of the displayed multiple voids 102 may be 1 nm or more and 70 nm or less.

[0042] The presence of first solid electrolyte 103 in voids 102 may be confirmed by observing a cross section of negative electrode active material 1000 with an SEM, or may be confirmed by mercury intrusion porosimetry.

[0043] In mercury intrusion porosimetry, high-pressure mercury is injected into a sample containing voids. The void distribution can be determined from the relationship between the pressure applied to the mercury and the amount of mercury injected into the sample. Specifically, the diameter D of the voids in the sample into which mercury has been injected can be determined from the following relational expression (I): In relational expression (I), γ is the surface tension of mercury, θ is the contact angle between the mercury and the wall surface of the sample, and P is the pressure applied to the mercury. D=-4γcosθ÷P (I)

[0044] The pressure P is changed in stages, and the amount of injected mercury is measured for each pressure P. The amount of injected mercury can be considered as the cumulative value of the void volume up to the diameter D corresponding to a specific pressure P. This makes it possible to obtain a void distribution in which the amount of voids is specified for each diameter D. The void distribution is, for example, a graph showing the relationship between the void diameter D and the Log differential void volume.

[0045] For example, mercury porosimetry is used to measure the negative electrode active material 1000 and the graphite particles 100 in which the first solid electrolyte 103 is not present in the voids 102. The graphite particles 100 in which the first solid electrolyte 103 is not present in the voids 102 may be graphite particles 100 before the first solid electrolyte 103 is introduced into the voids 102, or graphite particles 100 obtained by removing the first solid electrolyte 103 from the negative electrode active material 1000. The first solid electrolyte 103 can be removed from the negative electrode active material 1000 using, for example, a solvent. Mercury porosimetry can be used to obtain a pore distribution showing the relationship between the pore diameter and the Log differential pore volume for each of the negative electrode active material 1000 and the graphite particles 100. The pore diameter in the pore distribution of the graphite particles 100 corresponds to the pore size of the pores 102.

[0046] Based on the void distribution of the negative electrode active material 1000 and the void distribution of the graphite particles 100, it can be determined that the first solid electrolyte 103 is located in the voids 102 of the graphite particles 100 in the negative electrode active material 1000. For example, the Log differential void volume at a specific diameter is determined for each of the void distributions of the negative electrode active material 1000 and the graphite particles 100. When the Log differential void volume of the negative electrode active material 1000 at a specific diameter is smaller than the Log differential void volume of the graphite particles 100, it can be determined that the first solid electrolyte 103 is located in the voids 102 of the graphite particles 100. Furthermore, when the diameter at the peak of the void distribution of the negative electrode active material 1000 is smaller than the diameter at the peak of the void distribution of the graphite particles 100, it can also be determined that the first solid electrolyte 103 is located in the voids 102 of the graphite particles 100.

[0047] When graphite particles 100 have multiple voids therein, the average void diameter S of graphite particles 100 determined by mercury intrusion porosimetry is not particularly limited and is, for example, 1 nm or more and 300 nm or less. The average void diameter S may be 10 nm or more, 50 nm or more, 100 nm or more, or 150 nm or more. The average void diameter S may be 250 nm or less, or 200 nm or less.

[0048] The average pore diameter S of the graphite particles 100 can be determined, for example, by the following method. First, measurement is performed by mercury porosimetry on graphite particles 100 in which the first solid electrolyte 103 is not present in the pores 102. Graphite particles 100 in which the first solid electrolyte 103 is not present in the pores 102 can be graphite particles 100 before the first solid electrolyte 103 is introduced into the pores 102, or graphite particles 100 obtained by removing the first solid electrolyte 103 from the negative electrode active material 1000. Mercury porosimetry can be used to obtain a pore distribution for the graphite particles 100, which indicates the relationship between the pore diameter and the Log differential pore volume. Next, the peak of the pore distribution of the graphite particles 100 is identified. The diameter at the peak of the pore distribution can be considered as the average pore diameter S. The diameter at the peak of the pore distribution corresponds to the mode diameter of the pores.

[0049] The shape of the graphite particles 100 is not particularly limited and may be, for example, spherical or ellipsoidal. Spherical or ellipsoidal graphite particles 100 have few protrusions protruding from the particle surface. Therefore, a coating liquid containing such graphite particles 100 tends to reduce the resistance during coating. This coating liquid makes it easy to produce a negative electrode layer in which the graphite particles 100 are packed at a high density. However, the graphite particles 100 may have protrusions resulting from the plate-like primary particles 101.

[0050] The median diameter of the graphite particles 100 is not particularly limited and is, for example, 300 nm or more and 30 μm or less. Graphite particles 100 with a median diameter of 300 nm or more are easy to handle and suitable for producing the negative electrode active material 1000 and the negative electrode layer 201. Graphite particles 100 with a median diameter of 30 μm or less allow the first solid electrolyte 103 to be easily introduced therein. The median diameter of the graphite particles 100 may be 1 μm or more and 10 μm or less.

[0051] Generally, the term "median diameter" refers to the particle size where the cumulative volume in the volume-based particle size distribution is equal to 50%. The volume-based particle size distribution is measured, for example, by a laser diffraction measurement device.

[0052] The graphite particles 100 containing a plurality of voids 102 can be considered as a porous material. The specific surface area of ​​the graphite particles 100 is not particularly limited, and may be, for example, 5 m 2 / g or more. The specific surface area is 5m 2 / g or more, the inner surface of the graphite particle 100 surrounding the voids 102 can be coated with a sufficient amount of the first solid electrolyte 103. The larger the specific surface area of ​​the graphite particle 100, the greater the area of ​​the inner surface of the graphite particle 100 that can be coated with the first solid electrolyte 103. The specific surface area of ​​the graphite particle 100 can be measured, for example, by mercury intrusion porosimetry. The specific surface area of ​​the graphite particle 100 can also be obtained by converting data on an adsorption isotherm obtained by a gas adsorption method using nitrogen gas using the Brunauer-Emmett-Teller (BET) method.

[0053] The porosity of the graphite particle 100 may be 5% or more. In graphite particles 100 with a porosity of 5% or more, the inner surface of the graphite particle 100 can be coated with a sufficient amount of first solid electrolyte 103. The upper limit of the porosity of the graphite particle 100 is not particularly limited and is, for example, 50%. Graphite particles 100 with a porosity of 50% or less tend to have sufficiently high strength. The porosity of the graphite particle 100 can be measured, for example, by mercury intrusion porosimetry. The porosity of the graphite particle 100 can also be calculated from the volume of pores 102 obtained by gas adsorption using nitrogen gas.

[0054] The shape of the first solid electrolyte 103 is not particularly limited and may be acicular, spherical, oval, or the like. The first solid electrolyte 103 may be particulate. The first solid electrolyte 103 may have the shape of a film that covers the inner surface of the graphite particles 100. In a film-like first solid electrolyte 103, ion conduction tends to be promoted within the plane of the first solid electrolyte 103. The shape of the first solid electrolyte 103 can be identified by observing a cross section of the negative electrode active material 1000 with an electron microscope.

[0055] When first solid electrolyte 103 is in the form of particles, the median diameter of first solid electrolyte 103 may be 1 nm or more and 100 nm or less, or may be 1 nm or more and 70 nm or less.

[0056] The negative electrode active material 1000 may or may not further include a solid electrolyte attached to the outer surfaces of the graphite particles 100. In this specification, the solid electrolyte attached to the outer surfaces of the graphite particles 100 may be referred to as a "second solid electrolyte." The coverage of the outer surfaces of the graphite particles 100 with the second solid electrolyte is not particularly limited and is, for example, 10% or less. This coverage may be 5% or less, 3% or less, or 1% or less.

[0057] The coverage of the outer surfaces of the graphite particles 100 with the second solid electrolyte can be measured by the following method. First, the surface of the negative electrode active material 1000 is observed with a scanning electron microscope. By image processing, the area A1 of the negative electrode active material 1000 and the area A2 of the second solid electrolyte shown in the obtained electron microscope image are calculated. The ratio of area A2 to area A1 can be considered to be the coverage of the outer surfaces of the graphite particles 100 with the second solid electrolyte.

[0058] The second solid electrolyte is usually formed when the first solid electrolyte 103 is introduced into the voids 102 of the graphite particles 100. Therefore, the composition of the second solid electrolyte is, for example, the same as that of the first solid electrolyte 103. The first solid electrolyte 103 may have low crystallinity because it is introduced into the minute voids 102. A solid electrolyte with low crystallinity tends to have lower ionic conductivity than a solid electrolyte with high crystallinity. Therefore, the negative electrode material for preparing the negative electrode layer of the all-solid-state battery may further contain a solid electrolyte having higher ionic conductivity than the first solid electrolyte 103. If the coverage of the outer surface of the graphite particles 100 with the second solid electrolyte is 10% or less, the solid electrolyte having high ionic conductivity in the negative electrode material is likely to come into contact with the outer surface of the graphite particles 100. Therefore, such a negative electrode active material 1000 makes it easy to prepare a negative electrode layer with high ionic conductivity.

[0059] In the negative electrode active material 1000, the ratio P1 of the mass of the first solid electrolyte 103 to the mass of the graphite particles 100 is not particularly limited and may be 0.3 mass% to 20 mass% or less, 0.3 mass% to 10 mass% or less, or 1.0 mass% to 6.0 mass% or less. When the ratio P1 is 0.3 mass% or more, the ion conduction paths in the negative electrode active material 1000 can be sufficiently increased. When the ratio P1 is 20 mass% or less, a decrease in the capacity density of the negative electrode layer 201 can be sufficiently suppressed. Furthermore, in the negative electrode active material 1000, the ratio P2 of the sum of the mass of the first solid electrolyte 103 and the mass of the second solid electrolyte to the mass of the graphite particles 100 can be 0.3 mass% to 20 mass% or less, 0.3 mass% to 10 mass% or less, or 1.0 mass% to 6.0 mass% or less.

[0060] The first solid electrolyte 103 has, for example, lithium ion conductivity. The first solid electrolyte 103 includes, for example, at least one selected from the group consisting of inorganic solid electrolytes and organic solid electrolytes. The first solid electrolyte 103 may include a sulfide solid electrolyte. The sulfide solid electrolyte has excellent reduction stability and is therefore suitable for combination with the graphite particles 100, which are a low-potential negative electrode material.

[0061] The sulfide solid electrolyte contained in the first solid electrolyte 103 may contain lithium, phosphorus, sulfur, and a halogen. The first solid electrolyte 103 is represented by, for example, the following composition formula (1). Li α PS β X γ ...Equation (1)

[0062] In formula (1), α, β, and γ satisfy the relationships 5.5≦α≦6.5, 4.5≦β≦5.5, and 0.5≦γ≦1.5. X includes at least one selected from the group consisting of F, Cl, Br, and I. X may be Cl or Br, or may be Cl. The first solid electrolyte 103 may be Li6PS5X. The solid electrolyte represented by composition formula (1) has, for example, an argyrodite-type crystal structure. That is, the first solid electrolyte 103 may have an argyrodite-type crystal structure. A negative electrode active material 1000 including such a first solid electrolyte 103 tends to have high ionic conductivity.

[0063] Examples of sulfide solid electrolytes other than those represented by the composition formula (1) include Li2S-P2S5, Li2S-SiS2, Li2S-B2S3, Li2S-GeS2, and Li 3.25 Ge 0.25 P 0.75 S4, Li 10 GeP2S 12 These include LiX, LiO, MO q , Li p MO q The element X in "LiX" is at least one element selected from the group consisting of F, Cl, Br, and I. q " and "Li p MO q "The element M is at least one element selected from the group consisting of P, Si, Ge, B, Al, Ga, In, Fe, and Zn. q " and "Li p MO q " p and q in this expression are independent natural numbers.

[0064] The first solid electrolyte 103 may include at least one selected from the group consisting of an oxide solid electrolyte, a polymer solid electrolyte, and a complex hydride solid electrolyte.

[0065] Examples of oxide solid electrolytes include NASICON-type solid electrolytes, such as LiTi2(PO4)3 and its elemental substitution products, (LaLi)TiO3-based perovskite-type solid electrolytes, and Li 14 ZnGeO 16 , Li4SiO4, LiGeO4 and their element-substituted LISICON-type solid electrolytes, Li7La3Zr2O 12 Garnet-type solid electrolytes, such as those substituted with LiN and its element, LiN and its H-substituted compounds, LiPO4 and its N-substituted compounds, and glass or glass ceramics containing a base material containing Li-BO compounds such as LiBO2 and LiBO3 to which a material such as LiSO4 or LiCO3 has been added can be used.

[0066] As the polymer solid electrolyte, for example, a compound of a polymer compound and a lithium salt can be used. The polymer compound may have an ethylene oxide structure. By having an ethylene oxide structure, the polymer compound can contain a large amount of lithium salt, thereby further increasing ionic conductivity. As the lithium salt, LiPF6, LiBF4, LiSbF6, LiAsF6, LiSO3CF3, LiN(SO2CF3)2, LiN(SO2C2F5)2, LiN(SO2CF3)(SO2C4F9), LiC(SO2CF3)3, etc. can be used. As the lithium salt, one type of lithium salt selected from these may be used alone, or a mixture of two or more types of lithium salts selected from these may be used.

[0067] Examples of the complex hydride solid electrolyte that can be used include LiBH4-LiI and LiBH4-P2S5.

[0068] The shape of the negative electrode active material 1000 is not particularly limited and may be, for example, spherical or oval. The shape of the negative electrode active material 1000 may be particulate. When the negative electrode active material 1000 is particulate, the median diameter of the negative electrode active material 1000 is not particularly limited and may be, for example, 300 nm or more and 30 μm or less.

[0069] Next, a method for producing the negative electrode active material 1000 will be described. FIG. 3 is a flowchart showing the method for producing the negative electrode active material 1000. First, in step S11, a solution L containing a first solid electrolyte 103 is prepared. Specific examples of the solution L are described in non-patent documents such as J. Mater. Chem. A, 2019, 7, 558-566. The concentration of the first solid electrolyte 103 in the solution L is not particularly limited and is, for example, 1% by mass or more and 20% by mass or less.

[0070] The above-mentioned non-patent document discloses a method for preparing a sulfide solid electrolyte represented by Li6PS5Br from a solution. Specifically, the non-patent document discloses that the solid electrolyte is prepared by volatilizing and removing the solvent contained in the solution containing the solid electrolyte, followed by heat treatment. After extensive research, the present inventors have found that other solid electrolytes having an argyrodite-type crystal structure can also be synthesized by the method described in the non-patent document. Examples of other solid electrolytes include Li6PS5Cl.

[0071] Next, in step S12, graphite particles 100 having voids 102 therein are brought into contact with solution L. Solution L does not contain, for example, particles of first solid electrolyte 103. Therefore, when graphite particles 100 are brought into contact with solution L, solution L can easily penetrate into minute voids 102 of graphite particles 100. Specifically, solution L easily penetrates into the interior of graphite particles 100 due to capillary action. As a result, solution L is introduced into voids 102. The method for bringing graphite particles 100 into contact with solution L is not particularly limited. For example, graphite particles 100 may be brought into contact with solution L by kneading graphite particles 100 and solution L. When graphite particles 100 are brought into contact with solution L, the ratio of the mass of first solid electrolyte 103 to the total value of the mass of graphite particles 100 and the mass of first solid electrolyte 103 is not particularly limited, and is, for example, more than 0.2 mass % and not more than 20 mass %.

[0072] The method for producing graphite particles 100 having voids 102 therein is not particularly limited. Graphite particles 100 can be produced, for example, by subjecting a plurality of primary particles 101 to a known spheroidizing treatment. As an example, graphite particles 100 can be produced by dispersing a plurality of primary particles 101 in an inert gas flow and causing these particles to collide with each other in the air flow. The spheroidizing treatment can be carried out using a commercially available device.

[0073] Next, in step S13, the solvent contained in the solution L is removed. As a result, the first solid electrolyte 103 is precipitated in the voids 102. The solvent is removed, for example, by volatilizing the solvent. As an example, the solvent of the solution L may be volatilized while kneading the graphite particles 100 and the solution L. The solvent of the solution L that has penetrated the interior of the graphite particles 100 is less likely to volatilize than the solvent of the solution L present outside the graphite particles 100. Therefore, when the solvent contained in the solution L is volatilized, the first solid electrolyte 103 tends to be concentrated in the voids 102 of the graphite particles 100. When the solvent of the solution L is volatilized, the first solid electrolyte 103 is hardly present outside the graphite particles 100, but is supported by the graphite particles 100 in the voids 102. Therefore, this method makes it possible to easily produce an anode active material 1000 that hardly contains the second solid electrolyte attached to the outer surfaces of the graphite particles 100.

[0074] Next, in step S14, the graphite particles 100 may be heat-treated. The conditions for the heat treatment can be set appropriately depending on the composition of the first solid electrolyte 103, etc. The temperature for the heat treatment is not particularly limited and is, for example, 100°C or higher. The time for the heat treatment is not particularly limited and is, for example, 1 hour or longer. The heat treatment may be performed in a reduced pressure atmosphere or a vacuum atmosphere. Heat-treating the graphite particles 100 tends to improve the crystallinity of the first solid electrolyte 103.

[0075] The method for producing the negative electrode active material 1000 is not limited to the flowchart of Fig. 3. For example, the negative electrode active material 1000 may be produced by using a dispersion of the first solid electrolyte 103 instead of the solution L1.

[0076] Next, the anode active material 1000 in the anode layer 201 will be described. When an all-solid-state battery is produced using the anode active material 1000, the anode material containing the anode active material 1000 may be compression-molded. Compression-molding the anode material may cause the anode active material 1000 to deform. The deformation of the anode active material 1000 may reduce the volume of spaces where the first solid electrolyte 103 is not present, resulting in the loss of these spaces. Therefore, in the anode active material 1000 present in the anode layer 201, all of the voids 102 may be filled with the first solid electrolyte 103. FIG. 1 illustrates a state in which the anode active material 1000 has lost the spaces where the first solid electrolyte 103 is not present. In other words, in FIG. 1, all of the voids 102 are filled with the first solid electrolyte 103. However, in the anode active material 1000 in the anode layer 201, not all of the voids 102 may be filled with the first solid electrolyte 103. When the negative electrode material is compression-molded, the pressure applied to the negative electrode material can be appropriately set depending on the composition of the negative electrode material, as long as the negative electrode active material 1000 in the negative electrode material can be adhered to each other without being destroyed. The pressure applied to the negative electrode material is, for example, 1 MPa or more and 10 GPa or less.

[0077] In the negative electrode active material 1000 in the negative electrode layer 201, the shortest diameter of the voids 102 in which the first solid electrolyte 103 is located is, for example, not less than 1 nm and not more than 70 nm.

[0078] The shortest diameter of the voids 102 in the negative electrode active material 1000 in the negative electrode layer 201 can be determined by the following method. First, the negative electrode layer 201 is processed to expose a cross section of the negative electrode layer 201. The processing of the negative electrode layer 201 can be performed using, for example, a cross section polisher (registered trademark). The cross section polisher can form a smooth cross section of the negative electrode layer 201. Next, the cross section of the negative electrode layer 201 is observed with a scanning electron microscope (SEM). This allows an SEM image of the cross section of the negative electrode layer 201 to be obtained.

[0079] Next, the negative electrode active material 1000, graphite particles 100, voids 102, and first solid electrolyte 103 are identified from the obtained SEM image. These may be identified based on the contrast of the image, or may be identified based on the results of elemental analysis such as energy dispersive X-ray analysis (EDS). Next, the center of gravity of the voids 102 is identified from the SEM image. Of the diameters of the voids 102 that pass through the center of gravity, the shortest diameter can be considered to be the shortest diameter of the voids 102.

[0080] The shortest diameter of the voids 102 may be 10 nm or more, or may be 20 nm or more. The shortest diameter of the voids 102 may be 65 nm or less. Furthermore, the average shortest diameter of the voids 102 may be 1 nm or more and 70 nm or less. The average shortest diameter of the voids 102 can be determined by the following method. First, a cross section of the negative electrode layer 201 is observed using an SEM. From the obtained SEM image, the shortest diameters of any number of voids 102 (for example, five voids 102) are calculated. The average of the calculated values ​​is regarded as the average shortest diameter of the voids 102. When multiple voids 102 are displayed in the SEM image, the largest shortest diameter of the respective shortest diameters of the displayed multiple voids 102 may be 1 nm or more and 70 nm or less.

[0081] With respect to the negative electrode active material 1000 in the negative electrode layer 201, the fact that the first solid electrolyte 103 is located in the voids 102 can be confirmed by observing the cross section of the negative electrode layer 201 with an SEM.

[0082] In the negative electrode material in the negative electrode layer 201, a plurality of negative electrode active materials 1000 may be in contact with each other, thereby forming an electron conduction path.

[0083] The negative electrode material may further include a solid electrolyte 105 in addition to the negative electrode active material 1000. In this specification, the solid electrolyte 105 may be referred to as a "third solid electrolyte." The third solid electrolyte 105 may fill spaces between a plurality of negative electrode active materials 1000, for example. The third solid electrolyte 105 may have a particle shape. A large number of particles of the third solid electrolyte 105 may be compressed and bonded to each other, thereby forming an ion conduction path.

[0084] The third solid electrolyte 105 may or may not be in contact with the second solid electrolyte of the negative electrode active material 1000. When the third solid electrolyte 105 is in contact with the second solid electrolyte, ion conduction into the inside of the graphite particle 100 can occur efficiently.

[0085] The third solid electrolyte 105 has, for example, lithium ion conductivity. The third solid electrolyte 105 includes, for example, at least one selected from the group consisting of inorganic solid electrolytes and organic solid electrolytes. The third solid electrolyte 105 may include at least one selected from the group consisting of sulfide solid electrolytes, oxide solid electrolytes, halide solid electrolytes, polymer solid electrolytes, and complex hydride solid electrolytes, or may include a sulfide solid electrolyte. As the sulfide solid electrolyte, oxide solid electrolyte, polymer solid electrolyte, and complex hydride solid electrolyte, those described above for the first solid electrolyte 103 can be used. Specific examples of halide solid electrolytes will be described later for the solid electrolyte layer 202.

[0086] To achieve a good dispersion state, it is desirable that the third solid electrolyte 105 be made of a soft material. In this respect, at least one selected from the group consisting of sulfide solid electrolytes and halide solid electrolytes is suitable as the third solid electrolyte 105.

[0087] The composition of third solid electrolyte 105 may be the same as or different from that of first solid electrolyte 103. As an example, the composition of first solid electrolyte 103 may be adjusted so that first solid electrolyte 103 can be easily introduced into minute voids 102 of graphite particles 100. The composition of third solid electrolyte 105 may be adjusted so that third solid electrolyte 105 has high ionic conductivity.

[0088] The shape of third solid electrolyte 105 is not particularly limited, and may be needle-like, spherical, oval-spherical, scale-like, etc. Third solid electrolyte 105 may also be particulate.

[0089] When the third solid electrolyte 105 is particulate (e.g., spherical), the median diameter of the third solid electrolyte 105 may be 0.3 μm or more and 100 μm or less. When the median diameter is 0.3 μm or more, the number of contact interfaces between the particles of the third solid electrolyte 105 does not increase too much, and an increase in the ionic resistance inside the anode layer 201 can be suppressed. This enables the battery to operate at high power.

[0090] When the median diameter of third solid electrolyte 105 is 100 μm or less, negative electrode active material 1000 and third solid electrolyte 105 tend to be well dispersed in the negative electrode material, which facilitates achieving a high capacity battery.

[0091] The median diameter of the third solid electrolyte 105 may be smaller than the median diameter of the negative electrode active material 1000. This allows the negative electrode active material 1000 and the third solid electrolyte 105 to form a better dispersed state in the negative electrode material.

[0092] The negative electrode material may further contain an active material other than the negative electrode active material 1000. The shape of the other active material is not particularly limited and may be acicular, spherical, oval spherical, etc. The shape of the other active material may be particulate.

[0093] The median diameter of the other active material may be 0.1 μm or more and 100 μm or less.

[0094] When the median diameter of the other active material is 0.1 μm or more, the other active material and the third solid electrolyte 105 tend to form a good dispersion state in the negative electrode material, which results in improved charging characteristics of the battery.

[0095] When the median diameter of the other active material is 100 μm or less, the diffusion rate of lithium within the active material is sufficiently ensured, enabling the battery to operate at high power.

[0096] The median diameter of the other active material may be larger than the median diameter of the third solid electrolyte 105. This allows the active material and the third solid electrolyte 105 to form a good dispersed state.

[0097] The other active materials include materials that have the property of absorbing and releasing metal ions (e.g., lithium ions). Examples of the other active materials that can be used include metal materials, carbon materials, oxides, nitrides, tin compounds, and silicon compounds. The metal materials may be simple metals or alloys. Examples of metal materials include lithium metal and lithium alloys. Examples of carbon materials include natural graphite, coke, partially graphitized carbon, carbon fiber, spherical carbon, artificial graphite, and amorphous carbon. From the viewpoint of capacity density, silicon (Si), tin (Sn), silicon compounds, and tin compounds are preferably used. The other active materials may include a single active material or multiple active materials having different compositions.

[0098] The particles of the negative electrode active material 1000 and the third solid electrolyte 105 may be in contact with each other, as shown in Figure 1. The negative electrode material may include a plurality of particles of the negative electrode active material 1000 and a plurality of particles of the third solid electrolyte 105.

[0099] In the negative electrode material, the content of the third solid electrolyte 105 and the content of the negative electrode active material 1000 may be the same or different.

[0100] When the total amount of the negative electrode material is taken as 100 mass %, the content of the negative electrode active material 1000 may be 40 mass % or more and 90 mass % or less, or 40 mass % or more and 80 mass % or less. By appropriately adjusting the content of the negative electrode active material 1000, the negative electrode active material 1000 and the third solid electrolyte 105 are likely to form a well-dispersed state.

[0101] The negative electrode material may contain only the negative electrode active material 1000 and the third solid electrolyte 105. In other words, the negative electrode material may consist essentially of the negative electrode active material 1000 and the third solid electrolyte 105. This configuration can improve the energy density of the battery. "Containing only the negative electrode active material 1000 and the third solid electrolyte 105" means that, except for unavoidable impurities, no other materials are intentionally included in the negative electrode material.

[0102] The mass ratio "w1:100-w1" between the active material in the negative electrode layer 201 and the third solid electrolyte 105 may satisfy 40≦w1≦90, or 40≦w1≦80. When 40≦w1 is satisfied, the energy density of the solid battery 2000 is sufficiently ensured. Furthermore, when w1≦90 is satisfied, the solid battery 2000 can operate at high output.

[0103] The thickness of the negative electrode layer 201 may be 10 μm or more and 500 μm or less. When the thickness of the negative electrode layer 201 is 10 μm or more, the energy density of the solid battery 2000 is sufficiently ensured. When the thickness of the negative electrode layer 201 is 500 μm or less, the solid battery 2000 can operate at high output.

[0104] The solid electrolyte layer 202 is a layer containing a solid electrolyte.

[0105] For example, an inorganic solid electrolyte having lithium ion conductivity is used as the solid electrolyte contained in the solid electrolyte layer 202. Examples of the inorganic solid electrolyte that can be used include a sulfide solid electrolyte, an oxide solid electrolyte, and a halide solid electrolyte.

[0106] The solid electrolyte contained in the solid electrolyte layer 202 may be a halide solid electrolyte.

[0107] The halide solid electrolyte is represented, for example, by the following composition formula (2). In composition formula (2), α, β, and γ each independently have a value greater than 0. M includes at least one element selected from the group consisting of metal elements and metalloid elements other than Li. X includes at least one element selected from the group consisting of F, Cl, Br, and I.

[0108] Li α M β X γ ...Equation (2)

[0109] Metalloid elements include B, Si, Ge, As, Sb, and Te. Metal elements include all elements in groups 1 to 12 of the periodic table except for hydrogen, and all elements in groups 13 to 16 except for B, Si, Ge, As, Sb, Te, C, N, P, O, S, and Se. In other words, metal elements are a group of elements that can become cations when forming inorganic compounds with halides.

[0110] Examples of halide solid electrolytes that can be used include Li3YX6, Li2MgX4, Li2FeX4, Li(Al,Ga,In)X4, and Li3(Al,Ga,In)X6.

[0111] The above configuration can improve the output density of the solid-state battery 2000. Furthermore, the thermal stability of the solid-state battery 2000 can be improved, and the generation of harmful gases such as hydrogen sulfide can be suppressed.

[0112] In this disclosure, when an element in a formula is expressed as "(Al, Ga, In)", this notation indicates at least one element selected from the group of elements in parentheses. That is, "(Al, Ga, In)" is synonymous with "at least one element selected from the group consisting of Al, Ga, and In". The same applies to other elements. Halide solid electrolytes exhibit excellent ionic conductivity.

[0113] In composition formula (2), M may contain Y (=yttrium). That is, the halide solid electrolyte contained in solid electrolyte layer 202 may contain Y as a metal element.

[0114] The halide solid electrolyte containing Y may be a compound represented by the following composition formula (3).

[0115] Li a M b Y c X6...Formula (3)

[0116] Composition formula (3) satisfies a+mb+3c=6 and c>0. In composition formula (3), M includes at least one element selected from the group consisting of metal elements and metalloid elements other than Li and Y. m is the valence of M. X includes at least one element selected from the group consisting of F, Cl, Br, and I. M includes at least one element selected from the group consisting of Mg, Ca, Sr, Ba, Zn, Sc, Al, Ga, Bi, Zr, Hf, Ti, Sn, Ta, and Nb. Specific examples of Y-containing halide solid electrolytes include Li3YF6, Li3YCl6, Li3YBr6, Li3YI6, Li3YBrCl5, Li3YBr3Cl3, Li3YBr5Cl, Li3YBr5I, Li3YBr3I3, Li3YBrI5, Li3YClI5, Li3YCl3I3, Li3YCl5I, Li3YBr2Cl2I2, Li3YBrCl4I, Li 2.7 Y 1.1 Cl6, Li 2.5 Y 0.5 Zr 0.5 Cl6, Li 2.5 Y 0.3 Zr 0.7 Cl6 and the like can be used.

[0117] According to the above configuration, the output density of the solid state battery 2000 can be further improved.

[0118] The solid electrolyte contained in solid electrolyte layer 202 may include a sulfide solid electrolyte. As the sulfide solid electrolyte, the same as those described above for first solid electrolyte 103 can be used.

[0119] The solid electrolyte contained in the solid electrolyte layer 202 may include at least one selected from the group consisting of an oxide solid electrolyte, a polymer solid electrolyte, and a complex hydride solid electrolyte. As the oxide solid electrolyte, the polymer solid electrolyte, and the complex hydride solid electrolyte, those described above for the first solid electrolyte 103 can be used.

[0120] The solid electrolyte layer 202 may contain only one solid electrolyte selected from the above-mentioned group of solid electrolytes, or may contain two or more solid electrolytes selected from the above-mentioned group of solid electrolytes. The multiple solid electrolytes have different compositions. For example, the solid electrolyte layer 202 may contain a halide solid electrolyte and a sulfide solid electrolyte.

[0121] The thickness of the solid electrolyte layer 202 may be 1 μm or more and 300 μm or less. When the thickness of the solid electrolyte layer 202 is 1 μm or more, the anode layer 201 and the cathode layer 203 are less likely to short-circuit. When the thickness of the solid electrolyte layer 202 is 300 μm or less, the solid battery 2000 can operate at high output.

[0122] The positive electrode layer 203 contributes to the operation of the solid-state battery 2000 as a counter electrode to the negative electrode layer 201 .

[0123] The positive electrode layer 203 may include a material having the property of absorbing and releasing metal ions (e.g., lithium ions), such as a positive electrode active material. Examples of the positive electrode active material that can be used include metal composite oxides, transition metal fluorides, polyanionic materials, fluorinated polyanionic materials, transition metal sulfides, transition metal oxysulfides, and transition metal oxynitrides. In particular, using a lithium-containing transition metal oxide as the positive electrode active material can reduce manufacturing costs and increase the average discharge voltage.

[0124] The metal composite oxide selected as the positive electrode active material contained in the positive electrode layer 203 may contain Li and at least one element selected from the group consisting of Mn, Co, Ni, and Al. Examples of such materials include Li(NiCoAl)O2, Li(NiCoMn)O2, and LiCoO2. For example, the positive electrode active material may be Li(NiCoMn)O2.

[0125] The positive electrode layer 203 may contain a solid electrolyte. The above configuration increases the lithium ion conductivity inside the positive electrode layer 203, enabling the solid battery 2000 to operate at high power. The solid electrolyte in the positive electrode layer 203 may be any of the materials exemplified as the solid electrolyte contained in the solid electrolyte layer 202.

[0126] The median diameter of the active material particles contained in the positive electrode layer 203 may be 0.1 μm or more and 100 μm or less. When the median diameter of the active material particles is 0.1 μm or more, the active material particles and the solid electrolyte can form a well-dispersed state. This improves the charge capacity of the solid battery 2000. When the median diameter of the active material particles is 100 μm or less, the diffusion rate of lithium within the active material particles is sufficiently ensured. This enables the solid battery 2000 to operate at high power.

[0127] The median diameter of the active material particles may be larger than the median diameter of the solid electrolyte particles, thereby achieving a good dispersion state between the active material and the solid electrolyte.

[0128] The mass ratio "w2:100-w2" of the active material to the solid electrolyte contained in the positive electrode layer 203 may satisfy 40≦w2≦90. When 40≦w2 is satisfied, the energy density of the solid battery 2000 is sufficiently ensured. Furthermore, when w2≦90 is satisfied, the solid battery 2000 can operate at high output.

[0129] The thickness of the positive electrode layer 203 may be 10 μm or more and 500 μm or less. When the thickness of the positive electrode layer 203 is 10 μm or more, the energy density of the solid battery 2000 is sufficiently ensured. When the thickness of the positive electrode layer 203 is 500 μm or less, the solid battery 2000 can operate at high output.

[0130] At least one of the negative electrode layer 201, the solid electrolyte layer 202, and the positive electrode layer 203 may contain a binder to improve adhesion between particles. The binder is used, for example, to improve the binding properties of the materials constituting the electrodes. Examples of binders include polyvinylidene fluoride, polytetrafluoroethylene, polyethylene, polypropylene, aramid resin, polyamide, polyimide, polyamideimide, polyacrylonitrile, polyacrylic acid, polymethyl ester of acrylic acid, polyethyl ester of acrylic acid, polyhexyl ester of acrylic acid, polymethacrylic acid, polymethyl ester of methacrylic acid, polyethyl ester of methacrylic acid, polyhexyl ester of methacrylic acid, polyvinyl acetate, polyvinylpyrrolidone, polyether, polyethersulfone, hexafluoropolypropylene, styrene-butadiene rubber, and carboxymethyl cellulose. The binder may be a copolymer of two or more materials selected from tetrafluoroethylene, hexafluoroethylene, hexafluoropropylene, perfluoroalkyl vinyl ether, vinylidene fluoride, chlorotrifluoroethylene, ethylene, propylene, pentafluoropropylene, fluoromethyl vinyl ether, acrylic acid, and hexadiene. Alternatively, a mixture of two or more materials selected from these may be used as the binder.

[0131] At least one of the negative electrode layer 201 and the positive electrode layer 203 may contain a conductive additive to enhance electronic conductivity. Examples of conductive additives that can be used include graphites (natural graphite or artificial graphite), carbon blacks (acetylene black, ketjen black, etc.), conductive fibers (carbon fiber or metal fiber, etc.), metal powders (carbon fluoride, aluminum, etc.), conductive whiskers (zinc oxide, potassium titanate, etc.), conductive metal oxides (titanium oxide, etc.), and conductive polymer compounds (polyaniline, polypyrrole, polythiophene, etc.). Using a carbon conductive additive can reduce costs.

[0132] The solid-state battery 2000 can be configured as a battery of various shapes, such as a coin type, a cylindrical type, a square type, a sheet type, a button type, a flat type, or a laminated type. [Example]

[0133] The present disclosure will be described in detail below using examples and comparative examples, but the present disclosure is not limited to the following examples.

[0134] Example 1 [Preparation of a solution containing sulfide solid electrolyte] Li2S, P2S5, and ultra-dehydrated tetrahydrofuran (THF) were mixed in an argon glove box with an Ar atmosphere at a dew point of -60 °C or less. The molar ratio of Li2S to P2S5 was 3:1. The THF did not contain any stabilizers. The resulting mixture was stirred overnight to obtain a THF suspension containing Li3PS4.

[0135] Next, Li2S and LiCl were dissolved in ultra-dehydrated ethanol (EtOH) to obtain an EtOH solution. The molar ratio of Li2S to LiCl was 1:1. Next, the THF suspension and the EtOH solution were mixed to obtain a THF-EtOH solution containing Li6PS5Cl. In this solution, the molar ratio of Li2S, P2S5, and LiCl used as raw materials was 5:1:2. The concentration of Li6PS5Cl in this solution was 4.5 mass%.

[0136] [Composite of graphite particles and solid electrolyte] Next, spherical graphite particles with internal voids were prepared. The median diameter of the graphite particles was 8 μm. The average void diameter of the graphite particles, as determined by mercury intrusion porosimetry, was 190 nm. Next, in an argon glove box, graphite particles and a THF-EtOH solution containing Li6PS5Cl were weighed in a mass ratio of graphite particles:Li6PS5Cl = 97.5:2.5. These were then mixed in an agate mortar to bring the graphite particles into contact with the THF-EtOH solution. The solvent contained in the THF-EtOH solution was then evaporated while kneading. The resulting composite was then heat-treated at 150°C for 2 hours in a vacuum atmosphere to obtain a negative electrode active material. This negative electrode active material contained Li6PS5Cl as a solid electrolyte.

[0137] [Preparation of sulfide solid electrolyte A for secondary battery production] Li2S and P2S5 were weighed in an argon glove box with an Ar atmosphere and a dew point of -60°C or less. The molar ratio of Li2S to P2S5 was 75:25. These were ground and mixed in a mortar. Next, a planetary ball mill (Fritsch, P-7) was used to mill the mixture at 510 rpm for 10 hours to obtain a glassy solid electrolyte. The glassy solid electrolyte was then heat-treated at 270°C for 2 hours in an inert atmosphere. This resulted in the production of glass-ceramic sulfide solid electrolyte A, Li2S-P2S5.

[0138] [Preparation of positive electrode material B used in the positive electrode layer] In an argon glove box with an Ar atmosphere at a dew point of -60°C or less, the positive electrode active material Li(NiCoMn)O2 (hereinafter referred to as NCM) and sulfide solid electrolyte A were weighed. The mass ratio of NCM to sulfide solid electrolyte A was 85:15. These were mixed in an agate mortar to prepare positive electrode material B.

[0139] [Preparation of anode material C used in the anode layer] The negative electrode active material and sulfide solid electrolyte A were weighed in an argon glove box in an Ar atmosphere with a dew point of −60° C. The mass ratio of the negative electrode active material to the sulfide solid electrolyte A was 85:15. These were mixed in an agate mortar to produce negative electrode material C.

[0140] [Secondary battery production] First, 80 mg of sulfide solid electrolyte A and 20 mg of positive electrode material B were weighed and placed in an insulating outer cylinder. This was then press-molded at a pressure of 720 MPa to produce a positive electrode layer and a solid electrolyte layer.

[0141] Next, 19.5 mg of anode material C was weighed out. Anode material C was placed in an insulating outer cylinder so that it was in contact with the surface of the solid electrolyte layer opposite to the surface in contact with the cathode layer. This was then press-molded at a pressure of 360 MPa to produce a laminate consisting of the anode layer, solid electrolyte layer, and cathode layer.

[0142] Next, stainless steel current collectors were placed on the top and bottom of the laminate, and current collecting leads were attached to the current collectors.

[0143] Finally, the insulating outer cylinder was sealed using an insulating ferrule to isolate the inside of the insulating outer cylinder from the outside atmosphere, thereby producing the solid state battery of Example 1.

[0144] Example 2 A solid-state battery of Example 2 was obtained in the same manner as in Example 1, except that when preparing the negative electrode active material, the graphite particles and the THF-EtOH solution containing Li6PS5Cl were weighed in a mass ratio of graphite particles:Li6PS5Cl = 95.0:5.0.

[0145] Example 3 A solid state battery of Example 3 was obtained by the same method as in Example 1, except that LiBr was used instead of LiCl when preparing the negative electrode active material. In the solid state battery of Example 3, the negative electrode active material contained Li6PS5Br as a solid electrolyte.

[0146] Example 4 A solid-state battery of Example 4 was obtained in the same manner as in Example 1, except that when preparing the negative electrode active material, the graphite particles and the THF-EtOH solution containing Li6PS5Cl were weighed in a mass ratio of graphite particles:Li6PS5Cl = 88.0:12.0.

[0147] Comparative Example 1 A solid-state battery of Comparative Example 1 was obtained in the same manner as in Example 1, except that void-free plate-like graphite particles having a void diameter of 1 nm or more were used when preparing the negative electrode active material. The median diameter of the graphite particles used in Comparative Example 1 was 3 μm.

[0148] Comparative Example 2 A solid-state battery of Comparative Example 2 was obtained in the same manner as in Example 1, except that when preparing the negative electrode active material, a THF suspension containing Li3PS4 was used instead of a THF-EtOH solution containing Li6PS5Cl, and the graphite particles and the THF suspension containing Li3PS4 were weighed in a mass ratio of graphite particles:Li3PS4 = 97.5:2.5.

[0149] Comparative Example 3 A solid state battery of Comparative Example 3 was obtained in the same manner as in Example 1, except that the graphite particles were used as they were as the negative electrode active material without being combined with a solid electrolyte.

[0150] [Observation of particle cross section using SEM] The cross section of the graphite particles used in Example 1 was observed with an SEM (SU-70 manufactured by Hitachi High-Technologies Corporation). FIG. 4 is an SEM image of the cross section of the graphite particles used in Example 1. As can be seen from FIG. 4, the graphite particles were aggregates of plate-like primary particles capable of forming an intercalation compound containing carbon. In the graphite particles, voids existed between multiple primary particles.

[0151] Next, a cross section of the negative electrode active material prepared in Example 1 was observed by SEM. Fig. 5 is an SEM image of the cross section of the negative electrode active material prepared in Example 1. As can be seen from Fig. 5, in the negative electrode active material, precipitates of the solid electrolyte (white portions) were present in the voids inside the graphite particles.

[0152] [Evaluation of Solid-State Batteries of Examples 1 to 4 and Comparative Examples 1 to 3] The cross sections of the negative electrode layers of the solid-state batteries of Examples 1 to 4 and Comparative Examples 1 to 3 were observed by SEM. FIG. 6 is an SEM image of a cross section of the negative electrode active material included in the negative electrode layer of the solid-state battery of Example 1. As can be seen from FIG. 6, solid electrolyte deposits (white areas) were present in the voids inside the graphite particles in the negative electrode active material. Elemental analysis of these deposits was performed by EDS. The deposits contained P, S, and Cl due to Li6PS5Cl.

[0153] For each of the solid-state batteries of Examples 1 to 4 and Comparative Examples 1 to 3, it was determined from SEM images of the cross section of the negative electrode layer whether the solid electrolyte was located in the voids of the graphite particles in the negative electrode active material. The results are shown in Table 1. In Table 1, "Yes" means that the solid electrolyte was located in the voids of the graphite particles. "No" means that the solid electrolyte was not located in the voids of the graphite particles or that no voids existed inside the graphite particles.

[0154] Furthermore, the shortest diameter of the voids in the graphite particles where the solid electrolyte is located was determined from the SEM image of the cross section of the negative electrode layer. The results are shown in Table 1. Note that when multiple voids are displayed in the SEM image, Table 1 shows the largest shortest diameter of each of the multiple voids displayed.

[0155] In Examples 1 to 4, all of the voids in the graphite particles were filled with solid electrolyte, so the shortest diameter of the voids in Examples 1 to 4 can also be considered as the shortest diameter of the solid electrolyte located in the voids.

[0156] The negative electrode layers of the solid-state batteries of Examples 1 to 4 and Comparative Examples 1 to 3 were subjected to elemental analysis using EDS to determine whether the solid electrolyte used in preparing the negative electrode active material was present outside the negative electrode active material. For example, in Examples 1 to 4 and Comparative Example 1, it was determined whether Cl or Br derived from the solid electrolyte used in preparing the negative electrode active material was present outside the negative electrode active material. The results are shown in Table 1.

[0157] A charging test was carried out on each of the solid state batteries of Examples 1 to 4 and Comparative Examples 1 to 3 under the following conditions.

[0158] First, the solid-state battery was placed in a thermostatic chamber at 25°C. Constant-current charging was performed on the solid-state battery while pressurizing it at 150 MPa using a pressure jig. Constant-current charging was performed at a rate of 0.05C, 0.7C, or 1C (1-hour rate) based on the theoretical capacity of the solid-state battery. Based on the results obtained, the ratio of the battery's charge capacity at a 1C rate to the battery's charge capacity at a 0.05C rate was calculated. Furthermore, we checked whether potential disturbance occurred during constant-current charging at each rate. The results are shown in Table 1. In Table 1, "Yes" indicates that wavy potential fluctuations with an amplitude of 0.02 V or more were observed during constant-current charging. "No" indicates that the above-mentioned potential fluctuations were not observed.

[0159] [Table 1]

[0160] In the negative electrode active materials of the solid-state batteries of Examples 1 to 4, the solid electrolyte was located in the voids of the graphite particles. In particular, in the negative electrode active materials of the solid-state batteries of Examples 1 to 4, solid electrolyte particles having a shortest diameter of 70 nm or less were present in the voids of the graphite particles. Furthermore, in Examples 1 to 3, the solid electrolyte used in preparing the negative electrode active material was not present outside the negative electrode active material. This result indicates that in Examples 1 to 3, the sulfide solid electrolyte A in the negative electrode layer was in sufficient contact with the graphite particles of the negative electrode active material.

[0161] In Comparative Example 1, the graphite particles did not have voids, so the solid electrolyte was not present inside the graphite particles. In Comparative Example 1, the solid electrolyte used to prepare the negative electrode active material was precipitated on the outer surfaces of the graphite particles.

[0162] In Comparative Example 2, when the negative electrode active material was prepared, Li3PS4 was present as a solid in the THF suspension, and therefore, Li3PS4 was not introduced into the voids of the graphite particles, and a solid electrolyte was not formed in the voids of the graphite particles.

[0163] Furthermore, in Comparative Examples 2 and 3, the voids in the graphite particles disappeared due to deformation of the negative electrode active material during the preparation of the negative electrode layer, making it impossible to measure the shortest diameter of the voids in Comparative Examples 2 and 3.

[0164] In the solid-state batteries of Examples 1 to 4, no potential disturbance occurred when charging at a 0.7C rate. In particular, in the solid-state batteries of Examples 1 to 3, no potential disturbance occurred even when charging at a 1C rate. In contrast, in the solid-state batteries of Comparative Examples 1 to 3, no potential disturbance occurred when charging at a 0.05C rate, but potential disturbance occurred when charging at a 0.7C rate. Furthermore, in the solid-state batteries of Examples 1 to 4, the ratio of the battery charge capacity at a 1C rate to the battery charge capacity at a 0.05C rate was higher than in the solid-state batteries of Comparative Examples 1 to 3. Thus, the solid-state batteries of Examples 1 to 4 had superior rate characteristics compared to the solid-state batteries of Comparative Examples 1 to 3.

[0165] It is presumed that in the negative electrode layers of the solid state batteries of Comparative Examples 1 to 3, when the supply rate of lithium ions to the graphite particles was high, lithium ions were not inserted into the graphite particles, and lithium metal was precipitated near the electrode layer. It is presumed that in the negative electrode active materials of the solid state batteries of Examples 1 to 4, the solid electrolyte was located inside the graphite particles, so that lithium ions were easily inserted into the graphite particles.

[0166] The charge capacity ratios in Comparative Examples 1 and 2 were lower than that in Comparative Example 3. The following factors are thought to be responsible for this. First, in Comparative Examples 1 and 2, the ionic conductivity of the solid electrolyte used in preparing the negative electrode active material was lower than that of the solid electrolyte mixed into the negative electrode layer. Furthermore, in Comparative Examples 1 and 2, the solid electrolyte used in preparing the negative electrode active material was precipitated on the outside of the negative electrode active material, not inside the negative electrode active material. In Comparative Examples 1 and 2, it is presumed that the presence of a solid electrolyte with relatively low ionic conductivity around the negative electrode active material reduced the transportability of ions to the negative electrode active material. [Industrial Applicability]

[0167] The solid-state battery of the present disclosure can be used, for example, as an all-solid-state lithium secondary battery.

Claims

1. a negative electrode layer having a negative electrode active material; a positive electrode layer; a solid electrolyte layer located between the positive electrode layer and the negative electrode layer; Equipped with The negative electrode active material is graphite particles which are aggregates of a plurality of primary particles containing graphite and have voids therein; a solid electrolyte located in the void; Including, the solid electrolyte is a precipitate deposited in the voids of the graphite particles and has the form of a film covering the inner surfaces of the voids; At least a portion of the void is filled with the solid electrolyte, The shortest diameter of the voids is 1 nm or more and 70 nm or less. solid state battery.

2. The primary particles are plate-like or scale-like, In the graphite particles, a plurality of the primary particles are stacked. The solid-state battery according to claim 1 .

3. The solid electrolyte comprises lithium, phosphorus, sulfur, and a halogen. The solid-state battery according to claim 1 or 2.

4. The solid electrolyte is represented by the following composition formula (1): Li α PS β X γ ... Equation (1) α, β, and γ satisfy the following relationships: 5.5≦α≦6.5, 4.5≦β≦5.5, and 0.5≦γ≦1.5; X comprises at least one selected from the group consisting of F, Cl, Br and I; The solid-state battery according to claim 1 .

5. The solid electrolyte has an argyrodite-type crystal structure. The solid-state battery according to claim 1 .

6. a ratio of the mass of the solid electrolyte to the mass of the graphite particles is 0.3 mass% or more and 10 mass% or less; The solid-state battery according to claim 1 .

7. The graphite particles have a median diameter of 300 nm or more and 30 μm or less. The solid-state battery according to claim 1 .

8. the negative electrode layer further contains a solid electrolyte having a composition different from the solid electrolyte contained in the negative electrode active material, The solid-state battery according to claim 1 .

9. The solid electrolyte layer contains a solid electrolyte having lithium ion conductivity. The solid-state battery according to claim 1 .

Citation Information

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