WO2025028388A1 - Sintered silicon nitride object - Google Patents
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- C04B35/58—Shaped ceramic products characterised by their composition; Ceramics compositions; Processing powders of inorganic compounds preparatory to the manufacturing of ceramic products based on non-oxide ceramics based on borides, nitrides, i.e. nitrides, oxynitrides, carbonitrides or oxycarbonitrides or silicides
- C04B35/584—Shaped ceramic products characterised by their composition; Ceramics compositions; Processing powders of inorganic compounds preparatory to the manufacturing of ceramic products based on non-oxide ceramics based on borides, nitrides, i.e. nitrides, oxynitrides, carbonitrides or oxycarbonitrides or silicides based on silicon nitride
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- Patent Document 1 discloses a method for producing a silicon nitride sintered body, which comprises preparing silicon nitride powder with an oxygen content of 1.5 mass% or less, filling a sintering mold with the silicon nitride powder, and continuously applying a pulsed direct current with a voltage of 1 V or more but less than 10 V and an output current of 500 A or more and 40,000 A or less to the gaps between the particles of the raw material powder under a pressure of 70 MPa or more, thereby sintering the silicon nitride powder. It also describes that when the silicon nitride sintered body is used as a heat dissipation substrate for a power module, it is possible to efficiently release (dissipate) heat generated from the power module.
- FIG. 2 is a diagram for explaining vacancies in a crystal lattice of silicon nitride.
- FIG. 2 is a diagram for explaining vacancy cluster defects in a silicon nitride crystal lattice.
- 1 is an example of a TEM dark field image of a silicon nitride grain containing a helical dislocation.
- the left and right diagrams in Figure 2 each show a schematic representation of a silicon nitride crystal lattice with the same number of vacancies (five), but when five vacancies are dispersed as in the left diagram, each of the five vacancies is thought to be a phonon scattering source.
- the vacancy cluster defect becomes a single phonon scattering source. Therefore, it is thought that the case on the right diagram, where vacancy cluster defects are formed, has fewer phonon scattering sources and higher thermal conductivity.
- the method for adjusting the value of the crystal lattice distortion is not particularly limited, but it can be adjusted, for example, by the conditions when manufacturing the silicon nitride sintered body, particularly the cooling conditions after sintering.
- the solute oxygen concentration of the silicon nitride crystal grains constituting the silicon nitride sintered body of the present invention is preferably 500 to 2500 ppm, more preferably 1000 to 2500 ppm, and even more preferably 1300 to 2500 ppm.
- the silicon nitride sintered body of the present invention can maintain high thermal conductivity even when the dissolved oxygen concentration is relatively high, which eliminates the need to use high-purity raw materials to adjust the dissolved oxygen concentration to a low level, and also eliminates the need to apply special manufacturing conditions to reduce the dissolved oxygen concentration, thereby contributing to improved productivity.
- the average particle size of the silicon nitride crystal grains constituting the silicon nitride sintered body of the present invention is not particularly limited, but is preferably 1 to 5 ⁇ m, more preferably 2 to 5 ⁇ m, and even more preferably 3 to 5 ⁇ m. If the average particle size of the silicon nitride crystal grains is equal to or larger than these lower limits, the thermal conductivity of the sintered body tends to be high. If the average particle size of the silicon nitride crystal grains is equal to or smaller than these upper limits, the mechanical strength of the sintered body tends to be high.
- the average particle diameter of silicon nitride crystal particles in silicon nitride sintered bodies is a weighted average particle diameter based on a volumetric distribution, and is measured as follows. That is, a cross section of the silicon nitride sintered body is observed with a scanning electron microscope (SEM), and 300 or more particle images are analyzed with an image analyzer to determine the area circle equivalent diameter of each particle. Then, a weighted average particle diameter based on the volumetric distribution of the area circle equivalent diameters is calculated.
- SEM scanning electron microscope
- the silicon nitride sintered body of the present invention can be obtained by firing silicon nitride powder, and preferably by firing a mixed raw material containing silicon nitride powder and a sintering aid.
- the average particle size of the silicon nitride powder contained in the mixed raw material is not particularly limited, but from the viewpoint of setting the average particle size of the silicon nitride crystal particles in the silicon nitride sintered body in the desired range described above, it is preferably 0.5 to 3 ⁇ m, more preferably 0.5 to 2 ⁇ m.
- the average particle size of the silicon nitride powder can be measured by a laser diffraction/scattering particle size distribution measuring device, and a volume frequency distribution curve is obtained with the horizontal axis representing particle size ( ⁇ m) and the vertical axis representing volume frequency.
- the average particle size of the silicon nitride powder means the particle size (D50) at which the cumulative curve of the measured volume-based particle size distribution becomes 50%.
- Silicon nitride powder can be manufactured by known methods. Examples of methods for manufacturing silicon nitride powder include the reduction nitridation method, in which silica powder is used as the raw material and nitrogen gas is passed through in the presence of carbon powder to produce silicon nitride, the direct nitridation method, in which silicon powder is reacted with nitrogen at high temperatures, and the imide decomposition method, in which silicon halide is reacted with ammonia. Silicon nitride powder can also be manufactured by the combustion synthesis method, which is a direct nitridation method that utilizes self-combustion. The combustion synthesis method allows for stable production of silicon nitride powder without incurring energy costs.
- the reduction nitridation method in which silica powder is used as the raw material and nitrogen gas is passed through in the presence of carbon powder to produce silicon nitride
- the direct nitridation method in which silicon powder is reacted with nitrogen at high temperatures
- the imide decomposition method in which silicon
- the sintering aid As the sintering aid, it is preferable to use a metal oxide. By using a metal oxide as a sintering aid, the sintering of the silicon nitride powder is facilitated, and a denser and stronger sintered body is easily obtained.
- the metal oxide include yttria (Y 2 O 3 ), ceria (CeO), and magnesia (MgO). Among these, yttria is preferable.
- the metal oxide may be used alone or in combination of two or more kinds.
- the content of the sintering aid in the mixed raw material is preferably 3 to 12 parts by mass, more preferably 4 to 10 parts by mass, and even more preferably 5 to 8 parts by mass, relative to 100 parts by mass of the silicon nitride powder.
- ⁇ Solution oxygen concentration> The concentration of dissolved oxygen in the silicon nitride crystal grains constituting the silicon nitride sintered body was measured by secondary ion mass spectrometry (SIMS).
- the secondary ion mass spectrometer used was a PHI ADEPT-1010 manufactured by ULVAC-PHI, Inc.
- Cs + was used as the primary ion, and the Cs + beam was focused to about 50 nm and irradiated onto the surface of the sample to generate secondary ions.
- the generated secondary ions were measured through a mass spectrometer to measure the dissolved oxygen concentration.
- the dissolved oxygen concentration was quantified by determining the relative sensitivity factor (RSF) of a standard sample in which 16O was ion-implanted into 30Si .
- RSF relative sensitivity factor
- weighted average particle diameter based on the volume-based distribution of the area circle equivalent diameters was calculated.
- Example 1 To 100 parts by mass of silicon nitride powder, 3 parts by mass of Y2O3 , 1 part by mass of Al2O3 , and 2 parts by mass of MgO were added as sintering aids, and mixed in a planetary ball mill to obtain a mixed raw material. Next, the mixed raw material was used to perform uniaxial press molding and CIP molding to produce a molded body, which was introduced into a sintering furnace and sintered under a nitrogen atmosphere at atmospheric pressure. The sintering was performed under conditions of a maximum temperature of 1760°C and a holding time at the maximum temperature of 10 hours. Then, the material was cooled from the maximum temperature to 1000°C at a cooling rate of 20°C/min.
- Examples 2 to 5 Comparative Examples 1 and 2> A silicon nitride sintered body was produced in the same manner as in Example 1, except that the firing conditions were changed as shown in Table 1. The results of various evaluations of the produced silicon nitride sintered body are shown in Table 1.
- the silicon nitride sintered bodies of the Examples in which the crystal lattice distortion is 0.003 or more, have higher thermal conductivity than the silicon nitride sintered bodies of the Comparative Examples, in which the crystal lattice distortion is less than 0.003.
- the higher the dissolved oxygen concentration the lower the thermal conductivity, but the above-mentioned examples have higher thermal conductivity than the comparative examples, despite the higher dissolved oxygen concentration. From this, it can be said that it is effective to increase the crystal lattice distortion, especially in the region with a high dissolved oxygen concentration.
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Abstract
Description
本発明は、窒化ケイ素焼結体に関する。 The present invention relates to a silicon nitride sintered body.
窒化ケイ素焼結体は、高熱伝導性、高絶縁性、高強度等の優れた特性を有するため、各種工業分野のセラミックス材料として注目されており、例えば車載用や半導体用等のパワーモジュールの放熱基板として使用されている。
放熱基板として使用する際には、発熱による動作不良や部材割れなどを抑制するため基板の熱伝導率を高くする必要がある。そのため、熱伝導率の高い窒化ケイ素焼結体が求められている。
Silicon nitride sintered bodies have attracted attention as ceramic materials in various industrial fields due to their excellent properties such as high thermal conductivity, high insulation properties, and high strength. For example, they are used as heat dissipation substrates for power modules for automobiles and semiconductors.
When used as a heat dissipation substrate, the substrate needs to have high thermal conductivity to prevent malfunctions and component cracking caused by heat generation, so there is a demand for sintered silicon nitride with high thermal conductivity.
例えば、特許文献1では、酸素含有量が1.5質量%以下である窒化ケイ素粉末を用意し、前記窒化ケイ素粉末を焼結型に充填し、70MPa以上の加圧下で、原料粉末の粒子間隙に、電圧1V以上10V未満、出力電流500A以上40,000A以下のパルス状直流電流を連続印加し、前記窒化ケイ素粉末を焼結することを含んでなる、窒化ケイ素焼結体の製造方法が開示されている。そして、窒化ケイ素焼結体を、パワーモジュールの放熱基板として採用した場合、パワーモジュールから発生する熱を効率的に放出(放熱)することができることが記載されている。 For example, Patent Document 1 discloses a method for producing a silicon nitride sintered body, which comprises preparing silicon nitride powder with an oxygen content of 1.5 mass% or less, filling a sintering mold with the silicon nitride powder, and continuously applying a pulsed direct current with a voltage of 1 V or more but less than 10 V and an output current of 500 A or more and 40,000 A or less to the gaps between the particles of the raw material powder under a pressure of 70 MPa or more, thereby sintering the silicon nitride powder. It also describes that when the silicon nitride sintered body is used as a heat dissipation substrate for a power module, it is possible to efficiently release (dissipate) heat generated from the power module.
しかしながら、近年、電子機器や半導体デバイスの高密度化、高出力化に伴い、パワーモジュールの発熱密度が増加している。パワーモジュールの温度上昇は、基板の割れや、素子の動作不良の要因となる。そのため、放熱基板には従来よりも高い放熱性が求められており、放熱基板に用いられる窒化ケイ素焼結体の熱伝導率向上が必要となっている。 However, in recent years, the heat generation density of power modules has increased along with the increasing density and power output of electronic devices and semiconductor devices. Temperature rise in power modules can lead to cracking of the substrate and malfunction of elements. For this reason, heat dissipation substrates are required to have higher heat dissipation properties than before, and there is a need to improve the thermal conductivity of the silicon nitride sintered bodies used in heat dissipation substrates.
そこで本発明の目的は、熱伝導率の高い窒化ケイ素焼結体を提供することである。 The object of the present invention is to provide a silicon nitride sintered body with high thermal conductivity.
本発明者らは、前記目的を達成するために鋭意研究を重ねた。その結果、従来検討がなされてこなかった窒化ケイ素焼結体の結晶格子歪に着目し、該結晶格子歪が0.003以上である窒化ケイ素焼結体により上記課題が解決できることを見出し、本発明を完成させた。 The inventors conducted extensive research to achieve the above-mentioned objective. As a result, they focused on the crystal lattice distortion of silicon nitride sintered bodies, which had not previously been studied, and discovered that the above-mentioned problems could be solved by using silicon nitride sintered bodies with a crystal lattice distortion of 0.003 or more, thus completing the present invention.
本発明の要旨は、以下の[1]~[5]である。
[1]窒化ケイ素焼結体を構成する窒化ケイ素結晶粒子の結晶格子歪が0.003以上であることを特徴とする、窒化ケイ素焼結体。
[2]前記窒化ケイ素結晶粒子の固溶酸素濃度が500~2500ppmである、上記[1]に記載の窒化ケイ素焼結体。
[3]前記結晶格子歪と前記固溶酸素濃度(ppm)が、結晶格子歪/固溶酸素濃度>2.4×10-6を満足する、上記[2]に記載の窒化ケイ素焼結体。
[4]前記窒化ケイ素結晶粒子の平均粒子径が1~5μmである、上記[1]~[3]のいずれかに記載の窒化ケイ素焼結体。
[5]放熱基板である、上記[1]~[4]のいずれかに記載の窒化ケイ素焼結体。
The gist of the present invention is the following [1] to [5].
[1] A silicon nitride sintered body, characterized in that the crystal lattice distortion of silicon nitride crystal grains constituting the silicon nitride sintered body is 0.003 or more.
[2] The silicon nitride sintered body according to the above [1], wherein the silicon nitride crystal grains have a dissolved oxygen concentration of 500 to 2500 ppm.
[3] The silicon nitride sintered body according to the above [2], wherein the crystal lattice distortion and the dissolved oxygen concentration (ppm) satisfy the relationship: crystal lattice distortion/dissolved oxygen concentration>2.4×10 −6 .
[4] The silicon nitride sintered body according to any one of the above [1] to [3], wherein the average particle size of the silicon nitride crystal grains is 1 to 5 μm.
[5] The silicon nitride sintered body according to any one of the above [1] to [4], which is a heat dissipation substrate.
本発明によれば、熱伝導率が高い窒化ケイ素焼結体を提供することができる。 The present invention provides a silicon nitride sintered body with high thermal conductivity.
[窒化ケイ素焼結体]
以下、本発明の窒化ケイ素焼結体について詳細に説明する。
[Sintered silicon nitride]
The silicon nitride sintered body of the present invention will be described in detail below.
<結晶格子歪>
本発明の窒化ケイ素焼結体は、該窒化ケイ素焼結体を構成する窒化ケイ素結晶粒子の結晶格子歪が0.003以上である。結晶格子歪が0.003以上であると、後述する固溶酸素濃度が同じ場合、窒化ケイ素焼結体の熱伝導率が高くなる。熱伝導率をより高める観点から、窒化ケイ素結晶粒子の結晶格子歪は、好ましくは0.0035以上であり、より好ましくは0.004以上であり、さらに好ましくは0.005以上であり、さらに好ましくは0.006以上である。
窒化ケイ素焼結体を構成する窒化ケイ素結晶粒子の結晶格子歪の上限値は特に限定されないが、結晶格子歪は好ましくは0.01以下である。窒化ケイ素結晶粒子の結晶格子歪は、X線回折により測定できる。測定方法の詳細は、実施例において説明する。
<Crystal lattice distortion>
The silicon nitride sintered body of the present invention has a crystal lattice distortion of 0.003 or more in the silicon nitride crystal grains constituting the silicon nitride sintered body. When the crystal lattice distortion is 0.003 or more, the thermal conductivity of the silicon nitride sintered body is high when the solid solution oxygen concentration described later is the same. From the viewpoint of further increasing the thermal conductivity, the crystal lattice distortion of the silicon nitride crystal grains is preferably 0.0035 or more, more preferably 0.004 or more, even more preferably 0.005 or more, and even more preferably 0.006 or more.
The upper limit of the crystal lattice distortion of the silicon nitride crystal grains constituting the silicon nitride sintered body is not particularly limited, but the crystal lattice distortion is preferably 0.01 or less. The crystal lattice distortion of the silicon nitride crystal grains can be measured by X-ray diffraction. Details of the measurement method will be described in the examples.
窒化ケイ素結晶粒子の結晶格子歪を一定以上とすることにより、窒化ケイ素焼結体の熱伝導率が向上する理由については、以下のとおり推定される。
窒化ケイ素焼結体を構成する窒化ケイ素結晶粒子の結晶格子歪は、固溶酸素により形成される空孔が関係している。
窒化ケイ素焼結体を構成している窒化ケイ素結晶(Si3N4)には、原料の種類や製造方法などに起因して混入される、固溶酸素が存在することが知られている。酸素原子(O)が、窒化ケイ素結晶を構成している窒素原子(N)と置換固溶すると、電気的中性を満たすようにケイ素原子(Si)の空孔が生成する。
例えば図1には、窒化ケイ素の結晶格子において、4つの酸素原子が、4つの窒素原子と置換して、1つのケイ素原子が抜けて、空孔が生成している図を示している。
空孔が生成すると、これが格子振動(フォノン)の散乱源となり、熱伝導率が低下する原因となる。したがって、一般的には、窒化ケイ素焼結体中の固溶酸素の量が多いほどフォノン散乱源が多く、熱伝導率が低下する傾向がある。
The reason why the thermal conductivity of the silicon nitride sintered body is improved by setting the crystal lattice distortion of silicon nitride crystal grains to a certain level or more is presumed to be as follows.
The crystal lattice distortion of silicon nitride crystal grains constituting the silicon nitride sintered body is related to vacancies formed by dissolved oxygen.
It is known that silicon nitride crystals (Si 3 N 4 ) constituting silicon nitride sintered bodies contain dissolved oxygen due to the type of raw material, manufacturing method, etc. When oxygen atoms (O) dissolve in the silicon nitride crystals by substitution with nitrogen atoms (N), silicon atom (Si) vacancies are generated to satisfy electrical neutrality.
For example, FIG. 1 shows a diagram of a silicon nitride crystal lattice in which four oxygen atoms are substituted for four nitrogen atoms, and one silicon atom is removed to create a vacancy.
When vacancies are generated, they become a scattering source of lattice vibrations (phonons), which causes a decrease in thermal conductivity. Therefore, generally, the more dissolved oxygen there is in a silicon nitride sintered body, the more phonon scattering sources there are, and the lower the thermal conductivity tends to be.
一方で、窒化ケイ素焼結体において固溶酸素濃度が同程度の場合、焼結体内の空孔の分布の違いによっても、熱伝導率が変わると考えられる。すなわち、固溶酸素の量が同程度の場合、生成する空孔の数も同程度になると考えられるが、空孔が個別に分散して存在する場合と、いくつかの空孔が集合して空孔集合体欠陥を形成している場合とでは、後者の方が、フォノン散乱源が少なくなり、熱伝導率が高いと考えられる。 On the other hand, when the dissolved oxygen concentration in silicon nitride sintered bodies is about the same, it is thought that the thermal conductivity will also change depending on the distribution of vacancies within the sintered body. In other words, when the amount of dissolved oxygen is about the same, it is thought that the number of vacancies generated will also be about the same, but when the vacancies are individually dispersed and exist, compared to when several vacancies gather together to form vacancy cluster defects, the latter is thought to have fewer phonon scattering sources and therefore a higher thermal conductivity.
例えば、図2の左図と右図に、それぞれ空孔の数が同数(5個)の窒化ケイ素の結晶格子を模式的に示しているが、左図のように5つの空孔が分散して存在する場合は、5つの空孔がそれぞれフォノン散乱源になると考えられる。一方で、右図のようにいくつかの空孔が集合してAで示すように、空孔集合体欠陥を形成すると、その空孔集合体欠陥が1つのフォノン散乱源となる。そのため、空孔集合体欠陥を形成している右図の場合のほうが、フォノン散乱源が少なく熱伝導率が高いと考えられる。
空孔集合体欠陥の近傍は、結晶格子が歪むため、空孔集合体欠陥が多いと結晶格子歪が大きくなる。そのため、結晶格子歪が一定以上である本発明の窒化ケイ素焼結体は、熱伝導率が高くなると考えられる。
For example, the left and right diagrams in Figure 2 each show a schematic representation of a silicon nitride crystal lattice with the same number of vacancies (five), but when five vacancies are dispersed as in the left diagram, each of the five vacancies is thought to be a phonon scattering source. On the other hand, when several vacancies are aggregated to form a vacancy cluster defect as shown by A in the right diagram, the vacancy cluster defect becomes a single phonon scattering source. Therefore, it is thought that the case on the right diagram, where vacancy cluster defects are formed, has fewer phonon scattering sources and higher thermal conductivity.
Since the crystal lattice is distorted in the vicinity of the vacancy cluster defects, the greater the number of vacancy cluster defects, the greater the crystal lattice distortion. Therefore, it is believed that the silicon nitride sintered body of the present invention, which has a certain level of crystal lattice distortion or more, has high thermal conductivity.
窒化ケイ素焼結体中の空孔集合体欠陥の有無は、透過型電子顕微鏡(TEM)観察によって確認することができる。すなわち、空孔集合体欠陥は、例えば、転位ループやヘリカル転位としてTEMにより観察される。例えば、図3には、ヘリカル転位を含む窒化ケイ素粒子のTEM暗視野像の一例を示す。図3の中央部の窒化ケイ素粒子の内部に、らせん状の白線として、ヘリカル転位が観察されている。 The presence or absence of vacancy cluster defects in sintered silicon nitride can be confirmed by observation with a transmission electron microscope (TEM). That is, vacancy cluster defects are observed by TEM as, for example, dislocation loops or helical dislocations. For example, Figure 3 shows an example of a TEM dark-field image of a silicon nitride particle containing a helical dislocation. Inside the silicon nitride particle in the center of Figure 3, a helical dislocation is observed as a helical white line.
結晶格子歪の値の調整方法は、特に限定されないが、例えば、窒化ケイ素焼結体を製造する際の条件、特に焼成後の冷却条件により調整することができる。 The method for adjusting the value of the crystal lattice distortion is not particularly limited, but it can be adjusted, for example, by the conditions when manufacturing the silicon nitride sintered body, particularly the cooling conditions after sintering.
<固溶酸素>
本発明の窒化ケイ素焼結体を構成する窒化ケイ素結晶粒子の固溶酸素濃度は、特に限定されないが、例えば2500ppm以下である。固溶酸素濃度が2500ppm以下であると、窒化ケイ素焼結体の熱伝導率を高くすることができる。一方で、窒化ケイ素焼結体を構成する窒化ケイ素結晶粒子の固溶酸素濃度は、熱伝導率向上の観点から、低ければ低いほうがよいが、実用的には、100ppm以上である。
上記したとおり、固溶酸素濃度が高い場合は、一般にはSi原子の空孔が多く生成することで、熱伝導率が低下しやすい。一方、固溶酸素濃度が高い場合において、上記した空孔集合体欠陥を多く形成させると、フォノン散乱源が少なくなり、熱伝導率の低下を効果的に抑制することができる。すなわち、本発明においては、固溶酸素濃度がある程度高い場合において、熱伝導率低下を効果的に抑制しやすくなる。そのような観点から、本発明の窒化ケイ素焼結体を構成する窒化ケイ素結晶粒子の固溶酸素濃度は、好ましくは500~2500ppmであり、より好ましくは1000~2500ppmであり、さらに好ましくは1300~2500ppmである。
このように、本発明の窒化ケイ素焼結体は、固溶酸素濃度がある程度高い場合でも、熱伝導率を高く維持することが可能となる。そのため、固溶酸素濃度を低く調整するための高純度の原料を用いる必要がなく、また固溶酸素濃度低減のための特殊な製造条件を適用する必要もないので、生産性の向上にも寄与することとなる。
<Soluted oxygen>
The dissolved oxygen concentration of the silicon nitride crystal grains constituting the silicon nitride sintered body of the present invention is not particularly limited, but is, for example, 2500 ppm or less. If the dissolved oxygen concentration is 2500 ppm or less, the thermal conductivity of the silicon nitride sintered body can be increased. On the other hand, the dissolved oxygen concentration of the silicon nitride crystal grains constituting the silicon nitride sintered body is preferably as low as possible from the viewpoint of improving thermal conductivity, but is practically 100 ppm or more.
As described above, when the solute oxygen concentration is high, generally, many vacancies of Si atoms are generated, and the thermal conductivity is likely to decrease. On the other hand, when the solute oxygen concentration is high, if many vacancy aggregate defects are formed, the number of phonon scattering sources decreases, and the decrease in thermal conductivity can be effectively suppressed. That is, in the present invention, when the solute oxygen concentration is relatively high, the decrease in thermal conductivity can be effectively suppressed. From such a viewpoint, the solute oxygen concentration of the silicon nitride crystal grains constituting the silicon nitride sintered body of the present invention is preferably 500 to 2500 ppm, more preferably 1000 to 2500 ppm, and even more preferably 1300 to 2500 ppm.
Thus, the silicon nitride sintered body of the present invention can maintain high thermal conductivity even when the dissolved oxygen concentration is relatively high, which eliminates the need to use high-purity raw materials to adjust the dissolved oxygen concentration to a low level, and also eliminates the need to apply special manufacturing conditions to reduce the dissolved oxygen concentration, thereby contributing to improved productivity.
本発明において、結晶格子歪と固溶酸素濃度(ppm)が、結晶格子歪/固溶酸素濃度>2.4×10-6を満足することが好ましい。結晶格子歪/固溶酸素濃度が2.4×10-6超であると、固溶酸素濃度が同じ場合に、結晶格子歪が大きいことから、焼結体の熱伝導率が向上しやすくなる。このような観点から、結晶格子歪/固溶酸素濃度は2.5×10-6以上であることがより好ましく、3.0×10-6以上であることがさらに好ましい。 In the present invention, it is preferable that the crystal lattice distortion and the dissolved oxygen concentration (ppm) satisfy the following: crystal lattice distortion/dissolved oxygen concentration>2.4× 10-6 . If the crystal lattice distortion/dissolved oxygen concentration exceeds 2.4× 10-6 , the crystal lattice distortion is large when the dissolved oxygen concentration is the same, and the thermal conductivity of the sintered body is likely to be improved. From this viewpoint, the crystal lattice distortion/dissolved oxygen concentration is more preferably 2.5× 10-6 or more, and even more preferably 3.0× 10-6 or more.
本発明における固溶酸素濃度は、窒化ケイ素焼結体の内部に固溶された酸素(内部酸素)の濃度を意味し、焼結体表面に不可避的に存在する吸着酸素(外部酸素)は含まない。
固溶酸素濃度は、窒化ケイ素粉末を製造するための各種原料、焼結体を製造する際に用いる焼結助剤の種類及び量、焼成条件などにより調整することができる。
なお、固溶酸素濃度は、実施例に記載の方法で測定することができる。
The dissolved oxygen concentration in the present invention means the concentration of oxygen dissolved inside the silicon nitride sintered body (internal oxygen), and does not include adsorbed oxygen (external oxygen) that is inevitably present on the surface of the sintered body.
The dissolved oxygen concentration can be adjusted by various raw materials used to produce the silicon nitride powder, the type and amount of sintering aid used in producing the sintered body, sintering conditions, and the like.
The dissolved oxygen concentration can be measured by the method described in the Examples.
<平均粒子径>
本発明の窒化ケイ素焼結体を構成する窒化ケイ素結晶粒子の平均粒子径は、特に限定されないが、好ましくは1~5μmであり、より好ましくは2~5μmであり、さらに好ましくは3~5μmである。
窒化ケイ素結晶粒子の平均粒子径がこれら下限値以上であると、焼結体の熱伝導率が高くなる傾向がある。窒化ケイ素結晶粒子の平均粒子径がこれら上限値以下であると、焼結体の機械的強度が高くなる傾向がある。
<Average particle size>
The average particle size of the silicon nitride crystal grains constituting the silicon nitride sintered body of the present invention is not particularly limited, but is preferably 1 to 5 μm, more preferably 2 to 5 μm, and even more preferably 3 to 5 μm.
If the average particle size of the silicon nitride crystal grains is equal to or larger than these lower limits, the thermal conductivity of the sintered body tends to be high.If the average particle size of the silicon nitride crystal grains is equal to or smaller than these upper limits, the mechanical strength of the sintered body tends to be high.
窒化ケイ素焼結体における窒化ケイ素結晶粒子の平均粒子径は、体積基準の分布に基づく重み付き平均粒子径であり、次のように測定される。すなわち、窒化ケイ素焼結体の断面を走査型電子顕微鏡(SEM)により観察し、300個以上の粒子像を、画像解析装置にて画像解析し、それぞれの粒子の面積円相当径を求める。そして、前記面積円相当径の体積基準の分布に基づく重み付き平均粒子径を算出する。 The average particle diameter of silicon nitride crystal particles in silicon nitride sintered bodies is a weighted average particle diameter based on a volumetric distribution, and is measured as follows. That is, a cross section of the silicon nitride sintered body is observed with a scanning electron microscope (SEM), and 300 or more particle images are analyzed with an image analyzer to determine the area circle equivalent diameter of each particle. Then, a weighted average particle diameter based on the volumetric distribution of the area circle equivalent diameters is calculated.
<熱伝導率>
本発明の窒化ケイ素焼結体の熱伝導率は、放熱基板として用いた際の放熱性を向上させる観点などから、好ましくは85W/(m・K)以上であり、より好ましくは90W/(m・K)以上である。熱伝導率は、高ければ高いほどよいが、例えば150W/(m・K)以下であり、実用的には100W/(m・K)以下である。なお、熱伝導率は、実施例に記載の方法により測定できる。
<Thermal Conductivity>
The thermal conductivity of the silicon nitride sintered body of the present invention is preferably 85 W/(m·K) or more, more preferably 90 W/(m·K) or more, from the viewpoint of improving heat dissipation when used as a heat dissipation substrate. The higher the thermal conductivity, the better, but it is, for example, 150 W/(m·K) or less, and practically 100 W/(m·K) or less. The thermal conductivity can be measured by the method described in the examples.
[窒化ケイ素焼結体の製造方法]
本発明の窒化ケイ素焼結体は、窒化ケイ素粉末を焼成して得られることができ、好ましくは窒化ケイ素粉末及び焼結助剤を含有する混合原料を焼成して得ることができる。
[Method for producing sintered silicon nitride]
The silicon nitride sintered body of the present invention can be obtained by firing silicon nitride powder, and preferably by firing a mixed raw material containing silicon nitride powder and a sintering aid.
(窒化ケイ素粉末)
混合原料に含まれる窒化ケイ素粉末の平均粒子径は、特に限定されるものではないが、窒化ケイ素焼結体における窒化ケイ素結晶粒子の平均粒子径を上記した所望の範囲とする観点から、好ましくは0.5~3μmであり、より好ましくは0.5~2μmである。
窒化ケイ素粉末の平均粒子径は、レーザー回折・散乱法粒度分布測定装置により測定でき、横軸を粒径(μm)、縦軸を体積頻度とする体積頻度分布曲線を得て、測定された体積基準の粒子径分布の累積曲線が50%になる粒子径(D50)を意味することとする。
(Silicon nitride powder)
The average particle size of the silicon nitride powder contained in the mixed raw material is not particularly limited, but from the viewpoint of setting the average particle size of the silicon nitride crystal particles in the silicon nitride sintered body in the desired range described above, it is preferably 0.5 to 3 μm, more preferably 0.5 to 2 μm.
The average particle size of the silicon nitride powder can be measured by a laser diffraction/scattering particle size distribution measuring device, and a volume frequency distribution curve is obtained with the horizontal axis representing particle size (μm) and the vertical axis representing volume frequency. The average particle size of the silicon nitride powder means the particle size (D50) at which the cumulative curve of the measured volume-based particle size distribution becomes 50%.
窒化ケイ素粉末は、公知の方法で製造することができる。窒化ケイ素粉末の製造方法としては、シリカ粉末を原料として、炭素粉末存在下において、窒素ガスを流通させて窒化ケイ素を生成させる還元窒化法、シリコン粉末と窒素とを高温で反応させる直接窒化法、ハロゲン化ケイ素とアンモニアとを反応させるイミド分解法などが挙げられる。また、自己燃焼法を利用する直接窒化法である、燃焼合成法により、窒化ケイ素粉末を製造することもできる。燃焼合成法を利用すると、エネルギーコストをかけずに安定的に窒化ケイ素粉末を生産することができる。 Silicon nitride powder can be manufactured by known methods. Examples of methods for manufacturing silicon nitride powder include the reduction nitridation method, in which silica powder is used as the raw material and nitrogen gas is passed through in the presence of carbon powder to produce silicon nitride, the direct nitridation method, in which silicon powder is reacted with nitrogen at high temperatures, and the imide decomposition method, in which silicon halide is reacted with ammonia. Silicon nitride powder can also be manufactured by the combustion synthesis method, which is a direct nitridation method that utilizes self-combustion. The combustion synthesis method allows for stable production of silicon nitride powder without incurring energy costs.
燃焼合成法は、シリコン粉末を原料として使用し、窒素雰囲気下で原料粉末の一部を強制着火し、原料化合物の自己発熱により窒化ケイ素を合成する方法である。燃焼合成法は、公知の方法であり、例えば、特開2000-264608号公報、国際公開第2019/167879号などを参照することができる。 The combustion synthesis method uses silicon powder as a raw material, forcibly ignites a portion of the raw material powder in a nitrogen atmosphere, and synthesizes silicon nitride through the self-heating of the raw material compound. The combustion synthesis method is a well-known method, and reference can be made to, for example, JP 2000-264608 A and WO 2019/167879 A.
(焼結助剤)
焼結助剤としては、金属酸化物を用いることが好ましい。焼結助剤として、金属酸化物を使用することにより、窒化ケイ素粉末の焼結が進行し易くなり、より緻密で高強度の焼結体が得やすくなる。金属酸化物としては、イットリア(Y2O3)、セリア(CeO)、マグネシア(MgO)などが挙げられる。これらの中でも、イットリアが好ましい。金属酸化物は1種を単独で用いてもよいし、2種以上を併用してもよい。
(Sintering aid)
As the sintering aid, it is preferable to use a metal oxide. By using a metal oxide as a sintering aid, the sintering of the silicon nitride powder is facilitated, and a denser and stronger sintered body is easily obtained. Examples of the metal oxide include yttria (Y 2 O 3 ), ceria (CeO), and magnesia (MgO). Among these, yttria is preferable. The metal oxide may be used alone or in combination of two or more kinds.
混合原料における焼結助剤の含有量(すべての焼結助剤の合計の含有量)は、窒化ケイ素粉末100質量部に対して、好ましくは3~12質量部であり、より好ましくは4~10質量部であり、さらに好ましくは5~8質量部である。
焼結助剤の含有量を上記範囲に調整することで、焼結を進行させつつ、固溶酸素濃度を適切な範囲に調整しやすくなる。また、上記した通り、本発明の窒化ケイ素焼結体は、固溶酸素濃度が高くても、熱伝導率を高く維持できるため、焼結助剤の量を少なくすることも製造コストの観点から有効となる。
The content of the sintering aid in the mixed raw material (the total content of all sintering aids) is preferably 3 to 12 parts by mass, more preferably 4 to 10 parts by mass, and even more preferably 5 to 8 parts by mass, relative to 100 parts by mass of the silicon nitride powder.
By adjusting the content of the sintering aid to the above range, it becomes easy to adjust the dissolved oxygen concentration to an appropriate range while proceeding with sintering. Also, as described above, the silicon nitride sintered body of the present invention can maintain high thermal conductivity even if the dissolved oxygen concentration is high, so that reducing the amount of the sintering aid is also effective from the viewpoint of production costs.
(焼成条件)
本発明の窒化ケイ素焼結体は、上記した窒化ケイ素粉末及び焼結助剤を含む混合粉末を焼成して得ることができる。混合粉末は、プレス成形により成形体とした後、焼成炉内等で焼成するとよい。
上記のプレス成形は、一軸プレス成形が代表的であるが、一軸プレス成形した後にCIP(Cold Isostatic Pressing、冷間静水圧加圧)成形を行う方法が好適に採用される。
(Firing conditions)
The silicon nitride sintered body of the present invention can be obtained by sintering a mixed powder containing the above-mentioned silicon nitride powder and a sintering aid. The mixed powder is preferably press-molded into a molded body, and then sintered in a sintering furnace or the like.
The above press molding is typically uniaxial press molding, but a method in which uniaxial press molding is followed by CIP (Cold Isostatic Pressing) molding is preferably employed.
焼成する際の温度(焼成温度)は、例えば1500~1900℃で行うことができる。焼成時の最高温度は、好ましくは1700~1800℃であり、より好ましは1750~1800℃である。焼成時の温度をこのように高めに設定することで、粒成長が促進され、靭性の高い窒化ケイ素焼結体を得やすくなる。そして、最高温度での保持時間を例えば、3~20時間程度とするとよい。
そして、上記のとおり、最高温度で一定時間保持させ後、冷却する。ここで、最高温度から1000℃までの冷却速度は、好ましくは15~100℃/分であり、より好ましくは20~80℃/分である。このように冷却速度を速く設定することで、窒化ケイ素焼結体の結晶格子歪を大きくしやすくなる。
なお、1000℃から室温付近(例えば、25℃)まで冷却する際の条件は、結晶格子歪の大小にあまり影響を及ぼさないため、適宜設定するとよい。
The firing temperature can be, for example, 1500 to 1900°C. The maximum firing temperature is preferably 1700 to 1800°C, and more preferably 1750 to 1800°C. By setting the firing temperature at such a high level, grain growth is promoted, making it easier to obtain a silicon nitride sintered body with high toughness. The holding time at the maximum temperature should be, for example, about 3 to 20 hours.
As described above, the material is held at the maximum temperature for a certain period of time and then cooled. The cooling rate from the maximum temperature to 1000°C is preferably 15 to 100°C/min, more preferably 20 to 80°C/min. By setting the cooling rate at a high rate in this manner, it becomes easier to increase the crystal lattice distortion of the silicon nitride sintered body.
The conditions for cooling from 1000° C. to near room temperature (for example, 25° C.) do not significantly affect the magnitude of crystal lattice distortion, so may be set appropriately.
また、冷却は圧力(炉内圧力)を減圧にして行うことが好ましく、具体的には、冷却時の圧力は、好ましくは0.005~50kPaであり、より好ましくは0.008~10kPaであり、さらに好ましくは0.01~5kPaである。
冷却時の圧力を上記範囲に調整することで、断熱膨張の効果も加わり、窒化ケイ素焼結体の結晶格子歪を大きくしやすくなる。
窒化ケイ素焼結体の結晶格子歪を大きくする観点から、最高温度から1000℃までの冷却速度と、冷却時の圧力を共に上記した範囲に調整することが特に好ましい。
Moreover, it is preferable to perform the cooling under reduced pressure (furnace pressure). Specifically, the pressure during cooling is preferably 0.005 to 50 kPa, more preferably 0.008 to 10 kPa, and even more preferably 0.01 to 5 kPa.
By adjusting the pressure during cooling to within the above range, the effect of adiabatic expansion is also achieved, making it easier to increase the crystal lattice distortion of the silicon nitride sintered body.
From the viewpoint of increasing the crystal lattice distortion of the silicon nitride sintered body, it is particularly preferable to adjust both the cooling rate from the maximum temperature to 1000° C. and the pressure during cooling within the above-mentioned ranges.
焼成は、不活性ガス雰囲気下で行うことが好ましい。なお、不活性ガス雰囲気としては、窒素雰囲気、アルゴン雰囲気などが挙げられ、窒素雰囲気が好ましい。 The firing is preferably carried out in an inert gas atmosphere. Examples of the inert gas atmosphere include a nitrogen atmosphere and an argon atmosphere, with a nitrogen atmosphere being preferred.
本発明の窒化ケイ素焼結体は、結晶格子歪が大きく、優れた熱伝導性を備える。そのため、本発明の窒化ケイ素焼結体は、各種放熱基板として好適に使用することができる。 The silicon nitride sintered body of the present invention has large crystal lattice distortion and excellent thermal conductivity. Therefore, the silicon nitride sintered body of the present invention can be suitably used as various heat dissipation substrates.
以下、本発明をさらに具体的に説明するため実施例を示すが、本発明はこれらの実施例に限定されるものではない。 The following examples are provided to further explain the present invention, but the present invention is not limited to these examples.
[測定方法]
実施例および比較例における各種物性は、下記の方法により測定した。
[Measurement method]
Various physical properties in the examples and comparative examples were measured by the following methods.
<結晶格子歪>
(i)測定試料の作製
板状の窒化ケイ素焼結体(厚み約0.3mm)について、厚みが約0.2mmになるまで片側の表面を機械研磨し、X線回折測定用の試料とした。ただし、機械研磨の際には、研磨ダメージ層の生成抑制および除去のために、ダイヤモンドスラリーと共にCMP(化学的機械的研磨)用スラリーを同時に使用した。CMP用スラリーの種類は特に限定されないが、本実施例では、アルカリベースのコロイダルシリカ(粒径50nm)スラリーを用いた。
(ii)測定
上記のとおり作製したX線回折測定用の試料について、CuKα線を用いたX線回折(XRD)により次の手順で算定した。2θが15~80°の範囲を0.02°のステップでX線検出器を走査して得られたX線回折パターンより、β相の(101)、(110)、(200)、(201)および(210)面の各々の積分幅を算出し、前記積分幅を下記の式2のWilliamson-Hall式に代入した。なお、積分幅とは、X線回折で得られたピーク波形の面積からピークのバックグラウンドの面積を減じて求めた面積をピーク高さで割った値である。
下記の式2における「2sinθ/λ」をX軸、「βcosθ/λ」をY軸としてプロットし、最小二乗法により得られた直線の傾きより結晶格子歪(η)を算定した。
βcosθ/λ=η×(2sinθ/λ)+(1/Dc) (2)
(β:積分幅(rad)、θ:ブラッグ角度(rad)、η:結晶格子歪、λ:X線波長、Dc:結晶子サイズ(nm))
<Crystal lattice distortion>
(i) Preparation of measurement sample One side of a plate-shaped silicon nitride sintered body (thickness about 0.3 mm) was mechanically polished until the thickness became about 0.2 mm, and used as a sample for X-ray diffraction measurement. However, during mechanical polishing, a CMP (chemical mechanical polishing) slurry was used together with the diamond slurry to suppress and remove the generation of a polishing damage layer. The type of CMP slurry is not particularly limited, but in this embodiment, an alkali-based colloidal silica (particle size 50 nm) slurry was used.
(ii) Measurement The sample for X-ray diffraction measurement prepared as described above was calculated by the following procedure using X-ray diffraction (XRD) using CuKα radiation. From the X-ray diffraction pattern obtained by scanning the range of 2θ from 15 to 80° with an X-ray detector in steps of 0.02°, the integral widths of each of the (101), (110), (200), (201) and (210) planes of the β phase were calculated, and the integral widths were substituted into the Williamson-Hall formula of the following formula 2. The integral width is the value obtained by dividing the area obtained by subtracting the area of the peak background from the area of the peak waveform obtained by X-ray diffraction by the peak height.
The "2 sin θ/λ" in the following formula 2 was plotted on the X-axis and "β cos θ/λ" on the Y-axis, and the crystal lattice distortion (η) was calculated from the slope of the straight line obtained by the least squares method.
βcosθ/λ=η×(2sinθ/λ)+(1/Dc) (2)
(β: integral width (rad), θ: Bragg angle (rad), η: crystal lattice strain, λ: X-ray wavelength, Dc: crystallite size (nm))
<空孔集合体欠陥の有無>
(i)透過型電子顕微鏡(TEM)観察試料の作製
各実施例及び比較例で製造した板状の窒化ケイ素焼結体(厚み約0.3mm)について、厚みが約0.1mmになるまで両表面を機械研磨した後、日本電子社製のイオンスライサ「EM-09100IS」を用いて、6keVのアルゴンイオンを穿孔するまで照射して、TEM観察試料を作製した
(ii)TEM観察
日本電子社製の透過型電子顕微鏡「JEM-2100」を用いて、加速電圧200kV、観察倍率2000倍にて10視野を観察した。
観察した10視野のうち、少なくとも1つの視野において、転位ループ又はヘリカル転位が観察された場合を、「転位ループ、ヘリカル転位を含む粒子が有る」と評価した。観察した10視野のうち、すべての視野において、転位ループ又はヘリカル転位が観察されなかった場合を、「転位ループ、ヘリカル転位を含む粒子が無い」と評価した。
<Presence or absence of vacancy cluster defects>
(i) Preparation of Transmission Electron Microscope (TEM) Observation Samples For the plate-shaped silicon nitride sintered bodies (thickness about 0.3 mm) produced in each Example and Comparative Example, both surfaces were mechanically polished until the thickness was about 0.1 mm, and then 6 keV argon ions were irradiated until perforation was formed using an ion slicer "EM-09100IS" manufactured by JEOL Ltd. to prepare TEM observation samples. (ii) TEM Observation Using a transmission electron microscope "JEM-2100" manufactured by JEOL Ltd., 10 fields of view were observed at an accelerating voltage of 200 kV and an observation magnification of 2000 times.
When dislocation loops or helical dislocations were observed in at least one of the ten visual fields, it was evaluated as "there are particles containing dislocation loops or helical dislocations." When dislocation loops or helical dislocations were not observed in any of the ten visual fields, it was evaluated as "there are no particles containing dislocation loops or helical dislocations."
<固溶酸素濃度>
窒化ケイ素焼結体を構成する窒化ケイ素結晶粒子の固溶酸素濃度は、二次イオン質量分析(SIMS)法により測定した。二次イオン質量分析装置としては、アルバック・ファイ株式会社製「PHI ADEPT-1010」を使用した。
一次イオンとしてCs+を使用し、Cs+ビームを50nm程度まで収束させて、試料表面に照射して、二次イオンを発生させた。発生した二次イオンを、質量分析計を通して測定することで、固溶酸素濃度を測定した。なお、固溶酸素濃度の定量は、30Siに16Oをイオン注入した標準試料の相対感度係数(RSF)を求めて行った。
<Solution oxygen concentration>
The concentration of dissolved oxygen in the silicon nitride crystal grains constituting the silicon nitride sintered body was measured by secondary ion mass spectrometry (SIMS). The secondary ion mass spectrometer used was a PHI ADEPT-1010 manufactured by ULVAC-PHI, Inc.
Cs + was used as the primary ion, and the Cs + beam was focused to about 50 nm and irradiated onto the surface of the sample to generate secondary ions. The generated secondary ions were measured through a mass spectrometer to measure the dissolved oxygen concentration. The dissolved oxygen concentration was quantified by determining the relative sensitivity factor (RSF) of a standard sample in which 16O was ion-implanted into 30Si .
なお、試料表面には、吸着酸素が存在するため、SIMSにより固溶酸素濃度を定量する際には、吸着酸素を除いた試料中の16O/30Si強度比を求めることとなる。吸着酸素の影響を取り除いて、試料中の固溶酸素濃度を算出する方法として、特開2018-24548号公報に記載の方法を参照することができる。 In addition, since adsorbed oxygen exists on the sample surface, when quantifying the dissolved oxygen concentration by SIMS, the 16O / 30Si intensity ratio in the sample excluding the adsorbed oxygen is obtained. As a method for calculating the dissolved oxygen concentration in the sample by removing the influence of the adsorbed oxygen, the method described in JP 2018-24548 A can be referred to.
<窒化ケイ素結晶粒子の平均粒子径>
(i)走査型電子顕微鏡(SEM)観察試料の作製
各実施例及び比較例で製造した板状の窒化ケイ素焼結体の断面を鏡面になるまで機械研磨し、SEM観察試料を作製した。
(ii)SEM観察
日本電子社製の走査型電子顕微鏡「JCM-7000」を用いて、加速電圧15kV、観察倍率5000倍にて、1試料あたり5視野を観察し、300個以上の窒化ケイ素結晶粒子の粒子像を得た。
300個以上の粒子像を、SEM装置に付属の画像解析装置にて画像解析し、それぞれの粒子の面積円相当径を求めた。そして、前記面積円相当径の体積基準の分布に基づく重み付き平均粒子径を算出した。
なお、体積基準の分布に基づく重み付き平均粒子径は、以下の式に基づき計算することができる。
体積基準の分布に基づく重み付き平均粒子径=Σ(面積円相当径^4)/Σ(面積円相当径^3)
<Average particle size of silicon nitride crystal particles>
(i) Preparation of Scanning Electron Microscope (SEM) Observation Samples The cross sections of the plate-like silicon nitride sintered bodies produced in each of the Examples and Comparative Examples were mechanically polished until they had a mirror finish to prepare SEM observation samples.
(ii) SEM Observation Using a scanning electron microscope "JCM-7000" manufactured by JEOL Ltd., 5 visual fields were observed per sample at an acceleration voltage of 15 kV and an observation magnification of 5000 times, and particle images of 300 or more silicon nitride crystal particles were obtained.
The images of 300 or more particles were analyzed by an image analyzer attached to the SEM device to determine the area circle equivalent diameter of each particle. Then, the weighted average particle diameter based on the volume-based distribution of the area circle equivalent diameters was calculated.
The weighted average particle size based on the volume-based distribution can be calculated based on the following formula.
Weighted average particle size based on volume distribution = Σ (area equivalent circle diameter ^ 4) / Σ (area equivalent circle diameter ^ 3)
<熱伝導率>
ネッチ社製の熱伝導性測定器「LFA467」を用いて、レーザーフラッシュ法により、熱伝導率を測定した。
<Thermal Conductivity>
The thermal conductivity was measured by the laser flash method using a thermal conductivity measuring device "LFA467" manufactured by Netzsch.
窒化ケイ素焼結体を製造するための原料として、以下のものを使用した。
<窒化ケイ素粉末>
・窒化ケイ素粉末:燃焼合成法で製造した平均粒子径0.95μmの窒化ケイ素粉末
The following materials were used to manufacture the silicon nitride sintered body.
<Silicon nitride powder>
Silicon nitride powder: Silicon nitride powder with an average particle size of 0.95 μm produced by combustion synthesis.
<焼結助剤>
・金属酸化物:イットリア(Y2O3)、アルミナ(Al2O3)、マグネシア(MgO)
<Sintering aid>
Metal oxides: yttria (Y 2 O 3 ), alumina (Al 2 O 3 ), magnesia (MgO)
<実施例1>
窒化ケイ素粉末100質量部に、焼結助剤としてY2O3を3質量部、Al2O3を1質量部、MgOを2質量部添加して、遊星ボールミルで混合し混合原料を得た。次いで、該混合原料を用いて、一軸プレス成形とCIP成形を行い作製した成形体を焼成炉に導入し、大気圧の窒素雰囲気下で焼成した。焼成は、最高温度1760℃、最高温度での保持時間を10時間とする条件で行った。その後、最高温度から1000℃まで、20℃/minの冷却速度で冷却した。冷却は炉内圧力を1kPaにして行った。次いで、1000℃から室温まで自然冷却し、窒化ケイ素焼結体を得た。
作製した窒化ケイ素焼結体についての各種評価結果を表1に示した。
Example 1
To 100 parts by mass of silicon nitride powder, 3 parts by mass of Y2O3 , 1 part by mass of Al2O3 , and 2 parts by mass of MgO were added as sintering aids, and mixed in a planetary ball mill to obtain a mixed raw material. Next, the mixed raw material was used to perform uniaxial press molding and CIP molding to produce a molded body, which was introduced into a sintering furnace and sintered under a nitrogen atmosphere at atmospheric pressure. The sintering was performed under conditions of a maximum temperature of 1760°C and a holding time at the maximum temperature of 10 hours. Then, the material was cooled from the maximum temperature to 1000°C at a cooling rate of 20°C/min. The cooling was performed with the furnace pressure at 1 kPa. Next, the material was naturally cooled from 1000°C to room temperature to obtain a silicon nitride sintered body.
The results of various evaluations of the produced silicon nitride sintered bodies are shown in Table 1.
<実施例2~5、比較例1~2>
焼成条件を表1のとおり変更した以外は、実施例1と同様にして窒化ケイ素焼結体を作製した。作製した窒化ケイ素焼結体についての各種評価結果を表1に示した。
<Examples 2 to 5, Comparative Examples 1 and 2>
A silicon nitride sintered body was produced in the same manner as in Example 1, except that the firing conditions were changed as shown in Table 1. The results of various evaluations of the produced silicon nitride sintered body are shown in Table 1.
表1に示すように、結晶格子歪が0.003以上である各実施例の窒化ケイ素焼結体は、結晶格子歪が0.003未満である各比較例の窒化ケイ素焼結体と比較して、熱伝導率が高いことが分かる。
一般には、固溶酸素濃度が高いと熱伝導率が低くなる傾向があるが、上記実施例は、比較例と比較して、固溶酸素濃度が高いにもかかわらず、熱伝導率が高い結果となっている。このことから、特に固溶酸素濃度が高い領域において結晶格子歪を大きくすることが有効であると言える。
As shown in Table 1, the silicon nitride sintered bodies of the Examples, in which the crystal lattice distortion is 0.003 or more, have higher thermal conductivity than the silicon nitride sintered bodies of the Comparative Examples, in which the crystal lattice distortion is less than 0.003.
Generally, the higher the dissolved oxygen concentration, the lower the thermal conductivity, but the above-mentioned examples have higher thermal conductivity than the comparative examples, despite the higher dissolved oxygen concentration. From this, it can be said that it is effective to increase the crystal lattice distortion, especially in the region with a high dissolved oxygen concentration.
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| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| WO2025173745A1 (en) * | 2024-02-14 | 2025-08-21 | デンカ株式会社 | Silicon nitride sintered compact and circuit board |
| WO2025173742A1 (en) * | 2024-02-14 | 2025-08-21 | デンカ株式会社 | Silicon nitride sintered body and method for producing same, and circuit board and method for producing same |
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| WO1999011583A1 (en) * | 1997-09-03 | 1999-03-11 | Sumitomo Electric Industries, Ltd. | Silicon nitride sinter having high thermal conductivity and process for preparing the same |
| JP2005255462A (en) * | 2004-03-11 | 2005-09-22 | Hitachi Metals Ltd | Silicon nitride sintered compact, method for manufacturing the same and circuit board using the same |
| JP2018024548A (en) * | 2016-08-09 | 2018-02-15 | 住友電気工業株式会社 | Silicon nitride sintered body and method for producing the same |
| WO2020027077A1 (en) * | 2018-08-03 | 2020-02-06 | 株式会社 東芝 | Silicon nitride sintered body, silicon nitride substrate, and silicon nitride circuit substrate |
| WO2021107021A1 (en) * | 2019-11-28 | 2021-06-03 | 株式会社トクヤマ | Method for manufacturing silicon nitride sintered compact |
| WO2023032982A1 (en) * | 2021-09-03 | 2023-03-09 | 株式会社 東芝 | Highly thermally conductive silicon nitride sintered compact, silicon nitride substrate, silicon nitride circuit board, and semiconductor device |
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2024
- 2024-07-25 WO PCT/JP2024/026601 patent/WO2025028388A1/en active Pending
- 2024-07-26 TW TW113127844A patent/TW202513509A/en unknown
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| WO1999011583A1 (en) * | 1997-09-03 | 1999-03-11 | Sumitomo Electric Industries, Ltd. | Silicon nitride sinter having high thermal conductivity and process for preparing the same |
| JP2005255462A (en) * | 2004-03-11 | 2005-09-22 | Hitachi Metals Ltd | Silicon nitride sintered compact, method for manufacturing the same and circuit board using the same |
| JP2018024548A (en) * | 2016-08-09 | 2018-02-15 | 住友電気工業株式会社 | Silicon nitride sintered body and method for producing the same |
| WO2020027077A1 (en) * | 2018-08-03 | 2020-02-06 | 株式会社 東芝 | Silicon nitride sintered body, silicon nitride substrate, and silicon nitride circuit substrate |
| WO2021107021A1 (en) * | 2019-11-28 | 2021-06-03 | 株式会社トクヤマ | Method for manufacturing silicon nitride sintered compact |
| WO2023032982A1 (en) * | 2021-09-03 | 2023-03-09 | 株式会社 東芝 | Highly thermally conductive silicon nitride sintered compact, silicon nitride substrate, silicon nitride circuit board, and semiconductor device |
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| WO2025173745A1 (en) * | 2024-02-14 | 2025-08-21 | デンカ株式会社 | Silicon nitride sintered compact and circuit board |
| WO2025173742A1 (en) * | 2024-02-14 | 2025-08-21 | デンカ株式会社 | Silicon nitride sintered body and method for producing same, and circuit board and method for producing same |
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