JP2019218527A - Nanoparticle aggregate and production method of the same - Google Patents

Nanoparticle aggregate and production method of the same Download PDF

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JP2019218527A
JP2019218527A JP2018119332A JP2018119332A JP2019218527A JP 2019218527 A JP2019218527 A JP 2019218527A JP 2018119332 A JP2018119332 A JP 2018119332A JP 2018119332 A JP2018119332 A JP 2018119332A JP 2019218527 A JP2019218527 A JP 2019218527A
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crystal
light emitting
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nanoparticles
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JP7072169B2 (en
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拓也 風間
Takuya Kazama
拓也 風間
渉 田村
Wataru Tamura
渉 田村
康之 三宅
Yasuyuki Miyake
康之 三宅
淳司 村松
Junji Muramatsu
淳司 村松
澄志 蟹江
Kiyoshi Kanie
澄志 蟹江
昌史 中谷
Masashi Nakatani
昌史 中谷
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Tohoku University NUC
Stanley Electric Co Ltd
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Stanley Electric Co Ltd
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Abstract

To provide quantum dots having different particle sizes.SOLUTION: A nanoparticle aggregate is provided, in which each nanoparticle includes a light-emitting layer and a barrier layer and one nanoparticle includes a plurality of light-emitting layers having different thicknesses. The light-emitting layer and the barrier layer in the nanoparticle aggregate are made of a nitride semiconductor, and each nanoparticle includes a base crystal formed of a II-VI semiconductor containing Zn.SELECTED DRAWING: Figure 1

Description

本発明は、ナノ粒子と呼ばれる微細固体粒子とその製造方法に関する。   The present invention relates to fine solid particles called nanoparticles and a method for producing the same.

固体粒子のサイズを、マイクロメートル(μm)以下のナノメートル(nm)領域内で小さくしていくと、量子化等と呼ばれる、物質の性質が変わる現象が生じる。例えば、価電子帯と伝導帯との間の禁止帯(バンドギャップ)幅が変化する。量子化を生じるような微細固体半導体粒子を量子ドットと呼ぶ。このような微細固体粒子に関して種々の研究、開発が行われている。   As the size of the solid particles is reduced in the nanometer (nm) region of micrometer (μm) or less, a phenomenon called quantization or the like, which changes the properties of the substance, occurs. For example, the forbidden band (band gap) width between the valence band and the conduction band changes. Fine solid semiconductor particles that cause quantization are called quantum dots. Various researches and developments have been made on such fine solid particles.

半導体材料を含む固体粒子の用途として、蛍光体がある。蛍光体粒子は、高エネルギーの光や粒子線を受けて所定波長の蛍光を発する。非発光再結合の原因となる格子欠陥等は蛍光体の効率を低下するであろう。効率のよい蛍光体を形成するには、結晶性のよい蛍光体粒子を形成することが望ましいであろう。結晶性のよい蛍光体粒子を形成する方法として、液相原料からの蛍光体結晶の成長、下地結晶を用いた蛍光体のエピタキシャル成長、蛍光体結晶を保護する保護層の形成等が考えられる。   As an application of the solid particles containing a semiconductor material, there is a phosphor. The phosphor particles emit high-energy light or particle beams and emit fluorescence of a predetermined wavelength. Lattice defects that cause non-radiative recombination will reduce the efficiency of the phosphor. In order to form an efficient phosphor, it may be desirable to form phosphor particles having good crystallinity. As a method of forming phosphor particles having good crystallinity, growth of a phosphor crystal from a liquid phase material, epitaxial growth of a phosphor using a base crystal, formation of a protective layer for protecting the phosphor crystal, and the like can be considered.

CdSe,CdS,InP,GaP等のコアをZnS,ZnSe等のシェル層で覆ったコアシェル構造の蛍光体粒子が提案されている(例えば特許文献1)。また、III−V族半導体(InGaN)のコアをII−VI族半導体(ZnO,ZnS,ZnSe,ZnTe等)のシェルで覆う構造が提案されている(例えば特許文献2)。   There has been proposed a phosphor particle having a core-shell structure in which a core such as CdSe, CdS, InP, and GaP is covered with a shell layer such as ZnS or ZnSe (for example, Patent Document 1). Further, a structure has been proposed in which a core of a III-V semiconductor (InGaN) is covered with a shell of a II-VI semiconductor (ZnO, ZnS, ZnSe, ZnTe, etc.) (for example, Patent Document 2).

現在、可視光域の蛍光体粒子としてエネルギーギャップの小さいコアにエネルギーギャップの大きいシェルを積層したCdSe/ZnSやInP/ZnS等が利用されている。異なる化合物材料でコアシェル構造を構成した場合、格子不整合(CdSe/ZnS:11.1%、InP/ZnS:7.8%)が生じる。格子不整合は、結晶格子を歪ませ、発光効率や信頼性を低下させる原因となるであろう。   At present, CdSe / ZnS, InP / ZnS, and the like, in which a shell having a large energy gap is laminated on a core having a small energy gap, are used as the phosphor particles in the visible light region. When the core-shell structure is composed of different compound materials, lattice mismatch (CdSe / ZnS: 11.1%, InP / ZnS: 7.8%) occurs. Lattice mismatch will distort the crystal lattice and reduce luminous efficiency and reliability.

混晶組成を選択することにより格子整合を行うことができる。例えば、下地結晶としてZnOS混晶を用い、その上に格子整合するAlGaInN混晶を成長することにより、歪みを低減した量子ドットを形成することが提案されている(例えば特許文献3)。   Lattice matching can be performed by selecting the mixed crystal composition. For example, it has been proposed to form a quantum dot with reduced strain by using a ZnOS mixed crystal as a base crystal and growing a lattice-matched AlGaInN mixed crystal thereon (for example, Patent Document 3).

特開2011−76827号公報JP 2011-76827 A 特開2010−155872号公報(登録4936338号公報)Japanese Patent Application Laid-Open No. 2010-155873 (registered No. 4936338) 特開2016−145972号公報JP-A-2006-145972

量子ドットのサイズを小さくして量子化が生じると、エネルギーギャップが変化して発光波長が変化する。例えば演色性のよい白色光を形成するには、なるべく多くの波長光を含む白色光を用いるのが好ましいであろう。多くの波長光を発光することのできる蛍光体が望まれる。このような場合、積極的に異なる粒子サイズを有する量子ドットが望まれる。   When quantization occurs by reducing the size of the quantum dot, the energy gap changes and the emission wavelength changes. For example, in order to form white light having good color rendering properties, it may be preferable to use white light containing as much wavelength light as possible. A phosphor capable of emitting light of many wavelengths is desired. In such a case, quantum dots having different particle sizes are desired.

実施例によれば、
ナノ粒子の集合体であって、各ナノ粒子が発光層と障壁層とを含み、1つのナノ粒子内に厚さの異なる複数の発光層が含まれるナノ粒子集合体
が提供される。
According to the embodiment,
An aggregate of nanoparticles is provided, wherein each nanoparticle includes a light-emitting layer and a barrier layer, and includes a plurality of light-emitting layers having different thicknesses within one nanoparticle.

図1A,1B,1Cは第1の実施例により1次結晶上に複数の2次結晶をエピタキシャル成長する、ナノ結晶を製造する工程を示す概略側面図であり、図1L、1M,1N、1Oは第2の実施例により予備結晶上に1次結晶を成長し、予備結晶を除去した後1次結晶上に複数の2次結晶をエピタキシャル成長する、ナノ結晶を製造する工程を示す概略側面図である。FIGS. 1A, 1B, and 1C are schematic side views showing a process of manufacturing a nanocrystal by epitaxially growing a plurality of secondary crystals on a primary crystal according to the first embodiment. FIGS. FIG. 9 is a schematic side view showing a process of manufacturing a nanocrystal, in which a primary crystal is grown on a preliminary crystal according to a second embodiment, and after removing the preliminary crystal, a plurality of secondary crystals are epitaxially grown on the primary crystal. . 図2は、ZnO1−x混晶系、Al1−xInN混晶系、InGa1−xN混晶系のエネルギーギャップを格子定数の関数として示すグラフである。FIG. 2 is a graph showing the energy gaps of ZnO x S 1-x mixed crystal system, Al 1-x In x N mixed crystal system, and In x Ga 1-x N mixed crystal system as a function of lattice constant. 図3A,3Bは、液相成長を行う常圧容器、耐圧容器の例を示す側面図、断面図である。3A and 3B are a side view and a cross-sectional view illustrating an example of a normal pressure vessel and a pressure-resistant vessel for performing liquid phase growth. 図4AはInGaN結晶を所定量成長することができる液相原料中に、所定面積以上の成長表面を提供するZnOSナノ粒子を投入して、限られた層数のInGaN層をZnOSナノ粒子上に成長させた場合の、成長し得るInGaN層の層数のZnOSナノ粒子投入量に対する関係を示すグラフ、図4Bは上記と等量のInGaN液相原料中に、所定面積以上の成長表面を提供するInAlNナノ粒子を投入して、限られた層数のInGaN層をInAlNナノ粒子上に成長させた場合の、成長し得るInGaN層の層数のInAlNナノ粒子投入量に対する関係を示すグラフである。FIG. 4A shows that a ZnOS nanoparticle providing a growth surface having a predetermined area or more is put into a liquid phase raw material capable of growing a predetermined amount of InGaN crystal, and a limited number of InGaN layers are formed on the ZnOS nanoparticle. FIG. 4B is a graph showing the relationship between the number of layers of the InGaN layer that can be grown and the amount of ZnOS nanoparticles when grown, and FIG. 4B provides a growth surface having a predetermined area or more in the same amount of the InGaN liquid phase raw material as described above. 9 is a graph showing the relationship between the number of InGaN layers that can be grown and the amount of InAlN nanoparticles charged when InAlN nanoparticles are charged and a limited number of InGaN layers are grown on the InAlN nanoparticles. 図5Aは第1の実施例に従ってZnOSナノ粒子上にInGaN層を成長させ、さらにInAlN障壁層を形成したナノ粒子集合体から得られたホトルミネッセンス発光強度の波長分布を示すグラフ、図5Bは第2の実施例に従ってInAlNナノ粒子上にInGaN層を成長させ、さらにInAlN障壁層を形成したナノ粒子集合体から得られたホトルミネッセンス発光強度の波長分布を示すグラフである。FIG. 5A is a graph showing a wavelength distribution of photoluminescence emission intensity obtained from a nanoparticle aggregate obtained by growing an InGaN layer on ZnOS nanoparticles according to the first embodiment and further forming an InAlN barrier layer, and FIG. 9 is a graph showing a wavelength distribution of photoluminescence emission intensity obtained from a nanoparticle aggregate obtained by growing an InGaN layer on InAlN nanoparticles and further forming an InAlN barrier layer according to Example 2.

11 1次結晶、 12 2次結晶、 13 3次結晶、 15 予備結晶、
16 1次結晶、 17 2次結晶、 26 ポート、 27 シリンジ、
28 温度測定部、 29 ヒータ、 33 温度センサ、 34 ヒータ、
35 撹拌機構、 36,37 吸気口、 38 排気口、 39 フラスコ、
11 primary crystal, 12 secondary crystal, 13 tertiary crystal, 15 preliminary crystal,
16 primary crystal, 17 secondary crystal, 26 port, 27 syringe,
28 temperature measuring unit, 29 heater, 33 temperature sensor, 34 heater,
35 stirrer, 36,37 inlet, 38 outlet, 39 flask,

例えば、基材(シード、種結晶)となるナノ粒子上に発光層を形成し、その表面を発光層からの発光を透過させる保護層で覆う構成を想定する。発光層からの発光を外部に取り出すために、保護層は発光層からの発光を透過させる性質を有する。このような保護層を障壁層とも呼ぶ。基材も発光層からの発光を透過する材料で形成すれば、基材も障壁層と呼べる。   For example, it is assumed that a light emitting layer is formed on nanoparticles serving as a base material (seed, seed crystal), and the surface is covered with a protective layer that transmits light emitted from the light emitting layer. In order to extract light emitted from the light emitting layer to the outside, the protective layer has a property of transmitting light emitted from the light emitting layer. Such a protective layer is also called a barrier layer. If the base material is also formed of a material that transmits light emitted from the light emitting layer, the base material can be called a barrier layer.

図1A〜1Cは、第1の実施例によるナノ粒子の製造方法を概略的に示す側面図である。第1の実施例では、図1Aに示すように、まず結晶成長が比較的容易なZnO0.80.2ナノ結晶11を液相成長で成長する。同一条件で成長したZnO0.80.2ナノ結晶はほぼ同じサイズになる。液相成長したZnOSナノ結晶を1次結晶11と呼ぶ。1次結晶の表面を成長面として、その上に2次結晶を液相成長させる。結晶成長が比較的容易なZnOSは常圧で液相成長できる。ZnOS結晶の上に、格子整合するAlGaInN結晶を成長する場合は、高圧液相成長を行う。 1A to 1C are side views schematically illustrating a method for manufacturing nanoparticles according to a first embodiment. In the first embodiment, as shown in FIG. 1A, first, ZnO 0.8 S 0.2 nanocrystals 11 in which crystal growth is relatively easy are grown by liquid phase growth. ZnO 0.8 S 0.2 nanocrystals grown under the same conditions have almost the same size. The ZnOS nanocrystal grown in the liquid phase is called a primary crystal 11. The surface of the primary crystal is used as a growth surface, and a secondary crystal is grown thereon in a liquid phase. ZnOS, which is relatively easy to grow, can be grown in liquid phase at normal pressure. When growing a lattice-matched AlGaInN crystal on a ZnOS crystal, high-pressure liquid phase growth is performed.

図1Bに示すように、各ZnO0.80.21次結晶11表面上によりサイズの小さいIn0.5Ga0.5Nナノ結晶を複数個成長する。1次結晶11表面上に成長した複数のナノ結晶を2次結晶12と呼ぶ。 As shown in FIG. 1B, a plurality of smaller In 0.5 Ga 0.5 N nanocrystals are grown on the surface of each ZnO 0.8 S 0.2 primary crystal 11. A plurality of nanocrystals grown on the surface of the primary crystal 11 are called secondary crystals 12.

図2は、ZnOS混晶系、AlInN混晶系、InGaN混晶系の格子定数とエネルギーギャップの関係を示すグラフである。「混晶系」は、両端物質と中間の混晶を含む系を表す用語である。横軸がÅ(オングストローム、A)(=1nm/10)を単位とする格子定数を示し、縦軸がeV(エレクトロンボルト)を単位とするエネルギーギャップを示す。発光波長を決定するエネルギーギャップは、ZnO:3.2eV、ZnS:3.8eV、AlN:6.2eV、GaN:3.4eV、InN:0.64eVである。ZnO0.80.2の格子定数は3.37A(0.0337nm)、In0.5Ga0.5Nの格子定数も3.37A(0.0337nm)であり、両者は格子定数が整合する。 FIG. 2 is a graph showing the relationship between the lattice constant and the energy gap of a ZnOS mixed crystal system, an AlInN mixed crystal system, and an InGaN mixed crystal system. “Mixed crystal system” is a term that indicates a system that includes a mixed crystal that is intermediate with both materials. The horizontal axis indicates the lattice constant in units of Å (angstrom, A) (= 1 nm / 10), and the vertical axis indicates the energy gap in units of eV (electron volts). The energy gap that determines the emission wavelength is ZnO: 3.2 eV, ZnS: 3.8 eV, AlN: 6.2 eV, GaN: 3.4 eV, and InN: 0.64 eV. The lattice constant of ZnO 0.8 S 0.2 is 3.37 A (0.0337 nm) and the lattice constant of In 0.5 Ga 0.5 N is 3.37 A (0.0337 nm). Align.

優れた発光機能を有するInGaN結晶を蛍光体粒子の発光層として機能させる。発光層の結晶性が損なわれると、発光効率が低下する可能性がある。発光層を保護するように、発光層の上に保護層を設けることが好ましい。   An InGaN crystal having an excellent light emitting function is caused to function as a light emitting layer of the phosphor particles. When the crystallinity of the light emitting layer is impaired, the luminous efficiency may be reduced. It is preferable to provide a protective layer on the light emitting layer so as to protect the light emitting layer.

図1Cに示すように、In0.5Ga0.5N2次結晶12表面上に保護層となるIn0.6Al0.4Nナノ結晶の3次結晶13を液相成長する。In0.5Ga0.5N発光層の2次結晶と格子整合するように同じ格子定数3.37Aを有するIn0.6Al0.4Nで3次結晶13を形成する。図2から判るように、同じ格子定数の場合、InAlNのエネルギーギャップはInGaNのエネルギーギャップより大きく、InAlNはInGaNからの発光を透過させる。 As shown in FIG. 1C, a tertiary crystal 13 of In 0.6 Al 0.4 N nanocrystals serving as a protective layer is liquid-phase grown on the surface of the In 0.5 Ga 0.5 N secondary crystal 12. The tertiary crystal 13 is formed of In 0.6 Al 0.4 N having the same lattice constant of 3.37 A so as to lattice match with the secondary crystal of the In 0.5 Ga 0.5 N light emitting layer. As can be seen from FIG. 2, for the same lattice constant, the energy gap of InAlN is larger than the energy gap of InGaN, and InAlN transmits light emitted from InGaN.

図2において、同一の格子定数を有する混晶を選択して、下地層とその上にエピタキシャル成長する成長層を形成すれば、格子整合が成立する。歪みを低減することにより、結晶欠陥を低減し、高効率な量子ドットを実現できよう。   In FIG. 2, if a mixed crystal having the same lattice constant is selected and a base layer and a growth layer epitaxially grown thereon are formed, lattice matching is established. By reducing distortion, crystal defects will be reduced, and quantum dots with high efficiency will be realized.

実施例2においては、図1Lに示すように、ZnOSナノ粒子15を予備結晶として常圧で成長する。図1Mに示すように、予備結晶15上にInAlNの1次結晶16を高圧液相成長で成長する。図1Nに示すように、予備結晶15をエッチング等で除去する。残ったInAlNがその上に発光層を成長させる1次結晶16となる。図1Oに示すように、1次結晶16の上に、実施例1同様に、発光層としてInGaN2次結晶17を成長する。さらに、InGaN発光層を覆うInAlN保護層を形成することが好ましい。InAlN1次結晶16、InGaN2次結晶、InAlN保護層は高圧液相成長で成長する。製造されるナノ粒子全体がAlGaInN系材料で形成され、安定で優れた特性が期待できる。   In Example 2, as shown in FIG. 1L, the ZnOS nanoparticles 15 are grown as normal crystals under normal pressure. As shown in FIG. 1M, a primary crystal 16 of InAlN is grown on the preliminary crystal 15 by high-pressure liquid phase growth. As shown in FIG. 1N, the preliminary crystal 15 is removed by etching or the like. The remaining InAlN becomes the primary crystal 16 on which a light emitting layer is grown. As shown in FIG. 10, an InGaN secondary crystal 17 is grown as a light emitting layer on the primary crystal 16 as in the first embodiment. Further, it is preferable to form an InAlN protective layer covering the InGaN light emitting layer. The InAlN primary crystal 16, the InGaN secondary crystal, and the InAlN protective layer are grown by high-pressure liquid phase growth. The entire manufactured nanoparticles are formed of an AlGaInN-based material, and stable and excellent characteristics can be expected.

図3A,3Bを参照して、液相成長に用いる成長容器を簡潔に説明する。図3Aは常圧用成長容器を示す。フラスコ39は、取出し口の他、不活性ガスで置換できるポート26、反応前駆体を注入できるシリンジ27を備える複数の専用ポート、熱電対を取り付けた温度測定部28を備え、マントルヒータ29上に設置される。不活性ガスとしては、例えばアルゴン(Ar)を用いる。   With reference to FIGS. 3A and 3B, a growth vessel used for liquid phase growth will be briefly described. FIG. 3A shows a growth vessel for normal pressure. The flask 39 has, in addition to the outlet, a port 26 that can be replaced with an inert gas, a plurality of dedicated ports provided with a syringe 27 that can inject a reaction precursor, and a temperature measuring unit 28 equipped with a thermocouple. Will be installed. As the inert gas, for example, argon (Ar) is used.

図3Bは耐圧用成長容器を示す。反応容器32は、外側がステンレス、内側がハステロイにより構成される。反応容器32には、少なくとも2つの吸気口36,37と排気口38と、が設けられている。吸気口36,37は、それぞれバルブを介して,たとえばArガス供給源、Nガス供給源に接続されており、吸気口36,37から反応容器32内に、ArガスおよびNガスを供給することができる。また、排気口38は、バルブを介して、排気ポンプが接続されており、反応容器32内の雰囲気(ガス)を排気することができる。各バルブの調整により、反応容器32内における各種ガスの分圧、特にNガスの分圧を、精確に制御することができる。 FIG. 3B shows a pressure growing container. The outside of the reaction vessel 32 is made of stainless steel, and the inside is made of Hastelloy. The reaction vessel 32 is provided with at least two intake ports 36 and 37 and an exhaust port 38. The intake ports 36 and 37 are connected to, for example, an Ar gas supply source and an N 2 gas supply source via valves, respectively, and supply Ar gas and N 2 gas into the reaction vessel 32 from the intake ports 36 and 37. can do. The exhaust port 38 is connected to an exhaust pump via a valve, and can exhaust the atmosphere (gas) in the reaction vessel 32. By adjusting each valve, the partial pressure of various gases in the reaction vessel 32, particularly the partial pressure of N 2 gas, can be accurately controlled.

反応容器32には、温度センサ33、ヒータ34、撹拌機構35等が取り付けられている。温度センサ33は、反応容器32内の収容物の温度を測定することができる。ヒータ34は、収容物を加熱することができる。撹拌機構35(回転羽根)は、収容物を撹拌することができる。試料調整に関する全ての操作は、真空乾燥(140℃)した器具および装置を用いてグローブボックス内で実施することが好ましい。   The reaction container 32 is provided with a temperature sensor 33, a heater 34, a stirring mechanism 35, and the like. The temperature sensor 33 can measure the temperature of the contents in the reaction container 32. The heater 34 can heat the contents. The stirring mechanism 35 (rotary blade) can stir the contents. All operations relating to sample preparation are preferably carried out in a glove box using vacuum-dried (140 ° C.) instruments and equipment.

実施例1,2においては、ZnOS1次結晶上、又はInAlN1次結晶上に、InGaN2次結晶を成長する。1次結晶の表面前面に2次結晶の成長が起こり得ないように、2次結晶の原料の量に対して過剰となる表面を提供する1次結晶を投入する。すなわち、1次結晶の表面前面に2次結晶の成長が生じるとした場合の2次結晶の厚さを1原子層以下とする。成長する2次結晶の面積、厚さが広い範囲に分布するであろう。2次結晶の原料となるIII族材料の量を0.2mmolと設定して、発光層の厚さが1層以下となる、1次結晶の投入量を計算した。   In Examples 1 and 2, an InGaN secondary crystal is grown on a ZnOS primary crystal or an InAlN primary crystal. In order to prevent the secondary crystal from growing on the front surface of the primary crystal, a primary crystal which provides an excessive surface with respect to the amount of the raw material of the secondary crystal is introduced. That is, the thickness of the secondary crystal when the secondary crystal grows on the front surface of the surface of the primary crystal is set to one atomic layer or less. The area and thickness of the growing secondary crystal will be distributed over a wide range. The amount of the group III material used as the raw material of the secondary crystal was set to 0.2 mmol, and the input amount of the primary crystal at which the thickness of the light emitting layer became one layer or less was calculated.

図4Aは、実施例1に従って、ZnOSナノ粒子を1次結晶としてInGaN原料液中に投入する場合を示すグラフである。横軸が1次結晶(ZnOSナノ粒子)投入量を単位(mg)で示し、縦軸が成長するInGaN窒化物層の層数を示す。ZnOSナノ粒子の投入量が85mg以上であれば、成長するInGaN層の層数は1未満となる。   FIG. 4A is a graph showing a case where ZnOS nanoparticles are charged as a primary crystal into an InGaN raw material liquid according to Example 1. The horizontal axis indicates the amount of primary crystal (ZnOS nanoparticle) input in units (mg), and the vertical axis indicates the number of InGaN nitride layers to be grown. If the input amount of ZnOS nanoparticles is 85 mg or more, the number of grown InGaN layers is less than one.

図4Bは、実施例2に従って、InAlNナノ粒子を1次結晶としてInGaN原料液中に投入する場合を示すグラフである。横軸が1次結晶(InAlNナノ粒子)投入量を単位(mg)で示し、縦軸が成長するInGaN窒化物層の層数を示す。InAlNナノ粒子の投入量が65mg以上であれば、成長するInGaN層の層数は1未満となる。   FIG. 4B is a graph showing a case where InAlN nanoparticles are charged as a primary crystal into an InGaN raw material liquid according to Example 2. The horizontal axis indicates the amount of primary crystal (InAlN nanoparticles) charged in units (mg), and the vertical axis indicates the number of InGaN nitride layers to be grown. If the input amount of the InAlN nanoparticles is 65 mg or more, the number of the grown InGaN layers is less than one.

実施例1
工程a. ZnOS結晶(S組成:0.2)の合成
例えば図3Aに示す容器を用い、熱分解法による液相成長でZnOS結晶を作製する。溶媒であるオレイルアミン(10mL)にZn材料の酢酸亜鉛(2.0mmol)、S材料の硫黄(0.4mmol)を添加し、加熱して合成温度130℃で1時間、250℃で1時間、300℃で1時間、N雰囲気下で合成を行った。合成後、トルエンとエタノールにより遠心分離で洗浄し、S組成20% 格子定数a=3.37A、粒子サイズ10nmのZnOS結晶を作製した。ZnOS結晶は以後の工程で下地結晶として用いる。
Example 1
Step a. Synthesis of ZnOS Crystal (S Composition: 0.2) For example, a ZnOS crystal is produced by liquid phase growth by a thermal decomposition method using a container shown in FIG. 3A. Zinc acetate (2.0 mmol) as a Zn material and sulfur (0.4 mmol) as an S material are added to oleylamine (10 mL) as a solvent, and the mixture is heated and heated at a synthesis temperature of 130 ° C. for 1 hour, 250 ° C. for 1 hour, and 300 ° C. The synthesis was performed at a temperature of 1 ° C. for 1 hour under an N 2 atmosphere. After the synthesis, the precipitate was washed by centrifugation with toluene and ethanol to prepare a ZnOS crystal having an S composition of 20%, a lattice constant a of 3.37 A, and a particle size of 10 nm. The ZnOS crystal is used as a base crystal in the subsequent steps.

工程b. ZnOS結晶上にInGaN発光層(Ga組成:0.5)を合成
例えば図3Bに示す高圧容器中に、溶媒ベンゼン(6mL)、In材料としてInI(0.1mmol)、Ga材料としてGaI(0.1mmol)、窒素材料としてNaNH(2.0mmol)、ヘキサデシルアミン(0.2mmol)、ZnOS下地結晶(85mg)を投入し、合成温度300度、1時間でInGaN発光層の合成を行った。合成後、トルエンとエタノールにより遠心分離で洗浄し、ZnOS下地結晶上にInGaN発光層(Ga組成:0.5)を作製した。発光層はZnOS下地結晶全面は覆っておらず、2−5nm程度のサイズでの互いに独立な粒子として存在していた。
Step b. Synthesis of InGaN light emitting layer (Ga composition: 0.5) on ZnOS crystal For example, in a high-pressure container shown in FIG. 3B, a solvent benzene (6 mL), InI 3 (0.1 mmol) as an In material, and GaI 3 (Ga as a Ga material) 0.1 mmol), NaNH 2 (2.0 mmol), hexadecylamine (0.2 mmol), and ZnOS base crystal (85 mg) as a nitrogen material, and an InGaN light emitting layer is synthesized at a synthesis temperature of 300 ° C. for one hour. Was. After the synthesis, the resultant was washed by centrifugation with toluene and ethanol to form an InGaN light emitting layer (Ga composition: 0.5) on the ZnOS base crystal. The light emitting layer did not cover the entire surface of the ZnOS base crystal and existed as independent particles having a size of about 2 to 5 nm.

工程c. 工程bで合成した粒子上へのInAlN障壁層(Al組成:0.4)の合成
高圧容器中に、溶媒ベンゼン(6mL)、In材料としてInI(0.12mmol)、Al材料としてAlI (0.08mmol) 、窒素材料としてNaNH(2.0mmol)、工程bで作成したInGaN発光層付きZnOS結晶(100mg)を投入し、合成温度300℃、1時間で合成を行った。合成後、トルエンとエタノールにより遠心分離で洗浄し、InGaN発光層上にAl組成40% 格子定数a=3.37AのInAlN障壁層を作製した。
Step c. Synthesis of InAlN barrier layer (Al composition: 0.4) on particles synthesized in step b In a high-pressure vessel, solvent benzene (6 mL), InI 3 (0.12 mmol) as an In material, AlI 3 (Al as an Al material) 0.08 mmol), NaNH 2 (2.0 mmol) as a nitrogen material, and ZnOS crystal (100 mg) with an InGaN light-emitting layer created in step b, and synthesis was performed at a synthesis temperature of 300 ° C. for 1 hour. After the synthesis, the resultant was washed by centrifugation with toluene and ethanol to form an InAlN barrier layer having an Al composition of 40% and a lattice constant a of 3.37 A on the InGaN light emitting layer.

図5Aに合成したナノ粒子の発光スペクトルを示す。励起光として365nmを用いた。   FIG. 5A shows the emission spectrum of the synthesized nanoparticles. 365 nm was used as excitation light.

発光スペクトルは広い波長領域に分布している。発光スペクトルは540nm付近にピークを持つ成分と、640nm付近にピークをもつ成分とを含む。540nm付近の成分は厚みが抑制されたm面上の発光層由来、640nm付近の成分はc面上の発光層由来と考えられる。   The emission spectrum is distributed over a wide wavelength range. The emission spectrum includes a component having a peak near 540 nm and a component having a peak near 640 nm. It is considered that the component around 540 nm is derived from the light emitting layer on the m-plane whose thickness is suppressed, and the component around 640 nm is derived from the light emitting layer on the c-plane.

なお、基材はZnOSに限定されるものでなく、発光層のInGaNと同じ格子状数をもつものであればよい。また、基材の合成法や材料も上記に限定されるものではない。   The base material is not limited to ZnOS, and may be any material having the same lattice number as InGaN of the light emitting layer. Further, the synthesis method and material of the base material are not limited to the above.

実施例2
工程a. ZnOS結晶(S組成:0.2)の合成
熱分解法により成長下地用のZnOS結晶を作製する。溶媒オレイルアミン(10mL)にZn材料の酢酸亜鉛(2.0mmol)、S材料の硫黄(0.4mmol)を添加し、合成温度130℃−1時間、250℃−1時間、300℃−1時間、N雰囲気下で合成を行った。合成後、トルエンとエタノールにより遠心分離で洗浄し、S組成20% 格子定数a=3.37A、粒子サイズ10nmのZnOS結晶を作製した。最終的にメタノールを加え、分散液として回収する。
Example 2
Step a. Synthesis of ZnOS Crystal (S Composition: 0.2) A ZnOS crystal for a growth base is prepared by a thermal decomposition method. Zinc acetate (2.0 mmol) as a Zn material and sulfur (0.4 mmol) as a S material were added to the solvent oleylamine (10 mL), and the synthesis temperature was 130 ° C.-1 hour, 250 ° C.-1 hour, 300 ° C.-1 hour, N synthesis was carried out under 2 atmosphere. After the synthesis, the precipitate was washed with toluene and ethanol by centrifugation to prepare a ZnOS crystal having an S composition of 20%, a lattice constant a of 3.37 A, and a particle size of 10 nm. Finally, methanol is added and the mixture is recovered as a dispersion.

工程b. ZnOS結晶上に島状に分離したInAlN障壁層(Al組成:0.4)の合成
高圧容器中に、溶媒ベンゼン(6mL)、In材料としてInI(0.12mmol)、Al材料としてAlI (0.08mmol) 、窒素材料としてNaNH(2.0mmol)、ZnOS結晶(65mg)を投入し、合成温度300℃で3時間で合成を行った。合成後、トルエンとエタノールにより遠心分離で洗浄し、ZnOSシード上に独立したInAlN障壁層(Al組成:0.4)を作製した。
Step b. Synthesis of InAlN barrier layer (Al composition: 0.4) separated into island shape on ZnOS crystal In a high-pressure vessel, solvent benzene (6 mL), InI 3 (0.12 mmol) as In material, AlI 3 (Al material as Al material) 0.08 mmol), NaNH 2 (2.0 mmol) as a nitrogen material, and ZnOS crystal (65 mg) were added, and synthesis was performed at a synthesis temperature of 300 ° C. for 3 hours. After the synthesis, the resultant was washed by centrifugation with toluene and ethanol to form an independent InAlN barrier layer (Al composition: 0.4) on the ZnOS seed.

工程c.ZnOSシードの除去
ZnOS上に作製したInAlN島間の空隙部からZnOS結晶をウェットエッチングにより除去する。エッチング液は、たとえば純水および塩酸(濃度:36容量%)を容量比100:1で混合したもの(希塩酸)を用いる。これにより、ZnOS結晶が除去され、サイズ5nm程度のInAlN障壁層領域(以後ナノ粒子とも呼ぶ)のみが残される。
Step c. Removal of ZnOS seed The ZnOS crystal is removed from the gap between the InAlN islands formed on ZnOS by wet etching. As the etchant, for example, a mixture of pure water and hydrochloric acid (concentration: 36% by volume) at a volume ratio of 100: 1 (dilute hydrochloric acid) is used. As a result, the ZnOS crystal is removed, leaving only an InAlN barrier layer region (hereinafter, also referred to as nanoparticles) having a size of about 5 nm.

工程d.InAlN障壁層上へのInGaN発光層(Ga組成:0.5)の合成
高圧容器中に、溶媒ベンゼン(6mL)、In材料としてInI(0.1mmol)、Ga材料としてGaI(0.1mmol) 、窒素材料としてNaNH(2.0mmol)、ヘキサデシルアミン(0.2mmol)、工程cで作製したInAlNナノ粒子(65mg)を投入し合成温度300℃−1時間で、InGaN発光層(Ga組成:0.5)の合成を行った。合成後、トルエンとエタノールにより遠心分離で洗浄し、InAlNナノ粒子上にInGaN発光層(Ga組成:0.5)を作製した。発光層はナノ粒子全面を覆っておらず、2−3nm程度のサイズで独立して存在していた。
Step d. Synthesis of InGaN light emitting layer (Ga composition: 0.5) on InAlN barrier layer In a high-pressure container, solvent benzene (6 mL), InI 3 (0.1 mmol) as an In material, GaI 3 (0.1 mmol) as a Ga material, As a nitrogen material, NaNH 2 (2.0 mmol), hexadecylamine (0.2 mmol), and the InAlN nanoparticles (65 mg) produced in the step c were charged, and at a synthesis temperature of 300 ° C. for 1 hour, an InGaN light emitting layer (Ga composition: 0.5). After the synthesis, the resultant was washed with toluene and ethanol by centrifugation to produce an InGaN light emitting layer (Ga composition: 0.5) on the InAlN nanoparticles. The light emitting layer did not cover the entire surface of the nanoparticle, and was present independently with a size of about 2-3 nm.

工程e. InGaN発光層(Ga組成:0.5)を覆うInAlN障壁層の合成
高圧容器中に、溶媒ベンゼン(6mL)、In材料としてInI(0.1mmol)、Al材料としてAlI (0.1mmol) 、窒素材料としてNaNH (2.0mmol)、ヘキサデシルアミン(0.2mmol)、InGaN発光層を形成したInAlNナノ粒子(85mg)を投入し合成温度300℃−1時間でInAlN障壁層の合成を行った。合成後、トルエンとエタノールにより遠心分離で洗浄し、InGaN発光層を覆うInAlN障壁層(Al組成0.4)を作製した。
Step e. Synthesis of InAlN barrier layer covering InGaN light emitting layer (Ga composition: 0.5) In a high-pressure vessel, solvent benzene (6 mL), InI 3 (0.1 mmol) as an In material, AlI 3 (0.1 mmol) as an Al material, As a nitrogen material, NaNH 2 (2.0 mmol), hexadecylamine (0.2 mmol), and InAlN nanoparticles (85 mg) having an InGaN light-emitting layer were charged, and an InAlN barrier layer was synthesized at a synthesis temperature of 300 ° C. for 1 hour. Was. After the synthesis, the resultant was washed with toluene and ethanol by centrifugation to prepare an InAlN barrier layer (Al composition 0.4) covering the InGaN light emitting layer.

なお、シードはZnOSに限定されるものでなく、障壁層のInAlN、発光層のInGaNと同じ格子定数をもつものであればよい。また、下地となる成長結晶の合成法や材料も上記に限定されるものではない。   The seed is not limited to ZnOS, but may be any seed having the same lattice constant as InAlN of the barrier layer and InGaN of the light emitting layer. Further, the method and material for synthesizing the grown crystal serving as the base are not limited to those described above.

図5Bに合成したナノ粒子の発光スペクトルを示す。実施例1の発光スペクトルより更に広い波長範囲に分布した発光スペクトルが認められる。発光スペクトルは500nm付近にピークを持つ成分と、550nm付近にピークをもつ成分を含み、500nmの成分は厚みが抑制されたm面上の発光層由来、550nm付近の成分はc面上の発光層由来と考えられる。   FIG. 5B shows the emission spectrum of the synthesized nanoparticles. An emission spectrum distributed over a wider wavelength range than the emission spectrum of Example 1 is observed. The emission spectrum includes a component having a peak at around 500 nm and a component having a peak at around 550 nm. The component at 500 nm is derived from the light-emitting layer on the m-plane whose thickness is suppressed. The component at around 550 nm is a light-emitting layer on the c-plane. Probably originated.

実施例1と実施例2との発光層は、共にIn0.5Ga0.5Nである。通常、同一の化学組成の化合物からは、ほぼ同一の発光スペクトルを有する発光(蛍光)が出射する。発光層のサイズを縮小し、量子化を生じるナノ領域にした。上述のシードのような成長基板を用いた結晶成長を行う場合、シードの結晶面に依存してその上に成長する結晶の成長速度が異なる可能性があると考えられる。上述の例ではm面とc面がそれぞれ露出しているので、各発光層の厚さも均一ではないと考えられる。結果として得られた、サイズ、厚さの分布が広い波長領域に分布する発光形成に寄与した可能性があろうと考えられる。 The light emitting layers of Example 1 and Example 2 are both In 0.5 Ga 0.5 N. Normally, compounds having the same chemical composition emit luminescence (fluorescence) having substantially the same emission spectrum. The size of the light emitting layer was reduced to a nano region where quantization occurs. When crystal growth is performed using a growth substrate such as the seed described above, it is considered that the growth rate of the crystal grown thereon may vary depending on the crystal plane of the seed. In the above example, since the m-plane and the c-plane are respectively exposed, it is considered that the thickness of each light-emitting layer is not uniform. It is thought that the resulting distribution of size and thickness may have contributed to the formation of light emission distributed over a wide wavelength range.

実施例1と実施例2の発光スペクトルの波長分布形状は大きく異なる。実施例1と実施例2とでは下地結晶の格子定数はほぼ同一であるが、成長基板となる下地結晶の組成は異なる。下地結晶の組成がどのように発光波長の分布に影響するか、詳細は未だ不明である。   The wavelength distribution shapes of the emission spectra of Example 1 and Example 2 are significantly different. Example 1 and Example 2 have substantially the same lattice constant of the underlying crystal, but differ in the composition of the underlying crystal serving as the growth substrate. How the composition of the underlying crystal affects the emission wavelength distribution is not yet known in detail.

実施例1に従って製造した蛍光体ナノ粒子と実施例2に従って製造した蛍光体ナノ粒子とを混合したナノ粒子集合体を作成すれば、より広い波長範囲に分布する蛍光体ナノ粒子を提供できるであろう。   If a nanoparticle aggregate prepared by mixing the phosphor nanoparticles manufactured according to Example 1 and the phosphor nanoparticles manufactured according to Example 2 is prepared, it is possible to provide the phosphor nanoparticles distributed over a wider wavelength range. Would.

蛍光体ナノ粒子を構成する1次結晶、2次結晶、3次結晶の格子定数を変化させれば、得られる傾向の発光スペクトル模範化することが予想される。種々の格子定数を選択して、種々の蛍光体ナノ粒子を作成し、適宜混合することにより、種々の発光スペクトルを有する蛍光体ナノ粒子を提供できるであろう。   By changing the lattice constants of the primary crystal, the secondary crystal, and the tertiary crystal constituting the phosphor nanoparticles, it is expected that the obtained emission spectrum will be modeled. By selecting various lattice constants, preparing various phosphor nanoparticles, and mixing them appropriately, phosphor nanoparticles having various emission spectra can be provided.

以上、実施例に沿って本発明を説明したが、記載した数値、材料等は特に断らない限り制限的なものではない。種々の変更、置換、改良等が可能なことは当業者に自明であろう。   As described above, the present invention has been described with reference to the examples. However, the numerical values, materials, and the like are not limited unless otherwise specified. It will be apparent to those skilled in the art that various modifications, substitutions, improvements, and the like can be made.

Claims (10)

ナノ粒子の集合体であって、各ナノ粒子が発光層と障壁層とを含み、1つのナノ粒子内に厚さの異なる複数の発光層が含まれるナノ粒子集合体。   An aggregate of nanoparticles, wherein each nanoparticle includes a light-emitting layer and a barrier layer, and a single nanoparticle includes a plurality of light-emitting layers having different thicknesses. 前記発光層と前記障壁層が窒化物半導体である、請求項1に記載のナノ粒子集合体。   The nanoparticle assembly according to claim 1, wherein the light emitting layer and the barrier layer are nitride semiconductors. 前記各ナノ粒子が、Znを含むII-VI族半導体で形成された下地結晶を含む、請求項1または2に記載のナノ粒子集合体。   3. The nanoparticle assembly according to claim 1, wherein each of the nanoparticles includes a base crystal formed of a II-VI group semiconductor including Zn. 前記各ナノ粒子が、発光機能を有さないIII−V族半導体で形成された下地結晶を含む、請求項1または2に記載のナノ粒子集合体。   3. The nanoparticle assembly according to claim 1, wherein each of the nanoparticles includes a base crystal formed of a group III-V semiconductor having no light emitting function. 4. 多数の1次ナノ結晶を液相成長する第1工程と、
前記多数の1次ナノ結晶の各表面上に、発光機能を有するIII−V族半導体の2次結晶を液相成長する第2工程と、
前記2次結晶の各表面を覆う保護層を液相成長する第3工程と、
を含むナノ結晶集合体の製造方法。
A first step of liquid phase growth of a number of primary nanocrystals;
A second step of liquid phase growing a III-V semiconductor secondary crystal having a light emitting function on each surface of the plurality of primary nanocrystals;
A third step of performing liquid phase growth of a protective layer covering each surface of the secondary crystal;
A method for producing a nanocrystal aggregate comprising:
前記第1工程がII−VI族半導体混晶を成長する常圧の液相成長工程である、請求項5に記載のナノ結晶集合体の製造方法。   The method for producing a nanocrystal aggregate according to claim 5, wherein the first step is a normal-pressure liquid phase growth step of growing a group II-VI semiconductor mixed crystal. 前記第2、第3工程が耐圧容器を用いた加圧液相成長工程である請求項5又は6に記載のナノ粒子集合体の製造方法。   The method for producing a nanoparticle assembly according to claim 5 or 6, wherein the second and third steps are pressurized liquid phase growth steps using a pressure vessel. 前記第1工程が発光機能を有さないIII−V族半導体混晶を耐圧容器を用いて加圧下で行う液相成長工程である、請求項5に記載のナノ結晶集合体の製造方法。   The method for producing a nanocrystal aggregate according to claim 5, wherein the first step is a liquid phase growth step in which a group III-V semiconductor mixed crystal having no light emitting function is performed under pressure using a pressure vessel. 前記第1工程が、
多数の予備ナノ結晶を液相成長する第1予備工程と、
前記多数の予備ナノ結晶の各表面上に1次結晶を液相成長する第2予備工程と、
前記予備ナノ結晶を前記1次結晶から除去する第3予備工程と、
を含む、請求項5〜8のいずれか1項に記載のナノ結晶集合体の製造方法。
The first step includes:
A first preliminary step of liquid phase growing a number of preliminary nanocrystals;
A second preliminary step of liquid-phase growing a primary crystal on each surface of said plurality of preliminary nanocrystals;
A third preliminary step of removing the preliminary nanocrystal from the primary crystal;
The method for producing a nanocrystal aggregate according to any one of claims 5 to 8, comprising:
前記予備ナノ結晶がII−VI族半導体混晶であり、前記1次結晶が発光機能を有さないIII−V族半導体混晶である請求項9に記載のナノ粒子集合体の製造方法。   The method of manufacturing a nanoparticle assembly according to claim 9, wherein the preliminary nanocrystal is a II-VI group semiconductor mixed crystal, and the primary crystal is a III-V semiconductor mixed crystal having no light emitting function.
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