WO2017065294A1 - 窒化亜鉛系化合物およびその製造方法 - Google Patents

窒化亜鉛系化合物およびその製造方法 Download PDF

Info

Publication number
WO2017065294A1
WO2017065294A1 PCT/JP2016/080597 JP2016080597W WO2017065294A1 WO 2017065294 A1 WO2017065294 A1 WO 2017065294A1 JP 2016080597 W JP2016080597 W JP 2016080597W WO 2017065294 A1 WO2017065294 A1 WO 2017065294A1
Authority
WO
WIPO (PCT)
Prior art keywords
zinc nitride
chemical formula
compound represented
cazn
zinc
Prior art date
Application number
PCT/JP2016/080597
Other languages
English (en)
French (fr)
Inventor
史康 大場
細野 秀雄
秀典 平松
日出也 雲見
悠 熊谷
壮史 飯村
善行 村場
リー アラン バートン
田中 功
洋陽 日沼
Original Assignee
国立大学法人 東京工業大学
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by 国立大学法人 東京工業大学 filed Critical 国立大学法人 東京工業大学
Priority to JP2017545497A priority Critical patent/JP6773666B2/ja
Priority to US15/767,550 priority patent/US10308521B2/en
Publication of WO2017065294A1 publication Critical patent/WO2017065294A1/ja
Priority to US16/387,155 priority patent/US10737947B2/en

Links

Images

Classifications

    • CCHEMISTRY; METALLURGY
    • C01INORGANIC CHEMISTRY
    • C01GCOMPOUNDS CONTAINING METALS NOT COVERED BY SUBCLASSES C01D OR C01F
    • C01G9/00Compounds of zinc
    • C01G9/006Compounds containing, besides zinc, two ore more other elements, with the exception of oxygen or hydrogen
    • CCHEMISTRY; METALLURGY
    • C01INORGANIC CHEMISTRY
    • C01BNON-METALLIC ELEMENTS; COMPOUNDS THEREOF; METALLOIDS OR COMPOUNDS THEREOF NOT COVERED BY SUBCLASS C01C
    • C01B21/00Nitrogen; Compounds thereof
    • C01B21/06Binary compounds of nitrogen with metals, with silicon, or with boron, or with carbon, i.e. nitrides; Compounds of nitrogen with more than one metal, silicon or boron
    • C01B21/0602Binary compounds of nitrogen with metals, with silicon, or with boron, or with carbon, i.e. nitrides; Compounds of nitrogen with more than one metal, silicon or boron with two or more other elements chosen from metals, silicon or boron
    • CCHEMISTRY; METALLURGY
    • C01INORGANIC CHEMISTRY
    • C01GCOMPOUNDS CONTAINING METALS NOT COVERED BY SUBCLASSES C01D OR C01F
    • C01G9/00Compounds of zinc
    • CCHEMISTRY; METALLURGY
    • C01INORGANIC CHEMISTRY
    • C01GCOMPOUNDS CONTAINING METALS NOT COVERED BY SUBCLASSES C01D OR C01F
    • C01G9/00Compounds of zinc
    • C01G9/08Sulfides
    • CCHEMISTRY; METALLURGY
    • C09DYES; PAINTS; POLISHES; NATURAL RESINS; ADHESIVES; COMPOSITIONS NOT OTHERWISE PROVIDED FOR; APPLICATIONS OF MATERIALS NOT OTHERWISE PROVIDED FOR
    • C09KMATERIALS FOR MISCELLANEOUS APPLICATIONS, NOT PROVIDED FOR ELSEWHERE
    • C09K11/00Luminescent, e.g. electroluminescent, chemiluminescent materials
    • C09K11/08Luminescent, e.g. electroluminescent, chemiluminescent materials containing inorganic luminescent materials
    • C09K11/0883Arsenides; Nitrides; Phosphides
    • CCHEMISTRY; METALLURGY
    • C09DYES; PAINTS; POLISHES; NATURAL RESINS; ADHESIVES; COMPOSITIONS NOT OTHERWISE PROVIDED FOR; APPLICATIONS OF MATERIALS NOT OTHERWISE PROVIDED FOR
    • C09KMATERIALS FOR MISCELLANEOUS APPLICATIONS, NOT PROVIDED FOR ELSEWHERE
    • C09K11/00Luminescent, e.g. electroluminescent, chemiluminescent materials
    • C09K11/08Luminescent, e.g. electroluminescent, chemiluminescent materials containing inorganic luminescent materials
    • C09K11/54Luminescent, e.g. electroluminescent, chemiluminescent materials containing inorganic luminescent materials containing zinc or cadmium
    • CCHEMISTRY; METALLURGY
    • C09DYES; PAINTS; POLISHES; NATURAL RESINS; ADHESIVES; COMPOSITIONS NOT OTHERWISE PROVIDED FOR; APPLICATIONS OF MATERIALS NOT OTHERWISE PROVIDED FOR
    • C09KMATERIALS FOR MISCELLANEOUS APPLICATIONS, NOT PROVIDED FOR ELSEWHERE
    • C09K11/00Luminescent, e.g. electroluminescent, chemiluminescent materials
    • C09K11/08Luminescent, e.g. electroluminescent, chemiluminescent materials containing inorganic luminescent materials
    • C09K11/55Luminescent, e.g. electroluminescent, chemiluminescent materials containing inorganic luminescent materials containing beryllium, magnesium, alkali metals or alkaline earth metals
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L29/00Semiconductor devices specially adapted for rectifying, amplifying, oscillating or switching and having potential barriers; Capacitors or resistors having potential barriers, e.g. a PN-junction depletion layer or carrier concentration layer; Details of semiconductor bodies or of electrodes thereof ; Multistep manufacturing processes therefor
    • H01L29/02Semiconductor bodies ; Multistep manufacturing processes therefor
    • H01L29/12Semiconductor bodies ; Multistep manufacturing processes therefor characterised by the materials of which they are formed
    • H01L29/24Semiconductor bodies ; Multistep manufacturing processes therefor characterised by the materials of which they are formed including, apart from doping materials or other impurities, only semiconductor materials not provided for in groups H01L29/16, H01L29/18, H01L29/20, H01L29/22
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L31/00Semiconductor devices sensitive to infrared radiation, light, electromagnetic radiation of shorter wavelength or corpuscular radiation and specially adapted either for the conversion of the energy of such radiation into electrical energy or for the control of electrical energy by such radiation; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof
    • H01L31/0248Semiconductor devices sensitive to infrared radiation, light, electromagnetic radiation of shorter wavelength or corpuscular radiation and specially adapted either for the conversion of the energy of such radiation into electrical energy or for the control of electrical energy by such radiation; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof characterised by their semiconductor bodies
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L31/00Semiconductor devices sensitive to infrared radiation, light, electromagnetic radiation of shorter wavelength or corpuscular radiation and specially adapted either for the conversion of the energy of such radiation into electrical energy or for the control of electrical energy by such radiation; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof
    • H01L31/0248Semiconductor devices sensitive to infrared radiation, light, electromagnetic radiation of shorter wavelength or corpuscular radiation and specially adapted either for the conversion of the energy of such radiation into electrical energy or for the control of electrical energy by such radiation; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof characterised by their semiconductor bodies
    • H01L31/0256Semiconductor devices sensitive to infrared radiation, light, electromagnetic radiation of shorter wavelength or corpuscular radiation and specially adapted either for the conversion of the energy of such radiation into electrical energy or for the control of electrical energy by such radiation; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof characterised by their semiconductor bodies characterised by the material
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L31/00Semiconductor devices sensitive to infrared radiation, light, electromagnetic radiation of shorter wavelength or corpuscular radiation and specially adapted either for the conversion of the energy of such radiation into electrical energy or for the control of electrical energy by such radiation; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof
    • H01L31/0248Semiconductor devices sensitive to infrared radiation, light, electromagnetic radiation of shorter wavelength or corpuscular radiation and specially adapted either for the conversion of the energy of such radiation into electrical energy or for the control of electrical energy by such radiation; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof characterised by their semiconductor bodies
    • H01L31/0256Semiconductor devices sensitive to infrared radiation, light, electromagnetic radiation of shorter wavelength or corpuscular radiation and specially adapted either for the conversion of the energy of such radiation into electrical energy or for the control of electrical energy by such radiation; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof characterised by their semiconductor bodies characterised by the material
    • H01L31/0264Inorganic materials
    • H01L31/032Inorganic materials including, apart from doping materials or other impurities, only compounds not provided for in groups H01L31/0272 - H01L31/0312
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L31/00Semiconductor devices sensitive to infrared radiation, light, electromagnetic radiation of shorter wavelength or corpuscular radiation and specially adapted either for the conversion of the energy of such radiation into electrical energy or for the control of electrical energy by such radiation; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof
    • H01L31/18Processes or apparatus specially adapted for the manufacture or treatment of these devices or of parts thereof
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L33/00Semiconductor devices having potential barriers specially adapted for light emission; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L33/00Semiconductor devices having potential barriers specially adapted for light emission; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof
    • H01L33/02Semiconductor devices having potential barriers specially adapted for light emission; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof characterised by the semiconductor bodies
    • H01L33/26Materials of the light emitting region
    • CCHEMISTRY; METALLURGY
    • C01INORGANIC CHEMISTRY
    • C01PINDEXING SCHEME RELATING TO STRUCTURAL AND PHYSICAL ASPECTS OF SOLID INORGANIC COMPOUNDS
    • C01P2002/00Crystal-structural characteristics
    • C01P2002/70Crystal-structural characteristics defined by measured X-ray, neutron or electron diffraction data
    • C01P2002/72Crystal-structural characteristics defined by measured X-ray, neutron or electron diffraction data by d-values or two theta-values, e.g. as X-ray diagram
    • CCHEMISTRY; METALLURGY
    • C01INORGANIC CHEMISTRY
    • C01PINDEXING SCHEME RELATING TO STRUCTURAL AND PHYSICAL ASPECTS OF SOLID INORGANIC COMPOUNDS
    • C01P2002/00Crystal-structural characteristics
    • C01P2002/70Crystal-structural characteristics defined by measured X-ray, neutron or electron diffraction data
    • C01P2002/77Crystal-structural characteristics defined by measured X-ray, neutron or electron diffraction data by unit-cell parameters, atom positions or structure diagrams
    • CCHEMISTRY; METALLURGY
    • C01INORGANIC CHEMISTRY
    • C01PINDEXING SCHEME RELATING TO STRUCTURAL AND PHYSICAL ASPECTS OF SOLID INORGANIC COMPOUNDS
    • C01P2006/00Physical properties of inorganic compounds
    • C01P2006/40Electric properties
    • YGENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
    • Y02TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02PCLIMATE CHANGE MITIGATION TECHNOLOGIES IN THE PRODUCTION OR PROCESSING OF GOODS
    • Y02P70/00Climate change mitigation technologies in the production process for final industrial or consumer products
    • Y02P70/50Manufacturing or production processes characterised by the final manufactured product

Definitions

  • the present invention relates to a zinc nitride compound and a method for producing the same.
  • GaN is widely used in LED light sources, but cannot emit light in the visible light region because of its wide band gap. InN has a narrow band gap and cannot emit light in the visible light region. Furthermore, Ga is expensive and In is a rare element.
  • Various zinc nitride-based compounds have been proposed. For example, ZnSnN 2 is difficult to realize p-type, and Ca 2 ZnN 2 is an indirect transition type, which can be applied to light-emitting elements and high-efficiency solar cells. (Non-patent Document 1).
  • An object of the present invention is to solve the above-mentioned problems and provide a zinc nitride compound suitable for an electronic device such as a high-speed transistor, a high-efficiency visible light emitting device, a high-efficiency solar cell, or a high-sensitivity visible light sensor. .
  • a zinc nitride-based compound represented by the chemical formula CaZn 2 N 2 (2) A zinc nitride-based compound represented by the chemical formula X 1 2 ZnN 2 (X 1 is Be or Mg). (3) A zinc nitride compound represented by the chemical formula Zn 3 LaN 3 . (4) A zinc nitride compound represented by the chemical formula ZnTiN 2 . (5) A zinc nitride compound represented by the chemical formula ZnX 2 N 2 (X 2 is Zr or Hf). (6) A zinc nitride compound represented by a chemical formula Zn 2 X 3 N 3 (X 3 is V, Nb or Ta).
  • the zinc nitride compound of the present invention can provide a zinc nitride compound suitable for electronic devices such as high-speed transistors, high-efficiency visible light emitting elements, high-efficiency solar cells, and high-sensitivity visible light sensors.
  • a is a crystal structure of a zinc nitride compound represented by the chemical formula CaZn 2 N 2
  • b is a calculated phase diagram of the Ca—Zn—N system
  • c is a band structure of the zinc nitride compound represented by CaZn 2 N 2 (conductivity). Band and valence band)
  • d is a phase diagram in the chemical potential space of the Ca—Zn—N system. It illustrates the crystal structure of a typical zinc nitride-based compound of the present invention other than those represented by A) Formula CaZn 2 N 2.
  • the zinc nitride-based compound of the present invention can be represented by any of the following chemical formulas.
  • These zinc nitride compounds according to the present invention of A) to G) are novel compounds not recorded in ICSD (inorganic crystal structure database).
  • the basic electronic properties of these zinc nitride compounds according to the present invention of A) to G) are shown in FIG.
  • a is a band gap ( ⁇ is a direct gap, ⁇ is an indirect gap), and b is an effective mass of holes and electrons.
  • the zinc nitride compound according to the present invention is a compound semiconductor, and in particular, the zinc nitride compound according to the present invention represented by A) chemical formula CaZn 2 N 2 or C) chemical formula Zn 3 LaN 3 is a direct transition type. It is a compound semiconductor and is suitable for applications such as light emitting elements and thin film solar cells.
  • the space groups to which these zinc nitride compounds according to the present invention belong are as follows. A) It belongs to the space group P - 3m1. B) It belongs to the space group I4 / mmm. C) It belongs to the space group P6 3 / m. D) belong to the space group Pna2 1. E) Belongs to space group P3m1. F) It belongs to the space group Cmc2 1 . G) belong to the space group Pmn2 1.
  • A) a zinc nitride-based compound represented by the chemical formula CaZn 2 N 2 suitable as a direct transition type compound semiconductor will be described below.
  • the zinc nitride-based compound represented by) can be similarly understood from the entire detailed description.
  • a is A) a crystal structure of a zinc nitride compound represented by the chemical formula CaZn 2 N 2
  • b is a calculated phase diagram of the Ca—Zn—N system
  • c is zinc nitride represented by CaZn 2 N 2.
  • d is a phase diagram in the chemical potential space of the Ca—Zn—N system.
  • CaZn 2 N 2 exists stably under a high nitrogen chemical potential, that is, under a high nitrogen partial pressure.
  • a zinc nitride-based compound represented by the chemical formula CaZn 2 N 2 has a band gap of 1.9 eV, but by adding Mg, Sr, Ba or Cd, the chemical formula CaM 1 2x Zn 2 (1-x) N 2 (M 1 is Mg or Cd. 0 ⁇ x ⁇ 1) or M 2 x Ca 1-x Zn 2 N 2 (M 2 is Sr or Ba. 0 ⁇ x ⁇ 1),
  • the band gap can be controlled as a compound semiconductor having a band gap of 0.4 eV to 3.2 eV.
  • CaZn 2 N 2 easily forms nitrogen vacancies that become shallow donors, it can be n-type even when undoped, but it is preferable to form n-type by doping. Further, for example, carrier compensation by nitrogen vacancies is suppressed under a high nitrogen partial pressure, and a p-type can be formed by doping.
  • the zinc nitride compound represented by the chemical formula CaZn 2 N 2 is preferably synthesized under a high pressure of 1 GPa or more.
  • the raw material compounds preferably Ca 3 N 2 and 2Zn 3 N 2
  • the reaction is usually performed at 800 to 1500 ° C. and 1 to 10 GPa for 30 minutes to 5 hours. Is done.
  • the resulting high-pressure synthesis reaction product can be further purified by removing zinc in the product.
  • the resulting high-pressure synthesis reaction product powder and I 2 are placed in a glass container, for example, at about 15 to 30 ° C., preferably at room temperature for 5 to 10 minutes in an inert atmosphere such as argon or nitrogen.
  • an inert atmosphere such as argon or nitrogen.
  • zinc is converted to zinc iodide (ZnI 2 ).
  • the produced zinc iodide is dissolved in a solvent such as dimethyl ether to remove the solution.
  • the inert atmosphere is used to suppress oxidation of Zn 2+ and I ⁇ .
  • the zinc nitride-based compound of the present invention is a chemical vapor deposition method such as a physical vapor deposition method such as a sputtering method, a pulse laser deposition method, or a vacuum evaporation method, and a metal organic vapor deposition method. It can be obtained by depositing a thin film on a substrate using the method. As the substrate, an oxide substrate or the like can be appropriately selected according to the purpose.
  • CaZn 2 N 2 is composed of common elements on earth, directly a bandgap, further effective mass of small charge (0.17 m 0 in electronic, 0.91 m 0 with holes) are particularly useful in that it has a is there.
  • the direct band gap of 1.9 eV possessed by CaZn 2 N 2 corresponds to the red region of visible light, and high theoretical conversion efficiency can be expected as a solar cell light absorption layer.
  • an electronic element using CaZn 2 N 2 as an active layer is an electronic element (light emitting element) that emits light by injecting current in the visible light region, or an electronic element (solar cell) that absorbs visible light and generates a photovoltage or a photocurrent. Or an optical sensor).
  • FIGS. 3a to 3e show the crystal structures of other typical zinc nitride compounds of the present invention, as shown in FIG. 2a, for the zinc nitride compounds represented by the chemical formula CaZn 2 N 2 .
  • FIGS. 4a to 4g show A) a zinc nitride compound represented by the chemical formula CaZn 2 N 2 in the same manner as shown in FIG. 2b.
  • Other representative zinc nitride compounds of the present invention include Mg—Zn— The calculation state diagram of N system etc. is shown.
  • FIGS. 5a to 5g show the band structures (conduction bands) of other typical zinc nitride compounds of the present invention, as shown in FIG. 2c, for the zinc nitride compound represented by the chemical formula CaZn 2 N 2 . And valence band).
  • a zinc nitride compound suitable for electronic devices such as high-speed transistors, high-efficiency visible light emitting elements, high-efficiency solar cells, and high-sensitivity visible light sensors.
  • Example 1 Synthesis of zinc nitride compound represented by CaZn 2 N 2
  • the high-pressure synthesizer used is a belt-type high-pressure synthesizer, which is a sample holder: a high-pressure cell, a pressure control range: 2-5.5 GPa, and a temperature control range: room temperature to 1600 ° C.
  • the X-ray diffraction pattern of the resulting high pressure synthesis reaction product is shown in FIG. 6a.
  • About 69 wt% of the product was CaZn 2 N 2 and the rest was Zn.
  • the X-ray diffraction pattern of the obtained reaction product is shown in FIG. 6b.
  • the product was Ca 2 ZnN 2 .
  • Ca 2 ZnN 2 had an indirect gap of 1.6 eV (calculated value of 1.65 eV) and a direct gap of 1.9 eV (calculated value of 1.92 eV).
  • the high-pressure synthesizer used is a belt-type high-pressure synthesizer, which is a sample holder: a high-pressure cell, a pressure control range: 2-5.5 GPa, and a temperature control range: room temperature to 1600 ° C.
  • the X-ray diffraction pattern of the obtained high-pressure synthesis reaction product is shown in FIG.
  • About 80 wt% of the product was CaZn 2 N 2 and the rest was Zn or the like.
  • Photo which is light emission generated from CaZn 2 N 2 of the resulting high-pressure synthesis reaction product by photon excitation (wavelength: 355 nm, energy density: ⁇ 7 mJ / cm 2 ) using a Nd: YAG third harmonic pulse laser Luminescence was measured. The red photoluminescence was clearly observed visually at 10K. The result is shown in FIG. a shows the photoluminescence spectrum in 10, 100, 200, and 300K, b shows the temperature dependence of a spectrum peak position.

Landscapes

  • Chemical & Material Sciences (AREA)
  • Engineering & Computer Science (AREA)
  • Organic Chemistry (AREA)
  • Inorganic Chemistry (AREA)
  • Power Engineering (AREA)
  • Microelectronics & Electronic Packaging (AREA)
  • Computer Hardware Design (AREA)
  • General Physics & Mathematics (AREA)
  • Condensed Matter Physics & Semiconductors (AREA)
  • Physics & Mathematics (AREA)
  • Electromagnetism (AREA)
  • Manufacturing & Machinery (AREA)
  • Materials Engineering (AREA)
  • Ceramic Engineering (AREA)
  • Photovoltaic Devices (AREA)
  • Luminescent Compositions (AREA)
  • Light Receiving Elements (AREA)
  • Inorganic Compounds Of Heavy Metals (AREA)

Abstract

本発明は、高速トランジスタ、高効率可視光発光素子、高効率太陽電池、高感度可視光センサー等の電子素子に好適な窒化亜鉛系化合物を提供する。 化学式CaZn2N2、化学式X1 2ZnN2(X1はBeまたはMgである)等で表される窒化亜鉛系化合物。好適には、1 GPa以上の高圧下で合成される。

Description

窒化亜鉛系化合物およびその製造方法
 本発明は、窒化亜鉛系化合物およびその製造方法に関する。
 GaNはLED光源で広く実用化されているが、バンドギャップが広いために、そのまま可視光域で発光させることはできない。InNはバンドギャップが狭すぎて、可視光域で発光できない。さらに、Gaは高コストであり、Inは希少元素である。また、種々の窒化亜鉛系化合物が提案されているが、たとえばZnSnNはp型の実現が困難であり、CaZnNは間接遷移型であって、発光素子や高効率太陽電池への応用に適さない等の課題がある(非特許文献1)。
J.Solid State Chem.88,528-533(1990)
 本発明は、上記課題を解決して、高速トランジスタ、高効率可視光発光素子、高効率太陽電池、高感度可視光センサー等の電子素子に好適な窒化亜鉛系化合物を提供することを目的とする。
 本発明は上記の問題を解決するために、以下の発明を提供するものである。
(1)化学式CaZnで表される窒化亜鉛系化合物。
(2)化学式X ZnN(XはBeまたはMgである)で表される窒化亜鉛系化合物。
(3)化学式ZnLaNで表される窒化亜鉛系化合物。
(4)化学式ZnTiNで表される窒化亜鉛系化合物。
(5)化学式ZnX(XはZrまたはHfである)で表される窒化亜鉛系化合物。
(6)化学式Zn(XはV、NbまたはTaである)で表される窒化亜鉛系化合物。
(7)化学式ZnWNで表される窒化亜鉛系化合物。
(8)化合物半導体である上記(1)~(7)のいずれかに記載の窒化亜鉛系化合物。
(9)直接遷移型化合物半導体である上記(1)または(3)に記載の窒化亜鉛系化合物。
(10)化学式CaM 2xZn2(1-x)(MはMgまたはCdである。0≦x≦1)またはM Ca1-xZn (MはSrまたはBaである。0≦x≦1)で表され、バンドギャップが0.4eV~3.2eVである化合物半導体。
(11)上記(8)~(10)のいずれかに記載の化合物半導体を活性層に有する電子素子。
(12)可視光域で電流注入発光する上記(11)に記載の電子素子。
(13)可視光を吸収し光電圧あるいは光電流を発生する上記(11)に記載の電子素子。
(14)1GPa以上の高圧下で合成する上記(1)~(7)のいずれかに記載の窒化亜鉛系化合物の製造方法。
 本発明の窒化亜鉛系化合物は、高速トランジスタ、高効率可視光発光素子、高効率太陽電池、高感度可視光センサー等の電子素子に好適な窒化亜鉛系化合物を提供し得る。
本発明に係る窒化亜鉛系化合物の基礎電子的特性を示す図。 aは化学式CaZnで表される窒化亜鉛系化合物の結晶構造、bはCa-Zn-N系の計算状態図、cはCaZn表される窒化亜鉛系化合物のバンド構造(伝導帯および価電子帯)、dはCa-Zn-N系の化学ポテンシャル空間での状態図、を示す。 A)化学式CaZnで表される以外の本発明の代表的な窒化亜鉛系化合物の結晶構造を示す図。 A)化学式CaZnで表される以外の本発明の代表的な窒化亜鉛系化合物の、Mg-Zn-N系等の計算状態図を示す図。 A)化学式CaZnで表される以外の本発明の代表的な窒化亜鉛系化合物のバンド構造(伝導帯および価電子帯)を示す図。 実施例1および比較例1で得られた合成反応生成物のX線回折図形。 実施例1および比較例1で得られた合成反応生成物の吸収スペクトル図。 実施例2で得られた合成反応生成物のX線回折図形。 実施例2で得られた合成反応生成物のフォトルミネッセンス。 実施例2で得られた高純度化粉末生成物のX線回折図形。
 本発明の窒化亜鉛系化合物は、次の化学式のいずれかで表され得る。
A)化学式CaZnで表される窒化亜鉛系化合物。
B)化学式X ZnN(XはBeまたはMgである)で表される窒化亜鉛系化合物。
C)化学式ZnLaNで表される窒化亜鉛系化合物。
D)化学式ZnTiNで表される窒化亜鉛系化合物。
E)化学式ZnX(XはZrまたはHfである)で表される窒化亜鉛系化合物。
F)化学式Zn(XはV、NbまたはTaである)で表される窒化亜鉛系化合物。
G)化学式ZnWNで表される窒化亜鉛系化合物。
 これらのA)~G)の本発明に係る窒化亜鉛系化合物は、ICSD(無機結晶構造データベース)に未収録の新規化合物である。これらのA)~G)の本発明に係る窒化亜鉛系化合物の基礎電子的特性を図1に示す。図1において、aはバンドギャップ(●は直接ギャップ、○は間接ギャップ)、bはホールおよび電子の有効質量を示す。本発明に係る窒化亜鉛系化合物は、化合物半導体であり、特に、A)化学式CaZnまたはC)化学式ZnLaNで表される、本発明に係る窒化亜鉛系化合物は、直接遷移型化合物半導体であり、発光素子、薄膜太陽電池等の応用に好適である。
 これらの本発明に係る窒化亜鉛系化合物が属する空間群は次のとおりである。
A)空間群P-3m1に属する。
B)空間群I4/mmmに属する。
C)空間群P63/mに属する。
D)空間群Pna21に属する。
E)空間群P3m1に属する。
F)空間群Cmc21に属する。
G)空間群Pmn21に属する。
 本発明の窒化亜鉛系化合物のうち、直接遷移型化合物半導体として好適なA)化学式CaZnで表される窒化亜鉛系化合物について、代表的に以下に説明するが、その他のB)~G)で表される窒化亜鉛系化合物についても詳細な説明の全体から同様に理解され得る。
 図2において、aはA)化学式CaZnで表される窒化亜鉛系化合物の結晶構造、bはCa-Zn-N系の計算状態図、cはCaZnで表される窒化亜鉛系化合物のバンド構造(伝導帯および価電子帯)、dはCa-Zn-N系の化学ポテンシャル空間での状態図、を示す。dからわかるように、CaZnは高い窒素化学ポテンシャルの下、すなわち高い窒素分圧の下で安定に存在する。
 A)化学式CaZnで表される窒化亜鉛系化合物は、バンドギャップ1.9eVを有するが、Mg、Sr,BaまたはCdを添加することにより、化学式CaM 2xZn2(1-x)(MはMgまたはCdである。0≦x≦1)またはM Ca1-xZn (MはSrまたはBaである。0≦x≦1)で表され、バンドギャップが0.4eV~3.2eVである化合物半導体として、バンドギャップを制御し得る。また、CaZnは、浅いドナーになる窒素空孔が形成されやすいため、アンドープでもn型になり得るが、ドーピングにより、n型を形成するのが好適である。さらに、たとえば高窒素分圧下では窒素空孔によるキャリア補償が抑えられ、ドーピングによりp型を形成し得る。
 A)化学式CaZnで表される窒化亜鉛系化合物は、好適には、1 GPa以上の高圧下で合成される。この場合、高圧合成装置内に、好適にはCaおよび2Znである原料化合物を導入し、通常800~1500℃、1~10GPaで、30分間から5時間程度、反応に供される。
 得られる高圧合成反応生成物は、生成物中の亜鉛を除去することによりさらに高純度化し得る。好適には、得られる高圧合成反応生成物粉末とIを、たとえばガラス製容器に入れ、アルゴン、窒素等の不活性雰囲気下に、15~30℃程度、好ましくは室温で、5~10分間程度、保持して、亜鉛をヨウ化亜鉛(ZnI)に変換させる。ついで、生成したヨウ化亜鉛をジメチルエーテル等の溶媒に溶解させて、溶液を除去する。不活性雰囲気を用いるのは、Zn2+、I-の酸化を抑制するためである。
 本発明の窒化亜鉛系化合物は、上記の高圧合成法以外にも、スパッタ法、パルスレーザー堆積法、真空蒸着法等の物理的気相堆積法および有機金属気相堆積法等の化学気相堆積法を用いて、基板上に薄膜を堆積することにより、得られ得る。基板は、目的に応じて、酸化物基板等を適宜選択し得る。
 CaZnは、地球上にありふれた元素から構成され、直接バンドギャップであり、さらに小さな電荷の有効質量(電子で0.17m、ホールで0.91m)を有する点で特に有用である。CaZnが有する1.9eVの直接バンドギャップは、可視光の赤色領域に相当し、太陽電池光吸収層として高い理論変換効率が期待され得る。このように、CaZnを活性層とする電子素子は、可視光域で電流注入発光する電子素子(発光素子)、可視光を吸収し光電圧あるいは光電流を発生する電子素子(太陽電池、あるいは光センサー)として有用である。
 図3a~eは、A)化学式CaZnで表される窒化亜鉛系化合物について図2aに示されると同様に、それ以外の本発明の代表的な窒化亜鉛系化合物の結晶構造を示す。
 図4a~gは、A)化学式CaZnで表される窒化亜鉛系化合物について図2bに示されると同様に、それ以外の本発明の代表的な窒化亜鉛系化合物の、Mg-Zn-N系等の計算状態図を示す。
 図5a~gは、A)化学式CaZnで表される窒化亜鉛系化合物について図2cに示されると同様に、それ以外の本発明の代表的な窒化亜鉛系化合物のバンド構造(伝導帯および価電子帯)を示す。
 本発明によれば、高速トランジスタ、高効率可視光発光素子、高効率太陽電池、高感度可視光センサー等の電子素子に好適な窒化亜鉛系化合物を提供し得る。
 以下、実施例により、さらに本発明を詳細に説明する。
実施例1
 CaZnで表される窒化亜鉛系化合物の合成
高圧合成装置内に、モル比でCa:Zn=1:2となるように混合した原料化合物を導入し、2.5GPaで、1100℃、1時間保持した。用いた高圧合成装置は、ベルト式高圧合成装置であり、試料ホルダ:高圧セル、圧力制御範囲:2-5.5GPa、および温度制御範囲:室温~1600℃である。
 得られた高圧合成反応生成物のX線回折図形を図6aに示す。生成物の約69wt%はCaZnであり、残りはZnであった。CaZnの格子パラメータは、a=3.463150(44)Å、c=6.01055(11)Åであり、理論値であるa=3.454Å、c=5.990Åとの差異は0.3%であった。
 図7a~cに、拡散反射測定とKubelka-Munkの関係式による吸収スペクトルを比較例1のCaZnNとともに示す。CaZnは、急峻に立ち上がることがわかる。なお、CaZnは、直接ギャップ1.9eV(計算値1.83eV)であった。
比較例1
 CaZnNで表される窒化亜鉛系化合物の合成
電気炉内で、モル比でCa:Zn=2:1となるように混合した原料化合物をSUS管にAr封入して常圧で680℃、40時間保持した。試料ホルダは、SUSガス配管とスウェッジロックを用いた反応菅であった。
 得られた反応生成物のX線回折図形を図6bに示す。生成物はCaZnNであった。CaZnNの格子パラメータは、a=3.583646(65)Å、c=12.663346(26)Åであり、理論値であるa=3.575Å、c=12.607Åとの差異はそれぞれ0.2%、0.4%であった。
 図7a~cに、拡散反射測定とKubelka-Munkの関係式による吸収スペクトルを示す。なお、CaZnNは、間接ギャップ1.6eV(計算値1.65eV)、直接ギャップ1.9eV(計算値1.92eV)であった。
 因みに、上記実施例1の混合比の原材料を、本比較例1と同じ方法で合成を試みた場合、本発明のCaZnを得ることはできなかった。
実施例2
 CaZnで表される窒化亜鉛系化合物の合成
高圧セル内に、モル比でCa:Zn=1:2となるように混合した原料化合物を導入し、高圧合成にて5.0GPaを印加し、1200℃、1時間保持した。用いた高圧合成装置は、ベルト式高圧合成装置であり、試料ホルダ:高圧セル、圧力制御範囲:2-5.5GPa、および温度制御範囲:室温~1600℃である。
 得られた高圧合成反応生成物のX線回折図形を図8に示す。生成物の約80wt%はCaZnであり、残りはZn等であった。CaZnの格子パラメータは、a=3.46380(11)Å、c=6.00969(30)Åであり、理論値であるa=3.454Å、c=5.990Åとの差異は0.3%であった。
 Nd:YAG第3高調波パルスレーザーを使用する光子励起(波長:355nm、エネルギー密度:~7mJ/cm)によって、得られた高圧合成反応生成物のCaZnから生じる光放射であるフォトルミネッセンスを測定した。赤色のフォトルミネッセンスは10Kにおいて目視で明瞭に観測されるものであった。その結果を図9に示す。aは、10、100、200および300Kにおけるフォトルミネッセンススペクトルを示し、bは、スペクトルピーク位置の温度依存性を示す。
 (CaZnの高純度化)
 得られた高圧合成反応生成物(CaZn、Zn等)粉末とIをガラス製容器に入れ、アルゴン雰囲気下に約5分間、室温に保持し、亜鉛をヨウ化亜鉛に変換させた。ついで、生成したヨウ化亜鉛をジメチルエーテルに溶解させて、溶液を除去した。得られた粉末のCaZnは約87.3wt%、亜鉛等は約12.7wt%であった。得られた高純度化粉末生成物のX線回折図形を図10に示す。得られた高純度化粉末生成物約1gを用いて、冷間等方性加圧装置(CIP)により、パルスレーザー堆積ターゲット用のペレットが形成された。

Claims (14)

  1.  化学式CaZnで表される窒化亜鉛系化合物。
  2.  化学式X ZnN(XはBeまたはMgである)で表される窒化亜鉛系化合物。
  3.  化学式ZnLaNで表される窒化亜鉛系化合物。
  4.  化学式ZnTiNで表される窒化亜鉛系化合物。
  5.  化学式ZnX(XはZrまたはHfである)で表される窒化亜鉛系化合物。
  6.  化学式Zn(XはV、NbまたはTaである)で表される窒化亜鉛系化合物。
  7.  化学式ZnWNで表される窒化亜鉛系化合物。
  8.  化合物半導体である請求項1~7のいずれか1項に記載の窒化亜鉛系化合物。
  9.  直接遷移型化合物半導体である請求項1または3に記載の窒化亜鉛系化合物。
  10.  化学式CaM 2xZn2(1-x)(MはMgまたはCdである。0≦x≦1)またはM Ca1-xZn (MはSrまたはBaである。0≦x≦1)で表され、バンドギャップが0.4eV~3.2eVである化合物半導体。
  11.  請求項8~10のいずれか1項に記載の化合物半導体を活性層に有する電子素子。
  12.  可視光域で電流注入発光する請求項11に記載の電子素子。
  13.  可視光を吸収し光電圧あるいは光電流を発生する請求項11に記載の電子素子。
  14.  1 GPa以上の高圧下で合成する請求項1~7のいずれか1項に記載の窒化亜鉛系化合
    物の製造方法。
PCT/JP2016/080597 2015-10-15 2016-10-14 窒化亜鉛系化合物およびその製造方法 WO2017065294A1 (ja)

Priority Applications (3)

Application Number Priority Date Filing Date Title
JP2017545497A JP6773666B2 (ja) 2015-10-15 2016-10-14 窒化亜鉛系化合物およびその製造方法
US15/767,550 US10308521B2 (en) 2015-10-15 2016-10-14 Zinc nitride compound and method for producing same
US16/387,155 US10737947B2 (en) 2015-10-15 2019-04-17 Zinc nitride compound and method for producing same

Applications Claiming Priority (2)

Application Number Priority Date Filing Date Title
JP2015-203891 2015-10-15
JP2015203891 2015-10-15

Related Child Applications (2)

Application Number Title Priority Date Filing Date
US15/767,550 A-371-Of-International US10308521B2 (en) 2015-10-15 2016-10-14 Zinc nitride compound and method for producing same
US16/387,155 Continuation US10737947B2 (en) 2015-10-15 2019-04-17 Zinc nitride compound and method for producing same

Publications (1)

Publication Number Publication Date
WO2017065294A1 true WO2017065294A1 (ja) 2017-04-20

Family

ID=58517196

Family Applications (1)

Application Number Title Priority Date Filing Date
PCT/JP2016/080597 WO2017065294A1 (ja) 2015-10-15 2016-10-14 窒化亜鉛系化合物およびその製造方法

Country Status (3)

Country Link
US (2) US10308521B2 (ja)
JP (1) JP6773666B2 (ja)
WO (1) WO2017065294A1 (ja)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN111524997A (zh) * 2020-03-17 2020-08-11 湖北云邦科技有限公司 一种基于量子碳膜的异质结光电二极管结构及制作方法
US11417784B2 (en) 2018-03-30 2022-08-16 Panasonic Intellectual Property Management Co., Ltd. Multi-junction light energy conversion element, device comprising the same, and fabrication method of SnZn2N2
WO2023195413A1 (ja) * 2022-04-07 2023-10-12 Tdk株式会社 窒化物、圧電体、圧電素子、強誘電体、及び強誘電素子

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN113544307A (zh) * 2019-03-28 2021-10-22 松下知识产权经营株式会社 无机化合物半导体及其制造方法以及使用了该无机化合物半导体的光能转换元件

Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2001322814A (ja) * 2000-05-12 2001-11-20 Kenkichiro Kobayashi p型酸化物半導体およびその製造方法
JP2008084512A (ja) * 2005-12-13 2008-04-10 Toshiba Corp 情報記録再生装置
WO2009122567A1 (ja) * 2008-04-01 2009-10-08 株式会社 東芝 情報記録再生装置
JP2012031057A (ja) * 2010-07-28 2012-02-16 Sharp Corp Ii−iii−n半導体ナノ粒子および当該ii−iii−n半導体ナノ粒子の製造方法

Family Cites Families (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
FR2841893B1 (fr) * 2002-07-02 2004-08-27 Francois Lacoste Procede de synthese de nitrure de calcium
US20090160325A1 (en) * 2003-12-16 2009-06-25 Panasonic Corporation Organic electroluminescent device and method for manufacturing the same
EP1730795A2 (en) * 2004-03-31 2006-12-13 Matsushita Electric Industrial Co., Ltd. Organic photoelectric conversion element utilizing an inorganic buffer layer placed between an electrode and the active material
GB0522027D0 (en) * 2005-10-28 2005-12-07 Nanoco Technologies Ltd Controlled preparation of nanoparticle materials
US7733684B2 (en) 2005-12-13 2010-06-08 Kabushiki Kaisha Toshiba Data read/write device
WO2008148031A2 (en) * 2007-05-23 2008-12-04 University Of Florida Research Foundation, Inc Method and apparatus for light absorption and charged carrier transport
US8654807B2 (en) * 2010-11-18 2014-02-18 The Board Of Trustees Of The Leland Stanford Junior University Electrical devices formed using ternary semiconducting compounds

Patent Citations (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2001322814A (ja) * 2000-05-12 2001-11-20 Kenkichiro Kobayashi p型酸化物半導体およびその製造方法
JP2008084512A (ja) * 2005-12-13 2008-04-10 Toshiba Corp 情報記録再生装置
WO2009122567A1 (ja) * 2008-04-01 2009-10-08 株式会社 東芝 情報記録再生装置
JP2012031057A (ja) * 2010-07-28 2012-02-16 Sharp Corp Ii−iii−n半導体ナノ粒子および当該ii−iii−n半導体ナノ粒子の製造方法
JP2015078372A (ja) * 2010-07-28 2015-04-23 シャープ株式会社 半導体ナノ粒子、および、半導体ナノ粒子の製造方法

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US11417784B2 (en) 2018-03-30 2022-08-16 Panasonic Intellectual Property Management Co., Ltd. Multi-junction light energy conversion element, device comprising the same, and fabrication method of SnZn2N2
CN111524997A (zh) * 2020-03-17 2020-08-11 湖北云邦科技有限公司 一种基于量子碳膜的异质结光电二极管结构及制作方法
WO2023195413A1 (ja) * 2022-04-07 2023-10-12 Tdk株式会社 窒化物、圧電体、圧電素子、強誘電体、及び強誘電素子

Also Published As

Publication number Publication date
JP6773666B2 (ja) 2020-10-21
US20190248670A1 (en) 2019-08-15
US10308521B2 (en) 2019-06-04
US10737947B2 (en) 2020-08-11
JPWO2017065294A1 (ja) 2018-08-09
US20180354791A1 (en) 2018-12-13

Similar Documents

Publication Publication Date Title
US10737947B2 (en) Zinc nitride compound and method for producing same
Martinez et al. Synthesis, structure, and optoelectronic properties of II–IV–V 2 materials
Jing et al. Sb3+ doping-induced triplet self-trapped excitons emission in lead-free Cs2SnCl6 nanocrystals
Wang et al. Chemical vapor deposition growth of single-crystalline cesium lead halide microplatelets and heterostructures for optoelectronic applications
US7323356B2 (en) LnCuO(S,Se,Te)monocrystalline thin film, its manufacturing method, and optical device or electronic device using the monocrystalline thin film
Kirm et al. Thin films of HfO2 and ZrO2 as potential scintillators
Li et al. The incorporation of arsenic in GaN by metalorganic chemical vapor deposition
US9985173B2 (en) II-III-N semiconductor nanoparticles and method of making same
Ezema et al. Effect of annealing temperature on the structural and optical properties of zinc oxide (ZnO) nanocrystals prepared by sol gel
Khan et al. Recent developments of lead-free halide-perovskite nanocrystals: Synthesis strategies, stability, challenges, and potential in optoelectronic applications
KR20180051893A (ko) h-BN을 보호층으로 사용하는 봉지 재료 및 이의 제조방법
JP6712798B2 (ja) 窒化銅半導体およびその製造方法
US20120025139A1 (en) Ii-iii-v compound semiconductor
Han et al. Growth and optical properties of epitaxial BexZn1− xO alloy films
Chaudhari et al. Zinc oxide family semiconductors for ultraviolet radiation emission–A cathodoluminescence study
RU2737774C1 (ru) Способ химического осаждения перовскитов из газовой фазы для производства фотовольтаических устройств, светодиодов и фотодетекторов
Santana-Rodríguez et al. Close space vapor transport of gallium nitride in vacuum
Gapanovich et al. Synthesis and crystal and defect structures of polycrystalline Cu2SrSnS4 and Cu1. 9SrSnS4 powders
Parshina et al. Photoluminescence properties of thin nitrogen-and phosphorus-doped ZnO films fabricated using pulsed laser deposition
Hyun et al. Photoluminescence spectra of Zn 1− x Cd x Al 2 Se 4 single crystals
Alwadai Investigating Semiconductor Nanostructures Functionalized by Emerging Materials for Optoelectronic Devices
Choe et al. Photoluminescence spectra of Zn1− xCdxAl2Se4-4xS4x single crystals
Lee et al. ZnBeMgO Alloys and UV Optoelectronic Applications
Pandey et al. Room Temperature Synthesis of Low Cost and Highly Stable Cs2albicl6 for Photovoltaic Applications
Novikov et al. Growth by molecular beam epitaxy of GaNAs alloys with high as content for potential photoanode applications in hydrogen production

Legal Events

Date Code Title Description
121 Ep: the epo has been informed by wipo that ep was designated in this application

Ref document number: 16855547

Country of ref document: EP

Kind code of ref document: A1

ENP Entry into the national phase

Ref document number: 2017545497

Country of ref document: JP

Kind code of ref document: A

NENP Non-entry into the national phase

Ref country code: DE

122 Ep: pct application non-entry in european phase

Ref document number: 16855547

Country of ref document: EP

Kind code of ref document: A1