CN103972310B - A kind of preparation method of zinc oxide based p type material - Google Patents
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- XLOMVQKBTHCTTD-UHFFFAOYSA-N Zinc monoxide Chemical compound [Zn]=O XLOMVQKBTHCTTD-UHFFFAOYSA-N 0.000 title claims abstract description 114
- 239000000463 material Substances 0.000 title claims abstract description 61
- 239000011787 zinc oxide Substances 0.000 title claims abstract description 58
- 238000002360 preparation method Methods 0.000 title claims description 9
- 239000011701 zinc Substances 0.000 claims abstract description 48
- 238000000034 method Methods 0.000 claims abstract description 33
- 239000000203 mixture Substances 0.000 claims abstract description 16
- QVGXLLKOCUKJST-UHFFFAOYSA-N atomic oxygen Chemical compound [O] QVGXLLKOCUKJST-UHFFFAOYSA-N 0.000 claims abstract description 13
- 239000001301 oxygen Substances 0.000 claims abstract description 13
- 229910052760 oxygen Inorganic materials 0.000 claims abstract description 13
- 239000000758 substrate Substances 0.000 claims description 10
- 239000004065 semiconductor Substances 0.000 abstract description 12
- 239000011777 magnesium Substances 0.000 description 42
- 239000000370 acceptor Substances 0.000 description 25
- 230000010287 polarization Effects 0.000 description 17
- 239000012535 impurity Substances 0.000 description 14
- 229910052749 magnesium Inorganic materials 0.000 description 11
- FYYHWMGAXLPEAU-UHFFFAOYSA-N Magnesium Chemical compound [Mg] FYYHWMGAXLPEAU-UHFFFAOYSA-N 0.000 description 9
- 239000012159 carrier gas Substances 0.000 description 9
- 229910052725 zinc Inorganic materials 0.000 description 7
- 230000002269 spontaneous effect Effects 0.000 description 6
- HCHKCACWOHOZIP-UHFFFAOYSA-N Zinc Chemical compound [Zn] HCHKCACWOHOZIP-UHFFFAOYSA-N 0.000 description 5
- 238000009825 accumulation Methods 0.000 description 5
- 230000005693 optoelectronics Effects 0.000 description 5
- 238000011160 research Methods 0.000 description 5
- 230000004913 activation Effects 0.000 description 4
- 238000005401 electroluminescence Methods 0.000 description 4
- 230000006698 induction Effects 0.000 description 4
- 230000008859 change Effects 0.000 description 3
- 230000007423 decrease Effects 0.000 description 3
- 238000004020 luminiscence type Methods 0.000 description 3
- 238000002488 metal-organic chemical vapour deposition Methods 0.000 description 3
- 238000012986 modification Methods 0.000 description 3
- 230000004048 modification Effects 0.000 description 3
- 229910052594 sapphire Inorganic materials 0.000 description 3
- 239000010980 sapphire Substances 0.000 description 3
- IJGRMHOSHXDMSA-UHFFFAOYSA-N Atomic nitrogen Chemical compound N#N IJGRMHOSHXDMSA-UHFFFAOYSA-N 0.000 description 2
- 235000005811 Viola adunca Nutrition 0.000 description 2
- 240000009038 Viola odorata Species 0.000 description 2
- 235000013487 Viola odorata Nutrition 0.000 description 2
- 235000002254 Viola papilionacea Nutrition 0.000 description 2
- 230000003247 decreasing effect Effects 0.000 description 2
- 230000005684 electric field Effects 0.000 description 2
- 229910021478 group 5 element Inorganic materials 0.000 description 2
- 238000002347 injection Methods 0.000 description 2
- 239000007924 injection Substances 0.000 description 2
- 229910052757 nitrogen Inorganic materials 0.000 description 2
- 230000008569 process Effects 0.000 description 2
- 230000009471 action Effects 0.000 description 1
- 239000004480 active ingredient Substances 0.000 description 1
- 239000000956 alloy Substances 0.000 description 1
- 229910045601 alloy Inorganic materials 0.000 description 1
- WTKQDILJIUYBGG-UHFFFAOYSA-N aluminum;magnesium;oxygen(2-);scandium(3+) Chemical compound [O-2].[O-2].[O-2].[O-2].[Mg+2].[Al+3].[Sc+3] WTKQDILJIUYBGG-UHFFFAOYSA-N 0.000 description 1
- 229910052787 antimony Inorganic materials 0.000 description 1
- 229910052785 arsenic Inorganic materials 0.000 description 1
- 230000004888 barrier function Effects 0.000 description 1
- 230000009286 beneficial effect Effects 0.000 description 1
- 230000015572 biosynthetic process Effects 0.000 description 1
- 239000000969 carrier Substances 0.000 description 1
- 239000013078 crystal Substances 0.000 description 1
- 230000007547 defect Effects 0.000 description 1
- 230000007123 defense Effects 0.000 description 1
- 238000001514 detection method Methods 0.000 description 1
- 230000006866 deterioration Effects 0.000 description 1
- 238000011161 development Methods 0.000 description 1
- HQWPLXHWEZZGKY-UHFFFAOYSA-N diethylzinc Chemical compound CC[Zn]CC HQWPLXHWEZZGKY-UHFFFAOYSA-N 0.000 description 1
- 125000000118 dimethyl group Chemical group [H]C([H])([H])* 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 238000000407 epitaxy Methods 0.000 description 1
- 230000005525 hole transport Effects 0.000 description 1
- 230000010354 integration Effects 0.000 description 1
- 229910052751 metal Inorganic materials 0.000 description 1
- 239000002184 metal Substances 0.000 description 1
- 150000002739 metals Chemical class 0.000 description 1
- 230000007935 neutral effect Effects 0.000 description 1
- 231100000252 nontoxic Toxicity 0.000 description 1
- 230000003000 nontoxic effect Effects 0.000 description 1
- 229910052698 phosphorus Inorganic materials 0.000 description 1
- 230000000704 physical effect Effects 0.000 description 1
- 239000002994 raw material Substances 0.000 description 1
- 238000001039 wet etching Methods 0.000 description 1
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- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10F—INORGANIC SEMICONDUCTOR DEVICES SENSITIVE TO INFRARED RADIATION, LIGHT, ELECTROMAGNETIC RADIATION OF SHORTER WAVELENGTH OR CORPUSCULAR RADIATION
- H10F71/00—Manufacture or treatment of devices covered by this subclass
- H10F71/125—The active layers comprising only Group II-VI materials, e.g. CdS, ZnS or CdTe
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- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10F—INORGANIC SEMICONDUCTOR DEVICES SENSITIVE TO INFRARED RADIATION, LIGHT, ELECTROMAGNETIC RADIATION OF SHORTER WAVELENGTH OR CORPUSCULAR RADIATION
- H10F77/00—Constructional details of devices covered by this subclass
- H10F77/10—Semiconductor bodies
- H10F77/12—Active materials
- H10F77/123—Active materials comprising only Group II-VI materials, e.g. CdS, ZnS or HgCdTe
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Abstract
本发明提供一种氧化锌基p型材料的制备方法,属于半导体材料生长技术领域。该方法在基础层上制备渐变层;在渐变层上制备盖层;所述的基础层为氧极性表面的MgxZn1-xO(0.6≥x≥0.2)材料,基础层的厚度不小于5nm;渐变层具有组分渐变的结构,其结构自下而上为MgxZn1-xO/Mgx-δZn1-(x-δ)O/Mgx-2δZn1-(x-2δ)O/…/Mgx-(n-1)δZn1-[x-(n-1)δ]O/Mgx-nδZn1-(x-nδ)O(δ→0,n为自然数;nδ=x;),渐变层厚度不大于1μm;盖层的材料为ZnO,盖层的厚度不小于300nm。该方法制备的氧化锌基p型材料具有良好的温度稳定性。
The invention provides a method for preparing a zinc oxide-based p-type material, which belongs to the technical field of semiconductor material growth. The method prepares a gradient layer on the base layer; prepares a cover layer on the gradient layer; the base layer is a Mg x Zn 1-x O (0.6≥x≥0.2) material on the oxygen polar surface, and the thickness of the base layer is not Less than 5nm; the gradient layer has a composition gradient structure, and its structure from bottom to top is Mg x Zn 1-x O/Mg x-δ Zn 1-(x-δ) O/Mg x-2δ Zn 1-(x -2δ) O/.../Mg x-(n-1)δ Zn 1-[x-(n-1)δ] O/Mg x-nδ Zn 1-(x-nδ) O(δ→0,n is a natural number; nδ=x;), the thickness of the gradient layer is not greater than 1 μm; the material of the cover layer is ZnO, and the thickness of the cover layer is not less than 300nm. The zinc oxide-based p-type material prepared by the method has good temperature stability.
Description
技术领域technical field
本发明属于半导体材料生长技术领域,具体涉及一种氧化锌基p型材料的制备方法。The invention belongs to the technical field of semiconductor material growth, and in particular relates to a preparation method of a zinc oxide-based p-type material.
背景技术Background technique
宽禁带半导体,因其在固态照明、短波长半导体激光和紫外光探测方面的具有广阔的应用前景,被称作第三代半导体。ZnO是宽带隙半导体材料的代表之一,是一种单轴对称的直接带隙半导体,其室温下的禁带宽度为3.37eV,具有高达60meV的激子束缚能,这一数值远高于室温热离化能(26meV),可以保证其在室温下实现高效的激子发光和低阈值的受激发射。因此,ZnO被认为是制备短波长发光二极管(LED)尤其是激光器(LD)等光电子器件的理想材料。与其它宽带隙半导体材料相比,ZnO还具有资源丰富、原料成本低廉;环境友好,无毒无害;制膜方法简单多样,生长温度低;容易获得可作为衬底的半导体材料而实现同质外延;与湿法腐蚀工艺兼容,利于光电子集成等一系列优势。基于上述原因,针对氧化锌基半导体光电子材料的研究成为国际前沿和热点。而考虑到ZnO基材料可能满足国家在太空星际通讯等事关国防安全和国民经济发展的一系列重大问题上对短波长半导体激光器、紫外光电探测器等关键元器件战略需求。Wide bandgap semiconductors are called third-generation semiconductors because of their broad application prospects in solid-state lighting, short-wavelength semiconductor lasers, and ultraviolet light detection. ZnO is one of the representatives of wide bandgap semiconductor materials. It is a uniaxially symmetric direct bandgap semiconductor. The warm ionization energy (26meV) can ensure efficient exciton luminescence and low-threshold stimulated emission at room temperature. Therefore, ZnO is considered to be an ideal material for short-wavelength light-emitting diodes (LEDs), especially lasers (LDs) and other optoelectronic devices. Compared with other wide bandgap semiconductor materials, ZnO also has abundant resources and low cost of raw materials; it is environmentally friendly, non-toxic and harmless; the method of film formation is simple and diverse, and the growth temperature is low; it is easy to obtain semiconductor materials that can be used as substrates to achieve homogeneity Epitaxy; compatible with wet etching process, conducive to optoelectronic integration and other advantages. Based on the above reasons, research on ZnO-based semiconductor optoelectronic materials has become an international frontier and hot spot. Considering that ZnO-based materials may meet the country's strategic needs for key components such as short-wavelength semiconductor lasers and ultraviolet photodetectors on a series of major issues related to national defense security and national economic development such as space interstellar communications.
目前,国内外对ZnO的研究已经取得了一系列可喜的研究成果。继2004年日本科学家在低失配的铝镁酸钪衬底上获得ZnO同质结的电致发光后,2005年,发光学及应用国家重点实验室宽禁带II-VI族半导体研究组在国际上首次制备出基于蓝宝石衬底的ZnO同质pn结LED,并获得室温下的蓝紫色电致发光,随后,国内外许多研究组也相继报道了ZnO同质pn结以及基于量子阱结构的电致发光。值得一提的是Ryu等人以BeZnO为垒层,ZnO为阱层制备出量子阱型ZnO基的LED和LD,并获得紫外电致发光和激光发射,而我们于室温条件下在ZnO/GaN异质结构中也获得了属于ZnO的蓝紫波段的激光发射,其阈值电流仅0.8mA,这都说明ZnO基材料完全可以胜任紫外发光和低阈值紫外激光器件等短波光电器件的需要。At present, the research on ZnO at home and abroad has achieved a series of gratifying research results. After Japanese scientists obtained the electroluminescence of ZnO homojunction on a low-mismatch scandium aluminum magnesium oxide substrate in 2004, in 2005, the research group of wide-bandgap II-VI semiconductors of the State Key Laboratory of Luminescence and Applications in For the first time in the world, a ZnO homogeneous pn junction LED based on a sapphire substrate was prepared, and blue-violet electroluminescence at room temperature was obtained. Subsequently, many research groups at home and abroad have also reported ZnO homogeneous pn junctions and LEDs based on quantum well structures. Electroluminescence. It is worth mentioning that Ryu et al. used BeZnO as the barrier layer and ZnO as the well layer to prepare quantum well-type ZnO-based LEDs and LDs, and obtained ultraviolet electroluminescence and laser emission. The blue-violet band laser emission belonging to ZnO has also been obtained in the heterostructure, and its threshold current is only 0.8mA, which shows that ZnO-based materials are fully capable of meeting the needs of short-wave optoelectronic devices such as ultraviolet luminescence and low-threshold ultraviolet laser devices.
然而,由于ZnO中受主杂质的离化能高,使得传统方法制备的p型ZnO基材料性能不能满足器件需求。缺乏制备可重复性高、稳定、低阻、高迁移率的p型ZnO材料的方法和工艺仍旧是阻碍ZnO基光电子器件走出实验室的瓶颈所在。However, due to the high ionization energy of acceptor impurities in ZnO, the performance of p-type ZnO-based materials prepared by traditional methods cannot meet the device requirements. The lack of methods and processes for preparing p-type ZnO materials with high repeatability, stability, low resistance, and high mobility is still the bottleneck that prevents ZnO-based optoelectronic devices from going out of the laboratory.
传统的p型ZnO材料制备主要依赖于通过不同的技术手段将I族和V族元素分别或同时掺入材料内部,以期实现上述两族元素在ZnO中呈现受主态。但是,理论和实验结果表明,可应用于ZnO材料的受主杂质的受主激活能大多在200meV以上,而我们通过受主杂质离化率与受主激活能的关系不难得到,ZnO中的受主离化率还不足千分之一,根本无法有效提供空穴。于是人们不得不通过低温生长和重掺杂的方法来保证材料中有足够多的受主来提高空穴的浓度,然而,不论是降低生长温度和过量的杂质掺入都会引起材料结晶质量的恶化,加剧位错散射、中性杂质散射和电离杂质散射等对空穴传输的阻碍作用,直接影响材料的空穴迁移率和其它物理特性,并严重干扰材料性能的稳定性。也有人通过能带调制工程,期望降低受主能级,使受主杂质易于离化,但尚未得到可应用的有效技术手段。可以看到,受主激活能高是制备p型ZnO基材料的主要困难所在。如果有一种方法或工艺可以使p型ZnO掺杂摆脱高受主激活能的束缚,使空穴的产生不再依赖受主的“自发离化”,就可以在相对较低杂质掺杂浓度下获得较高的空穴浓度,提高受主杂质有效性,减少缺陷对空穴的阻碍,实现高效、稳定、可重复的p-ZnO。The traditional preparation of p-type ZnO materials mainly relies on the doping of group I and group V elements into the material through different technical means, respectively or simultaneously, in order to realize the acceptor state of the above two groups of elements in ZnO. However, theoretical and experimental results show that the acceptor activation energy of acceptor impurities that can be applied to ZnO materials is mostly above 200meV, and we can easily obtain the relationship between the ionization rate of acceptor impurities and the acceptor activation energy. The acceptor ionization rate is less than 1/1000, so it cannot effectively provide holes at all. Therefore, people have to use low-temperature growth and heavy doping to ensure that there are enough acceptors in the material to increase the concentration of holes. However, both lower growth temperature and excessive doping of impurities will cause the deterioration of the crystal quality of the material. , aggravate the hindering effect of dislocation scattering, neutral impurity scattering and ionized impurity scattering on hole transport, directly affect the hole mobility and other physical properties of the material, and seriously interfere with the stability of material performance. Some people also expect to reduce the acceptor energy level through energy band modulation engineering, so that acceptor impurities can be easily ionized, but no effective technical means have been obtained yet. It can be seen that the high activation energy of the acceptor is the main difficulty in preparing p-type ZnO-based materials. If there is a method or process that can make p-type ZnO doping get rid of the constraints of high acceptor activation energy, so that the generation of holes no longer depends on the "spontaneous ionization" of the acceptor, it can be obtained at a relatively low impurity doping concentration. Obtain higher hole concentration, improve the effectiveness of acceptor impurities, reduce the hindrance of defects to holes, and realize efficient, stable and repeatable p-ZnO.
发明内容Contents of the invention
本发明的目的是为了解决现有的氧化锌基p型材料的制备方法稳定性差、可重复性低的问题,而提供一种氧化锌基p型材料的制备方法。The object of the present invention is to provide a method for preparing a zinc oxide-based p-type material in order to solve the problems of poor stability and low repeatability of the existing zinc oxide-based p-type material preparation method.
本发明提供一种氧化锌基p型材料的制备方法,该方法包括:The invention provides a method for preparing a zinc oxide-based p-type material, the method comprising:
在基础层上制备渐变层;Prepare a gradient layer on top of the base layer;
在所述的渐变层上制备盖层;preparing a cover layer on the gradient layer;
所述的基础层为氧极性表面的MgxZn1-xO(0.6≥x≥0.2)材料,所述的基础层的厚度不小于5nm;The base layer is a Mg x Zn 1-x O (0.6≥x≥0.2) material with an oxygen polar surface, and the thickness of the base layer is not less than 5nm;
所述的渐变层具有组分渐变的结构,其结构自下而上表示为MgxZn1-xO/Mgx-δZn1-(x-δ)O/Mgx-2δZn1-(x-2δ)O/…/Mgx-(n-1)δZn1-[x-(n-1)δ]O/Mgx-nδZn1-(x-nδ)O(δ→0,n为自然数;nδ=x;简写为graded-MgZnO),所述渐变层厚度不大于1μm;The graded layer has a composition graded structure, and its structure is expressed as Mg x Zn 1-x O/Mg x-δ Zn 1-(x-δ) O/Mg x-2δ Zn 1-( x-2δ) O/.../Mg x-(n-1)δ Zn 1-[x-(n-1)δ] O/Mg x-nδ Zn 1-(x-nδ) O(δ→0, n is a natural number; nδ=x; abbreviated as graded-MgZnO), the thickness of the graded layer is not greater than 1 μm;
所述的盖层的材料为ZnO,盖层的厚度不小于300nm。The material of the cover layer is ZnO, and the thickness of the cover layer is not less than 300nm.
优选的是,所述的基础层的厚度为20-50nm。Preferably, the thickness of the base layer is 20-50nm.
优选的是,所述的渐变层的厚度为50nm~200nm。Preferably, the gradient layer has a thickness of 50nm-200nm.
优选的是,所述的盖层的厚度为1μm~3μm。Preferably, the thickness of the cover layer is 1 μm-3 μm.
优选的是,所述的基础层是在衬底上制备得到的。Preferably, the base layer is prepared on a substrate.
本发明的原理Principle of the invention
本发明提供一种氧化锌基p型材料的制备方法,该方法是通过在氧极性面的MgxZn1-xO材料上生长组分渐变的graded-MgZnO材料层,使材料内部产生的压电极化和自发极化方向一致,在两种极化的共同作用下,组分相邻的Mgy-δZn1-(y-δ)O/MgyZn1-yO(y为δ至nδ间任一值,δ→0)高镁组分一侧会产生电荷积累,电荷积累的量随着graded-MgZnO材料层厚度的增加而增加,而由于电荷积累所形成的电场会使能带发生倾斜,为了中和由极化产生的电荷和小能带倾斜,使体系处于平衡态,受主将被迫离化并产生空穴,这些空穴最终将在graded-MgZnO材料层一侧富集并形成三维空穴层,并以载流子身份进行工作。本发明的方法在没有受主杂质掺入的情况下,只通过异质结构产生的场致空穴注入就可以实现空穴注入;而对于有受主杂质掺入的材料,只要极化电荷积累充足,多数受主都会离化,而这种离化不会受到离化能的限制,同样由于不受受主离化能的影响,利用极化诱导方法获得的p-ZnO基材料其空穴浓度受温度影响不大,这使它具有良好的温度稳定性。The invention provides a method for preparing a zinc oxide-based p-type material. The method is to grow a graded-MgZnO material layer with a gradually changing composition on the Mg x Zn 1-x O material on the oxygen polar surface, so that the material is generated inside the material. The directions of piezoelectric polarization and spontaneous polarization are consistent, and under the combined action of the two polarizations, the adjacent Mg y-δ Zn 1-(y-δ) O/Mg y Zn 1-y O (y is Any value between δ to nδ, δ→0) Charge accumulation will occur on the high magnesium component side, and the amount of charge accumulation increases with the increase of the thickness of the graded-MgZnO material layer, and the electric field formed due to charge accumulation will make The energy band is tilted, in order to neutralize the charge generated by the polarization and the small energy band tilt, so that the system is in an equilibrium state, the acceptor will be forced to ionize and generate holes, and these holes will eventually be on the side of the graded-MgZnO material layer Enrich and form a three-dimensional hole layer, and work as carriers. The method of the present invention can achieve hole injection only through the field-induced hole injection generated by the heterostructure without the doping of acceptor impurities; and for materials doped with acceptor impurities, as long as the polarization charge accumulation Sufficient, most acceptors will ionize, and this ionization will not be limited by the ionization energy, also because it is not affected by the main ionization energy, the p-ZnO-based material obtained by the polarization induction method has a hole The concentration is not greatly affected by temperature, which makes it have good temperature stability.
本发明的有益效果Beneficial effects of the present invention
本发明提供一种氧化锌基p型材料的制备方法,该方法将极化诱导方法应用于ZnO基宽禁带材料体系,进行p型ZnO基材料的制备,极化诱导方法利用极化作用积累的电荷和电场促进受主的离化,它的应用使ZnO基材料摆脱了受主离化能高的限制,与传统方法“坐等”受主“自发离化”相比,可谓“主动出击”;通过极化诱导的办法,可以大大提高受主的离化率和受主杂质的掺杂效率,解决ZnO基材料p型掺杂的难题,本发明的方法可重复性高,同时由于不受受主离化能的影响,通过该方法制备的材料电学性能受温度影响不大,具有较好的温度稳定性。The invention provides a method for preparing a zinc oxide-based p-type material. The method applies a polarization induction method to a ZnO-based wide bandgap material system to prepare a p-type ZnO-based material. The polarization induction method utilizes polarization accumulation The charge and electric field promote the ionization of acceptors, and its application makes ZnO-based materials get rid of the limitation of high ionization energy of acceptors. Compared with the traditional method of "spontaneous ionization" of "sit and wait" acceptors, it can be called "active attack". ; By means of polarization induction, the ionization rate of the acceptor and the doping efficiency of the acceptor impurity can be greatly improved, and the difficult problem of p-type doping of ZnO-based materials can be solved. Affected by the main ionization energy, the electrical properties of the material prepared by this method are not greatly affected by temperature, and have good temperature stability.
附图说明Description of drawings
图1为本发明制备方法得到的氧化锌基p型材料的结构示意图。Fig. 1 is a schematic structural view of the zinc oxide-based p-type material obtained by the preparation method of the present invention.
图2为本发明方法制备的ZnO基p型材料中渐变层中Mg和Zn组分随渐变层厚度的变化的关系曲线。Fig. 2 is a graph showing the relationship between the Mg and Zn components in the graded layer of the ZnO-based p-type material prepared by the method of the present invention and the thickness of the graded layer.
具体实施方式detailed description
本发明提供一种氧化锌基p型材料的制备方法,如图1所示,该方法包括:The present invention provides a kind of preparation method of zinc oxide-based p-type material, as shown in Figure 1, the method comprises:
在基础层102上制备渐变层103;Prepare a gradient layer 103 on the base layer 102;
在所述的渐变层103上制备盖层104;Prepare a cover layer 104 on the gradient layer 103;
所述的基础层102为氧极性表面的MgxZn1-xO材料,所述的基础层的厚度不小于5nm,优选为20-50nm,须使其自身具有完整结构,对后续结构的极性实现控制;The base layer 102 is a Mg x Zn 1-x O material with an oxygen polar surface, and the thickness of the base layer is not less than 5 nm, preferably 20-50 nm. polarity control;
所述的渐变层103具有组分渐变结构,渐变层Mg组分从基础层中的x(0.6≥x≥0.2)随厚度变化逐渐减至0,其结构自下而上可表示为MgxZn1-xO/Mgx-δZn1-(x-δ)O/Mgx-2δZn1-(x-2δ)O/…/Mgx-(n-1)δZn1-[x-(n-1)δ]O/Mgx-nδZn1-(x-nδ)O(ZnO)(δ→0,n为自然数;nδ=x;简写为graded-MgZnO),δ是0-1间某一趋近于0的数值,以保证Mg组分从x以某一梯度值连续变化,可认为是Mg组分的梯度,渐变层下表面Mg组分与基础层一致,即MgxZn1-xO(0.6≥x≥0.2),渐变层上表面Mg含量为0,即ZnO,所述渐变层厚度不大于1μm(微米),优选为50nm~200nm;The gradient layer 103 has a composition gradient structure, and the Mg composition of the gradient layer gradually decreases from x (0.6≥x≥0.2) in the base layer to 0 as the thickness changes, and its structure can be expressed as Mg x Zn from bottom to top 1-x O/Mg x-δ Zn 1-(x-δ) O/Mg x-2δ Zn 1-(x-2δ) O/…/Mg x-(n-1)δ Zn 1-[x- (n-1)δ] O/Mg x-nδ Zn 1-(x-nδ) O(ZnO) (δ→0, n is a natural number; nδ=x; abbreviated as graded-MgZnO), δ is 0-1 A certain value close to 0 in order to ensure that the Mg composition changes continuously from x with a certain gradient value, which can be considered as the gradient of the Mg composition. The Mg composition on the lower surface of the gradient layer is consistent with the base layer, that is, Mg x Zn 1-x O (0.6≥x≥0.2), the Mg content on the upper surface of the gradient layer is 0, that is, ZnO, and the thickness of the gradient layer is not greater than 1 μm (micrometer), preferably 50nm to 200nm;
所述的盖层104的材料为ZnO,盖层的厚度不小于300nm,优选范围为1μm~3μm,须使其自身具有完整晶格结构,并对渐变层晶格产生束缚,使渐变层中压电极化与材料自发极化方向一致。The material of the cover layer 104 is ZnO, and the thickness of the cover layer is not less than 300nm, preferably in the range of 1 μm to 3 μm. The electric polarization is in the same direction as the spontaneous polarization of the material.
本发明所述的基础层102可以独立存在,优选是在衬底101上制备得到的。The base layer 102 of the present invention can exist independently, and is preferably prepared on the substrate 101 .
本发明所述基础层102、渐变层103和盖层104均为氧极性。The base layer 102, gradient layer 103 and cover layer 104 of the present invention are all oxygen polar.
本发明所述的渐变层的材料的制备为现有技术,本发明所述渐变层不是唯一的,也可以为除Mg外的其它金属与ZnO的合金,如BexZn1-xO/Bex-δZn1-(x-δ)O/Bex-2δZn1-(x-2δ)O/…/Bex-(n-1)δZn1-[x-(n-1)δ]O/Bex-nδZn1-(x-nδ)O(ZnO)(δ→0,n为自然数;nδ=x),但选取基础层和盖层应与渐变层相匹配,使整个结构中的自发极化与压电极化方向一致。本发明所述基础层可进行已知的ZnO受主杂质掺杂,例如,受主杂质可为:N、P、As、Sb等V族元素,或Li、Na、K等I族元素。The preparation of the material of the graded layer of the present invention is prior art, the graded layer of the present invention is not unique, also can be the alloy of other metals except Mg and ZnO, as Be x Zn 1-x O/Be x-δ Zn 1-(x-δ) O/Be x-2δ Zn 1-(x-2δ) O/…/Be x-(n-1)δ Zn 1-[x-(n-1)δ ] O/Be x-nδ Zn 1-(x-nδ) O(ZnO) (δ→0, n is a natural number; nδ=x), but the selected base layer and cover layer should match the gradient layer, so that the whole structure The spontaneous polarization in is in the same direction as the piezoelectric polarization. The base layer of the present invention can be doped with known ZnO acceptor impurities. For example, the acceptor impurities can be group V elements such as N, P, As, Sb, or group I elements such as Li, Na, and K.
图2为本发明方法制备的ZnO基p型材料中渐变层中Mg和Zn组分随厚度的变化的关系曲线,图中横轴表示组分,纵轴表示从衬底表面算起的厚度,X指渐变层上表面中Mg的组分,曲线201表示的是Mg组分随厚度的变化,曲线202所示的是Zn组分随厚度的变化,曲线201和曲线202是与右侧的结构有对应关系的。从曲线201中,我们可以看到,Mg组分随渐变层厚度逐渐从X减少到0,相应地,曲线202中所示Zn组分随渐变层厚度增加而逐渐从(1-X)增加到1,注意到,这种变化趋势是呈线性变化的。这样,基础层可以实现对渐变层下表面的晶格束缚,渐变层中相邻Mgy-δZn1-(y-δ)O/MgyZn1-yO(y为δ至nδ间任一值,δ→0)层间的自发极化和压电极化同向迭加,盖层对渐变层上表面进行束缚。Fig. 2 is the relationship curve of the change of Mg and Zn composition with the thickness in the graded layer in the ZnO-based p-type material prepared by the inventive method, in the figure, the horizontal axis represents the composition, and the vertical axis represents the thickness counted from the substrate surface, X refers to the composition of Mg in the upper surface of the gradient layer. Curve 201 shows the change of Mg composition with thickness, and curve 202 shows the change of Zn composition with thickness. Curve 201 and curve 202 are the structures on the right There is a corresponding relationship. From the curve 201, we can see that the Mg composition gradually decreases from X to 0 with the thickness of the gradient layer, and correspondingly, the Zn composition shown in the curve 202 gradually increases from (1-X) to 1. Note that this trend is linear. In this way, the base layer can realize lattice restraint to the lower surface of the graded layer, and in the graded layer, adjacent Mg y-δ Zn 1-(y-δ) O/Mg y Zn 1-y O (y is any One value, δ→0) The spontaneous polarization and piezoelectric polarization between the layers are superimposed in the same direction, and the capping layer binds the upper surface of the gradient layer.
下面结合实施例对本发明做进一步详细的描述。The present invention will be further described in detail below in conjunction with the examples.
实施例1Example 1
用MOCVD制备极化诱导p型ZnO材料的具体实施方法The specific implementation method of preparing polarization-induced p-type ZnO material by MOCVD
锌源采用二乙基锌、镁源采用二甲基二茂镁、氧源采用氧气,锌源、镁源盛装于鼓泡瓶中,通过载气(氮气)将鼓泡瓶中的有效成份带出,本实施例中MOCVD系统有机源管路为标准管路,故通入反应腔室的源的量与源的温度和载气流量有关(源的温度越高、载气流量越大,通入反应腔室的源的量越多)。Zinc source adopts diethyl zinc, magnesium source adopts dimethyl dimagnesocene, oxygen source adopts oxygen, zinc source and magnesium source are contained in bubble bottles, and the active ingredients in the bubble bottles are carried by carrier gas (nitrogen) It can be seen that the organic source pipeline of the MOCVD system in this embodiment is a standard pipeline, so the amount of the source passed into the reaction chamber is related to the temperature of the source and the flow rate of the carrier gas (the higher the temperature of the source, the greater the flow rate of the carrier gas, the greater the flow rate of the carrier gas through the greater the amount of source that enters the reaction chamber).
步骤1,衬底准备:将氧极性的C面蓝宝石衬底洗净,置于MOCVD反应腔室中(对应图1中所示101)Step 1, substrate preparation: clean the C-plane sapphire substrate with oxygen polarity, and place it in the MOCVD reaction chamber (corresponding to 101 shown in Figure 1)
步骤2,在蓝宝石衬底表面进行MgxZn1-xO基础层的生长:锌源温度为0℃,载气流量10sccm,氧气流量60sccm;镁源70℃,载气流量20sccm。在渐变层表面生长30nm的基础层。MgxZn1-xO中Mg组分为30%,即Mg0.3Zn0.7O,为氧极性(对应图1中所示102)Step 2, growing the Mg x Zn 1-x O base layer on the surface of the sapphire substrate: zinc source temperature is 0°C, carrier gas flow rate is 10 sccm, oxygen flow rate is 60 sccm; magnesium source is 70°C, carrier gas flow rate is 20 sccm. A 30nm base layer is grown on the surface of the graded layer. The Mg component in Mg x Zn 1-x O is 30%, that is, Mg 0.3 Zn 0.7 O, which is oxygen polarity (corresponding to 102 shown in Figure 1)
步骤3,在基础层上进行渐变层的生长:保持锌源温度为0℃,载气流量10sccm,氧气流量60sccm,继续通入反应室;同时将镁源通入反应腔室,镁源温度从70℃以0.05℃/5s速率降温至20℃,载气流量20sccm,由于源温的下降,反应腔室中镁源含量逐渐减少,使得所制备的薄膜中镁的含量逐渐减少。在基础层上生长70nm的渐变层。(对应图1中所示103)Step 3, grow the gradient layer on the base layer: keep the temperature of the zinc source at 0°C, the flow rate of the carrier gas at 10 sccm, and the flow rate of oxygen at 60 sccm, and continue to pass into the reaction chamber; at the same time, the magnesium source is passed into the reaction chamber, and the temperature of the magnesium source is from The temperature was lowered from 70°C to 20°C at a rate of 0.05°C/5s, and the carrier gas flow rate was 20sccm. Due to the decrease of source temperature, the content of magnesium source in the reaction chamber gradually decreased, so that the content of magnesium in the prepared film gradually decreased. A 70nm graded layer is grown on the base layer. (corresponding to 103 shown in Figure 1)
步骤4,在渐变层上进行ZnO盖层的生长:保持锌源温度为0℃,载气流量为10sccm,氧气流量为60sccm,停止通入镁源。在渐变层上沉积1μm厚的Zn极性表面ZnO基础层(对应图1中所示104)。Step 4, growing the ZnO capping layer on the graded layer: keep the temperature of the zinc source at 0° C., the flow rate of the carrier gas at 10 sccm, the flow rate of oxygen at 60 sccm, and stop feeding the magnesium source. A 1 μm thick Zn polar surface ZnO base layer (corresponding to 104 shown in FIG. 1 ) is deposited on the graded layer.
以上实施例的说明只是用于帮助理解本发明的方法及其核心思想。应当指出,对于本技术领域的普通技术人员来说,在不脱离本发明原理的前提下,还可以对本发明进行若干改进和修饰,这些改进和修饰也落入本发明权利要求的保护范围内。The descriptions of the above embodiments are only used to help understand the method and core idea of the present invention. It should be pointed out that for those skilled in the art, without departing from the principles of the present invention, some improvements and modifications can be made to the present invention, and these improvements and modifications also fall within the protection scope of the claims of the present invention.
对所公开的实施例的上述说明,使本领域专业技术人员能够实现或使用本发明。对这些实施例的多种修改对本领域的专业技术人员来说将是显而易见的,本文中所定义的一般原理可以在不脱离本发明的精神或范围的情况下,在其它实施例中实现。因此,本发明将不会被限制于本文所示的这些实施例,而是要符合与本文所公开的原理和新颖特点相一致的最宽的范围。The above description of the disclosed embodiments is provided to enable any person skilled in the art to make or use the invention. Various modifications to these embodiments will be readily apparent to those skilled in the art, and the general principles defined herein may be implemented in other embodiments without departing from the spirit or scope of the invention. Therefore, the present invention will not be limited to the embodiments shown herein, but is to be accorded the widest scope consistent with the principles and novel features disclosed herein.
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