CN111470528A - Tin-containing semiconductor material and preparation method thereof - Google Patents
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- 239000004065 semiconductor Substances 0.000 title claims abstract description 54
- 239000000463 material Substances 0.000 title claims abstract description 44
- ATJFFYVFTNAWJD-UHFFFAOYSA-N Tin Chemical compound [Sn] ATJFFYVFTNAWJD-UHFFFAOYSA-N 0.000 title claims abstract description 39
- 238000002360 preparation method Methods 0.000 title claims abstract description 17
- LYQFWZFBNBDLEO-UHFFFAOYSA-M caesium bromide Chemical compound [Br-].[Cs+] LYQFWZFBNBDLEO-UHFFFAOYSA-M 0.000 claims abstract description 26
- 239000013078 crystal Substances 0.000 claims abstract description 25
- 239000002184 metal Substances 0.000 claims abstract description 14
- 229910052751 metal Inorganic materials 0.000 claims abstract description 14
- 150000002736 metal compounds Chemical class 0.000 claims abstract description 12
- 238000010438 heat treatment Methods 0.000 claims abstract description 4
- 239000011261 inert gas Substances 0.000 claims abstract description 3
- 238000001816 cooling Methods 0.000 claims abstract 2
- 238000000034 method Methods 0.000 claims description 13
- KLRHPHDUDFIRKB-UHFFFAOYSA-M indium(i) bromide Chemical compound [Br-].[In+] KLRHPHDUDFIRKB-UHFFFAOYSA-M 0.000 claims description 6
- 150000003606 tin compounds Chemical class 0.000 claims description 6
- ADZWSOLPGZMUMY-UHFFFAOYSA-M silver bromide Chemical compound [Ag]Br ADZWSOLPGZMUMY-UHFFFAOYSA-M 0.000 claims description 5
- 150000002472 indium compounds Chemical class 0.000 claims description 4
- 229940100890 silver compound Drugs 0.000 claims description 4
- 150000003379 silver compounds Chemical class 0.000 claims description 4
- 229910052738 indium Inorganic materials 0.000 claims description 3
- APFVFJFRJDLVQX-UHFFFAOYSA-N indium atom Chemical compound [In] APFVFJFRJDLVQX-UHFFFAOYSA-N 0.000 claims description 3
- 229910052709 silver Inorganic materials 0.000 claims description 2
- 239000004332 silver Substances 0.000 claims description 2
- ZSUXOVNWDZTCFN-UHFFFAOYSA-L Tin(II) bromide Inorganic materials Br[Sn]Br ZSUXOVNWDZTCFN-UHFFFAOYSA-L 0.000 claims 4
- 239000000126 substance Substances 0.000 claims 2
- 229910021623 Tin(IV) bromide Inorganic materials 0.000 claims 1
- 239000002178 crystalline material Substances 0.000 claims 1
- 239000007858 starting material Substances 0.000 claims 1
- 230000007547 defect Effects 0.000 abstract description 10
- 230000003247 decreasing effect Effects 0.000 abstract 1
- IJGRMHOSHXDMSA-UHFFFAOYSA-N Atomic nitrogen Chemical compound N#N IJGRMHOSHXDMSA-UHFFFAOYSA-N 0.000 description 22
- 239000007787 solid Substances 0.000 description 12
- 229910052757 nitrogen Inorganic materials 0.000 description 11
- 239000003708 ampul Substances 0.000 description 7
- PCHJSUWPFVWCPO-UHFFFAOYSA-N gold Chemical compound [Au] PCHJSUWPFVWCPO-UHFFFAOYSA-N 0.000 description 7
- 229910052737 gold Inorganic materials 0.000 description 7
- 239000010931 gold Substances 0.000 description 7
- 230000005355 Hall effect Effects 0.000 description 5
- 239000012298 atmosphere Substances 0.000 description 5
- 239000000969 carrier Substances 0.000 description 5
- 239000011521 glass Substances 0.000 description 5
- 239000000203 mixture Substances 0.000 description 5
- 238000000137 annealing Methods 0.000 description 4
- 150000001768 cations Chemical class 0.000 description 4
- 150000004820 halides Chemical class 0.000 description 4
- 239000012299 nitrogen atmosphere Substances 0.000 description 4
- 238000001894 space-charge-limited current method Methods 0.000 description 4
- 238000002441 X-ray diffraction Methods 0.000 description 3
- 230000000052 comparative effect Effects 0.000 description 3
- -1 formamidine cations Chemical class 0.000 description 3
- 239000007788 liquid Substances 0.000 description 3
- 239000000843 powder Substances 0.000 description 3
- 238000006243 chemical reaction Methods 0.000 description 2
- 239000000047 product Substances 0.000 description 2
- 239000002994 raw material Substances 0.000 description 2
- 239000010409 thin film Substances 0.000 description 2
- BAVYZALUXZFZLV-UHFFFAOYSA-O Methylammonium ion Chemical compound [NH3+]C BAVYZALUXZFZLV-UHFFFAOYSA-O 0.000 description 1
- BQCADISMDOOEFD-UHFFFAOYSA-N Silver Chemical compound [Ag] BQCADISMDOOEFD-UHFFFAOYSA-N 0.000 description 1
- 229910008449 SnF 2 Inorganic materials 0.000 description 1
- QVGXLLKOCUKJST-UHFFFAOYSA-N atomic oxygen Chemical compound [O] QVGXLLKOCUKJST-UHFFFAOYSA-N 0.000 description 1
- 230000009286 beneficial effect Effects 0.000 description 1
- 239000006227 byproduct Substances 0.000 description 1
- 229910052793 cadmium Inorganic materials 0.000 description 1
- BDOSMKKIYDKNTQ-UHFFFAOYSA-N cadmium atom Chemical compound [Cd] BDOSMKKIYDKNTQ-UHFFFAOYSA-N 0.000 description 1
- 229910052792 caesium Inorganic materials 0.000 description 1
- 239000003153 chemical reaction reagent Substances 0.000 description 1
- 150000001875 compounds Chemical class 0.000 description 1
- 238000009792 diffusion process Methods 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 238000011049 filling Methods 0.000 description 1
- 229910052732 germanium Inorganic materials 0.000 description 1
- GNPVGFCGXDBREM-UHFFFAOYSA-N germanium atom Chemical compound [Ge] GNPVGFCGXDBREM-UHFFFAOYSA-N 0.000 description 1
- 238000000227 grinding Methods 0.000 description 1
- 229910052736 halogen Inorganic materials 0.000 description 1
- 229910001502 inorganic halide Inorganic materials 0.000 description 1
- 238000011031 large-scale manufacturing process Methods 0.000 description 1
- 239000012263 liquid product Substances 0.000 description 1
- 230000008018 melting Effects 0.000 description 1
- 238000002844 melting Methods 0.000 description 1
- 230000003287 optical effect Effects 0.000 description 1
- 150000002892 organic cations Chemical class 0.000 description 1
- 239000001301 oxygen Substances 0.000 description 1
- 229910052760 oxygen Inorganic materials 0.000 description 1
- 239000002245 particle Substances 0.000 description 1
- 239000008188 pellet Substances 0.000 description 1
- 238000005191 phase separation Methods 0.000 description 1
- 239000011148 porous material Substances 0.000 description 1
- 238000000634 powder X-ray diffraction Methods 0.000 description 1
- 230000006798 recombination Effects 0.000 description 1
- 238000005215 recombination Methods 0.000 description 1
- 230000001105 regulatory effect Effects 0.000 description 1
- 238000004528 spin coating Methods 0.000 description 1
- 231100000701 toxic element Toxicity 0.000 description 1
- 238000007740 vapor deposition Methods 0.000 description 1
- 239000002699 waste material Substances 0.000 description 1
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- C01G19/00—Compounds of tin
- C01G19/006—Compounds containing tin, with or without oxygen or hydrogen, and containing two or more other elements
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Abstract
本发明公开了一种含锡半导体材料及其制备方法。所述的半导体材料为一种在CsSnBr3的制备过程中通过添加金属单质或金属化合物进行掺杂生长出的不同载流子浓度的晶体。制备方法为:将CsBr、SnBr2与金属单质或金属化合物混合,在惰性气体保护下加热反应,缓慢冷却后得到具有不同载流子浓度的CsSnBr3半导体晶体材料。在制备过程添加单质锡的CsSnBr3半导体与未添加时相比,其载流子浓度下降1个数量级,缺陷态密度显著减少。掺杂铟的CsSnBr3半导体具有1010cm‑3浓度的载流子,接近本征半导体;掺杂银的CsSnBr3半导体具有1019cm‑3浓度的p型载流子,成为简并半导体。
The invention discloses a tin-containing semiconductor material and a preparation method thereof. The semiconductor material is a crystal with different carrier concentrations grown by adding a metal element or a metal compound during the preparation process of CsSnBr 3 . The preparation method is as follows: mixing CsBr and SnBr 2 with a metal element or metal compound, heating and reacting under the protection of an inert gas, and slowly cooling to obtain CsSnBr 3 semiconductor crystal materials with different carrier concentrations. Compared with the CsSnBr 3 semiconductor with elemental tin added during the preparation process, its carrier concentration decreased by one order of magnitude, and the defect state density was significantly reduced. The indium-doped CsSnBr 3 semiconductor has a carrier concentration of 10 10 cm -3 , which is close to an intrinsic semiconductor; the silver-doped CsSnBr 3 semiconductor has a p-type carrier concentration of 10 19 cm -3 , becoming a degenerate semiconductor.
Description
技术领域technical field
本发明涉及一种新型含锡半导体材料,通过改变CsSnBr3钙钛矿材料的制备条件和掺杂元素,得到一系列具有不同载流子浓度的半导体材料,属于新材料技术领域。The invention relates to a novel tin-containing semiconductor material. By changing the preparation conditions and doping elements of the CsSnBr3 perovskite material, a series of semiconductor materials with different carrier concentrations are obtained, which belongs to the technical field of new materials.
背景技术Background technique
近年来,卤化物钙钛矿材料由于其优异的半导体性质和不断提升的光电转化性能而备受关注。在卤化物钙钛矿材料的ABX3结构中,A位元素一般为大离子半径的甲铵、甲脒阳离子或铯离子,B位一般为铅、锡和锗的二价阳离子,X为卤素阴离子。B位阳离子与六个卤素阴离子形成共顶点的八面体,A位阳离子位于八面体之间的空隙内,构成钙钛矿结构。In recent years, halide perovskite materials have attracted much attention due to their excellent semiconducting properties and improving photoelectric conversion performance. In the ABX 3 structure of halide perovskite materials, the A-site elements are generally methylammonium, formamidine cations or cesium ions with large ionic radius, the B-sites are generally divalent cations of lead, tin and germanium, and X is a halogen anion . The B-site cations and six halide anions form a common vertex octahedron, and the A-site cations are located in the gaps between the octahedrons, forming a perovskite structure.
为了研究卤化物钙钛矿材料的性质,目前通常使用旋涂和气相沉积来产生薄膜。但如此获得的微晶薄膜材料有较多的孔隙、晶界夹杂物和其他缺陷,不但阻碍载流子在钙钛矿材料中的传输,同时还使得钙钛矿在环境中快速降解。相比之下,单晶块体钙钛矿材料可以具有更高的载流子迁移率,更长的载流子扩散长度,同时也更高的对环境中水分和氧气的稳定性。含有有机阳离子的卤化物钙钛矿通常从溶液中生长,而全无机卤化物钙钛矿在熔化时不分解,更适合用布里奇曼法来生长单晶。例如,CsPbBr3已经通过布里奇曼法获得了大尺寸高质量的单晶。(Adv.Optical Mater.2017,5,1700157;Nat.Commun.2018,9,1609;J.Phys.Chem.Lett.2018,9,5040)但含铅钙钛矿材料容易污染环境、危害人体健康,因而被RoHS标准禁止,在实际应用过程中受到巨大的限制,而使用锡取代铅作为B位阳离子可以获得一类新的钙钛矿材料。To study the properties of halide perovskite materials, spin coating and vapor deposition are currently commonly used to produce thin films. However, the microcrystalline thin film material thus obtained has many pores, grain boundary inclusions and other defects, which not only hinder the transport of carriers in the perovskite material, but also make the perovskite degrade rapidly in the environment. In contrast, single-crystal bulk perovskite materials can have higher carrier mobility, longer carrier diffusion lengths, and higher stability to ambient moisture and oxygen. Halide perovskites containing organic cations are usually grown from solution, whereas all-inorganic halide perovskites do not decompose upon melting and are more suitable for growing single crystals using the Bridgman method. For example, CsPbBr3 has obtained large-sized and high-quality single crystals by the Bridgeman method. (Adv.Optical Mater.2017,5,1700157; Nat.Commun.2018,9,1609; J.Phys.Chem.Lett.2018,9,5040) But lead-containing perovskite materials are easy to pollute the environment and endanger human health , thus banned by the RoHS standard and subject to huge restrictions in practical applications, while the use of tin instead of lead as the B-site cation can lead to a new class of perovskite materials.
CsSnBr3在室温以立方相稳定存在,有良好的热稳定性,能够被空气钝化,而且带隙大小适合制备光电转化器件(Angew.Chem.Int.Ed.2018,57,13154)。需要注意到与铅元素不同的是,锡元素同时稳定存在Sn2+与Sn4+两种价态,这使得含锡钙钛矿材料容易包含Sn4 +,产生Sn空位缺陷和对应的p型掺杂(J.Am.Chem.Soc.2012,134,8579;J.Phys.Chem.C.2018,122,13926)。对半导体掺杂能够提升材料的电导率,但将加速电子和空穴的复合。因此,根据不同的应用方向来调节含锡钙钛矿材料的掺杂状态是目前的一个重要研究方向。有报道(Adv.Mater.2014,26,7122)在生长CsSnI3晶体时加入20%摩尔比的SnF2,能够使其载流子浓度由1019cm-3降低至1017cm-3,但如此高的添加比例已经超过了正常的掺杂浓度范围,而且对载流子浓度的调节效果还不够显著。CsSnBr 3 exists stably in a cubic phase at room temperature, has good thermal stability, can be passivated by air, and has a band gap suitable for the preparation of photoelectric conversion devices (Angew. Chem. Int. Ed. 2018, 57, 13154). It should be noted that, unlike the lead element, the tin element has two stable valence states of Sn 2+ and Sn 4+ at the same time, which makes the tin-containing perovskite materials easy to contain Sn 4+ , resulting in Sn vacancy defects and corresponding p-type Doping (J.Am.Chem.Soc. 2012, 134, 8579; J. Phys. Chem. C. 2018, 122, 13926). Doping a semiconductor can improve the conductivity of the material, but it will speed up the recombination of electrons and holes. Therefore, it is an important research direction to adjust the doping state of tin-containing perovskite materials according to different application directions. It has been reported (Adv.Mater.2014, 26, 7122) that adding 20% molar ratio of SnF 2 during the growth of CsSnI 3 crystal can reduce the carrier concentration from 10 19 cm -3 to 10 17 cm -3 , but Such a high addition ratio has exceeded the normal doping concentration range, and the adjustment effect on the carrier concentration is not significant enough.
发明内容SUMMARY OF THE INVENTION
本发明所要解决的技术问题是:提供一种含锡半导体材料及其制备方法,通过改变制备和掺杂条件来调控半导体中的载流子浓度。The technical problem to be solved by the present invention is to provide a tin-containing semiconductor material and a preparation method thereof, which can control the carrier concentration in the semiconductor by changing the preparation and doping conditions.
为了解决上述问题,本发明提供了一种含锡半导体材料,其特征在于,为一种在CsSnBr3的制备过程中通过添加金属单质或金属化合物进行掺杂生长出的不同载流子浓度的晶体。In order to solve the above problems, the present invention provides a tin-containing semiconductor material, which is characterized in that it is a crystal with different carrier concentrations grown by adding a metal element or a metal compound for doping during the preparation process of CsSnBr 3 .
优选地,上述含锡半导体材料的原料包括CsBr、SnBr2及金属单质或金属化合物。Preferably, the raw materials of the above-mentioned tin-containing semiconductor material include CsBr, SnBr 2 and metal element or metal compound.
更优选地,所述的金属单质或金属化合物为锡单质或四价锡化合物、铟单质或铟化合物和银单质或银化合物中的任意一种或几种。More preferably, the metal element or metal compound is any one or more of tin element or tetravalent tin compound, indium element or indium compound and silver element or silver compound.
进一步地,所述的四价锡化合物为SnBr4或Cs2SnBr6。Further, the tetravalent tin compound is SnBr 4 or Cs 2 SnBr 6 .
进一步地,所述的铟化合物为InBr。Further, the indium compound is InBr.
进一步地,所述的银化合物为AgBr。Further, the silver compound is AgBr.
进一步地,所述的锡单质的质量不小于CsBr与SnBr2的质量之和。Further, the mass of the tin element is not less than the sum of the mass of CsBr and SnBr 2 .
进一步地,所述的四价锡化合物、其它金属单质或金属化合物的摩尔数不大于SnBr2摩尔数的5%。Further, the mole number of the tetravalent tin compound, other metal element or metal compound is not more than 5% of the mole number of SnBr 2 .
本发明还提供了上述含锡半导体材料的制备方法,其特征在于,将CsBr、SnBr2与金属单质或金属化合物混合,在惰性气体保护下加热反应,缓慢冷却后得到具有不同载流子浓度的CsSnBr3半导体晶体材料。The present invention also provides a method for preparing the above-mentioned tin-containing semiconductor material, which is characterized in that CsBr and SnBr 2 are mixed with a metal element or a metal compound, heated and reacted under the protection of an inert gas, and slowly cooled to obtain compounds with different carrier concentrations. CsSnBr 3 semiconductor crystal material.
与现有技术相比,本发明的有益效果是:Compared with the prior art, the beneficial effects of the present invention are:
1.本发明通过在CsSnBr3半导体材料中掺杂In元素,使其载流子浓度下降了6个数量级,接近本征半导体的水平。1. In the present invention, by doping In element in the CsSnBr 3 semiconductor material, the carrier concentration is reduced by 6 orders of magnitude, which is close to the level of the intrinsic semiconductor.
2.本发明通过在CsSnBr3半导体材料的制备过程中添加单质锡,使其载流子浓度下降了1个数量级,缺陷态密度显著降低。2. In the present invention, by adding elemental tin during the preparation of the CsSnBr 3 semiconductor material, the carrier concentration is reduced by one order of magnitude, and the defect state density is significantly reduced.
3.本发明通过在CsSnBr3半导体材料中掺杂Ag元素,使其载流子浓度上升了3个数量级,达到了简并半导体的水平。3. In the present invention, by doping Ag element in the CsSnBr 3 semiconductor material, the carrier concentration is increased by 3 orders of magnitude, reaching the level of degenerate semiconductor.
4.本发明提供了在1010至1019cm-3范围内调控含锡半导体材料的载流子浓度的方法。4. The present invention provides a method for regulating the carrier concentration of the tin-containing semiconductor material in the range of 10 10 to 10 19 cm -3 .
5.本发明中的掺杂含锡半导体材料不包含有毒元素铅或镉。5. The doped tin-containing semiconductor material in the present invention does not contain the toxic elements lead or cadmium.
6.本发明中的掺杂含锡半导体材料制备方法简单,不产生废液或副产物,适合规模化生产。6. The preparation method of the doped tin-containing semiconductor material in the present invention is simple, does not generate waste liquid or by-products, and is suitable for large-scale production.
附图说明Description of drawings
图1为金属锡处理的CsSnBr3晶体照片;Fig. 1 is the CsSnBr 3 crystal photograph of metal tin treatment;
图2为金属锡处理的CsSnBr3晶体与粉末的X射线衍射图谱;Fig. 2 is the X-ray diffraction pattern of CsSnBr crystal and powder treated with metal tin;
图3为掺杂铟的CsSnBr3半导体器件结构以及空间电荷限制电流(SCLC)测试结果;Figure 3 shows the structure of the indium-doped CsSnBr 3 semiconductor device and the space charge limited current (SCLC) test results;
图4为掺杂InBr的CsSnBr3晶体照片;Figure 4 is a photo of InBr-doped CsSnBr 3 crystal;
图5为掺杂AgBr的CsSnBr3粉末X射线衍射图谱;Fig. 5 is the powder X-ray diffraction pattern of CsSnBr doped with AgBr;
图6为未掺杂的CsSnBr3半导体器件结构以及空间电荷限制电流(SCLC)测试结果。FIG. 6 shows the structure of the undoped CsSnBr 3 semiconductor device and the space charge limited current (SCLC) test results.
具体实施方式Detailed ways
为使本发明更明显易懂,兹以优选实施例,并配合附图作详细说明如下。In order to make the present invention more obvious and comprehensible, preferred embodiments are described in detail below with reference to the accompanying drawings.
实施例1-4和对比例1中涉及的原料CsBr参照J.Phys.Chem.Lett.2019,10,3699的方法从市售试剂提纯,SnBr2参照Angew.Chem.Int.Ed.2018,57,13154的方法合成并提纯。The raw material CsBr involved in Examples 1-4 and Comparative Example 1 was purified from commercially available reagents according to the method of J.Phys.Chem.Lett.2019,10,3699, and SnBr 2 was purified according to Angew.Chem.Int.Ed.2018,57 , The method of 13154 was synthesized and purified.
实施例1:金属锡处理的CsSnBr3半导体Example 1: Metal Tin Treated CsSnBr Semiconductor
一种含锡半导体材料,制备方法为:在氮气环境中,称取10.6g(50.0mmol)CsBr和13.9g(50.0mmol)SnBr2固体,混合均匀并充分研磨后,与40g锡粒一起装入含约1/3大气压氮气的玻璃安瓿中并熔封。将此安瓿的颈部垂直朝下进行布里奇曼晶体生长,条件如下:升温速率5℃·min-1,保温温度490℃,保温时间3h,籽晶杆下降速率2mm·h-1,退火温度280℃,退火时间3h,最后随炉冷却至室温。得到的样品如图1所示,晶体表面光亮且无裂纹,无明显宏观夹杂物。A tin-containing semiconductor material, the preparation method is: in a nitrogen environment, weigh 10.6g (50.0mmol) of CsBr and 13.9g (50.0mmol) of SnBr 2 solids, mix them evenly and fully grind them, and put them together with 40g of tin particles. In a glass ampoule containing about 1/3 atmosphere nitrogen and melt-sealed. The neck of this ampoule is vertically downward for Bridgman crystal growth, and the conditions are as follows: heating rate 5℃·min -1 , holding temperature 490℃, holding time 3h, seed rod descending rate 2mm·h -1 , annealing The temperature was 280°C, the annealing time was 3h, and finally cooled to room temperature with the furnace. The obtained sample is shown in Figure 1, and the crystal surface is bright and free of cracks and no obvious macroscopic inclusions.
在氮气环境中,将晶体切割、打磨、抛光成直径约为13mm、厚度为0.95mm的圆形薄片,其X射线衍射图谱为图2(a)所示,表现为[100]晶向。将部分晶体研磨成粉末后的X射线衍射图谱为图2(b)所示,此衍射图的指标化结果为:立方晶系,Pm-3m空间群,晶胞参数为此结果说明本实施例产物为CsSnBr3的单一晶相。In a nitrogen environment, the crystals were cut, ground, and polished into circular slices with a diameter of about 13 mm and a thickness of 0.95 mm. The X-ray diffraction pattern after grinding part of the crystals into powder is shown in Figure 2(b). The indexing result of this diffraction pattern is: cubic crystal system, Pm-3m space group, and unit cell parameters are This result indicates that the product of this example is a single crystal phase of CsSnBr 3 .
在CsSnBr3圆片的边缘蒸镀四个金电极,采用范德堡法测量其霍尔效应,结果表明样品含p型载流子浓度为6.2×1015cm-3,载流子迁移率为67cm2·V-1·s-1。与对比例1相比,此结果说明金属锡处理使CsSnBr3半导体内的缺陷态密度降低了一个数量级。Four gold electrodes were evaporated on the edge of the CsSnBr 3 wafer, and the Hall effect was measured by the van der Pauw method. The results show that the sample contains p-type carrier concentration of 6.2×10 15 cm -3 , and the carrier mobility is 67cm 2 ·V -1 ·s -1 . Compared to Comparative Example 1, this result demonstrates that the metallic tin treatment reduces the density of defect states within the CsSnBr3 semiconductor by an order of magnitude.
实施例2:掺杂In的CsSnBr3半导体Example 2: In-doped CsSnBr semiconductor
一种含锡半导体材料,制备方法为:在氮气环境中,称取10.6g(50.0mmol)CsBr和13.9g(50.0mmol)SnBr2固体,混合均匀并充分研磨后,与0.057g(0.50mmol)铟粒一起装入含约1/3大气压氮气的玻璃安瓿中并熔封。此安瓿在460℃下滚动加热8小时,得到深色液体,冷却至室温后得到黑色固体。A tin-containing semiconductor material, the preparation method is as follows: in a nitrogen environment, weigh 10.6g (50.0mmol) of CsBr and 13.9g (50.0mmol) of SnBr 2 solids, mix them uniformly and fully grind them, and mix them with 0.057g (0.50mmol) The indium pellets are together filled into glass ampoules containing about 1/3 atmosphere of nitrogen and sealed. The ampoule was tumble heated at 460°C for 8 hours to give a dark liquid which was cooled to room temperature to give a black solid.
在氮气环境中,取部分黑色固体打磨抛光成尺寸约为1×1cm2、厚度为0.82mm的方形薄片。在薄片的四角蒸镀金电极,采用范德堡法测量其霍尔效应,结果表明样品含p型载流子浓度为4.1×1010cm-3,载流子迁移率为61cm2·V-1·s-1。In a nitrogen atmosphere, a part of the black solid was ground and polished into a square sheet with a size of about 1×1 cm 2 and a thickness of 0.82 mm. Gold electrodes were evaporated on the four corners of the sheet, and the Hall effect was measured by the van der Pauw method. The results show that the sample contains p-type carriers with a concentration of 4.1×10 10 cm -3 and a carrier mobility of 61 cm 2 ·V -1 ·s -1 .
在另一厚度为1.02mm的晶体薄片上下两面蒸镀金电极,其器件结构和电流–电压特性曲线如图3所示,缺陷填充限制电压VTFL为16V。按照标准空间电荷限制电流模型分析此结果,得到样品中的缺陷态密度为6.7×1010cm-3。以上结果均说明掺杂铟的CsSnBr3半导体内的缺陷已被显著地消除。Gold electrodes were evaporated on the upper and lower sides of another crystal sheet with a thickness of 1.02 mm. The device structure and current-voltage characteristic curve are shown in Figure 3. The defect filling limit voltage V TFL is 16V. Analyzing this result according to the standard space charge confined current model yields a defect state density of 6.7×10 10 cm −3 in the sample. All the above results indicate that the defects in the indium-doped CsSnBr 3 semiconductor have been significantly eliminated.
实施例3:掺杂InBr的CsSnBr3半导体Example 3 : InBr-doped CsSnBr semiconductor
一种含锡半导体材料,制备方法为:在氮气环境中,称取10.6g(50.0mmol)CsBr、13.9g(50.0mmol)SnBr2以及0.10g(0.50mmol)InBr固体,混合均匀并充分研磨后,装入底部为锥形、含约1/3大气压氮气的玻璃管中并熔封。布里奇曼晶体生长条件如下:升温速率5℃·min-1,保温温度490℃,保温时间3h,籽晶杆下降速率2mm·h-1,退火温度280℃,退火时间3h,最后随炉冷却至室温。得到的样品如图4所示,晶体表面光亮且无裂纹,无明显宏观夹杂物。A tin-containing semiconductor material, the preparation method is as follows: in a nitrogen environment, weigh 10.6g (50.0mmol) CsBr, 13.9g (50.0mmol) SnBr 2 and 0.10g (0.50mmol) InBr solid, mix well and fully grind , loaded into a glass tube with a conical bottom, containing about 1/3 atmosphere of nitrogen, and sealed. The growth conditions of Bridgman crystals are as follows: heating rate 5°C·min -1 , holding temperature 490°C, holding time 3h, seed rod descending rate 2mm·h -1 , annealing temperature 280°C, annealing time 3h, and finally with the furnace Cool to room temperature. The obtained sample is shown in Figure 4, and the crystal surface is bright and free of cracks and no obvious macroscopic inclusions.
在氮气环境中,将晶体切割、打磨、抛光成直径约为13mm、厚度为2.30mm的圆形薄片。在薄片的边缘蒸镀四个金电极,采用范德堡法测量其霍尔效应,结果表明样品含p型载流子浓度为3.0×1010cm-3,载流子迁移率为74cm2·V-1·s-1。此结果说明掺杂InBr的CsSnBr3半导体内的缺陷已被显著地消除。In a nitrogen atmosphere, the crystals were cut, ground, and polished into circular flakes with a diameter of approximately 13 mm and a thickness of 2.30 mm. Four gold electrodes were vapor-deposited on the edges of the flakes, and the Hall effect was measured by the van der Pauw method. The results show that the sample contains p-type carriers with a concentration of 3.0×10 10 cm -3 and a carrier mobility of 74 cm 2 · V -1 ·s -1 . This result indicates that the defects in the InBr-doped CsSnBr3 semiconductor have been significantly eliminated.
实施例4:掺杂AgBr的CsSnBr3半导体Example 4: AgBr-doped CsSnBr semiconductor
一种含锡半导体材料,制备方法为:在氮气环境中,称取4.17g(19.6mmol)CsBr、5.40g(19.4mmol)SnBr2、0.17g(0.20mmol)Cs2SnBr6以及0.075g(0.40mmol)AgBr固体,混合均匀并充分研磨后,装入含约1/3大气压氮气的玻璃安瓿中并熔封。此安瓿在460℃下滚动加热12小时,得到深色液体,冷却至室温后得到黑色固体。A tin-containing semiconductor material, the preparation method is as follows: in a nitrogen environment, weigh 4.17g (19.6mmol) CsBr, 5.40g (19.4mmol) SnBr 2 , 0.17g (0.20mmol) Cs 2 SnBr 6 and 0.075g (0.40g) mmol) AgBr solid, mixed well and thoroughly ground, then charged into a glass ampoule containing about 1/3 atmosphere of nitrogen and sealed. The ampoule was tumble heated at 460°C for 12 hours to give a dark liquid which was cooled to room temperature to give a black solid.
在氮气环境中,取部分黑色固体研磨成粉末,其X射线衍射图谱为图5所示。此衍射图的指标化结果为:立方晶系,Pm-3m空间群,晶胞参数为此结果说明本实施例产物为CsSnBr3的单一晶相,AgBr未产生相分离。In a nitrogen environment, a part of the black solid was ground into powder, and its X-ray diffraction pattern was shown in Figure 5. The indexed result of this diffractogram is: cubic crystal system, Pm-3m space group, and the unit cell parameter is This result indicates that the product of this example is a single crystal phase of CsSnBr 3 , and no phase separation of AgBr occurs.
取部分黑色固体打磨抛光成尺寸约为5×4mm2、厚度为1.02mm的方形薄片。在薄片的四角蒸镀金电极,采用范德堡法测量其霍尔效应,结果表明样品含p型载流子浓度为1.5×1019cm-3,载流子迁移率为20cm2·V-1·s-1。此结果说明掺杂AgBr的CsSnBr3半导体内的载流子浓度显著增加,成为简并掺杂半导体。A part of the black solid was ground and polished into a square sheet with a size of about 5×4 mm 2 and a thickness of 1.02 mm. Gold electrodes were evaporated on the four corners of the sheet, and the Hall effect was measured by the van der Pauw method. The results show that the sample contains p-type carriers with a concentration of 1.5×10 19 cm -3 and a carrier mobility of 20cm 2 ·V -1 ·s -1 . This result indicates that the carrier concentration in the AgBr-doped CsSnBr 3 semiconductor increases significantly, becoming a degenerate doped semiconductor.
对比例1:未掺杂的CsSnBr3半导体Comparative Example 1: Undoped CsSnBr Semiconductor
在氮气环境中,称取10.6g(50.0mmol)CsBr和13.9g(50.0mmol)SnBr2固体,混合均匀并充分研磨后,装入含约1/3大气压氮气的玻璃安瓿中并熔封。此安瓿在460℃下加热8小时,得到澄清酒红色液体,冷却至室温后得到黑色固体。In a nitrogen atmosphere, weigh 10.6 g (50.0 mmol) of CsBr and 13.9 g (50.0 mmol) of SnBr 2 as solids, mix them well and grind them well, put them into a glass ampoule containing about 1/3 atmosphere of nitrogen and seal them. The ampoule was heated at 460°C for 8 hours to obtain a clear wine red liquid which was cooled to room temperature to obtain a black solid.
在氮气环境中,取部分黑色固体打磨抛光成尺寸约为1×1cm2、厚度为1.32mm的方形薄片。在薄片的四角蒸镀金电极,采用范德堡法测量其霍尔效应,结果表明样品含p型载流子浓度为8.5×1016cm-3,载流子迁移率为23cm2·V-1·s-1。在另一厚度为1.13mm的晶体薄片上下两面蒸镀金电极,其器件结构和电流–电压特性曲线如图6所示,在施加电压范围0-40V内,只出现电流随电压线性变化的欧姆特性区。以上结果均说明未掺杂的CsSnBr3半导体材料内存在大量的缺陷。In a nitrogen atmosphere, a part of the black solid was ground and polished into a square sheet with a size of about 1×1 cm 2 and a thickness of 1.32 mm. Gold electrodes were evaporated on the four corners of the sheet, and the Hall effect was measured by the van der Pauw method. The results show that the sample contains p-type carriers with a concentration of 8.5×10 16 cm -3 and a carrier mobility of 23cm 2 ·V -1 ·s -1 . Gold electrodes were evaporated on the upper and lower sides of another crystal sheet with a thickness of 1.13mm. The device structure and current-voltage characteristic curve are shown in Figure 6. Within the applied voltage range of 0-40V, only the ohmic characteristic of the current linearly changing with the voltage appears. Area. The above results all indicate that there are a lot of defects in the undoped CsSnBr 3 semiconductor material.
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