CN100557770C - A method for preparing GaMnN dilute magnetic semiconductor nanowires - Google Patents
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Abstract
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技术领域 technical field
本发明涉及纳米线的制备方法,特别是涉及一种制备GaMnN稀磁半导体纳米线的方法。The invention relates to a method for preparing nanowires, in particular to a method for preparing GaMnN dilute magnetic semiconductor nanowires.
背景技术 Background technique
稀磁半导体材料的室温铁磁性是其能否用于自旋电子器件的制造的重要性能,GaN作为一种宽禁带半导体材料,具有优良的光学、电学性质,理论上GaN掺杂Mn将使其具有高于室温的铁磁序,因而GaMnN稀磁半导体材料是目前的研究热点。然而,由于磁性离子在半导体中的固溶度较低,利用传统方法制备高掺杂的、Mn替代晶格阳离子的GaMnN稀磁半导体材料仍然非常困难,而且,也曾有文献报道,采用上述方法制备时GaN中如果Mn的掺杂浓度大于3at.%,Mn离子就会填充在晶格间隙位置,而不是替代Ga,从而形成GaxMny晶粒,对材料的磁学性能产生影响,存在磁性杂质相析出问题。Deepak等人(F.L.Deepak,P.U.Vanitha,A.Fovindaraj,C.N.R.Rao,Chem.Phys.Lett.374(2003)314)利用碳纳米管作为摸板,制备了GaMnN稀磁半导体纳米线,但是样品产量较少。The room temperature ferromagnetism of dilute magnetic semiconductor materials is an important property of whether it can be used in the manufacture of spintronic devices. As a wide bandgap semiconductor material, GaN has excellent optical and electrical properties. In theory, GaN doped with Mn will make It has a ferromagnetic order higher than room temperature, so GaMnN dilute magnetic semiconductor materials are current research hotspots. However, due to the low solid solubility of magnetic ions in semiconductors, it is still very difficult to prepare highly doped GaMnN dilute magnetic semiconductor materials with Mn replacing lattice cations by traditional methods. Moreover, it has been reported in the literature that using the above method If the doping concentration of Mn in GaN is greater than 3 at.% during preparation, Mn ions will fill in the lattice gap instead of replacing Ga, thus forming Ga x Mn y grains, which will affect the magnetic properties of the material. Magnetic impurity phase precipitation problem. Deepak et al. (FLDeepak, PU Vanitha, A. Fovindaraj, CNRRao, Chem. Phys. Lett. 374 (2003) 314) used carbon nanotubes as a template to prepare GaMnN dilute magnetic semiconductor nanowires, but the yield of samples was less.
发明内容 Contents of the invention
本发明的目的是提供一种制备GaMnN稀磁半导体纳米线的方法。The purpose of the present invention is to provide a method for preparing GaMnN dilute magnetic semiconductor nanowires.
本发明所提供的制备GaMnN稀磁半导体纳米线的方法,包括如下步骤:The method for preparing GaMnN dilute magnetic semiconductor nanowires provided by the present invention comprises the following steps:
1)Mn掺杂:Ga2O3纳米线原位掺杂Mn;1) Mn doping: Ga 2 O 3 nanowires are in-situ doped with Mn;
2)氨化:将掺有Mn的Ga2O3纳米线在氨气气氛下进行氨化,得到GaMnN稀磁半导体纳米线。2) Ammonification: the Ga 2 O 3 nanowires doped with Mn are ammonified in an ammonia atmosphere to obtain GaMnN dilute magnetic semiconductor nanowires.
其中,步骤1)所述在Ga2O3纳米线上原位掺杂Mn的条件为:Wherein, the conditions for in-situ doping Mn on Ga2O3 nanowires in step 1) are:
将MnCl2·4H2O粉末、镓源衬底和收集衬底依次放入一端开口的石英舟中,然后再把石英舟放入管式炉,并使开口端迎着气流方向;封闭系统、抽真空,再通入氩气进行清洗,控制炉内压强为0.6~0.9标准大气压,通入氩气作为载气;并设定升温速度为15~20℃/分钟,使管式炉温度升到900℃,保持温度,在收集衬底上得到掺杂有Mn的Ga2O3纳米线。Put the MnCl 2 ·4H 2 O powder, gallium source substrate and collection substrate in turn into a quartz boat with one end open, then put the quartz boat into the tube furnace, and make the open end face the airflow direction; closed system, Vacuumize, then pass in argon for cleaning, control the pressure in the furnace to 0.6-0.9 standard atmospheric pressure, and pass in argon as a carrier gas; and set the heating rate at 15-20°C/min, so that the temperature of the tube furnace rises to Keep the temperature at 900°C, and obtain Ga 2 O 3 nanowires doped with Mn on the collecting substrate.
在上述温度、气压条件下,在收集衬底上生长出Ga2O3纳米线。而且,在Ga2O3纳米线生长过程中,由于氯化锰不断分解,并通过载气气流的输运,锰进入到Ga2O3的晶格中,实现Mn掺杂。通过放入不同的MnCl2·4H2O粉末量及其与源衬底和收集衬底的相对位置,可控制Mn的掺杂浓度。Under the above temperature and pressure conditions, Ga 2 O 3 nanowires are grown on the collection substrate. Moreover, during the growth process of Ga 2 O 3 nanowires, due to the continuous decomposition of manganese chloride and the transport of the carrier gas flow, manganese enters the crystal lattice of Ga 2 O 3 to achieve Mn doping. The doping concentration of Mn can be controlled by putting in different amounts of MnCl 2 ·4H 2 O powder and its relative positions with the source substrate and the collection substrate.
步骤2)所述进行氨化的条件为:Step 2) the described condition of carrying out ammoniation is:
将炉温升高至1050℃,关闭氩气,通入氨气并保温40分钟,控制压强为0.9大气压,对掺杂有Mn的Ga2O3纳米线进行氨化处理,得到GaMnN稀磁半导体纳米线。Raise the temperature of the furnace to 1050°C, turn off the argon gas, pass through the ammonia gas and keep it warm for 40 minutes, and control the pressure to 0.9 atmospheric pressure, and perform ammoniation treatment on the Mn-doped Ga 2 O 3 nanowires to obtain the GaMnN dilute magnetic semiconductor Nanowires.
根据Ga2O3纳米线中Mn的掺杂浓度不同,即可得到不同Mn掺杂浓度的GaMnN稀磁半导体纳米线。另外,在氨化处理结束后,为防止纳米线被氧化,关闭氨气后需通入氩气,自然降温至室温,这样即在Si衬底上生长有GaMnN稀磁半导体纳米线。GaMnN dilute magnetic semiconductor nanowires with different Mn doping concentrations can be obtained according to the different doping concentrations of Mn in the Ga 2 O 3 nanowires. In addition, after the ammonification treatment, in order to prevent the nanowires from being oxidized, argon gas must be introduced after the ammonia gas is turned off, and the temperature is naturally lowered to room temperature, so that GaMnN dilute magnetic semiconductor nanowires grow on the Si substrate.
本发明采用氧化物氨化法来制备GaMnN稀磁半导体纳米线(DMS NWs),主要分为两步:第一步,首先在Ga2O3纳米线的生长阶段,原位进行Mn掺杂,因为Mn在氧镓锰体系中的高固溶度,所以可以得到较高浓度的Mn掺杂;然后第二步,在高温氨气氛下进行氨化处理,氮原子逐步取代氧原子的晶格位置,使得纳米线逐步转化为GaMnN纳米线。在制备过程中,Mn原子被冻结在GaN晶格结构中,阻止了磁性Mn离子的析出,从而可以避免GaN材料常规方法进行Mn掺杂所带来的磁性杂质相析出问题。结构分析表明,利用本发明方法制备的GaMnN纳米线具有单一的六角GaN晶体结构,不存在磁性杂质相;磁学测量表明,GaMnN纳米线具有室温铁磁性,居里温度至少高于室温。本发明方法简单,对设备要求较低,利用普通管式炉即可进行;所制备的GaMnN纳米线具有很强的铁磁性,居里温度高于室温,而且其磁性掺杂浓度可控,可以利用样品中锰、氮掺杂浓度的变化调控样品纳米线的磁性和居里温度;纳米线纯度高,产量大,线形可控(调节气压等生长参数可以制备出直径几十纳米到几百纳米的纳米线),可以用于自旋场效应三极管(spin-FET),自旋发光二极管(spin-LED),自旋共振隧穿器件(spin-RTD)等纳米自旋电子器件的制造,具有广阔的应用前景。The present invention uses the oxide ammonification method to prepare GaMnN dilute magnetic semiconductor nanowires (DMS NWs), which is mainly divided into two steps: the first step is to perform Mn doping in situ during the growth stage of Ga2O3 nanowires, Because of the high solid solubility of Mn in the oxygallium manganese system, a higher concentration of Mn doping can be obtained; then in the second step, ammoniation treatment is carried out under a high-temperature ammonia atmosphere, and nitrogen atoms gradually replace the lattice positions of oxygen atoms , making the nanowires gradually transform into GaMnN nanowires. During the preparation process, Mn atoms are frozen in the GaN lattice structure, which prevents the precipitation of magnetic Mn ions, thereby avoiding the problem of magnetic impurity phase precipitation caused by Mn doping of GaN materials by conventional methods. Structural analysis shows that the GaMnN nanowire prepared by the method of the invention has a single hexagonal GaN crystal structure without magnetic impurity phases; magnetic measurement shows that the GaMnN nanowire has ferromagnetism at room temperature, and the Curie temperature is at least higher than room temperature. The method of the present invention is simple, requires less equipment, and can be carried out by using an ordinary tube furnace; the prepared GaMnN nanowire has strong ferromagnetism, the Curie temperature is higher than room temperature, and its magnetic doping concentration is controllable, which can The magnetic properties and Curie temperature of sample nanowires can be controlled by changing the doping concentration of manganese and nitrogen in the sample; the nanowires have high purity, large output, and controllable line shape (adjusting growth parameters such as gas pressure can prepare tens of nanometers to hundreds of nanometers in diameter) nanowires), which can be used in the manufacture of spin-field-effect transistors (spin-FETs), spin-light-emitting diodes (spin-LEDs), spin-resonance tunneling devices (spin-RTDs) and other nano-spintronic devices, with Broad application prospects.
附图说明 Description of drawings
图1为纳米线的扫描电镜图;Fig. 1 is the scanning electron microscope picture of nanowire;
图2为纳米线的X射线衍射谱;Fig. 2 is the X-ray diffraction spectrum of nanowire;
图3为纳米线的分析照片;Fig. 3 is the analysis photograph of nanowire;
图4为纳米线在室温下的M-H曲线。Figure 4 is the M-H curve of the nanowire at room temperature.
具体实施方式 Detailed ways
实施例1、
一、采用氧化物氨化法制备大产量GaMnN稀磁半导体纳米线。1. GaMnN dilute magnetic semiconductor nanowires were prepared in large quantities by oxide ammoniation method.
用镀有5nm金膜的Si片作为产物的收集衬底,将装有MnCl2·4H2O粉末的小陶瓷杯、镓源衬底(放置有100毫克金属镓的Si片)和三片收集衬底依次放入一端开口的石英舟中,小陶瓷杯距离镓源衬底10cm左右。然后再把石英舟放在管式炉的中央部位,并使开口端迎着气流方向。封闭系统后,开启机械泵抽至真空,通入氩气进行清洗,使系统压强升至常压,如此重复三次。实验开始后,通过手动控制针阀保持所需压强(0.6~0.9标准大气压),并设定升温曲线(升温速度:15~20℃/分钟)。通入80sccm氩气作为载气,在50分钟内使管式炉温度升到900℃,并保持30分钟;随后直接将炉温升高至1050℃,关闭氩气,通入氨气并保温40分钟,控制压强为0.9大气压,进行氮掺杂;氨化处理结束后,关闭氨气并通入氩气80sccm,自然降温至室温,即在Si衬底上生长有GaMnN稀磁半导体纳米线,由此制备出不同Mn掺杂浓度的样品A和样品B。A Si chip coated with a 5nm gold film was used as the collection substrate of the product, and a small ceramic cup filled with MnCl 2 4H 2 O powder, a gallium source substrate (a Si chip with 100 mg of metal gallium placed on it) and three collection substrates were used. The substrates are placed in a quartz boat with one end open in turn, and the small ceramic cup is about 10cm away from the gallium source substrate. Then place the quartz boat in the center of the tube furnace with the open end facing the direction of the airflow. After closing the system, turn on the mechanical pump to evacuate to a vacuum, pass in argon gas for cleaning, and raise the system pressure to normal pressure, and repeat this three times. After the experiment started, the required pressure (0.6-0.9 standard atmospheric pressure) was maintained by manually controlling the needle valve, and the heating curve was set (heating rate: 15-20° C./min). Introduce 80 sccm argon as the carrier gas, raise the temperature of the tube furnace to 900°C within 50 minutes, and keep it for 30 minutes; then directly raise the furnace temperature to 1050°C, turn off the argon, feed ammonia and keep it warm for 40 minutes Minutes, control the pressure to be 0.9 atmospheric pressure, and carry out nitrogen doping; after the ammoniation treatment is completed, turn off the ammonia gas and feed argon gas 80sccm, and naturally cool down to room temperature, that is, GaMnN dilute magnetic semiconductor nanowires grow on the Si substrate, by This prepared sample A and sample B with different Mn doping concentrations.
样品按照如下表示方式进行表述:氨化温度/氨化时间/氨气流量/放入MnCl2·4H2O量/Mn浓度(at.%为原子百分比浓度),上述实施例所得到的样品A:1050℃/40min/100sccm/0.80g/4at.%);样品B:1050℃/40min/100sccm/1.1g/8at.%。The sample is expressed in the following way: ammoniation temperature/ammoniation time/ammonia gas flow/put MnCl 2 4H 2 O amount/Mn concentration (at.% is the atomic percentage concentration), the sample A obtained in the above examples : 1050°C/40min/100sccm/0.80g/4at.%); Sample B: 1050°C/40min/100sccm/1.1g/8at.%.
二、GaMnN稀磁半导体纳米线的形貌、结构和磁性分析2. Morphology, structure and magnetic analysis of GaMnN dilute magnetic semiconductor nanowires
1、形貌及尺寸1. Appearance and size
纳米线的扫描电镜图如图1所示,结果表明在硅衬底上生长出大量的纳米线,纳米线平均直径约为100nm,长度约几十微米。The scanning electron microscope image of the nanowires is shown in Figure 1. The results show that a large number of nanowires are grown on the silicon substrate. The average diameter of the nanowires is about 100 nm and the length is about tens of microns.
2、晶相2. Crystal phase
所得纳米线X射线衍射表明,晶相为六方相(wurzite),不存在磁性杂质相,如图2所示。X-ray diffraction of the obtained nanowires shows that the crystal phase is a hexagonal phase (wurzite), and there is no magnetic impurity phase, as shown in FIG. 2 .
3、结构分析3. Structural analysis
图3a、图3b分别是Mn掺杂浓度为4at.%的纳米线(样品A)和8at.%的纳米线(样品B)的TEM低分辨图像;样品A纳米线的电子衍射谱如图3c和图3d所示(对应样品A中两根不同纳米线),样品B纳米线的电子衍射谱如图3e和图3f所示(对应样品B中两根不同纳米线),对应[0001]晶轴的电子衍射,晶格结构可以标定为六角纤锌矿GaN结构;图3g、图3h分别是Mn掺杂浓度为4at.%和8at.%的纳米线的高分辨透射图像。Figure 3a and Figure 3b are TEM low-resolution images of nanowires (sample A) and 8at.% nanowires (sample B) with a Mn doping concentration of 4at.% respectively; the electron diffraction spectrum of sample A nanowires is shown in Figure 3c As shown in Figure 3d (corresponding to two different nanowires in sample A), the electron diffraction spectrum of sample B nanowires is shown in Figure 3e and Figure 3f (corresponding to two different nanowires in sample B), corresponding to [0001] Axis electron diffraction, the lattice structure can be calibrated as a hexagonal wurtzite GaN structure; Figure 3g and Figure 3h are high-resolution transmission images of nanowires with Mn doping concentrations of 4at.% and 8at.%, respectively.
以上结果可见,所得纳米线的电子衍射斑均呈现对应六角GaN结构的六次对称性,没有出现4次对称性等其他杂质相的衍射斑,这表明所得纳米线中不存在四角(Mn3N2、MnN、GaMn、Ga0.4Mn0.6)或者立方(Mn4N、Mn、Ga7.7Mn2.3、Ga5Mn8)杂质相,而且由于没有一种Mn氧化物具有六角结构,说明纳米线中也不存在Mn氧化物杂质相;另外,纳米线的XRD图谱中没有发现与GaMn3相对应的衍射峰,而且GaMn3的晶格常数( )与纳米线的电子衍射分析得到的晶格常数差别很大,也表明在所制备的纳米线中同样不存在GaMn3晶型结构,本发明所制备的GaMnN纳米线具有单一的GaN相结构。高分辨透射图像(图2g、图2h)中清晰的条纹像表明纳米线具有单晶结构,纳米线表面干净而且结构完整,进一步证实在GaMnN纳米线中Mn离子掺入到了GaN晶格结构中,而不是以Mn的析出相或Mn的杂质相形式存在于纳米线中:对Mn掺杂浓度4at.%的纳米线,条纹像间距为0.244nm,对应于六角GaN结构(-1 01 1)面的面间距;对Mn掺杂浓度8at.%的纳米线,条纹像间距为0.276nm,对应于GaN结构(1 0 -1 1)面间距。From the above results, it can be seen that the electron diffraction spots of the obtained nanowires all present the six-fold symmetry corresponding to the hexagonal GaN structure, and there are no diffraction spots of other impurity phases such as four-fold symmetry, which indicates that there is no tetragonal (Mn 3 N 2 , MnN, GaMn, Ga 0.4 Mn 0.6 ) or cubic (Mn 4 N, Mn, Ga 7.7 Mn 2.3 , Ga 5 Mn 8 ) impurity phases, and since none of the Mn oxides has a hexagonal structure, it means that nanowires also have There is no Mn oxide impurity phase; in addition, no diffraction peak corresponding to GaMn3 is found in the XRD spectrum of the nanowire, and the lattice constant of GaMn3 ( ) is very different from the lattice constant obtained by the electron diffraction analysis of the nanowire, which also shows that there is no GaMn 3 crystal structure in the prepared nanowire, and the GaMnN nanowire prepared by the present invention has a single GaN phase structure. The clear fringe images in the high-resolution transmission images (Figure 2g, Figure 2h) indicate that the nanowires have a single crystal structure, and the surface of the nanowires is clean and structurally complete, which further confirms that Mn ions are incorporated into the GaN lattice structure in the GaMnN nanowires, It does not exist in the nanowires in the form of Mn precipitates or Mn impurity phases: for nanowires with a Mn doping concentration of 4at.%, the fringe image spacing is 0.244nm, corresponding to the hexagonal GaN structure (-1 01 1) plane The interplanetary spacing; for nanowires with a Mn doping concentration of 8at.%, the fringe image spacing is 0.276nm, corresponding to the GaN structure (1 0 -1 1) interplanetary spacing.
4、磁性测量4. Magnetic measurement
Mn掺杂浓度8at.%的纳米线在室温下的M-H曲线如图4所示,由图可见,该纳米线在室温下仍有明显的磁滞回线,矫顽力达到1270e,这清楚的表明本发明GaMnN纳米线在室温下存在铁磁态,具有室温铁磁性,居里温度至少高于室温。The M-H curve of the nanowire with a Mn doping concentration of 8at.% at room temperature is shown in Figure 4. It can be seen from the figure that the nanowire still has an obvious hysteresis loop at room temperature, and the coercive force reaches 1270e, which is clear It shows that the GaMnN nanowire of the present invention exists ferromagnetic state at room temperature, has room temperature ferromagnetism, and the Curie temperature is at least higher than room temperature.
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