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1.
在用二次氧化法制备的高度有序的氧化铝模板上通过交流电化学方法制备了Co纳米线阵列.研究了外加磁场及电解液pH值对纳米线生长的影响.在pH值为6.0和6.5的电解液中分别在不加磁场和沿纳米线轴向施加0.3 T磁场情况下制备了hcp结构的Co纳米线阵列.实验数据表明,沉积时外加磁场和调节pH值能有效影响纳米线中hcp结构的Co晶粒的易磁化轴沿纳米线长轴方向生长.由于晶粒的磁晶各向异性和纳米线沿长度方向的宏观形状各向异性叠加,制备的Co纳米线阵列具有高垂直各向异性,高矫顽力和较高矩形比. 关键词: Co纳米线阵列 织构 磁性  相似文献   

2.
BaFe12O19 nanowire arrays having single magnetic domain size (≤460 nm) in anodic aluminum oxide (AAO) templates were prepared by sol-gel and self-propagating high-temperature synthesis techniques. The diameter of the nanowire arrays is approximately 70 nm and the length is about 2-4 μm. The specimens were characterized using X-ray diffraction, vibrating sample magnetometer, field emission scan electron microscope, atomic force microscopy and microwave vector network analyzer. The magnetic properties of BaFe12O19 nanowire arrays embedded in AAO templates were measured by VSM with a field up to 1274 KA/m at room temperature. The results indicate that the nanowire arrays exhibit large saturation magnetization and high coercivity in the range of 6000 Oe and an obvious magnetic anisotropy with the easy magnetizing axis along the length of the nanowire arrays, probably due to the shape anisotropy and magneto-crystalline anisotropy. Finally the microwave absorption properties of the nanowires were discussed.  相似文献   

3.
Co-Ni合金纳米线有序阵列的制备与磁性研究   总被引:16,自引:2,他引:16       下载免费PDF全文
关键词:  相似文献   

4.
Highly textured Ni nanowire arrays were fabricated into anodic aluminum oxide(AAO) templates by pulse DC electrodeposition.The applied voltage and pH value of electrolytes were found strongly affecting the microstructure and magnetic properties of Ni nanowire arrays.Low applied potential and pH value both prefer to form polycrystalline fcc Ni nanowires.Increasing the applied potential or pH value favors the Ni [220] texture and even eventually forms the [220] oriented single crystal Ni wires,while exorbitan...  相似文献   

5.
Spinel CoFe2O4 nanowire arrays were synthesized in nanopores of anodic aluminum oxide (AAO) template using aqueous solution of cobalt and iron nitrates as precursor. The precursor was filled into the nanopores by vacuum impregnation. After heat treatment, it transformed to spinel CoFe2O4 nanowires. The structure, morphology and magnetic properties of the sample were studied by X-ray diffraction (XRD), scanning electron microscopy (SEM), transmission electron microscopy (TEM) and vibrating sample magnetometer (VSM). The results indicate that the nanowire arrays are compact. And the individual nanowires have a high aspect ratio, which are about 80 nm in diameter and 10 μm in length. The nanowires are polycrystalline spinel phase. Magnetic measurements indicate that the nanowire arrays are nearly magnetic isotropic. The reason is briefly discussed. Moreover, the temperature dependence of the coercive force of the nanowire arrays was studied.  相似文献   

6.
Anodic aluminum oxide(AAO) with highly ordered nanoscale pores which are monodisperse and mutually parallel can be produced through a self-organized electrochemical process.Subsequent deposition of materials into the nanopores produces AAO embedded nanowire arrays.Whilst the templates can be further removed to obtain free individual nanowires,the embedded nanowires form an interesting nanocomposite structure.Recent research activities on the fabrication and characteriza-tion of AAO template based magnetic n...  相似文献   

7.
NiFe2O4纳米线阵列的制备与磁性   总被引:4,自引:0,他引:4       下载免费PDF全文
于冬亮  都有为 《物理学报》2005,54(2):930-934
在氧化铝模板的纳米孔洞中, 用电化学的方法沉积铁镍合金纳米线,经过550℃30h氧化处理 , 成功制备出 NiFe2O4纳米线阵列. 分别用扫描电子显微镜 (SEM) 、透射电 子显微镜 (TEM) 、x射线衍射仪 (XRD) 和振动样品磁场计 (VSM) 对样品的形貌、晶体结构 和磁学性质进行了表征测试. SEM和TEM观察结果显示氧化铝模板的孔洞分布均匀,孔心距约 为110nm; 纳米线的直径约为70nm. XRD显示纳米线阵列的物相结构为NiFe2O4; VSM测试结果表明,NiFe2O4纳米线阵列膜的易磁化方向垂直于膜面. 当垂直 磁化时磁滞回线的矩形比约为05,矫顽力为41×103A/m,比氧化处理前的铁镍合金 纳米线阵列都有显著提高. 关键词: 纳米线 Ni Fe2O4 矫顽力  相似文献   

8.
Ni nanowire arrays with different diameters have now been extended to directly fabricate in porous anodic alumina oxide (AAO) templates on Ti/Si substrate by direct current (DC) electrodeposition. An aluminum film is firstly sputter-deposited on a silicon substrate coated with a 300 nm Ti film. AAO/Ti/Si substrate is synthesized by a two-step electrochemical anodization of the aluminum film on the Ti/Si substrate and then used as template to grow Ni nanowire arrays with different diameters. The coercivity and the squareness in parallel direction of Ni nanowires with about 10 nm diameters are 664 Oe and 0.90, respectively. The Ni nanowire arrays fabricated on AAO/Ti/Si substrates should lead to practical applications in ultrahigh-density magnetic storage devices because of the excellent properties.  相似文献   

9.
CoPt3/Co multilayered nanowire(NW) arrays are synthesized by pulsed electrodeposition into nanoporous anodic aluminum oxide(AAO) templates. The electrochemistry deposition parameters are determined by cyclic voltammetry to realize the well control of the ratio of Co to Pt and the length of every segment. The x-ray diffraction(XRD) patterns show that both Co and CoPt3 NWs exhibit face-centered cubic( fcc) structures. In the UV-visible absorption spectra,CoPt3/Co NW arrays show a red-shift with respect to pure CoPt3 NWs. Compared with the pure Co nanowire arrays, the CoPt3/Co multilayered nanowire arrays show a weak shape anisotropy and well-modulated magnetic properties. CoPt3/Co multilayered nanowires are highly encouraging that new families of bimetallic nanosystems may be developed to meet the needs of nanomaterials in emerging multifunctional nanotechnologies.  相似文献   

10.
张鹭  潘曹峰  朱静 《中国物理快报》2008,25(8):3056-3058
Nation-115 nanowire arrays are synthesized with an extrusion method using AAO membranes as templates. It is indicated that the vacuum treating of AAO templates before surface decoration plays an important role in obtaining high filling rate of the Nation-115 nanowires in the AAO templates, vchile the concentration of Nafion-115 DMSO solutions does not affect the flling rate greatly. The optimized parameters to synthesize the Nation-115 nanowire arrays are studied. The filling rate of the Nadion-115 nanowires in the AAO templates synthesized with the optimized parameters is about 95% discussed to qualitatively explain the experimental results The growth mechanism of Nafion-115 nanowires is  相似文献   

11.
Co100?xSnx alloy nanowires were fabricated by electrodeposition of Co2+ and Sn2+ into anodic aluminum oxide (AAO) templates. X-ray diffraction results indicate that the crystal structures of the nanowires changed from polycrystal to amorphism, and then to polycrystal again with the increase of Sn content in the nanowires. Transmission electron microscopy result shows that the nanowires are about 50 nm in diameter and the aspect ratio is approximately 75. The magnetic response of the arrays was measured using vibrating sample magnetometry at room temperature. The results show that the coercivity and squareness with the magnetic field along the nanowire arrays decrease with the increase of the Sn content. Nanowires exhibit obviously uniaxial magnetic anisotropy, and the easy magnetizing axis is parallel to the nanowires owing to the large shape anisotropy.  相似文献   

12.
Ordered ferromagnetic-nonmagnetic heterogeneous Fe60Pb40 nanowire arrays were successfully fabricated by alternating current (AC) electrodeposition into nanoporous alumina templates. Transmission electron microscopy (TEM) image and selected-area diffraction (SAED) pattern analysis showed that the Fe60Pb40 nanowires are polycrystalline with an average diameter of 22 nm and lengths up to several micrometers. X-ray diffraction (XRD) observations indicated that α-Fe and fcc Pb phase coexist and do not form metastable alloy phase. The as-deposited samples were annealed at 200, 300, 400 and 500 °C, respectively. Magnetic measurements showed that nanowires have high magnetic anisotropy with their easy axis parallel to the nanowire arrays, and the coercivity of the samples increased with the annealing temperature up to 400 °C and reached a maximum (2650 Oe). The change of magnetic properties associated with the microstructure was discussed.  相似文献   

13.
The Ni 300 nm wide nanowires were fabricated inside the as-synthesized nanochannels of anodic aluminum oxide (AAO) template by electrochemical deposition method. The angular dependence of coercivity and remanence of Ni nanowire arrays with various lengths have been comparatively studied. Investigation results demonstrate that the easy axis is along the wire axis for the longer nanowires of 4 μm or 9 μm in length due to their large shape anisotropy. However, the magnetostatic coupling is dominant for the shorter nanowires of 0.9 μm in length resulting in the change of magnetization behaviors, including coercivity and easy axis. A further explanation was also given by simple calculation in the paper.  相似文献   

14.
Systematic study of magnetic nanowire arrays grown in anodic alumina membranes (AAM) has been done by means of Rutherford backscattering spectroscopy (RBS). The AAM used as templates were morphologically characterized by using high resolution scanning electron microscopy (HRSEM), fast Fourier transform (FFT) and atomic force microscopy (AFM). The highly ordered templates with a mean pore diameter size of 30 nanometers, a mean inter-pore spacing of 100 nm and lengths ranging from 4 to 180 microns were obtained through two-steps anodization process, and the Ni and Co nanowire arrays were grown by electrodeposition techniques. The main attention is addressed to Ni nanowire arrays. RBS results allowed us to determine the real depth profile of atomic composition of the obtained nanowire arrays. In addition, the RBS spectra fitting showed that the porosity increased from the top to the bottom of the samples. Two phenomenological models are proposed to understand the apparition of that secondary porosity and a linear relation between the total amount of electrodeposited Ni and the electrodeposition time was obtained. As an example, it is also reported the relation between RBS results and magnetic properties, such as coercive field and remanence/saturation magnetization ratio of the samples. Particularly, for Ni nanowires arrays obtained by using voltage pulses, it is demonstrated that the larger the nanowires, the higher the definition for easy axis parallel to the nanowire length is possible. PACS 82.80.Yc; 81.16-c; 75.75.+a  相似文献   

15.
Orientation control and the magnetic properties of single crystalline Co nanowires fabricated by electrodeposition have been systematically investigated. It is found that the orientation of Co nanowires can be effectively controlled by varying either the current density or the pore diameter of AAO templates. Lower current density or small diameter is favorable for forming the (1 0 0) texture, while higher current values or larger diameter leads to the emergence and enhancement of (1 1 0) texture of Co nanowires. The mechanism for the manipulated growth characterization is discussed in detail. The orientation of Co nanowires has a significant influence on the magnetic properties, resulting from the competition between the magneto-crystalline and shape anisotropy of Co nanowires. This work offers a simple method to manipulate the orientation and magnetic properties of nanowires for future applications.  相似文献   

16.
β-FeOOH nanowire arrays with diameters of 50–200 nm have been fabricated by electrochemical deposition using two-step anodic porous alumina templates. The as-prepared nanowires are homogeneous and have large aspect ratios. The selected area electron diffraction photo performed on a single wire was used to confirm the amorphous crystal structure further. The magnetic properties of these nanowire arrays were firstly investigated by using a SQUID magnetometry. The ZFC and FC studies show that these nanowire arrays exhibit spin-freezing phenomena at low temperature. The temperature-dependent magnetization curves show that the Neel transition temperatures are much lower than that of bulk material. Moreover, hysteresis was found at 5 K and the coercivities up to about 1500 Oe. The size-dependent magnetic properties were also investigated. These abnormal magnetic behaviours can be interpreted in terms of the amorphous crystal structure and the low dimensionality of the nanowire arrays.  相似文献   

17.
Ni纳米线阵列的铁磁共振研究   总被引:4,自引:0,他引:4       下载免费PDF全文
袁淑娟  周仕明  鹿牧 《物理学报》2006,55(2):891-896
通过改变氧化电压和酸性溶液制备了孔径、孔隙率不同的阳极氧化铝模板,用电沉积方法在模板中制备了Ni有序纳米线阵列,并用铁磁共振技术和振动样品磁强计对其进行了研究.研究表明Ni纳米线阵列存在着较强的偶极相互作用,偶极相互作用与纳米线的形状各向异性之间的竞争决定了纳米线的易磁化方向.随着纳米线阵列密度的增加,线间的偶极相互作用增加,使得纳米线易磁化方向从平行于纳米线方向渐趋向于垂直于纳米线的平面内. 关键词: 纳米线 铁磁共振 偶极相互作用 氧化铝模板  相似文献   

18.
史慧刚  付军丽  薛德胜 《物理学报》2005,54(8):3862-3866
利用电化学沉积方法在阳极氧化铝模板中制备了Fe89.7P10.3非晶 合金纳 米线阵列.利用x射线衍射仪、透射电子显微镜、振动样品磁强计和穆斯堡尔谱仪研究了样品的结构和磁性,发现纳米线阵列是非晶结构,且拥有垂直磁各向异性和高的矫顽力,Hc =304×104A/m.纳米线内部的平均超精细场和平均同质异能移分别为2 15×106 A/m和007 mm/s;而纳米线末端的平均超精细场(233×106 A/m )大于内 部的值,平均同质异能移(004 mm/s)小于内部的值.另外,纳米线内部Fe原子磁矩与线轴的夹角约为16°,而在纳米线末端Fe原子磁矩与线轴的夹角约为28°.这些结果表明,由于形状各 向异性,在纳米线中实现了无序非晶合金磁矩的有序排列. 关键词: 非晶合金 纳米线阵列 垂直磁各向异性 穆斯堡尔谱  相似文献   

19.
赵荣  顾建军  刘力虎  徐芹  蔡宁  孙会元 《物理学报》2012,61(2):27504-027504
利用交流电化学沉积方法在氧化铝模板中制备了一维结构的FexCo1-x(0 ≤ x ≤ 0.51)二元合金纳米线阵列.X射线衍射结果显示,单质Co纳米线为(100)择优取向的hcp结构,FeCo合金纳米线则呈现(110)择优取向的bcc结构,而且衍射峰随纳米线中Fe含量的增加向低角度偏移.室温磁性测量结果显示, FeCo合金纳米线具有较好的磁特性.与Co纳米线相比,Fe的引入改善了Co纳米线的磁性能,使其呈现出较大的矫顽力和较高的矩形比.采用一致转动模型和对称扇形机理的球链模型分别计算了FeCo合金纳米线的矫顽力, 发现其磁化反转机理与对称扇形机理的球链模型相符合.  相似文献   

20.
α-Fe纳米线阵列膜磁各向异性的穆斯堡尔谱研究   总被引:17,自引:2,他引:17       下载免费PDF全文
王成伟  彭勇  潘善林  张浩力  力虎林 《物理学报》1999,48(11):2146-2150
在具有纳米级孔洞的多孔氧化铝模板上,用电沉积方法成功地制备出α-Fe纳米线有序阵列组装膜.分别用透射电子显微镜(TEM)、穆斯堡尔谱仪(MS)和振动样品磁强计(VMS)对样品进行了测试分析.TEM和电子衍射的结果显示,阵列中的纳米线均匀有序,彼此独立,由一串α-Fe单晶磁性颗粒构成.VSM测试结果表明,这种纳米阵列结构具有高度垂直磁各向异性.当外磁场垂直磁化时,磁滞回线具有很高矩形比(0.98)和矫顽力(1.76×105A/m).尤其MS的测试结果显示,阵列中的每根纳米线的总磁矩都沿 关键词:  相似文献   

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