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21.
《Fullerenes, Nanotubes and Carbon Nanostructures》2013,21(1-2):123-127
Abstract Considering the nanotube as effective conducting media the magnetoresistance is calculated. For an electron motion along nanotube axis the spin–orbital interaction is considered as perturbation and the Dirac equation is solved for longitudinal wave functions. It is shown that in this case a magnetic field can be considered as perturbation for energy spectrum and density matrix diagonal components for each spin orientation are needed to calculate the nanotube conductivity. For narrow gap nanotube the magnetoresistance depends linearly on a weak magnetic field. Our results show that in nanotubes the negative magnetoresistance (NMR) can be described without theory of weak localization. 相似文献
22.
Yong-Gang Tang Gui-Ying Wang Guo-Qing Yan Qi-Xiang Song Ming-Yu Zhang Zhen-Sheng Peng 《稀有金属(英文版)》2013,32(3):258-263
The perovskite samples La1-x (Sr1-yKy )xMnO3 (y = 0.0, 0.2, 04, 0.6, 0.8) were prepared by the solid-state reaction method with comparatively low sintering temperature and with comparatively short sintering time, and the electric transport property and temperature stability of MR of this system were studied. The q-T curves show the abnormal phenomenon that with the increase of K doping amount, resistivity increases, and the insulator-metal transition temperature decreases, which is because the influence of the occupation disorder degree of A-site ions σ2 on the electric transport property of perovskite manganites is larger than that of the radius of A-site ions. In the temperature range below 225 K, MR increases continuously with the decrease of temperature, which is the characteristic of low-field magnetoresistance; in the comparatively wide temperature range near 250 K, the MR-T curves of all the samples are comparatively flat, and the value of MR almost does not change with temperature, which shows the temperature stability of magnetoresistance, and can be explained by the competition between the low-field magnetoresistance induced by spin-dependent tunneling of surface phase and the intrinsic magnetoresistance of grain phase. The magnetoresistance value of the sample with y = 0.8 keeps at (7.92 ± 0.36) % in the very wide temperature range of 225-275 K, and this is a good reference for the preparation of this kind of sample with practical application value in the future. 相似文献
23.
Debabrata Pradhan 《Electrochimica acta》2008,54(2):430-433
Electrodeposition of metallic multilayers on Si is normally preceded by the vapour deposition of a metallic layer. Since vapour deposition produces an additional step in the production process, direct electrodeposition of multilayers on Si is desirable. However, direct electrodeposition on Si has resulted in low magnetoresistance (MR) - of the order of 1% - at room temperature. With the use of (i) electroless plated copper back contact, (ii) composite potentiostatic pulses, (iii) horizontal electrode configuration and (iv) non-continuous mode of deposition, a room temperature MR of 5.8% has been achieved. 相似文献
24.
Sr2FexMo2−xO6 (x = 0.8, 0.9, 1.0, 1.1, 1.2, 1.3, 1.4 and 1.5 wt.%) (SFMO) double perovskite oxides of different compositions have been prepared by sol-gel method. These materials were subjected to X-ray diffraction and found that crystal structure changes from tetragonal to cubic around x = 1.2 wt.%. Lattice parameters and unit cell volume have been calculated using X-ray diffraction data. Magnetization studies have been carried out using Vibrating Sample Magnetometer ranging from −15 kOe to +15 kOe and saturation magnetization (Ms) has been determined. Electrical resistivity and magnetoresistance studies have been carried out in the magnetic field range of −40 kOe to +40 kOe keeping the temperature constant at 5, 150 and 300 K using standard four-probe method. Resistivity studies have also been carried out in the temperature ranging from 5 to 300 K keeping the magnetic field constant at 0, 10, 20 and 40 kOe. Maximum degree of Fe/Mo ordering (ηmax) of SFMO has been calculated and compared with magnetic and transport properties. It has been found that there is a strong correlation between 3 parameters ηmax, Ms and MR (%), i.e. all of them show a maximum at x = 1.0 wt.% and decreases as x deviates from 1.0 in SFMO. It has been also found that there is a different resistivity behavior between x ≤ 1.2 wt.% and x > 1.2 wt.% samples of SFMO. Semiconductor metal transition temperature was found to be maximum at x = 1.0 wt.%. 相似文献
25.
Hongbo Gu Huige Wei Jiang Guo Neel Haldolaarachige David P. Young Suying Wei Zhanhu Guo 《Polymer》2013
In this work, the oxidant Cr(VI) dose was observed to have influenced the polyaniline (PANI) nanostructures as well as the crystallization structure. The temperature dependent resistivity study revealed a quasi 3-dimensional variable range hopping (VRH) electrical conduction mechanism. The permittivity was found to be affected by the PANI nanostructures. The observed positive MR at room temperature in the synthesized PANI samples was analyzed by the wave-function shrinkage model. The electrochemical energy storage was investigated using the cyclic voltammetry (CV) and galvanostatic charge–discharge measurements. The highest gravimetric capacitance of 298.5 F g−1 was obtained in the prepared PANI sample using 3 mmol K2Cr2O7 derived from the CV at a scan rate of 5 mV s−1 and the maximum value of gravimetric capacitance of 330.2 F g−1 was achieved in the galvanostatic charge–discharge measurements at a current density of 0.5 A g−1. After applying an external magnetic field, the capacitance decreased due to the observed positive magnetoresistance phenomenon. The cyclic stability studies revealed that the synthesized PANI samples exhibited good durability and retained around 80% of the capacitance even after 1000 charge–discharge galvanostatic cycles. 相似文献
26.
27.
Sunil Nair M. Nicklas J. L. Sarrao J. D. Thompson F. Steglich S. Wirth 《Journal of Superconductivity and Novel Magnetism》2009,22(2):201-204
We present an overview of magnetotransport measurements on the heavy-fermion superconductor CeIrIn5. Sensitive measurements of the Hall effect and magnetoresistance are used to elucidate the low-temperature phase diagram
of this system. The normal-state magnetotransport is highly anomalous, and experimental signatures of a pseudogap-like precursor
state to superconductivity, as well as evidence for two distinct scattering times governing the Hall effect and the MR, are
observed. Our observations point out the influence of antiferromagnetic fluctuations on the magnetotransport in this class
of materials. The implications of these findings, both in the context of unconventional superconductivity in heavy-fermion
systems and in relation to the high-temperature superconducting cuprates, are discussed. 相似文献
28.
Yuncai Xue Zhenping Chen Xiaoyong Zhang Yuling Su Shixun Cao Jincang Zhang 《Journal of Superconductivity and Novel Magnetism》2009,22(7):637-642
The dependence of dc magnetization and electrical transport on temperature were systemically studied for the layered Gd5Ge4 compound. A complex coexistence behavior of ferromagnetism (FM) with antiferromagnetism (AFM) phase and significant magnetoresistance
effect were found under the inducement by the applied magnetic field. The results show an unusual magnetoresistance (MR) effect
with opposite behavior at the high and low temperatures, which is positive at high temperature region and negative at low
temperature region for the layered Gd5Ge4 alloy. And its MR maximum is close to 50%, which can be a very large numerical value e.g. for giant magnetoresistance (GMR)
materials. From the magnetization loop under different temperatures, also a magnetization step behavior was found below ∼6.2 K.
The results proved an existence of reentrance AFM phase at low temperature. From experimental data, also the magnetic phase
diagram is obtained. This kind of complex magnetization is analyzed and discussed in the frame of phase separation. The experimental
results opened also the possibility of application of the layered Gd5Ge4 compound in the fields of information record and sensor technique.
相似文献
29.
磁性金属基体上非磁性涂层厚度的无损检测方法 总被引:1,自引:0,他引:1
论述了磁性金属基体上非磁性涂层厚度的无损测量方法,介绍了机械法和磁阻法两种涂层厚度测量仪的测量原理,以及国内市场上几种涂层测量仪的技术特性。 相似文献
30.