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921.
The interaction and its variation between magnetic grains
in two kinds of magnetic recording tapes are investigated by
first-order reversal curves (FORC) and the $\delta M$ method. The
composition and microstructure of the samples are characterised by
x-ray diffraction and scanning electron microscope. The FORC diagram
can provide more accurate information of the interaction and its
variation, but the $\delta M$ curves cannot. The positive
interaction field and the large variation of the interaction field
have opposite effects on the $\delta M$ curve. 相似文献
922.
An anomalous temperature T dependence of the field Hon for the onset of the second magnetization peak (SMP) in La1.81Sr0.19CuO4 single crystals (with the external magnetic field H oriented parallel to the c axis) is discussed. While the peak field Hp and the magnetization at Hp have a continuous variation with T, Hon exhibits a sudden decrease with increasing T for T 11 K–15 K. The analysis of the nature of the SMP in La2−xSrxCuO4 single crystals in terms of a simple dynamic energy balance relation suggests that the observed behaviour could be related to the particular T dependence of the superfluid density in the case of two-band superconductivity, affecting the T variation of the elastic energy of the vortex system at low H. 相似文献
923.
利用高精度的多组态相互作用及Davidson修正方法 (MRCI+Q),采用ACV5Z-DK全电子基组计算了BH~+离子的前4个离解通道B~+(~1S_g)+H(~2S_g),B~+(~3Pu)+H(~2S_g),B(~2P_u)+H~+(~1Sg)和B~+(~1Pu)+H(~2Sg)的9个Λ—S态的势能曲线.X~2Σ~+,A~2Π和B~2Σ~+态的光谱常数和已有实验值符合得很好,其中b~4Σ~+,3~2Σ~+,3~2Π和4~2Σ~+态的光谱常数为首次报道,3~2Π和4~2Σ~+态具有双势阱结构.预测了A~2Π和B~2Σ~+态的辐射寿命:τ(A~2Π)=239.2 ns和τ(B~2Σ~+)=431.2 ns.最后在考虑自旋轨道耦合效应下讨论了B~2Σ~+与A~2Π态的势能曲线的相交对激光冷却BH~+离子的影响. 相似文献
924.
925.
提出一种新型的OADM结构,并对这种结构的各种特性做了详细的分析,指出该OADM结构在未增加器件和成本的条件下,能完成上下路,组播,再生,波长变换,通道保护和复用段保护等多种功能. 相似文献
926.
927.
928.
In this paper, potential energy curves for the X 1 Σ+ , a3 Π, a′3 Σ+ , d3 , A1 Π and I 1 Σ states of CO have been calculated using complete active space self-consistent field and multi-reference configuration interaction methods. The calculations have been performed at 108 nuclear separations from 0.7 to 4.0 A by the aug-cc-PV5Z basis set. Spectroscopic constants for the six low-lying electronic states are found in good agreement with experimental data. The vibrational states of the X1Σ+ and A1Π states are also calculated, which are reliable and accurate by comparison with the experimental data and the other theoretical values. The transition dipole moment (TDM) shows that the TDM of the two states (X1Σ + A1Π) are reduced strongly with increase of bond length. 相似文献
929.
T. Okuno K. Shigeto T. Ono K. Mibu T. Shinjo 《Journal of magnetism and magnetic materials》2002,240(1-3):1-6
In a circular dot of permalloy with an appropriate size, a vortex structure with perpendicular (turned-up) magnetization at the core is realized. The existence of the perpendicular magnetization spot has been confirmed and the direction of the magnetization, up or down, has been determined by magnetic force microscopy (MFM) for permalloy dots with the diameter of 0.1–1 μm. The switching field of turned-up magnetization is determined by applying external fields perpendicularly and in tilted directions to the plane. By comparing the MFM results and the magnetization curves measured by a SQUID magnetometer, the switching process of turned-up magnetization is argued. 相似文献
930.
J. Ding L. Wang A. Roy J. Ghose 《The European Physical Journal B - Condensed Matter and Complex Systems》2002,28(1):49-54
A compensation temperature of 138 K was observed in the temperature-dependent magnetization curves of MoFe2O4. Relatively slow magnetization relaxation characterized the transitions between different spin states (compensated and uncompensated).
Large magnetic after effect was found in time-dependent magnetization curves after heating or cooling from different characteristic
temperatures for different spin states. The magnetic relaxation was nearly independent on magnetic field, supporting the presence
of spin states and no involvement of domain structure. For the Ti substituted Mo0.6Ti0.4Fe2O4 sample, there were a compensation at ∼ 100 K and a maximum of magnetization at ∼ 175 K. Similar results of anomalous magnetic
relaxation was observed in Ti substituted Mo-ferrite (Mo0.6Ti0.4Fe2O4). If the Mo0.6Ti0.4Fe2O4 sample was heated from 100 K to 235 K, the time-dependent magnetization curve could be considered as a combination of two
magnetic relaxation processes. However, if the sample was heated from 100 K to 295 K, the time- dependent magnetization curve
became complex.
Received 30 October 2001 and Received in final form 21 January 2002 相似文献