• 한국진공학회지
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• 제6권S1호
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• pp.53-58
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• 1997

It is well known that the equiatomic FeAl alloy crystallizes in a paramagnetic CsCl structure and is very stable in a wide temperature range owing to a significant charge transfer from Al to Fe. A presence of structural defects normally enhances the magnetic and magneto-optical properties of this alloy. In this study spin-resolved photoemission and magnetic circular dichroism (MCD) were carried out on both ordered and disordered $Fe_{0.52}Al_{0.48}$ alloy films. The disordered state in the alloy films was obtained by a vapor quenching deposition on cooled substrates. It is shown that the order-disorder transition in the Fe0.52Al0.48 alloy films leads to a significant change in the spin polarization. Form the MCD results the orbital and spin magnetic moments of the constituent atoms are obtained. According to the sum rule the spin and orbital magnetic moments of Fe in the disordered FeAl film are $\mu\frac{SR}{spin}=0.8\mu_B$ and $\mu\frac{SR}{orb}=0.14\mu_B$ respectively. The spin magnetic moment is also evaluated to be $\mu\frac{BR}{spin}=0.77\mu_B$ by the branching ration method employing a photon polarization of 90%.

• 한국자기공명학회논문지
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• 제15권1호
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• pp.40-53
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• 2011

The NMR spectra of $Li_3Rb(SO_4)_2$ crystals and their relaxation processes were investigated by using $^7Li$ and $^{87}Rb$ NMR. The relaxation rates of the $^7Li$ and $^{87}Rb$ nuclei in the crystals were found to increase with increasing temperature, and can be described by the relation $T_1^{-1}{\propto}AT^2$. The dominant relaxation mechanism for these nuclei with electric quadrupole moments is provided by the coupling of these moments to the thermal fluctuations of the local electric field gradient via Raman spin-phonon processes.

• 한국자기학회지
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• 제14권3호
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• pp.94-98
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• 2004

MgCCo$_3$에서 Mg와 Co로 이루어진 (001)표면(MgCo-Term) 또는 C와 Co로 이루어진 (001표면(CCo-term)의 전자구조와 자성을 FLAPW 에너지띠 방법을 이용하여 이론적으로 계산하였다. MgCo-Term의 경우 표면에서 Co원자의 자기모멘트는 1.00$\mu$$_{B}$로서 가운데층에 비하여 많이 증가하였고 표면 바로 밑층에서는 가운데층과 비슷한 값을 보였다. CCo-Term의 경우 Co원자의 자기모멘트는 표면에서 뿐만 아니라 표면 바로 밑층에서도 증가하여 각각 0.75와 0.80$\mu$$_{B}$의 값을 나타내고 있다. C와 Mg원자는 두 경우 모두 Co원자와 반대방향으로 스핀분극되었다. 계산된 상태밀도로부터 이러한 표면에서의 자기모멘트의 증가는 Co-3d 띠의 국소화에 의함을 알 수 있었고 여기서 Co-3d와 C-2p 사이의 띠 혼성이 중요한 역할을 하였다.

• Journal of Magnetics
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• 제6권3호
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• pp.80-82
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• 2001

We have investigated magnetism of $Fe_2 /Ir_4$(001) superlattice in terms of a first-principles calculation by using an all-electron full-potential linearized augmented plane-wave (FLAPW) method within the generalized gradient approximation (GGA). We considered two magnetic states, the ferromagnetic (FM) and antiferromagnetic (AFM) coupled states between the Fe layers. It was found that the FM state was energetically more stable than the AFM one by 0.166 eV. Calculated magnetic moments of the Fe layers were, in absolute values, 2.45$\mu_B$ and 2.30 $\mu_B$for the FM and AFM states, respectively. We also found that the Ir layers had very small magnetic moments less than 0.1 $\mu_B$ for both magnetic states. In all the magnetic states, the subinterface Ir layers were coupled antiferromagnetically to the interface Ir layers, while the interface Ir layers were always coupled frerromagnetically to the interface Fe layers. These results contradicted to recent experimental reports of magnetically "dead"Fe layers in Fe/Ir superlattices for which the Fe layer thickness was less than two atomic layers. We attributed that the experimentally observed "dead"Fe layers were due to possible interdiffusion between Ir and Fe layers.en Ir and Fe layers.

• 한국자기학회지
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• 제15권6호
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• pp.299-302
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• 2005

전이금속 Fe-Pt 나노선의 자기적 성질을 수도퍼텐셜 및 전전자(all-electron) 제일원리 전자구조 계산 방법으로 연구하였다. 직선 구조와 지그재그 구조에 대해서 결합에너지를 계산함으로써 안정된 구조를 결정했고, 결합거리, 결합각도, 자기모멘트, 스핀밀도, 상태밀도 등을 계산함으로써 전이금속 나노선의 구조적 성질과 자기적 성질을 연구하였다. Fe-Pt 나노선의 경우에 지그재그 구조가 직선 구조보다 더 안정된 것으로 계산되었고, 직선 구조에 비해서 결합길이는 증가하지만 자기모멘트는 감소하였다.

• 대한화학회지
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• 제23권1호
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• pp.1-6
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• 1979

사각형 및 사면체 $[M(II)N_2S_2]$형태 착물의 쌍극자모멘트를 spherical harmonics의 전개방법에 의하여 계산하였다. [M(II) = Co(II), Ni(II), Cu(II) 또는 Zn(II)]. 이들 착물에 대한 쌍극자모멘트의 계산치가 실험치 범위안에 들었다. 계산한 쌍극자모멘트와 자기적 성질을 기초로하여 벤젠용액에서 이들 착물에 대한 가능한 구조를 고찰하였다.

• 한국자기학회지
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• 제18권1호
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• pp.1-8
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• 2008

최근 발전하는 초박막 자기 시료의 정확한 자기 모멘트 측정을 위하여 저자기 모멘트 표준 시료를 제작하였다. 정밀한 저자기 모멘트 표준시료를 제작하기 위해서 자력계를 미리 자기잡음으로부터 차폐시켰고, 시료준비과정에서 강자성 불순물을 고려한 시료의 순도, 절단 방법, 시료의 모양과 두께 등을 고려하였다. 본 연구에서는 SQUID 자력계를 이용한 자기 모멘트 측정에 적합하게 $4mm{\times}6mm$ 면적을 갖는 Al, Ti과 W로 된 판상형 시료 3 개를 준비하였다. Pd 금속의 경우는 이미 잘 보정된 실린더형 시료를 사용하였다. 준비된 세 개의 판상형 시료의 경우 50,000 Oe 이내의 자기장영역에서 자기이력현상이 관측되지 않았고 모두 양호한 선형성을 보였다. 290K에서 310K까지의 온도영역에서 Ti, Al, W의 자기모멘트 값의 변화는 각각 0.7%, 1.5%, 0.1% 이내로 작았다. 본 연구에서 준비된 각각의 시편에 대해 자기모멘트 값을 결정하였으며, round robin test를 통하여 측정값의 신뢰도를 확인하였다. 그 결과 본 연구에서 제작한 표준시료는 저자기 모멘트 측정에 편리하고 적합하게 활용될 수 있음을 알 수 있었다.

• 한국소음진동공학회:학술대회논문집
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• 한국소음진동공학회 2009년도 추계학술대회 논문집
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• pp.176-181
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• 2009

In this article, excitation forces due to unbalance mass in a flywheel energy storage system will be discussed, which mainly consists of a composite flywheel and active magnetic bearings and a motor/generator. Unbalance mass causes moments as well as centrifugal forces to the center of the flywheel when the flywheel rotates. The moment excites the flywheel to revolve in the shape of conical revolution and in real operation, the flywheel shows an aspect that conical revolution is a main mode when system failure occurs. Although there are several excitation sources to the flywheel including unbalance mass, an excitation from motor and control issues of the magnetic bearings, we could infer unbalance mass is the main cause of the failure from a comparison between a composite flywheel and a steel flywheel in the same condition. In this of view, excitation forces and moments induced by unbalance mass should be carefully considered in dynamics of the flywheel so that the energy storage system can be operated in more stable conditions.

• 한국자기학회:학술대회 개요집
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• 한국자기학회 2012년도 자성 및 자성재료 국제학술대회
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• pp.172-172
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• 2012

A Pt-skin $Pt_3Ni$(111) surface was reported to show high catalytic activity. In this study, we investigated the magnetic properties and electronic structures of the various oriented surfaces of bulk-terminated and Pt-segregated $Pt_3Ni$ by using a first-principles calculation method. The magnetic moments of Pt and Ni are appreciably enhanced at the bulk-terminated surfaces compared to the corresponding bulk values, whereas the magnetic moment of Pt on the Pt-segregated $Pt_3Ni$(111) surface is just slightly enhanced because of the reduced number of Ni neighboring atoms. Spin-decomposed density of states shows that the dz2 orbital plays a dominant role in determining the magnetic moments of Pt atoms in the different orientations. The lowering of the d-band center energy (-2.22 eV to -2.46 eV to -2.51 eV to -2.65 eV) in the sequence of bulk-terminated (100), (110), (111), and Pt-segregated (111) may explain the observed dependence of catalytic activity on surface orientation. Our d-band center calculation suggests that an observed enhanced catalytic activity of a $Pt_3Ni$(111) surface originates from the Pt-segregation.

• Journal of Magnetics
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• 제11권1호
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• pp.20-24
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• 2006

Very recently, it was presented that the one dimensional (1D) CuO atomic chains can maintain large magnetic moments. In this work, we analyzed m-resolved density of states (DOS) to understand the peculiar spin polarization occurred in Cu atoms. It was found that the $\mid{m}\mid=1$ states play an essential role in the spin polarization of Cu atoms. In addition, we calculated magnetic anisotropy energy (MAE) and observed that the distribution of MAE is strongly sensitive to the interatomic distance between Cu and O atoms. Besides, it was revealed that the contribution to MAE comes for the second half of Brillouin zone (BZ).