• Title/Summary/Keyword: spin wave

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Magnetic Properties of Carbon Chains Doped with 4d Transition Metals

  • Jang, Y.R.;Lee, J.I.
    • Journal of Magnetics
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    • v.13 no.1
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    • pp.7-10
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    • 2008
  • The structural and magnetic properties of functionalized carbon chains doped with 4d transition metals, such as Ru, Rh, and Pd, were investigated using the full-potential linearized augmented plane wave (FLAPW) method. The carbon nanowire doped with Ru exhibited a ferromagnetic ground state with a sizable magnetic moment, while those doped with Rh and Pd had nonmagnetic ground states. For the Ru-doped chain, the density of states at the Fermi level showed large spin polarization, which suggests that the doped nanowire could be used for spintronic applications.

Mossbauer studies of Iron Compounds (철화합물에 대한 뫼스바우어 연구)

  • 김철성
    • Proceedings of the Korean Magnestics Society Conference
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    • 2002.12a
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    • pp.18-19
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    • 2002
  • $^{57}$ Fe화합물에 대한 Mossbauer 분광학 연구로부터 이들 자성물질의 이성핵적이동값, 전기사중극자 분열값 및 초미세자기장의 크기를 결정하였으며 이들값으로부터 Fe의 이온상태, 큐리온도, 각 Site의 점유율, Debye온도, spin wave상수, exchange integral을 계산하였다. $^{57}$ Co감마선을 사용하는 등가속도형 Mossbauer 분광기를 이용하여 4.2 K 부터 900 K 온도영역에서 실험을 하였다. (중략)

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표면, 계면, 초격자에서의 자기이방성과 자기원 이색성의 이론적 계산

  • 이재일;홍순철
    • Journal of the Korean Magnetics Society
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    • v.5 no.4
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    • pp.324-334
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    • 1995
  • 앞의 논문에서 살펴 본바와 같이 밀도 범함수 이론에 바탕을 둔 제일 원리적 에너지 띠 계산 방법의 하나인 FLAPW(Full-potential Linearized Augmented Plane Wave) 방법 에 의해 표면, 계면, 초격자에서의 전자 구조및 자기적 성질, 그리고 구조적 성질이 잘 설명될수 있음을 보았다. 이러한 성공적 결과에도 불구하고 전자구조 계산 방법은 풀어야할 새로운 문제에 직면하고 있는데 그 중 중요한 것은 스핀-궤도 결합(spin-orbit coupling : SOC)을 어떻게 취급하며, 그 결과로 나타나는 자기 결정 이방성( magnetocrystallinge anisotropy : MCA)과 강자성 금속에서 나타나는 광자기적 효과를 설명하는 것이다.

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Pressure-Temperature Phase Diagram of $(TMTSF)_2BF_4$ ($(TMTSF)_2BF_4$의 압력-온도 상태도 연구)

  • Jo, Y.J.
    • Progress in Superconductivity
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    • v.14 no.1
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    • pp.24-29
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    • 2012
  • $(TMTSF)_2BF_4$ containing non-centrosymmetric anions is well known to exhibit a metal insulator transition around 37 K by ordering of the anions with a $q_2$=(1/2, 1/2, 1/2) wave vector. We established pressure-temperature phase diagram of the $(TMTSF)_2BF_4$ compound and showed that it can belong to the general phase diagram of the $(TMTSF)_2X$ family. Application of hydrostatic pressure decreases the anion ordering transition temperature and the superconducting state is finally stabilized below 3.77 K under 7.7 kbar. Magnetoresistance measurement on the $(TMTSF)_2BF_4$ under 7.8 kbar is performed but neither the field-induced spin-density-wave state nor the rapid oscillation is observed up to 9 T.

Populations Accessible to Gravitational Wave and Multi-Messenger Astronomy Within 10 Years

  • Kim, Chunglee
    • The Bulletin of The Korean Astronomical Society
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    • v.44 no.1
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    • pp.58.1-58.1
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    • 2019
  • Gravitational-wave (GW) sources for the next decades would be in majority binaries consisting of neutron stars and/or black holes reside in the extragalactic environment. For example, GW170817 was the first extragalactic neutron star - neutron star binary found by GW observations and it was proved the power of multi-messenger astronomy (MMA) including the KMTNet observations. With the ever increased sensitivity, the $3^{rd}$ observation run (O3) led by the advanced LIGO and advanced Virgo this year aims to search for more 'standard' populations as well as 'exotic' ones expected by stellar evolution. I will present highlights of on-going efforts by researchers in Korea and those in abroad for estimating physical parameters of a source. Mass, spin, distance, and location are prerequisite information to constrain theoretical understanding of the source formation and evolution. Furthermore, these information are to be shared with the international community for follow-up multi-messenger observations. I will present the observational accuracy expected for the future GW observations and discuss their implications. If time allows, I will make a few remarks on prospects of O3 with KAGRA collaborations, which many domestic researchers are closely involved in.

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Electrical Characteristics and Microwave Properties of MgO Bicrystal Josephson Junction with Polyvinylidene Fluoride Gate Electrode (Polyvinylidene Fluoride를 게이트 전극으로 이용한 MgO bicrystal Josephson junction의 전기 특성 및 마이크로파 특성 연구)

  • Yun, Yongju;Kim, Hyeoungmin;Park, Gwangseo;Kim, Jin-Tae
    • Progress in Superconductivity
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    • v.3 no.1
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    • pp.74-77
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    • 2001
  • We have fabricated a high-Tc superconductive transistor with polyvinylidene fluoride (PVDF) gate electrode on MgO bicrystal Josephson junction by spin-coating method. The PVDF ferroelectric film is found to be suitable fur a gate electrode of the superconductive transistor since it has not only small leakage current but also high dieletric constant at low temperature. For the application of superconducting-FET, we investigated millimeter wave properties (60 GHz band) of the Josephson junction with PVDF gate electrode.

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The Electronic and Magnetic Properties of Fe Overlayers on W(110) (W(110)위에 성장한 Fe 웃층의 전자 및 자기적 성질)

  • ;;A. J. Freeman
    • Journal of the Korean Magnetics Society
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    • v.1 no.2
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    • pp.1-8
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    • 1991
  • The electronic and magnetic structure of Fe overlayers on W(110) is determined by means of the all-electron local spin density full potential linearized augmented plane wave (FLAPW) method with a single slab approach. Charge and spin densities, magnetic moments, contact hyperfine fields, and layer projected density of states (LDOS) are presented. For bilayer Fe coverage, we find magnetic moments to be 2.90 and 2.30 ${\mu}_B$ for the surface and subsurface Fe layers, respectively, corresponding to a 18% enhancement of the total magnetization compared with the calculated bulk value (2.22${\mu}_B$);For monolayer coverage the moment is 2.56 ${\mu}_B$ which is enhanced by 16% compared to bulk. Unusual changes in the magnetic hyperfine interaction are found in going from a monolayer to a bilayer coverage. Comparison of the results to the theoretical ones of the clean Fe(110) to discuss the hybridization and the negative pressure effects. We discuss our results by comparing them to experimental results.

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The Magnetic Properties of Amorphus Phase in Mechanically Alloyed $Fe_{50}Zr_{50}$ Powders (기계적 합금화한 비정질 $Fe_{50}Zr_{50}$ 분말의 자기특성)

  • 이성의;나형용;김원태;유성초
    • Journal of the Korean Magnetics Society
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    • v.7 no.1
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    • pp.7-12
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    • 1997
  • Amorphous $Fe_{50}Zr_{50}$ alloy has been manufactured by mechanical alloying from pure elemental powders of Fe and Zr in conventional ball mill under an Ar atmosphere. Structure and magnetic properties of the amorphous phase were studied by transmission electron microscopy and SQUID magnetometry. Selected area diffraction patterns taken from the mechanically alloyed powders showed two halo rings, indicating coexistence of Fe rich and Zr rich amorphous phases in mechanically alloyed powder. Curie temperature of the Fe rich amorphous phase, measured by Arrot plot, was 195 K. Fe content in the ferromagnetic amorphous phase, estimated from the Curie temperature, was about 65 at%. Spin wave stiffness constant of $Fe_{50} Zr_{50}$ alloys processed for 100 and 200 hrs were 52.2 and 63.8 meV, respectively. The higher spin wave stiffness constant in 200 hrs milled powders may arise from the precipitation of $\alpha$-Fe by partial crystallization of amorphous phase.

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Mossbauer Spectroscopy Studies of Garnet $Y_{2.5}La_{0.5}Fe_5O_{12}$ (Garnet $Y_{2.5}La_{0.5}Fe_5O_{12}$의 Mossbauer 분광학 연구)

  • 염영랑;김철성
    • Journal of the Korean Magnetics Society
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    • v.9 no.1
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    • pp.29-34
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    • 1999
  • $Y_{2.5}La_{0.5}Fe_5O_{12}$ is fabricated by a sol-gel method and the magnetic properties of single phase garnet are investigated by using X-ray diffraction, vibrating sample magnetometer, scanning electron microscopy and M$\"{o}$ssbauer spectroscopy. The single phase powders garnet was fired at 100$0^{\circ}C$ for 8 hours. The crystal structures of samples are cubic garnet. Mossbauer spectroscopy were measured from 13 K to 750 K. M$\"{o}$ssbauer spectra show that the iron exist ferric trivalence in sample. The spin wave constants were determined $B_{3/2}=0.32{\pm}0.05,\; C_{5/2}=0.18{\pm}0.05$ and Debye temperature were determined 382 K at 24(d) site and 246 K at 16(a)-site. The saturation magnetization $M_s$ of powder is 25 emu/g. 25 emu/g.

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