• 한국진공학회:학술대회논문집
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• 한국진공학회 2009년도 제38회 동계학술대회 초록집
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• pp.135-135
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• 2010

In Mn-Ge equilibrium phase diagram, many Mn-Ge intermetallic phases can be formed with difference structures and magnetic properties. The MnGe has the cubic structure and antiferromagnetic(AFM) with Neel temperature of 197 K. The calculation predicted that the $MnGe_2$ with $Al_2Cu$-type is hard to separate between the paramagnetic(PM) states and the AFM states because this compound displays PM and AFM configuration swith similar energy. Mn-doped Ge showed the FM with Currie temperature of 285 K for bulk samples and 116 K for thin films. In addition, the $Mn_5Ge_3$ compound has hexagonal structure and FM with Curie temperature around 296K. The $Mn_{11}Ge_8$ compound has the orthorhombic structure and Tc is low at 274 K and spin flopping transition is near to 140 K. While the bulk $Mn_3Ge_2$ exhibited tetragonal structure ($a=5.745{\AA}$;$c=13.89{\AA}$) with the FM near to 300K and AFM below 150K. However, amorphous $Mn_3Ge_2$ ($a-Mn_3Ge_2$) was reported to show spin glass behavior with spin-glass transition temperature (Tg) of 53 K. In addition, the transition of crystalline $Mn_3Ge_2$ shifts under high pressure. At the atmospheric pressure, $Mn_3Ge_2$ undergoes the magnetic phase transition from AFM to FM at 158 K. The pressure dependence of the phase transition in $Mn_3Ge_2$ has been determined up to 1 GPa. The transition was found to occur at 1 GPa and 155 K with dT/dP=-0.3K/0.1 GPa. Here report that Ferromagnetic $Mn_3Ge_2$ thin films were successfully grown on GaAs(001) and GaSb(001) substrates using molecular beam epitaxy. Our result revealed that the substrate facilitates to modify magnetic and electrical properties due to tensile/compressive strain effect. The spin-flopping transition around 145 K remained for samples grown on GaSb(001) while it completely disappeared for samples grown on GaAs(001). The antiferromagnetism below 145K changed to ferromagnetism and remained upto 327K. The saturation magnetization was found to be 1.32 and $0.23\;{\mu}B/Mn$ at 5 K for samples grown on GaAs(001) and GaSb(001), respectively.

• 새물리
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• 제68권12호
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• pp.1302-1307
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• 2018

마그네타이트 분말에 대해 Verwey 전이 전후에서의 구조적, 전기적 및 자기적 성질을 고찰하였다. 마그네타이트 시료는 고온열분해법으로 합성한 나노입자를 $800^{\circ}C$, 진공을 뽑는 상태에서 1시간동안 열처리하여 얻었다. 시료의 형태학적, 결정학적 분석은 주사전자현미경(scanning electron microscope, SEM)과 X-선 회절(X-ray diffraction, XRD)을 이용하였으며 시료진동형 자기력계(vibrating sample magnetometer, VSM)와 뫼스바우어 분광법, 비저항 측정 등을 통해 미시적/거시적 자성 및 전기적 특성을 각각 관찰하였다. Verwey 전이점에서 비저항과 자기모멘트의 불연속적 온도의존성을 관측하였으며 자기이방성상수가 $T_V$ 부근에서 약간 감소하는 것이 관찰되었다. 뫼스바우어 스펙트럼은 $T_V$ 전후에서 모두 사면체적 (A) 자리와 팔면체적 (B) 자리에 기인하는 2개의 6선 스펙트럼의 중첩으로 나타났으며 B자리에서 철 이온의 원자가에 따른 흡수선의 구분은 불가능하였다. $T_V$ 를 중심으로 하여 저온영역의 정상스피넬(normal spinel)에서 고온영역의 역스피넬(inverse spinel)의 배위교차(coordination crossover)가 발생하였다.

• 한국자기학회지
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• 제10권4호
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• pp.149-153
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• 2000

변하는 자기장을 단결정 및 다결정 망간 산화물 La$_{0.7}$Ca$_{0.3}$MnO$_3$에 인가하였을 때 자기 엔트로피가 크게 변하는(거대 자기 엔트로피 변화)현상이 관측되었다. 이 거대 자기 엔트로피 변화는 Curie온도에서 유사 1차상전이에 의한 자화값의 급격한 변화에 의한 것으로 추측된다. 이 거대 자기 엔트로피 변화와 망간 산화물 Curie 온도의 100 K＜T＜400 K 내의 조절 용이성은 상온을 포함한 넓은 온도에서 망간 산화물을 이용한 자기 냉각 기관의 개발 가능성을 제시하고 있다. 있다.

• Journal of Magnetics
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• 제9권4호
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• pp.113-115
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• 2004

The magnetization properties have been measured for amorphous $Fe_{82}Mn_{8-x}B_xZr_{10}$ (x = 0-8) alloys. The temperature dependence of magnetization for these alloys shows the existence of antiferromagnetic couplings between Fe atoms in low fields at low temperatures. The magnetic parameters, obtained from the magnetization behavior are consistent with the presence of mixed magnetic state. The Curie temperature and magnetic moment increased with an increase of the concentration of B and spin glass like transition observed at low temperature decreases and finally vanishes at x = 8 at %. Our result suggests that the substitution of B for Mn seems to cause an increase of magnetic order.

• 한국자기공명학회논문지
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• 제14권2호
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• pp.76-87
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• 2010

The structural phase transition of $Cs_2MnCl_4{\cdot}2H_2O$ single crystals was investigated by determining the $^{133}Cs$ spin-lattice relaxation time $T_1$. The number of resonance lines in the $^{133}Cs$ spectrum changes from seven to one near 375 K, which means that above 375 K the Cs sites are symmetric. Further, the $T_1$ of the $^{133}Cs$ nucleus undergoes a significant change near 375 K, which coincides with the change in the splitting of the $^{133}Cs$ resonance lines. The change in $T_1$ near $T_C$ is related to the loss of $H_2O$, and means that the forms of the octahedra of water molecules surrounding $Cs^+$ are disrupted.

• 한국재료학회지
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• 제28권8호
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• pp.445-451
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• 2018

We report the structural, magnetic and magnetocaloric properties of $Sr_{1.8}Pr_{0.2}FeMo_{1-x}W_xO_6$($0.0{\leq}x{\leq}0.4$) samples prepared by the conventional solid state reaction method. The X-ray diffraction analysis confirms the formation of the tetragonal double perovskite structure with a I4/mmm space group in all the synthesized samples. The temperature dependent magnetization measurements reveal that all the samples go through a ferromagnetic to paramagnetic phase transition with an increasing temperature. The Arrott plot obtained for each synthesized sample demonstrates the second order nature of the magnetic phase transition. A magnetic entropy change is obtained from the magnetic isotherms. The values of maximum magnetic entropy change and relative cooling power at an applied field of 2.5 T are found to be $0.40Jkg^{-1}K^{-1}$ and $69Jkg^{-1}$ respectively for the $Sr_{1.8}Pr_{0.2}FeMoO_6$ sample. The tunability of magnetization and excellent magnetocaloric features at low applied magnetic field make these materials attractive for use in magnetic refrigeration technology.

• Food Science and Biotechnology
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• 제16권4호
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• pp.646-649
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• 2007

The effect of the addition of 2 kinds of chemically modified starches (the anti-caking agents; tapioca starch and com starch) on caking of ramen soup was observed using a low-resolution proton-pulsed nuclear magnetic resonance (NMR) technique. After storing ramen soup samples with diverse compositions of modified starch at 20-40% relative humidity for 4 weeks, changes in the spin-spin relaxation time constant ($T_2$) were measured as a function of temperature. $T_2-Temperature$ curves for ramen soup containing modified starches showed that the caking initiation temperature (glass transition temperature) was increased by $5^{\circ}C$ following the addition of only 0.5% modified cornstarch. The results indicate that the modified com starch used in this study would be an effective anti-caking agent for ramen soup, thus prolonging the shelf life of the product.

• 한국재료학회지
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• 제21권2호
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• pp.73-77
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• 2011

Specific heat of a crystal is the sum of electronic specific heat, which is the specific heat of conduction electrons, and lattice specific heat, which is the specific heat of the lattice. Since properties such as crystal structure and Debye temperature do not change even in the superconducting state, the lattice specific heat may remain unchanged between the normal and the superconducting state. The difference of specific heat between the normal and superconducting state may be caused only by the electronic specific heat difference between the normal and superconducting states. Critical temperature, at which transition occurs, becomes lower than $T_{c0}$ under the influence of a magnetic field. It is well known that specific heat also changes abruptly at this critical temperature, but magnetic field dependence of jump of specific heat has not yet been developed theoretically. In this paper, specific heat jump of superconducting crystals at low temperature is derived as an explicit function of applied magnetic field H by using the thermodynamic relations of A. C. Rose-Innes and E. H. Rhoderick. The derived specific heat jump is compared with experimental data for superconducting crystals of $MgCNi_3$, $LiTi_2O_4$ and $Nd_{0.5}Ca_{0.5}MnO_3$. Our specific heat jump function well explains the jump up or down phenomena of superconducting crystals.

• 한국진공학회:학술대회논문집
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• 한국진공학회 2014년도 제46회 동계 정기학술대회 초록집
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• pp.294-294
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• 2014

Developing magnetic thin films with desirable physical properties is a key step to promote research in spintronics. Organic-based magnetic material is a relatively new kind of materials which has magnetic properties in a molecular and microscopic level. These materials have been constructed by the coordination between 3d transition metal and organic materials producing long-range magnetic orders with a relatively high transition temperature. However, these materials were mostly synthesized as a form of powder, which is difficult to study for their physical properties as well as apply for electronic/spintronic devices. In this study, we have employed physical vapor deposition (PVD) to develop a new organic-based hybrid magnetic film that is achieved by the coordination of Fe and tetracyanoquinodimethane (TCNQ). The IR spectra of the grown film show modified CN vibration modes in TCNQ, which suggest a strong bonding between Fe and TCNQ. The thin film has both ferromagnetic and semiconducting behaviors, which is suitable for molecular spintronic applications. The high resolution photoemission (HRPES) spectra also show shift of 1s peak point of nitrogen and the carbon 1s peaks display traces of charge transfer from Fe to TCNQ as well as shake-up features, which suggest strong bonding and anti-bonding nature of coordination between Fe and TCNQ.

• 한국광물학회지
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• 제24권1호
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• pp.37-42
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• 2011

지구의 암권에서 가장 중요한 자성광물은 자철석이다. 암석 내에 존재하는 자철석의 성분과 입자 크기에 관한 정보를 알아내는데 저온 자화특성을 이용하려 한다. 물리적 방법의 하나인 저온 자화특성 실험은 비파괴적이며 운석과 같이 연구 대상 시료의 수량이 제한된 경우 특히 유용하게 사용된다. 금번 연구에서는 세 종류의 합성 자철석 시료와 세 종류의 자철석 함유 암석 시료에 대해 저온포화잔류자화의 가열실험과 실온포화잔류자화의 냉각/가열 실험을 수행하였다. 실험 결과 저온포화잔류자화는 가열함에 따라 자철석의 버웨이변환온도(~105~120 K)를 지나며 급격히 감소한다. 자철석의 버웨이변환온도와 등방점(135 K)를 모두 거치는 실온포화잔류자화의 냉각과 가열 실험 결과에서는 저온포화잔류자화의 가열 실험 결과와 비교하였을 때 자화회복력이 뛰어나고, 자화상실이 상대적으로 완만히 진행된다. 저온포화잔류자화와 실온포화잔류자화 모두 자철석의 입자 크기가 증가할수록 소실되는 포화잔류자화의 비가 증가한다. 결국 저온포화잔류자화기억도와 실온포화잔류자화기억도 모두 자철석의 입자가 커질수록 감소한다. 따라서 저온 자화특성을 이용하면 암석 내 자철석 입자의 크기를 비파괴적인 방법으로 유추할 수 있다.