• Title/Summary/Keyword: $GdB_4$

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Synthesis and Magnetic Relaxation Properties of Paramagnetic Gd-complexes of New DTPA-bis-amides. The X-ray Crystal Structure of [Gd(L)(H2O)]·3H2O (L = DTPA-bis(4-carboxylicphenyl)amide)

  • Dutta, Sujit;Kim, Suk-Kyung;Lee, Eun-Jung;Kim, Tae-Jeong;Kang, Duk-Sik;Chang, Yong-min;Kang, Sang-Ook;Han, Won-Sik
    • Bulletin of the Korean Chemical Society
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    • v.27 no.7
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    • pp.1038-1042
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    • 2006
  • A new type of DTPA-bis-amides (L1-L4) and their Gd(III)-complexes of the type $[Gd(L)(H_2O)]{\cdot}nH_2O$ (5: L1; 6: L2; 7: L3; 8: L4) have been prepared and characterized by analytical and spectroscopic techniques. The X-ray crystal structure of 8 has been determined for structural confirmation. The coordination geometry adopts a tricapped trigonal prism geometry with L4 acting as a chelate octadentate and a water molecule in the coordination sphere. Crystals are monoclinic, $P2_1$, a = 14.468(3), b = 19.235(4), c = 13.527(2) $\AA$ $\beta$ = $107.245(3)^{\circ}$, V = 3595.2(11) $\AA^3$, Z = 4, $D_{calc}$ = 1.570. Significant increases in relaxivities are observed with 6 and 7 as compared with that of $Omniscan^{(R)}$, a commercial MR agent: R1 = 12.46 $mM^{-1}\;s^{-1}$, R2 = 8.76 $mM^{-1}\;s^{-1}$ for 6; R1 = 12.77 nm-1 s-1, R2 = 7.60 mM-1 s-1 for 7; R1 = 4.9 $mM^{-1}\;s^{-1}$, R2 = 4.8 $mm^{-1}\;s^{-1}$ for $Omniscan^{(R)}$. In the case of 5, however, both R1 and R2 are found to be lower to show 2.09 $mM^{-1}\;s^{-1}$, and 1.82 $mM^{-1}\;s^{-1}$, respectively.

Synthesis and Crystal Structure of a New Quaternary Chalcoantimonide: KLa2Sb3S9 and KSm2Sb3Se8

  • Kim, Sung-Jin;Park, Sun-Ju;Yim, Sun-Ah
    • Bulletin of the Korean Chemical Society
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    • v.25 no.4
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    • pp.485-490
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    • 2004
  • Silver-needle shaped crystals of $KLa_2Sb_3S_9$ from $K_2S_x$ flux and $KSm_2Sb_3Se_8$ from NaCl/KCl flux reactions were obtained and their crystal structures were determined by the single crystal X-ray diffraction method. $KLa_2Sb_3S_9$ crystallizes in the orthorhombic noncentrosymmetric space group $P2_12_12_1$ (No.19) with a unit cell of a = 4.220(3) ${\AA}$, b = 24.145(2) ${\AA}$, c = 14.757(5) ${\AA}$ and Z = 4. $KSm_2Sb_3Se_8$ crystallizes in the orthorhombic space group Pnma (No.62) with a unit cell of a = 16.719(3) ${\AA}$, b = 4.1236(8) ${\AA}$, c = 22.151(4) ${\AA}$ and Z = 4. Both structures have three-dimensional tunnel frameworks filled with $K^+$ ions. $KSm_2Sb_3Se_8$ is an ordered version of $ALn_{1{\pm}X}B_i{4{\pm}X}S_8$, and it is made up of NaCl-type and $Gd_2S_3$-type fragments. $KLa_2Sb_3S_9$ also contains building fragments similar to those of $KSm_2Sb_3Se_8$, however, there are chalcogen-chalcogen bonds in the $Gd_2S_3$-type fragment. The formula of $KLa_2Sb_3S_9$ can be described as $(K^+ )(La^{3+})_2(Sb^{3+})^3(S^{2-})_7(S_2^{2-})$.

Microstructure and high temperature mechanical properties of sapphire/R-Al-O(R = Y, Gd, Er, Ho, Dy) eutectic fibers grown by micro-pulling-down method

  • Hasegawa, K.;Yoshikawa, A.;Durbin, S.D.;Epellbaum, B.M.;Fukuda, T.;Waku, Y.
    • Journal of the Korean Crystal Growth and Crystal Technology
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    • v.9 no.4
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    • pp.432-436
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    • 1999
  • Fiber growth of $Al_{2}O_{3}/R-Al-O$ (R = Y, Gd, Dy, Ho, Er) eutectic by the micro-pulling down method is described. The thermal stability and strength at elevated temperature of each materials is evaluated in relation to the microstructure.

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Estimation of Neutron Absorption Ratio of Energy Dependent Function for $^{157}Gd$ in Energy Region from 0.003 to 100 eV by MCNP-4B Code

  • Lee, Sam-Yol
    • Journal of the Korean Society of Radiology
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    • v.3 no.3
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    • pp.23-25
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    • 2009
  • Gd-157 material has very large neutron capture cross section in the thermal region. So it is very useful to shield material for thermal neutrons. Futhermore, in the neutron capture experiment and calculation, the neutron absorption and scattering are very important. Especially these effects are conspicuous in the resonance energy region and below the thermal energy region. In the case of very narrow resonance, the effect of scattering is to be more considerable factor. In the present study, we obtained energy dependent neutron absorption ratios of natural indium in energy region from 0.003 to 100 keV by MCNP-4B Code. The coefficients for neutron absorption was calculated for circular type and 1 mm thickness. In the lower energy region, neutron absorption is larger than higher region, because of large capture cross section (1/v). Furthermore it seems very different neutron absorption in the large resonance energy region. These results are very useful to decide the thickness of sample and shielding materials.

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자기냉동/냉장고와 공조기

  • 이종석
    • The Magazine of the Society of Air-Conditioning and Refrigerating Engineers of Korea
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    • v.30 no.6
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    • pp.49-54
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    • 2001
  • 1990년대 중반부터 후반에 결쳐 미국의 Astronautics사와 Ames연구소에 의한 공동연구결과는 자기냉동이 실현 가능한기술이며 가스액화,음식 냉동 및 저장, 대규모 건물 공조 등에 있어서 기존의 증기압축냉동에 필적할 만하다는 것을 밝혔다. 더 최근의 연구와 개발 노력은 자기장 원(source)으로 $Nd_2Fe_{14}B$ 영구자석배열을 이용한 회전식 자기냉동기가 가정용 공조기나 냉동/냉장고에 사용될 수 있음을 나타내고있다. Gd 금속구를 사용한 2단 자기 냉동/냉장고의 예비설계는 냉동실 온도가 $-12^{\circ}C(10^{\circ}F)$, 냉동실 온도가 $-1^{\circ}C(30^{\circ}F)$에서 전체 성능계수 3 그리고 냉각능력 120W를 얻을 수 있음을 제시한다. 자기장 원으로서 개선된 영구자석 배열을 이용한다면 카르노 효율의 60%와 성능계수 4.5에 이를 수 있을 것으로 보여진다. 그리고 자기냉동은 오존층 파괴물질 (CFC's)이나 온설가스(HCFC's와 HFC's)를 사용하지 않기 때문에 깨끗한 환경을 만드는데 기여한다. 동시에 상용 Gd으로부터 거대한 자기열량효과를 가진 재료인 $Gd_5(Si_2Ge_2)$를 kg 단위로 생산할 수 있는 정도로 연구가 진전되었다. 이 신재료를 저렴한 가격에 얻을 수 있게 됨으로써 Gd 금속을 자기냉매로 사용하도록 설계 되었던 공조기나 냉동/냉장고의 효율이 더 좋아질 것으로 예상된다.

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Optical Properties of Infinite-Layer Superconductors $Sr_{0.9}$$Ln_{0.1}$Cu$O_2$ (LnLa, Gd, Sm) (무한층 초전도체 $Sr_{0.9}Ln_{0.1}CuO_2$(Ln=La, Gd, Sm)의 광학적 성질)

  • Mun, Mi-Ock;Park, Young-Sub;Kim, Kibum;Kim, Jae H.;A. B. Kuzmenko
    • Progress in Superconductivity
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    • v.3 no.1
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    • pp.13-16
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    • 2001
  • We have measured the reflectivity of superconducting infinite-layer compounds $Sr_{0.9}$ $Ln_{0.1}$ Cu $O_2$ (Ln=La, Gd, Sm) with $T_{c}$ : 39 K using a Fourier-transform infrared spectrometer. We have identified the optical phonon modes from their infrared reflectivity and conductivity spectra and have proposed possible displacement patterns. The La- and the Gd-doped compounds exhibited only four ($2A_{2u}$ $+2E_{u}$) out of the five ($2A_{2u}$ $3E_{u}$) infrared-active phonons predicted by a group theoretical analysis whereas the Sm-doped compound exhibited all five modes. For the La-doped sample, we investigated the temperature dependence of the optical response functions in a wide temperature range of 7 - 300 K. In FIR region, the reflectivity is apparently enhanced below ~120 $cm^{-1}$ as temperature decreases across $T_{c}$. The value of $2$\Delta$/k_{B}$ $T_{c}$ is about 4.5, which is consistent with maximum gap value of d-wave $high- T_{c}$ cuprates.> c/ cuprates.uprates.s.

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Preparation of Metal-p-aminobenzyl-DOTA Complex Using Magnetic Particles for Bio-tagging in Laser Ablation ICP-MS

  • Yoon, S.Y.;Lim, H.B.
    • Bulletin of the Korean Chemical Society
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    • v.33 no.11
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    • pp.3665-3670
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    • 2012
  • Metal-p-$NH_2$-Bn-DOTA (paraammionobenzyl-1,4,7,10-tetraazacyclododecane-1,4,7,10-tetraacetic acid: ABDOTA) complex was synthesized and purified for bio-tagging to quantify biological target materials using laser ablation (LA)-ICP-MS. Since the preparation of a pure and stable tagging complex is the key procedure for quantification, magnetic particles were used to purify the synthesized metal-ABDOTA complex. The magnetic particles immobilized with the complex attracted to a permanent magnet, resulting in fast separation from free un-reacted metal ions in solution. Gd ions formed the metal-complex with a higher yield of 64.3% (${\pm}3.9%$ relative standard deviation (RSD)) than Y ions, 52.3% (${\pm}2.5%$ RSD), in the pH range 4-7. The complex bound to the magnetic particles was released by treatment with a strong base, of which the recovery was 81.7%. As a reference, a solid phase extraction (SPE) column packed with Chelex-100 resin was employed for separation under similar conditions and produced comparable results. The tagging technique complemented polydimethylsiloxane (PDMS) microarray chip sampling in LA-ICP-MS, allowing determination of small sample volumes at high throughputs. For application, immunoglobulin G (IgG) was immobilized on the pillars of PDMS microarray chips and then tagged with the prepared Gd complex. IgG could then be determined through measurement of Gd by LA-ICP-MS. A detection limit of 1.61 ng/mL (${\pm}0.75%$ RSD) for Gd was obtained.

Micro gadolinium oxide dispersed flexible composites developed for the shielding of thermal neutron/gamma rays

  • Boyu Wang;Xiaolin Guo;Lin Yuan;Qinglong Fang;Xiaojuan Wang;Tianyi Qiu;Caifeng Lai;Qi Wang;Yang Liu
    • Nuclear Engineering and Technology
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    • v.55 no.5
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    • pp.1763-1774
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    • 2023
  • In this study, a series of flexible neutron/gamma shielding composites are fabricated through the doping of Gd2O3 into the matrix of SEBS with (MGd2O3: MSEBS) % from 5% to 100%. Neutron transmittance test shows an exponential attenuation with the increase of areal density of Gd, in which the transmittance T ranges from 59.1440% to 35.3026%, with standard deviation less than 2.2743%, mass attenuation coefficient 𝜇m from 0.3194 cm2/g to 0.4999 cm2/g, and half value layer-HVL value from 2.4530 mm to 1.1313 mm. Shielding efficiency of the Gd2O3/SEBS composites is basically improved in comparison with that of B4C/SEBS. The transmittance T, mass/linear attenuation coefficient 𝜇m and 𝜇, HVL and effective atomic number Zeff for the shielding of γ rays (39 keV, 59 keV and 122 keV) are measured and calculated with XCOM as well as MCX programs. Finally, plots of the three dimensional relationships between transmittance, doping amount and thickness are provided to the guidance for engineering shielding design. In summary, the Gd2O3/SEBS composite is proved to be an effective flexible neutron/low energy γ rays shielding material, which could be of potential applications in the field of nuclear technology and nuclear engineering.