• Journal of Photoscience
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• 제9권2호
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• pp.460-462
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• 2002

Absorption spectra of biological specimens in the soft X-ray region have been presented with special reference to the XANES (X-ray absorption Near Edge Structure) of constituent elements. Absorption spectrum in this wavelength region is characterized by the absorption edges from which elemental content could be derived. In addition, XANES has a characteristic profile for chemical environment around the element such as chemical bond. Using the specific absorption peak we can assign not only the chemical bond but also molecules having such a chemical bond. In the present paper, absorption spectrum of DNA was measured in the wavelength range from 1.5nm to 5nm. Spectrum of Chinese Hamster Ovary (CHO) cells was compared with the DNA spectrum. XANES were distinct at the K absorption edges of major elements, C, N and O. In the spectrum of the cells prominent peaks at the L absorption edge of minor element Ca were also detectable. XANES profiles in small local areas in a cell could also be measured in combination with X-ray microscopy. These give information about local chemical environment in a cell. XANES at the phosphorus K absorption edge in a human HeLa cell was successfully obtained corresponding to a sharp and intensive XANES peak of DNA.

• 한국재료학회:학술대회논문집
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• 한국재료학회 2003년도 추계학술발표강연 및 논문개요집
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• pp.184-184
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• 2003

• 한국표면공학회:학술대회논문집
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• 한국표면공학회 1998년도 춘계학술발표회 초록집
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• pp.11-12
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• 1998

• 암석학회지
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• 제10권3호
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• pp.212-221
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• 2001

방사광의 특성과 방사광의 발생원리에 대한 소개를 하였다. 매우 높은 스펙트럼 휘도와 매우 넓은 영역의 스펙트럼 범위, X-선 파장 조절 가능성과 고도의 지향성 및 집속성, 그리고 시간에 따른 순간파동 구조를 갖는 방사광을 이용하여 지질학 및 지구환경과학에 적용할 수 있는 실험기법을 기술하였다. 이에는 X선 토모그라피, XRF, XANES, EXAFS, 다이아몬드 앤빌 기기 및 라지 발륨 프레스를 이용한 고온-고압 연구와 에너지문제와 관련하여 원자력발전과 핵폐기물처리에 대한 것이 포함되어 있다. 이러한 실험기법은 광물 및 암석에 대한 화학성분, 결정구조 및 결합상태 분석이 가능하며, 광상학과 고생물학 및 환경학 분야에 적용할 수 있다. 또한 이 연구방법을 이용하면 지구내부물질의 거동에 관한 정보를 얻을 수 있다.

• Journal of Applied Biological Chemistry
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• 제58권1호
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• pp.65-74
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• 2015

X선 흡수분광법(X-ray absorption spectroscopy, XAS)을 이용하는 X선 흡수미세구조(X-ray absorption fine structure, XAFS)의 분석은 다양한 학문분야에서 적용되고 있다. 본 연구에서는 XAFS 분석을 위한 토양 시료의 준비에서부터 XAFS 측정 후 X선 흡수 끝머리 부근 미세구조(X-ray absorption near edge structure, XANES) 및 광범위 X선 흡수 미세구조(extended Xray absorption fine structure, EXAFS) 데이터를 추출하여 연구에 활용하는 것에 대해 간략하게 소개하였다. 특히 토양환경 분야에서 XANES 및 EXAFS 분석을 활용한 선행연구들에 대해 비소(As) 및 중금속 주요 원소(Cd, Cu, Ni, Pb, Zn)별로 그 내용을 정리하였다. 토양환경 분야에서 XAFS의 응용은 납(Pb)의 화학종 규명에 관한 연구가 가장 많은 것으로 나타났다. 이와 함께 대부분의 연구들은 오염토양 내 중금속 화학종의 규명을 통해 중금속의 유입 원인 등에 대해 기술하고 있으며, 이를 정화하기 위한 다양한 방법들(개량제 처리, 식물정화)을 적용한 후, 안정화된 중금속 화학종을 XANES 및 EXAFS 분석을 통해 규명하여 정화 방법들의 효율성과 안정성에 대해 보고하였다.

• Bulletin of the Korean Chemical Society
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• 제26권4호
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• pp.671-674
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• 2005

• 한국진공학회:학술대회논문집
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• 한국진공학회 2012년도 제43회 하계 정기 학술대회 초록집
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• pp.166-166
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• 2012

We examined the distribution of Co ions of ferromagnetic n-type Zn(1-x)Co(x)O semiconducting films with the Co concentrations of 0.03~0.07 using x-ray absorption fine structure (XAFS) measurements at the Co and Zn K edges. Extended XAFS (EXAFS) revealed that Co ions mainly occupied the zinc sites of the films. X-ray absorption near edge structure (XANES) spectra demonstrated that the pre-edge peak of the Co K edge was substantially affected by the second neighboring Co ions at the zinc sites due to hybridizing of the Co 4p conduction electrons with the Co 3d bounded electrons. From XANES and EXAFS analysis using ab initio calculations, we found that Co ions uniformly occupied the zinc sites of the Zn (0.93) Co (0.07)O film, whereas the Co ions of the Zn (0.97) Co (0.03)O and Zn (0.95) Co (0.05)O films were substituted at localized zinc sites. The ferromagnetic properties of the Zn (0.93) Co(0.07)O film could be induced by direct interaction between the magnetic dipoles of the Co ions with a mean distance of 4.3 A or by Co 4p electron mediation.

• Bulletin of the Korean Chemical Society
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• 제18권10호
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• pp.1047-1050
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• 1997

• Bulletin of the Korean Chemical Society
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• 제25권4호
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• pp.511-516
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• 2004

A Li$[Co_{0.17}Li_{0.28}Mn_{0.55}]O_2$ cathode compound was prepared by a simple combustion method. The X-ray diffraction pattern showed that this compound could be classified as ${\alpha} -NaFeO_2$ structure type with the lattice constants of a = 2.8405(9) ${\AA}$ and c = 14.228(4) ${\AA}$. According to XANES analysis, the oxidation state of Mn and Co ions in the compound were 4+ and 3+, respectively. During the first charge process, the irreversible voltage plateau at around 4.65 V was observed. The similar voltage-plateau was observed in the initial charge profile of other solid solution series between $Li_2MnO_3\;and\;LiMnO_2$ (M=Ni, Cr...). The first discharge capacity was 187 mAh/g and the second discharge capacity increased to 204 mAh/g. As the increase of cycling number, one smooth discharge profile was converted to two distinct sub-plateaus and the discharge capacity was slowly decreased. From the Co and Mn K-edge XANES spectra measured at different cyclic process, it can be concluded that irreversible transformation of phase is occurred during continuous cycling process.

• 한국세라믹학회지
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• 제43권3호
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• pp.177-184
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• 2006

Dy $L_3$-edge XANES and EXAFS spectra of chalcogenide Ge-As-S glass doped with ca. 0.2 wt% dysprosium have been investigated along with some reference Dy-containing crystals. Amplitude of the white-line peak in XANES spectrum of the glass sample turns out to be stronger than that of other reference crystals, i.e., $DY_2S_3,\;Dy_2O_3\;and\;DyBr_3$. It has been verified from the Dy $L_3$-edge EXAFS spectra that a central Dy atom is surrounded by $6.7{\pm}0.5$ sulfur atoms in its first coordination shell in the Ge-As-S glass, which is relatively smaller than 7.5 of the $Dy_2S_3$ crystal. Averaged Dy-S inter-atomic-distance of the glass ($2.78{\pm}0.01{\AA}$) also turns out to be somewhat shorter than that of the $Dy_2S_3$ crystal ($2.82{\pm}0.01{\AA}$). Such nanostructural changes occurring at Dy atoms imply there being stronger covalency of Dy-S chemical bonds in the Ge-As-S glass than in the crystal counterpart. The enhanced covalency in the nanostructural environment of $Dy^{3+}$ ions inside the glass would then be responsible for optical characteristics of the $4f{\leftrightarrow}4f$ transitions of the dopants, i.e., increase of oscillator strengths and spontaneous radiative transition probabilities.