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      • 경도관 동맥색전술을 이용한 비정상 자궁출혈의 치료

        양승부,최교창,이상진,정영진,임한혁,한효상,황인철,조환성 순천향의학연구소 2005 Journal of Soonchunhyang Medical Science Vol.11 No.1

        Objective : Our purpose of this study is to evaluate the effectiveness of the transcatheter arterial embolization for the management of abnormal uterine bleeding. Materials and Methods : 14 patients with massive or recurrent uterine bleeding underwent percutaneous transcatheter arterial embolization between February 2003 and September 2004. We reviewed 14 cases of uterine artery or internal iliac artery embolization using gelfoam or PVA particles. Results : Good management of uterine bleeding was achieved in 13 of 14(93%) cases. The cause of abnormal uterine bleeding was myoma(5 case), post D & E bleeding(3), acquired vascular malformation(3), pseudoaneurysm(1), adenomyosis(1), and endometrial hyperplasia(1). Conclusion : Transcatheter artery embolization is an effective and life-saving procedure in massive or recurrent uterine bleeding. Early diagnosis and prompt transcatheter arterial embolization is a useful mangement of uterine bleeding.

      • 다결정니켈 표면에서의 산소와 일산화탄소간의 상호작용

        이순보,부진효,김우섭 성균관대학교 기초과학연구소 1989 論文集 Vol.40 No.2

        Interactions between oxygen and carbon monoxide on Ni surface were studied by means of XPS at room temperature in UHV system attached with a. quadrupole mass spectrometer. Adsorption of CO on Ni surface precovered with oxygen are followed by three step. It was noted that CO₂ gas are formed by reaction of preadsorbed oxygen and CO molecules at initial step, and the second step is followed that precovered oxygen and CO molecules are coadsorbed, and during the high CO exposure the less pread-sorbed oxygen is, the more adsorbed CO. It could be attributed to the fact that the existence of oxygen on the Ni surface reduced the sticking coefficient of CO. Dissociative adsorption of O₂ on Ni surface were inhibited by the preadsorbed CO molecule at initial oxygen exposure. The dissociative adsorption of the preadsorbed CO increased with increasing exposures of O₂ and Ar. This was very well explained by the model of a collision-energy transfer, that a collision between the preadsorbed CO and O₂ or Ar gas cause to increase an amplitude of vibration mode contributed to dissociative adsorption so that the preadsorbed CO molecule is dissociated by the interaction of oxygen atom of adsorbed CO and Ni atoms.

      • Ar 이온에 의해 Sputtering된 Pt(111) 표면의 NO 흡착

        이순보,부진효,이성용,박종윤,곽현태 성균관대학교 기초과학연구소 1992 論文集 Vol.43 No.1

        Adsorption of nitric oxide on the Pt(111) surface sputtered by Ar-ion has been studied using thermal desorption spectroscopy, Auger electron spectroscopy, and low energy electron diffraction. A thermal desorption spectrum obtained from the perfect Pt(111) saturated with NO at 300K is quite simillar to those reported previously. The main portion desorbs at about 370K(α-state) with a shoulder at about 470K(β-state). The chemisorption of nitric oxide is predominantly molecular on the Pt(111) surface, accompanied by a small amount of dissociation which becomes negligible when the Pt(111) surface is perfect. When the Pt(111) surface is sputtered by Ar-ion with 2KeV, the thermal desorption spectrum becomes quite complex. The shoulder peak, which appears on the perfect surface spectrum, increases with Ar-ion sputtering time. The maximum desorption spectra of N₂ and N₂O are observed simultaneously between 470 and 600K. The desorption mechanisms for N₂O are proposed. The increasing N₂ with the β-state of NO indicates that the β-state is a precursor to the NO dissociation.

      • 다결정 Ni 표면과 CO의 상호작용

        李淳甫,이순영,부진효 성균관대학교 기초과학연구소 1985 論文集 Vol.36 No.2

        The chemisorption properties of CO on polycrystalline Ni surface are studied by XPS at 150K, 300K and 400K. The CO are adsorbed only molecularly at lower temperature than room-temperature having a adsorption energy of about 87KJ/mol. At 400K, the CO are dissociated, so that the carbon remains as 'carbidic' carbon on the surface, which is stable at lower temperature about 620K, and above this temperature it is transformed to graphite. On the other hand, atomic oxygen species on the surface may be reduced by CO in gas phase. A possible mechanism for the formation of 'carbidic' carbon is proporsed.

      • 이온 펌프의 제작과 특성에 관한 연구

        박종윤,이순보,부진효,신익조 성균관대학교 기초과학연구소 1990 論文集 Vol.41 No.1

        By using theoretical model suggested by H. Hartwig et al., performance of sputter ion pump (SIP) was calculated and a SIP was constructed. Measurement of pumping speed of the SIP has been performed with the differential pumping method. The pumping speed for N_2 gas is 48 l/s, and for Ar gas is 20 l/s. These results agree with the theoreticaly expected values.

      • 다결정 니켈표면과 산소 기체와의 상호 작용

        안운선,이순보,부진효,박유용 성균관대학교 기초과학연구소 1986 論文集 Vol.37 No.2

        The interaction of the gaseous oxygen molecule with polycrystalline nickel surface has been studied by the XPS through the wide range above the room temperature. For relatively lower oxygen exposure, only an O(1s) peak was observed at 530.2 eV, which is associated with the dissociative adsorption. On the other hand, with increasing oxygen exposures, two peaks was appeared at 529.7eV and 531.3eV. These peaks are attributed to nickel oxide and Ni_2O_3, respectively. The latter oxide is ascribed due to the excess adsorption over the NiO stoichiometry. However at high temperatures above 423K, the dissociative adsorption and oxidation was found to take place simultaneously. As a whole, through these XPS study it is found that the interaction of the oxygen with the polycrystalline nickel surface commences through three steps: the fast dissociative adsorption following slow initiation process, rapid oxidation corresponding to the epitaxial NiO formation, and finally the bulk oxide formation.

      • 초고진공 장치의 설계 및 제작과 LEED Optics에 의한 Auger Electron Spectrometer의 분해능 측정

        이순보,박종윤,곽현태,부진효,이성용 성균관대학교 1992 論文集 Vol.42 No.2

        A multipurpose Ultra High Vacuum chamber was designed and constructed in this laboratory. This enables us to be equipped with various analytical instruments such as Ar-ion gun LEED optics, Electron analyzer, and Quadrupole mass spectrometer etc. The 4-Grid LEED optics, a product of Omicron company in West Germany, was equipped with the UHV chamber and the LEED power supply was designed by this group. Turbo-C language figured out Auger spectra of the ad-species by means of the computer interface. The resolution of Auger electron spectrometer was measured with a constant primary electron beam energy. The results showed that the resolution was independent of the primary electron beam energy, but depends on the modulation voltage. Also, it was revealed that the resolution of 4-Grid optics was more improved than that of 3-Grid optics.

      • W(110) 표면에 CO의 흡착

        이경희,유위량,한현석,부진효,이순보,곽현태 성균관대학교 기초과학연구소 1998 論文集 Vol.49 No.-

        The interaction of CO with W(110) surface was investigated through LEED, TDS, and photoelectron spectroscopy using synchrotron radiation under UHV condition. After CO saturation at RT, two desorption states, called α and β , were observed at about 400 and 1150 K in thermal desorption spectra, respectively. The kinetics of 3-CO followed the first order kinetics, indicating the existence of molecular CO on W(110) surface. This is contrary to the previous results. The O 1s BE(binding energy) of CO adsorbed on W(110) surface at room temperature was 529.9 eV. On the other hand, the O 1s BE of β-CO after heating to 900 K was different from that of oxygen adsorbed W(110) surface, suggesting a different adsorption state. According to the UP valence band spectra, we observed two peaks at near -10.7 eV (4σ) and -7.0 eV (5σ+1π), indicating the molecular adsorption of CO at room temperature. Furthermore we could see the 4σ peak at the various photon energy and elevated temperatures. Comparing the energy separation, Δ(4σ-1π) , between 4σ and 1π UP peaks of chemisorbed CO, we found that an increased separation reflects an decreased C-O bond strength. Therefore on the basis of TDS and photoelectron spectroscopy, we could suggest that β state of CO on W(110) may not be dissociated and has an adsorption geometry of lying-down mode.

      • KCI등재

        PECVD법으로 증착된 전자소자용 thiophene 박막의 전기화학적 신뢰성에 관한 연구

        김정구,박진택,최윤석,부진효,유용재 대한금속재료학회 2003 대한금속·재료학회지 Vol.41 No.6

        The corrosion failure of electronic devices has been a major reliability concern lately. This failure is an ongoing concern because of miniaturization of integrated circuits(IC) and the increased use of polymers in electronic packaging. In this paper plasma-polymerized thiophene films were considered as a possible candidate for an interlayer dielectric for multilever metallization of ultra large scale integrated (ULSI) semiconductor devices. The protective ability of above films as a function RF power in an 3.5 wt.% NaCl solution was examined by electrochemical methods and contact angle measurement. The protective efficiency of the film increased with increasing RF power, which induced the higher degree of cross-linking and hydrophobicity of the films.

      • 열탈착 분석법에 의한 Pt(111) 표면위의 NO와 CO의 흡착

        이순보,박종윤,곽현태,부진효,강용철 성균관대학교 1992 論文集 Vol.42 No.2

        The adsorptions of nitric oxide and carbon monoxide on Pt(111) surfaces have been studied by using LEED, AES, and TDS(Thermal Desorption spectroscopy). The adsorbed species of NO is predominantly molecular on the Pt(111) surface at room temperature. A main desorption peak of TDS is attributed to the molecular adsorption at 360K. With increasing No exposures, a shoulder peak at 480K which may be attributed to the defect site adsorption is appeared. The desorption rate order for No desorption is 1st order and the desorption energy for NO calculated by Redhead equation assuming pre-exponential factor v_1=10^13 sec^-1 is 21.7Kcal/mol. The adsorption of carbon monoxide is also molecular on Pt(111) surface at room temperature. The TDS results showed only a single broad peak at 460K, which is attributed to molecular adsorption. The desorption order for CO desorption is 1st order as well as NO and the desorption energy for CO is 28Kcal/mol.

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