http://chineseinput.net/에서 pinyin(병음)방식으로 중국어를 변환할 수 있습니다.
변환된 중국어를 복사하여 사용하시면 됩니다.
김태균,김영유,서영석,조창호,나훈균 公州大學校 基礎科學硏究所 1998 自然科學硏究 Vol.7 No.-
양극반응 전류밀도를 변화시키면서 다공질 규소를 제작하여 라만산란을 관측하였다. 전류밀도가 증가함에 따라 라만신호는 520.5㎝-₁에서 멀어졌으며, 봉우리의 반치폭이 증가하였다. 또한 전류밀도 증가에 따라 원통형 다공질 결정의 직경은 감소함이 계산되었으며, 길이가 길어짐을 AFM으로 관찰하였다. The Raman scattering was studied from the porous silicons which were made by changing anodization current. As the current density was increased, it was observed that Raman was gradually far from the value of 520.5 cm ̄¹and the full width half maximum increased. The decrease of radius of cylindrical porous crystal was calculated and the increase of its length was investigated through AFM.
柳鍾仁,羅勳均 崇實大學校 1986 論文集 Vol.16 No.-
TEA N₂laser was constructed using a simple Blumlein transmission line. The relative output power of the N₂laser relative to the electrode distance, and spark gap distance was measured. The optimum condition of the E/P was 79V/cm-torr.
고온초전도체 $Y_{1-X}Sm_{X}Ba_{2}Cu_{3}O_{7-y}$의 자기적 성질 연구
김채옥,김재욱,김의훈,나훈균,Kim, Chae-Ok,Kim, Jae-Uk,Kim, Ui-Hun,Na, Hun-Gyun 한국재료학회 1992 한국재료학회지 Vol.2 No.3
The temperature dependence of the magentic moment was determined for the system of high $T_{c}$ superconductor $Y_{1-X}Sm_{x}Ba_2Cu_3O_{7-y}$ with x=0, 0.2, 0.4, 0, 6, 0.8 and 1.0. Also the magnetic susceptibility and the magnetic critical current density were measured from the magnetic hysterisis loops obtained at 30 K. From the results of the magnetic susceptibility measurements, the high $T_{c}$ phase were ranged from 14.7 to 49.1%. The values of the magnetic critical current densities were in the range of $10^3~10^4A/cm^2$. The penetration depth was approximately ninety times larger than the coherence length. 고은 초전도체 $Y_{1-X}Sm_{x}Ba_{2}Cu_{3}O_{7-y}$(x=0, 0.2, 0.4, 0.6, 0.8, 1.0)의 시료들을 제조하여 온도에 따른 자기 모우먼트를 측정하였다. 또한 자화율과 자기 임계전류밀도 같은 30K의 온도에서 자기이력 곡선으로부터 구하였다. 자화율 측정 결과로부터 고온 초전도상의 양이 14.7~49.175 범위에 있었으며, 입계전류밀도의 값은 $10^{3}~10^{4}A/cm^2$범위에 있었다. 그리고 침투깊이는 간섭성 길이보다 대략90배 정도 큼을 알 수 있었다
2H-$PbI_2$ 단결정의 엑시톤 반사 및 $A_{EP}$선에 관한 연구
김현철,송인걸,유종인,유연석,나훈균 한국광학회 1996 한국광학회지 Vol.7 No.3
2H-Pb $I_{2}$ 단결정의 반사스펙트럼을 10K에서 측정하였으며 기초흡수단 근처에서 n=1, 2, 3의 Wannier 엑시톤 계열과 $A_{EP}$ 선을 얻었다. $A_{EP}$ 선은 Nagamune 등의 보고와는 달리 라만스펙트럼의 2nd 포논에너지로부터 n=2 엑시톤과 2nd 포논의 결합상태로 생각된다. 또 2nd 포논은 이차 라만산란과정에서 LO 포논과 관련된 라만선으로 생각된다. Wannier 엑시톤 계열로부터 기상법으로 성장시킨 2H-Pb $I_{2}$ 단결정의 엑시톤 결합에너지와 반경은 각각 33meV와 14.angs.이었으며 n=1 엑시톤의 L-T 분리 에너지 값은 10K 에서 6.56meV로 동일 온도에서 측정된 발광스펙트럼에서도 같은 값으로 나타났다. 또 반사스펙트럼을 온도의 함수로 측정하였으며 그 결과 n=1 엑시톤의 반사선은 온도가 증가함에 따라 장파장 쪽으로 이동하였고 L-T 분리에너지가 증가하면서 엑시톤 반사선의 예리도도 감소함을 알 수 있었다. The reflection spectrum of a $2H-PbI_2$ single crystal grown by vapour phase method were measured at 10 K near the fundamental absorption edge. The n= 1,2,3 Wannier exciton series and $A_{EP}$ reflection line were obtained from the reflection spectrum. Based on the 2nd phonon energy in the Raman spectrum, which is different from Nagamune's report, we suggest that $A_{EP}$ line is due to the bound state between the n=2 exciton and the 2nd phonon which surmise that this is LO phnon due to the second Raman process. The L-T splitting energy of n=1 exciton line was 6.56 meV and was consistent with the emission spectrum. The temperature dependence of the reflection spectrum showed that n=1 exciton peak was shifted to longer wavelength while, as the temperatre is raised, the sharpness of that with the increase of the L-T splitting energy decrease. From Wannier exiton series, the exciton binding energy and exciton radius was 30 meV and 14$\AA$, respectively.
조창호,김태균,서영석,나훈균,김영유 한국결정성장학회 1998 韓國結晶成長學會誌 Vol.8 No.1
양극반응 전류밀도를 변화시키면서 다공질 규소를 제작하여 라만산란을 관측하였다. 전류밀도가 증가함에 따라 라만신호는 520.5$\textrm{cm}^{-1}$에서 멀어졌으며, 봉우리의 반치폭이 증가하였다. 또한 전류밀도 증가에 따라 원통형 다공질 결정의 직경은 감소함이 계산되었으며, 길이가 길어짐을 AFM으로 관찰하였다. The Raman scattering was studied from the porous silicons which were made by changing anodization current. As the current density was increased, it was observed that Raman was gradually far from the value of 520.5 $\textrm{cm}^{-1}$ and the full width half maximum increased. The decrease of radius of cylindrical porous crystal was calculated and the increase of its length was investigated through AFM.