• Proceedings of the KIEE Conference
• /
• 1999.11d
• /
• pp.915-917
• /
• 1999

We investigated the effects of doping elements on the Bi system superconductor. The doping elements can be classified into two groups depending on their supeconducting characteristics in the Bi-Sr-Ca-Cu-O structure. The first group of doping elements(P and K) have a tendency to decompose the superconducting phase and reduce the optimal sintering temperature. The second group of doping elements(B, Si, Sn and Ba) almost uneffected the superconductivity of the 2223 and 2212 phase.

• Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
• /
• 2008.06a
• /
• pp.55-55
• /
• 2008

이차전지의 음극 중 $LiC_6$는 높은 용량을 보이나 완충하는 프로세스 동안에 금속리튬에 가까운 potential을 갖게 되어 조작에 어려움이 있다. 이러한 대용물질로서 $Li_4Ti_5O_{12}$ spinel은 가볍고 높은 에너지 밀도를 가지고 있고 낮은 전압영역이 가능하여 이차전지의 음극 물질로서 유용하다. 그러나 $Li_4Ti_5O_{12}$ 물질 자체가 insulation이며, 고상합성법을 사용하게 되면 좋은 특성을 나타내기가 어렵다. 이번 실험에서는 고상합성을 통하여 $Ba^{2+}$와 $Sr^{2+}$이온을doping한 후 전기화학적 특성이 어떻게 향상되었는가를 연구하였다. Ba와 Sr을 첨가한 $Li_4Ti_5O_{12}$는 첨가하지 않은 물질에 비하여 보다 안정적인 평탄구역을 갖게 되었으며 방전용량이 $40mAhg^{-1}$의 향상을 가져왔다. 또한 Li half cell에서 100cycle 진행하는 동안 보다 안정적인 전극구조를 유지하였다.

• Proceedings of the Materials Research Society of Korea Conference
• /
• 2011.05a
• /
• pp.31.2-31.2
• /
• 2011

We have investigated frequency dependant conductivity (or permittivity) of low dimensional oxide structures represented by [($Sr_{0.75}$, $La_{0.25}$)$TiO_3$]$_1$/1$[SrTiO_3]_n$ superlattices. The low dimensional oxide superlattice was made by cumulative stacking of one unit cell thick La doped $SrTiO_3$ and $SrTiO_3$ with variable thickness from 1 to 6 unit cell, i,e, [($Sr_{0.75}$, $La_{0.25}$)$TiO_3$]$_1$/$[SrTiO_3]_n$ (n=1, 2, 3, 4, 5, 6). We found two kinds of relaxation when n is 3 and 4, while, inductance component was observed at n=1. This behavior can be explained by electron modulation in ($Sr_{0.75}$, $La_{0.25}$)$TiO_3/SrTiO_3$ superlattices. When n is 1, electrons by La doping well extend to un-doped layer. Therefore, the transport of superlattices follows bulk-like behavior. On the other hand, as n increased, the doped electrons became two types of carrier: one localized and the other extended. These results in two kinds of transport phase. At further increase of n, most of doped electrons are localized at the doped layer. This result shows that dimensionality of the oxide structure significantly affect the transport of oxide nanostructures.

• Proceedings of the Korean Vacuum Society Conference
• /
• 2010.08a
• /
• pp.308-308
• /
• 2010

산업의 기반이 되는 화석연료의 고갈과 화석연료의 사용으로 야기되는 환경오염 문제로 인하여 새로운 에너지원의 개발이 요구되고 있다. 이러한 시대적 요구에 부흥하고자 신재생 에너지원에 관한 많은 연구가 진행되고 있으며, 그중에 태양전지가 가장 주목받고 있다. 그러나 태양전지는 기존 전력 생산 방법에 비해 경제성이 낮아 이를 극복하기 위한 다양한 연구가 진행되고 있다. 특히 결정질 태양전지에 관한 연구가 가장 활발한데 경제성과 변환효율을 향상시키기 위해 태양전지의 전면에 선택적 doping 형성법이 사용되고 있는데, 선택적 doping 구조의 태양전지는 기존의 태양전지보다 변환효율이 높으면서 양산에서 사용 가능한 구조이기 때문에 경제적 측면에서 더 유리한 구조라 할 수 있다. 하지만 선택적 doping 형성을 위한 실험적인 분석 방법에는 많은 시간과 노력이 필요하며 많은 시행착오를 겪어야 한다. 따라서 이러한 시간과 노력을 줄이고 실험을 하기 이전에 결과를 예측하여 실험의 방향을 제시하고자 TCAD simulation을 이용하여 결정질 태양전지의 전면에 형성한 선택적 doping 농도에 따른 pn 접합 형성 구조와 doping profile에 따른 전기적, 광학적 특성을 예측하고 효과적인 특성을 가질 수 있는 구조를 제시하고자 한다. 선택적 doping의 효과를 확인하기 위해 SR로 각 파장별 양자효율의 변화와 전기적 특성을 분석하여 selective emitter 태양전지에 적합한 pn 접합 형성구조를 제시하고자 한다.

• 한국초전도학회:학술대회논문집
• /
• v.13
• /
• pp.26-26
• /
• 2003

• Proceedings of the Materials Research Society of Korea Conference
• /
• 2007.11a
• /
• pp.154.1-154.1
• /
• 2007

• Proceedings of the Materials Research Society of Korea Conference
• /
• 2007.11a
• /
• pp.154.2-154.2
• /
• 2007

• Progress in Superconductivity
• /
• v.11 no.1
• /
• pp.67-71
• /
• 2009

The effect of Cu substitution on the structural and superconducting properties of the $(Ru_{1-x}Cu_x)Sr_2(Eu_{1.34{\cdot}}Ce_{0.66})Cu_2O_z$ system with x = 0, 0.25 and 0.5 prepared under ambient pressure have been investigated. The X-ray diffraction patterns indicated that the Ru ions are replaced by the Cu ions. It is found that the Cu substitution for Ru significantly reduces the ferromagnetic component of field-cooled magnetic susceptibility, but results in a small change in diamagnetic onset transition temperature of zero-field-cooled magnetic susceptibility. In contrast to the Ru $Sr_2(Eu_{1.34{\cdot}}Ce_{0.66})Cu_2O_z$, bulk Meissner effect is observed in the field-cooled magnetization measurements of the Cu doped samples. The experimental results are discussed in connection with the spontaneous vortex phase interpretation.

• Korean Journal of Materials Research
• /
• v.14 no.2
• /
• pp.115-120
• /
• 2004

Perovskite barium-strontium titanate, $(Ba, Sr)TiO_3$ was prepared and effects of $Sb_2$O$_3$ additives on its PTCR properties were investigated. $The (Ba,Sr)TiO_3$ with 0.05～0.25 mol% $Sb_2$$O_3$ showed semiconducting PTCR behavior and anomalous grain growth was also observed when it was sintered above $1330^{\circ}C$. It was considered that charge compensation by doping 8b203 as well as abnormal grain growth by sintering lead to resistivity reduction from insulating to semiconducting transition.

• Applied Chemistry for Engineering
• /
• v.7 no.6
• /
• pp.1125-1131
• /
• 1996

Ca or Sr-doped $PrMnO_3$ were prepared for cathode material of solid oxide fuel cell. The characteristics such as the electrical conductivity and the cathodic overpotential were investigated as to doping contents. Also the reactivity with yttria stabilized zirconia of electrolyte, and the thermal expansion coefficient were studied. The prepared perovskite powder had the mean particle size of $2{\sim}5{\mu}m$, and the particle size and the surface area was out of relation to the doping content. When Ca doping amount of electrode material was 30mol%, the electrical conductivity was the highest value of $266S{\cdot}cm^{-1}$ at $1000^{\circ}C$, and also the polarization characteristics showed the best property. The reactivity between YSZ and Ca-doped $PrMnO_3$ at $1200^{\circ}C$ for 100hours was lower than that between YSZ and Sr-doped $PrMnO_3$. The thermal expansion coefficient of $Pr_{0.7}Ca_{0.3}MnO_3$ was $1.19{\times}10^{-5}K^{-1}$ in the temperature range of $300{\sim}1000^{\circ}C$, and this value was similar to that of YSZ, $1.15{\times}10^{-5}K^{-1}$.