• Proceedings of the Korean Vacuum Society Conference
• /
• 2010.02a
• /
• pp.122-122
• /
• 2010

ZnO is a widely investigated material for the blue and ultraviolet solid-state emitters and detectors. It has been promoted due to a wide-band gap semiconductor which has large exciton binding energy of 60 meV, chemical stability and low radiation damage. However, there are many problems to be solved for the growth of p-type ZnO for practical device applications. Many researchers have made an efforts to achieve p-type conductivity using group-V element of N, P, As, and Sb. In this letter, we have studied the optical characteristics of the antimony-doped ZnO (ZnO:Sb) thin films by means of photoluminescence (PL), PL excitation, temperature-dependent PL, and time-resolved PL techniques. We observed donor-to-acceptor-pair transition at about 3.24 eV with its phonon replicas with a periodic spacing of about 72 meV in the PL spectra of antimony-doped ZnO (ZnO:Sb) thin films at 12 K. We also investigate thermal activation energy and carrier recombination lifetime for the samples. Our result reflects that the antimony doping can generate shallow acceptor states, leading to a good p-type conductivity in ZnO.

• Proceedings of the Korean Vacuum Society Conference
• /
• 2010.02a
• /
• pp.170-170
• /
• 2010

a-plane 혹은 m-plane면을 사용하는 무분극 GaN LED는 c축 방향으로 발생하는 분극의 영향을 받지 않기 때문에 분극 GaN LED에 비해 높은 내부 양자효율을 가진다. 또한 무분극 GaN는 상대적으로 고농도의 p-type 도핑이 가능하기 때문에 광효율을 높일 수 있다. 하지만 이와 같은 장점에도 불구하고 무분극 GaN는 성장모드의 비대칭으로 인해 높은 결정성과 mirror-like한 표면을 얻기가 힘들다. 본 논문에서는 Metalorganic chemical-vapor deposition (MOCVD) 장비를 사용하여 r-plane 사파이어 기판위에 a-plane GaN을 성장시켰다. 일반적으로 사용하는 저온에서의 nucleation layer 성장 대신 $1050^{\circ}$의 고온에서 성장 시킨후 일반적으로 사용하는 two-step 성장방법으로 그위에 5.5um정도의 GaN을 성장시켰다. 성장시 Trimethylgallium(TMGa)와 암모니아를 각각 Ga과 N 소스로 이용하였고 캐리어 가스는 수소를 사용하였다. 비대칭 결정성을 줄이기 위해 3D island growth mode에서의 성장조건을 바꾸어 c축과 m축 방향으로의 X-ray 결정성(FWHM) 차이가 564 arcsec에서 206 arcsec로 변화 시켰다. Normarski 현미경으로 표면을 관찰한 결과 v-defect이 없고 a-plane GaN에서 볼 수 있는 전형적인 줄무늬 패턴을 가지는 표면을 얻었으며 광학적 특성을 보기 위해 Photoluminescence (PL)을 측정하였다.

• Journal of Mechanical Science and Technology
• /
• v.19 no.6
• /
• pp.1338-1346
• /
• 2005

Effects of thermal contact resistance between heater and susceptor, susceptor and graphite board in a MOCVD reactor on temperature distribution and film growth rate were analyzed. One-dimensional thermal resistance model considering thermal contact resistance and heat transfer area was made up at first to find the temperature drop at the surface of graphite board. This one-dimensional model predicted the temperature drop of 18K at the board surface. Temperature distribution of a reactor wall from the three-dimensional computational fluid dynamics analysis including the gap at the wafer position showed the temperature drop of 20K. Film growth rates of InP and GaAs were predicted using computational fluid dynamics technique with chemical reaction model. Temperature distribution from the three-dimensional heat transfer calculation was used as a thermal boundary condition to the film growth rate simulations. Temperature drop due to the thermal contact resistance affected to the GaAs film growth a little but not to the InP film growth.

• Korean Journal of Materials Research
• /
• v.31 no.2
• /
• pp.92-96
• /
• 2021

We report the growth and enhanced photoelectrochemcial (PEC) water-splitting reactivity of few-layer MoS2 nanosheets on TiO2 nanowires. TiO2 nanowires with lengths of ~1.5 ~ 2.0 ㎛ and widths of ~50~300 nm are synthesized on fluorine-doped tin oxide substrates at 180 ℃ using hydrothermal methods with Ti(C4H9O)4. Few-layer MoS2 nanosheets with heights of ~250 ~ 300 nm are vertically grown on TiO2 nanowires at a moderate growth temperature of 300 ℃ using metalorganic chemical vapor deposition. The MoS2 nanosheets on TiO2 nanowires exhibit typical Raman and ultraviolet-visible light absorption spectra corresponding to few-layer thick MoS2. The PEC performance of the MoS2 nanosheet/TiO2 nanowire heterostructure is superior to that of bare TiO2 nanowires. MoS2/TiO2 heterostructure shows three times higher photocurrent than that of bare TiO2 nanowires at 0.6 V. The enhanced PEC photocurrent is attributed to improved light absorption of MoS2 nanosheets and efficient charge separation through the heterojunction. The photoelectrode of the MoS2/TiO2 heterostructure is stably sustained during on-off switching PEC cycle.

• Proceedings of the Korean Vacuum Society Conference
• /
• 1998.02a
• /
• pp.120-120
• /
• 1998

Boron nitride (BN) films have attracted a growing interest for a variety of t technological applications due to their excellent characteristics, namely hardness, c chemical inertness, and dielectrical behavior, etc. There are two crystalline phases 1551; of BN that are analogous to phases of carbon. Hexagonal boron nitride (h-BN) has a a layered s$\sigma$ucture which is spz-bonded structure similar to that of graphite, and is t the stable ordered phase at ambient conditions. Cubic boron nitride (c-BN) has a z zinc blende structure with sp3-bonding like as diamond, 따ld is the metastable phase a at ambient conditions. Among of their prototypes, especially 삼Ie c-BN is an i interesting material because it has almost the same hardness and thermal c conductivity as di없nond. C Conventionally, significant progress has been made in the experimental t techniques for synthesizing BN films using various of the physical vapor deposition 밍ld chemical vapor deposition. But, the major disadvantage of c-BN films is that t they are much more difficult to synthesize than h-BN films due to its narrow s stability phase region, high compression stress, and problem of nitrogen source c control. Recent studies of the metalorganic chemical vapor deposition (MOCVD) of I III - V compound have established that a molecular level understanding of the d deposition process is mandatory in controlling the selectivity parameters. This led t to the concept of using a single source organometallic precursor, having the c constituent elements in stoichiometric ratio, for MOCVD growth of 삼Ie required b binary compound. I In this study, therefore, we have been carried out the growth of h-BN thin f films on silicon substrates using a single source precursors. Polycrystalline h-BN t thin films were deposited on silicon in the temperature range of $\alpha$)() - 900 $^{\circ}$C from t the organometallic precursors of Boron-Triethylamine complex, (CZHs)3N:BRJ, and T Tris(dimethylamino)Borane, [CH3}zNhB, by supersonic molecular jet and remote p plasma assisted MOCVD. Hydrogen was used as carrier gas, and additional nitrogen w was supplied by either aDlIDonia through a nozzle, or nitrogen via a remote plasma. T The as-grown films were characterized by Fourier transform infrared spectroscopy, x x-ray pthotoelectron spectroscopy, Auger electron spectroscopy, x-ray diffraction, t transmission electron diffraction, optical transmission, and atomic force microscopy.roscopy.

• Korean Journal of Materials Research
• /
• v.10 no.4
• /
• pp.282-289
• /
• 2000

$PbTiO_3$ films were fabricated by electron cyclotron resonance plasma enhanced chemical vapor deposition(ECR-PECVD). Deposition characteristics of $PbTiO_3$films on $RuO_2$ and Pt substrates were investigated with varying the flow rate of metalorganic source and substrate temperature. The residence time of Pb-oxide molecules in much longer on $RuO_2$ than on Pt substrate, while the perovskite nucleation is more difficult on $RuO_2$ than on Pt substrate. Therefore, the process conditions to obtain the single perovskite $PbTiO_3$ phase are more restricted on $RuO_2$ than on Pt substrates. An introduction of Ti-oxide seed layer increases perovskite nucleation density and thus enlarges the process window to obtain the single perovkite phase. The introduction of Ti-oxide seed layer make the PZT film that Ti-components of $PbTiO_3$ are partially substituted with Zr atoms have single perovskite phase for the wide range of Zr/(Zr+Ti) concentration ratios.

• Korean Journal of Materials Research
• /
• v.10 no.4
• /
• pp.270-275
• /
• 2000

The Pt/YMnO$_3$/Y$_2$O$_3$/Si structure for metal/ferroelectric/insulator/semiconductor(MFIS)-FET was fabricated and effect of $Y_2$O$_3$layer on the properties of MFIS structure was investigated. The $Y_2$O$_3$ thin films on p-type Si(111) substrate deposited by Pulsed Laser Deposition were crystallized along (111) orientation irrespective of the deposition temperatures. Ferroelectric YMnO$_3$ thin films deposited directly on p-type Si (111) by MOCVD resulted in Mn deficient layer between Si and YMnO$_3$. However, YMnO$_3$ thin films having good quality and stoichiometric composition can be obtained by adopting $Y_2$O$_3$ buffer layer. The memory window of the $Y_2$O$_3$thin films with YMnO$_3$ film is greater than that of the YMnO$_3$ thin films without $Y_2$O$_3$ film after the annealing at 85$0^{\circ}C$ in vacuum ambient(100mtorr). The memory window is 1.3V at an applied voltage of 5V.

• Journal of the Korean Vacuum Society
• /
• v.17 no.1
• /
• pp.34-39
• /
• 2008

We have investigated the characteristics of $Al_{0.55}Ga_{0.45}N$/GaN heterostructures with and without low-temperature (LT) AlN interlayer grown by metalorganic chemical vapor deposition. The structural and optical properties were systematically studied by Rutherford backscattering spectroscopy (RBS), X-ray diffraction (XRD), optical microscopy (OMS), scanning electron microscopy (SEM), and photoluminescence (PL). The Al content (x) of 55% and the structural properties of $Al_xGa_{1-x}N$/GaN heterostructures were investigated by using RBS and XRD, respectively. We carried out OMS and SEM experiments and obtained a decrease of the crack network in $Al_{0.55}Ga_{0.45}N$ layer with LT-AlN interlayer. A two-dimensional electron gas (2DEG)-related PL peak located at ${\sim}3.437eV$ was observed at 10 K for $Al_{0.55}Ga_{0.45}N$/GaN with LT-AlN interlayer. The 2DEG-related emission intensity gradually decreased with increasing temperature and disappeared at temperatures around 100 K. In addition, with increasing the excitation power above 3.0 mW, two 2DEG-related PL peaks were observed at ${\sim}3.411$ and ${\sim}3.437eV$. The observed lower-energy and higher-energy side 2DEG peaks were attributed to the transitions from the sub-band level and the Fermi energy level of 2DEG at the AlGaN/LT-AlN/GaN heterointerface, respectively.

• Proceedings of the Korean Vacuum Society Conference
• /
• 2012.08a
• /
• pp.63-63
• /
• 2012

편광분석법(ellipsometry)은 대상 물질의 유전율 함수의 실수부와 허수부를 Kramers-Kronig 관계식의 도움 없이 그 물질상수를 정확히 측정할 수 있는 매우 우수한 기술이다. 이 기술의 큰 장점 중 하나는 빛의 편광상태의 변화를 이용한 비파괴적인 방법으로써 실시간 측정이 가능하며, 박막의 두께측정의 오차범위는 0.1 nm 이하로써 매우 정확하다는 것이다. 본 연구자는 이러한 우수한 측정 기술인 편광분석법을 고진공의 분자살박막증착장치(MBE) 와 결합하여 AlSb, AlP의 유전율 함수를 측정하였다. Al 계열을 포함하는 반도체 화합물은 Al의 산소친화력이 강해 대기 중에서 순수한 유전율 함수를 얻기가 불가능하다. 하지만 본 연구실에서 초고진공 상태의 MBE 챔버에서 시료를 성장시키는 동시에 실시간으로 편광분석기를 이용하여 측정하였고, 지금까지 발표된 결과들 중 가장 순수한 상태의 AlSb 유전율 함수를 얻어낼 수 있었다. 또한 순수한 AlP의 유전함수를 측정할 수 있었고, 이는 편광분석기를 이용한 최초의 실험결과로써 이차미분을 이용한 전이점 분석결과 이론적인 전자밴드구조에서 E1, E1+${\Delta}1$, E2에 해당하는 밴드갭들을 확인할 수 있었다. 또한 표면의 원자배열 구조와 실시간으로 일어나는 그들의 역학적인 현상들에 관한 정보를 얻을 수 있는 surface photoabsorption (SPA)를 metalorganic chemical vapor deposition (MOCVD)에 장착하여 실시간 모니터링이 가능하도록 하였다. SPA를 이용하여 GaAs/AlGaAs 양자우물구조의 성장을 원자층 수준으로 실시간 모니터링을 할 수 있었다. 그리고 SPA를 이용하여 MOCVD 안에서 InP에 As가 흡착 및 탈착되는 현상을 분석하여, As의 흡착이 두 단계에 의해 이루어짐을 분석하였다. 그리고 편광분석법의 빠르고 정확한 측정 기술을 규칙적인 구조체에서 전자기파의 회절을 구할 수 있는 Rigorous Coupled-Wave Analysis (RCWA) 계산방법과 결합하여 나노구조의 기하학적인 모양을 정확하고 빠르게 구할 수 있었다. 본 연구를 위해 규칙적인 3차원 Si 구조체 제작하여 편광분석기로 측정하고 $SiO_2$와 표면 거칠기를 고려하여 RCWA로 분석한 결과, 규칙적인 Si 구조와 산화막 층까지 정확하게 분석할 수 있음을 확인하였다. 또한 규칙적인 나노구조분석 연구를 넘어 불규칙적인 나노구조에 대한 분석 가능성을 보이기 위해 InAs 양자점을 증착하여 분석하였고, 이를 통해 편광분석법과 RCWA를 이용하여 불규칙적인 나노구조의 모양과 크기, 분포의 분석이 가능함을 보였다.

• Journal of the Korean Crystal Growth and Crystal Technology
• /
• v.9 no.6
• /
• pp.553-557
• /
• 1999

In order to investigate the optical properties of the $Al_XGa_{1-X}N/GaN$ thin film grown by metalorganic chemical vapor deposition (MOCVD) method, the photoluminescene (PL), photocurrent (PC) and persistent photoconductivity (PPC) measurements were carried out at room temperature. The band gap of the $A1_x$$Ga_{1-x}$N/GaN was determined to 3.70 eV by the PL and PC measurements. The PC measurement on the light illumination from the top of the $A1_x$$Ga_{1-x}$N/GaN thin film provides peaks at 3.70, 3.43, and around 2.2 eV. The PC spectrum by the illumination passing through from the substrate of the sample can be shown at 3.43 eV together with a broad tail band from the GaN band edge to around 2.23 eV. The photocurrent quenching and anomalous PPC decay observed in PPC measurements indicate that metastable electron states are fomed in the band gap of GaN layer to trap electrons which can be tunneled the potential barrier for long recovery time.