• Proceedings of the Korean Vacuum Society Conference
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• 2015.08a
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• pp.211.1-211.1
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• 2015

최근 용액 공정을 이용한 산화물 반도체에 대한 연구가 활발히 진행되고 있다. 넓은 밴드갭을 가지고 있는 산화물 반도체는 높은 투과율을 가지고 있어 투명 디스플레이에 적용이 가능하다. 기존의 박막 진공증착 방법은 진공상태를 유지하기 위한 장비의 가격이 비싸며, 대면적의 어려움, 높은 생산단가 등으로 생산율이 높지 않다. 하지만 용액 공정을 이용하면 대기압에서 증착이 가능하고 대면적화가 가능하다. 그리고 각각의 조성비를 조절하는 것이 가능하다. 이러한 장점에도 불구하고, 소자의 신뢰성이나 저온공정은 중요한 이슈이다. Instability는 threshold voltage (Vth)의 shift 및 on/off switching의 신뢰성과 관련된 parameter이다. 용액은 소자의 전기적 특성을 열화 시키는 수분 과 탄소계열의 불순물을 다량 포함 하고 있어 고품질의 박막을 형성하기 위해서는 고온의 열처리가 필요하다. 기존의 열처리는 고온에서 장시간 이루어지기 때문에 유리나 플라스틱, 종이 기판의 소자에서는 불가능하지만 $100^{\circ}C$ 이하의 저온 공정인 microwave를 이용하면 유리, 플라스틱, 종이 기판에서도 적용이 가능하다. 본 연구에서는 산화물 반도체 중에서 InGaZnO (IGZO)를 용액 공정으로 제작한 juctionless thin-film transistor를 제작하여 기존의 열처리를 이용하여 처리한 소자와 microwave를 이용해서 열처리한 소자의 전기적 특성을 한 달 동안 관찰 하였다. 또한 In:Zn의 비율을 고정한 후 Ga의 비율을 달리하여 특성을 비교하였다. 먼저 p-type bulk silicon 위에 SiO2 산화막이 100 nm 증착된 기판에 RCA 클리닝을 진행 하였고, solution InGaZnO 용액을 spin coating 방식으로 증착하였다. Coating 후에, solvent와 수분을 제거하기 위해서 $180^{\circ}C$에서 10분 동안 baking공정을 하였다. 이후 furnace열처리와 microwave열처리를 비교하기 위해 post-deposition-annealing (PDA)으로 furnace N2 분위기에서 $600^{\circ}C$에서 30분, microwave를 1800 W로 2분 동안 각각의 샘플에 진행하였다. 또한, HP 4156B semiconductor parameter analyzer를 이용하여 제작된 TFT의 transfer curve를 측정하였다. 그 결과, microwave 열처리한 소자의 경우 기존의 furnace 열처리 소자와 비교하여 높은 mobility, 낮은 hysteresis 값을 나타내었으며, 1달간 소자의 특성을 관찰하였을 때 microwave 열처리한 소자의 경우 전기적 특성이 거의 변하지 않는 것을 확인하였다. 따라서 향후 용액공정, 저온공정을 요구하는 소자 공정에 있어 열처리방법으로 microwave를 이용한 활용이 기대된다.

• 한국신재생에너지학회:학술대회논문집
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• 2009.06a
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• pp.23-23
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• 2009

CIGS 박막 태양전지는 제조단가가 낮고 박막 태양전지 중에서 변환효율이 가장 높아 발전 가능성이 큰 태양전지로 인식되고 있다. 이미 일본, 독일, 미국을 비롯한 선진국에서는 30-50 MW 급의 양산 라인이 구축되고 있어 2010년 이후에는 본격적인 상용화가 진행될 것으로 보인다. CIGS 광흡수층은 진공증발, 셀렌화, 나노입자, 전기도금등 다양한 방식으로 제조가 가능한데 이 중에서도 동시진공증발공정은 고효율 CIGS 박막 태양전지 제조에 적합하다. 본 연구에서는 동시진공증발법을 이용하여 CIGS 박막을 증착하였으며 소다회유리/Mo/CIGS/CdS/i-ZnO/n-ZnO/Al/AR 구조의 태양전지를 제조하였다. 기판온도 모니터링을 통한 Cu 이차상 조절 기술을 이용하여 결정립이 매우 큰 CIGS 박막을 증착하였으며 Ga/(In+Ga) 조성비의 조절을 통하여 밴드갭 에너지를 최적화하였다. 또한 QCM 장치를 활용하여 용액 속에서 성장되는 CdS 박막의 두께와 특성을 조절하였다. 이러한 공정최적화를 통하여 개방전압 0.65 V, 단락전류밀도 38.8 $mA/cm^2$, 충실도 0.74 그리고 변환효율 18.8% 의 CIGS 박막 태양전지를 얻었다.

• Proceedings of the Korean Vacuum Society Conference
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• 2013.08a
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• pp.99-99
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• 2013

In this talk, I will present two research works in progress, which are: i) mapping of piezoelectric polarization and associated charge density distribution in the heteroepitaxial InGaN/GaN multi-quantum well (MQW) structure of a light emitting diode (LED) by using inline electron holography and ii) in-situ observation of the polarization switching process of an ferroelectric Pb(Zr1-x,Tix)O3 (PZT) thin film capacitor under an applied electric field in transmission electron microscope (TEM). In the first part, I will show that strain as well as total charge density distributions can be mapped quantitatively across all the functional layers constituting a LED, including n-type GaN, InGaN/GaN MQWs, and p-type GaN with sub-nm spatial resolution (~0.8 nm) by using inline electron holography. The experimentally obtained strain maps were verified by comparison with finite element method simulations and confirmed that not only InGaN QWs (2.5 nm in thickness) but also GaN QBs (10 nm in thickness) in the MQW structure are strained complementary to accommodate the lattice misfit strain. Because of this complementary strain of GaN QBs, the strain gradient and also (piezoelectric) polarization gradient across the MQW changes more steeply than expected, resulting in more polarization charge density at the MQW interfaces than the typically expected value from the spontaneous polarization mismatch alone. By quantitative and comparative analysis of the total charge density map with the polarization charge map, we can clarify what extent of the polarization charges are compensated by the electrons supplied from the n-doped GaN QBs. Comparison with the simulated energy band diagrams with various screening parameters show that only 60% of the net polarization charges are compensated by the electrons from the GaN QBs, which results in the internal field of ~2.0 MV cm-1 across each pair of GaN/InGaN of the MQW structure. In the second part of my talk, I will present in-situ observations of the polarization switching process of a planar Ni/PZT/SrRuO3 capacitor using TEM. We observed the preferential, but asymmetric, nucleation and forward growth of switched c-domains at the PZT/electrode interfaces arising from the built-in electric field beneath each interface. The subsequent sideways growth was inhibited by the depolarization field due to the imperfect charge compensation at the counter electrode and preexisting a-domain walls, leading to asymmetric switching. It was found that the preexisting a-domains split into fine a- and c-domains constituting a $90^{\circ}$ stripe domain pattern during the $180^{\circ}$ polarization switching process, revealing that these domains also actively participated in the out-of-plane polarization switching. The real-time observations uncovered the origin of the switching asymmetry and further clarified the importance of charged domain walls and the interfaces with electrodes in the ferroelectric switching processes.

• Korean Journal of Materials Research
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• v.25 no.3
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• pp.138-143
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• 2015

Aluminum nitride, a compound semiconductor, has a Wurtzite structure; good material properties such as high thermal conductivity, great electric conductivity, high dielectric breakdown strength, a wide energy band gap (6.2eV), a fast elastic wave speed; and excellent in thermal and chemical stability. Furthermore, the thermal expansion coefficient of the aluminum nitride is similar to those of Si and GaAs. Due to these characteristics, aluminum nitride can be applied to electric packaging components, dielectric materials, SAW (surface acoustic wave) devices, and photoelectric devices. In this study, we surveyed the crystallization and preferred orientation of AlN thin films with an X-ray diffractometer. To fabricate the AlN thin film, we used the magnetron sputtering method with $N_2$, NH3 and Ar. According to an increase in the partial pressures of $N_2$ and $NH_3$, Al was nitrified and deposited onto a substrate in a molecular form. When AlN was fabricated with $N_2$, it showed a c-axis orientation and tended toward a high orientation with an increase in the temperature. On the other hand, when AlN was fabricated with $NH_3$, it showed a-axis orientation. This result is coincident with the proposed mechanism. We fabricated AlN thin films with an a-axis orientation by controlling the sputtering electric power, $NH_3$ pressure, deposition speed, and substrate temperature. According to the proposed mechanism, we also fabricated AlN thin films which demonstrated high a-axis and c-axis orientations.

• Journal of the Korean Institute of Telematics and Electronics D
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• v.35D no.8
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• pp.15-23
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• 1998

Single crystalline I $n_{x}$G $a_{1-x}$ N thin film was grwon by MOCVD on (001) sapphire substrate for the blue light emitting devices. A good quality of I $n_{0.13}$G $a_{0.87}$N/GaN heterostructure grwon above 700.deg. C was confiremed by various characterization techniques of AFM, RHEED and DC-XRD. Through PL measurement at room temperautre for the Si-Zn co-doped I $n_{x}$G $a_{a-x}$N/GaN structure grwon at 800.deg. C to obtain blue wavelength emission, 460-470 nm and 425 nm emission peak were observed, which are believed to be from donor-to-acceptor pair transition and band edge emission of In/x/G $a_{1-x}$ N, respectively. The result of PL measurement of the undoped MQW I $n_{x}$G $a_{1-x}$ N layer at low temperature confirmed that the strong MQW peak was resulted by exciton from the GAN barrier and carrier of DA pair confined into the well layer.ll layer.yer.r.

• Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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• 2010.06a
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• pp.165-165
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• 2010

AZO:H films were prepared by RF magnetron sputtering system with a AZO (2wt% $Al_2O_3$) ceramic target at a temperature of $150^{\circ}C$. The annealing treatments were carried out in hydrogen ambient for 1hr at a temperature of $400^{\circ}C$. The AZO:H films were etched with 1 % HCl. The influence of the properties of AZO:H films deposited in various working pressures is investigated. As a result, the AZO:H film deposited in 4mTorr showed excellent electrical property of $\rho=5.036{\times}10^{-4}{\Omega}cm$ and strongly oriented (002) peak. The transmittance in the wavelength of 450nm was above 80%. It can be used as front electrode for increasing efficiency of GaN LED.

• Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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• 2008.06a
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• pp.178-178
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• 2008

초소형 박막의 열전 발전모듈은 작은 부피와 한번 설치시 교체없이 지속적인 전원공급으로 소형의 센서 노드에 전원으로 각광 받고 있다. 이에 본 논문에서는 In Plane방식의 PIN Junction의 박막형 열전소자를 제작하여 보았다. 열전 박막인 P-type의 $BiSbTe_3$와 N-type의 $Bi_2Te_3$은 (001)GaAs 기판에 MOCVD(Metal Organic Chemical Vapour Deposition)방식으로 성장하였으며 전극으로는 E-Beam Evaporator를 이용하여 금(Au), 알루미늄(Al)을 사용하였다. 열전박막의 두께는 MOCVD의 성장시간과 온도 MO-x 가스의 압력으로 조절하여 주었다. 제작결과 1Pairs 당 약 $63{\mu}V$/K을 나타내었다.

• Journal of the Korean Crystal Growth and Crystal Technology
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• v.14 no.6
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• pp.244-252
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• 2004

A stoichiometric mixture of evaporating materials for $CuInSe_2$ single crystal thin films was prepared from horizontal electric furnace. To obtain the single crystal thin films, $_CuInSe2$ mixed crystal was deposited on thoroughly etched semi-insulating GaAs(100) substrate by the hot wall epitaxy (HWE) system. The source and substrate temperatures were $620^{\circ}C$ and $410^{\circ}C$, respectively. The crystalline structure of the single crystal thin films was investigated by the photoluminescence and double crystal X-ray diffraction (DCXD). The carrier density and mobility of $CuInSe_2$ single crystal thin films measured with Hall effect by van der Pauw method are $9.62\times10^{16}/\textrm{cm}^3$, 296 $\textrm{cm}^2$/Vㆍs at 293 K, respectively. The temperature dependence of the energy band gap of the $CuInSe_2$ obtained from the absorption spectra was well described by the Varshni's relation, $E_g$(T) = 1.1851 eV -($8.99\times10^{-4} eV/K)T^2$(T + 153 K). The crystal field and the spin-orbit splitting energies for the valence band of the CuInSe$_2$ have been estimated to be 0.0087 eV and 0.2329 eV at 10 K, respectively, by means of the photocurrent spectra and the Hopfield quasicubic model. These results indicate that the splitting of the Δso definitely exists in the $\Gamma$6 states of the valence band of the $CuInSe_2$. The three photocurrent peaks observed at 10 K are ascribed to the $A_1-, B_1$-와 $C_1$-exciton peaks for n = 1.

• Journal of the Korean Institute of Electrical and Electronic Material Engineers
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• v.29 no.1
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• pp.1-5
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• 2016

The ultimate aims of display market is transparent or flexible. Researches have been carried out for various applications. It has been possible to reduced the process steps and get good electrical properties for semiconductors with large optical bandgaps. Oxide semiconductors have been established as one of the leading and promising technology for next generation display panels. In this paper, alternative treatment processes have been tried for oxide semiconductors of thin film transistors to increase the electrical properties of the thin film transistors and to investigate the mechanisms. There exist a various oxide semiconductors. Here, we focused on InGaZnO, ZnO and InSnZnO which are commercialized or researched actively.

• Proceedings of the KIEE Conference
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• 2006.10a
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• pp.53-54
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• 2006

Arsenic doped p-type ZnO thin films have been realized on intrinsic (100) GaAs substrate by RF magnetron sputtering and thermal annealing treatment. p-Type ZnO exhibits the hole concentration of $9.684{\times}10^{19}cm^3$, resistivity of $2.54{\times}10^{-3}{\Omega}cm$, and mobility of $25.37\;cm^2/Vs$. Photoluminescence (PL) spectra of As doped p-type ZnO thin films reveal neutral acceptor bound exciton ($A^{0}X$) of 3.3437 eV and a transition between free electrons and acceptor levels (FA) of 3.2924 eV. Calculated acceptor binding energy ($E_A$) is about 0.1455 eV. Thermal activation and doping mechanism of this film have been suggested by using X-ray photoelectron spectroscopy (XPS). p-Type formation mechanism of As doped ZnO thin film is more related to the complex model, namely, $As_{Zn}-2V_{Zn}$, in which the As substitutes on the Zn site, rather than simple model, Aso, in which the As substitutes on the O site. ZnO-based p-n junction was fabricated by the deposition of an undoped n-type ZnO layer on an As doped p-type ZnO layer.