• Current Photovoltaic Research
• /
• v.8 no.3
• /
• pp.102-106
• /
• 2020

In this paper, the effect of MoSe₂ on the contact resistance (R_C) of the transparent conducting oxide (TCO) and Mo junction in the scribed P2 region of the Cu(In,Ga)Se₂ (CIGS) solar module was analyzed. The CIGS/Mo junction becomes ohmic-contact by MoSe₂, so the formation of the MoSe₂ layer is essential. However, the CIGS solar module has a TCO/MoSe₂/Mo junction in the P2 region due to structural differences from the cell. The contact resistance (R_C) of the P2 region was calculated using the transmission line method, and MoSe₂ was confirmed to increase R_C of the TCO/Mo junction. B doped ZnO (BZO) was used as TCO, and when BZO/MoSe₂ junction was formed, conduction band offset (CBO) of 0.6 eV was generated due to the difference in their electron affinities. It is expected that this CBO acts as a carrier transport barrier that disturbs the flow of current, resulting in increased R_C. In order to reduce the R_C caused by CBO, MoSe₂ must be made thin in a CIGS solar module.

• Current Photovoltaic Research
• /
• v.3 no.3
• /
• pp.85-90
• /
• 2015

Two-step processes for preparing $Cu(In,Ga)Se_2$ absorber layers consist of precursor layer formation and subsequent annealing in a Se-containing atmosphere. Among the various deposition methods for precursor layer, the nonvacuum (wet) processes have been spotlighted as alternatives to vacuum-based methods due to their potential to realize low-cost, scalable PV devices. However, due to its porous nature, the precursor layer deposited on Mo substrate by nonvacuum methods often suffers from thick $MoSe_2$ formation during selenization under a high Se vapor pressure. On the contrary, selenization under a low Se pressure to avoid $MoSe_2$ formation typically leads to low crystal quality of absorber films. Although TiN has been reported as a diffusion barrier against Se, the additional sputtering to deposit TiN layer may induce the complexity of fabrication process and nullify the advantages of nonvacuum deposition of absorber film. In this work, Mo oxide layers via thermal oxidation of Mo substrate have been explored as an alternative diffusion barrier. The morphology and phase evolution was examined as a function of oxidation temperature. The resulting Mo/Mo oxides double layers were employed as a back contact electrode for $CuInSe_2$ solar cells and were found to effectively suppress the formation of $MoSe_2$ layer.

• Journal of the Korean Vacuum Society
• /
• v.21 no.3
• /
• pp.142-150
• /
• 2012

In this Study, Mo back electrode were deposited as the functions of various working pressure, deposition time and plasma per-treatment on sodalime glass (SLG) for application to CIGS thin film solar cell using by DC sputtering method, and were analyzed Mo change to $MoSe_2$ layer through selenization processes. And finally Mo back electrode characteristics were evaluated as application to CIGS device after Al/AZO/ZnO/CdS/CIGS/Mo/SLG fabrication. Mo films fabricated as a function of the working pressure from 1.3 to 4.9mTorr are that physical thickness changed to increase from 1.24 to 1.27 ${\mu}m$ and electrical characteristics of sheet resistance changed to increase from 0.195 to 0.242 ${\Omega}/sq$ as according to the higher working pressure. We could find out that Mo film have more dense in lower working pressure because positive Ar ions have higher energy in lower pressure when ions impact to Mo target, and have dominated (100) columnar structure without working pressure. Also Mo films fabricated as a function of the deposition time are that physical thickness changed to increase from 0.15 to 1.24 ${\mu}m$ and electrical characteristics of sheet resistance changed to decrease from 2.75 to 0.195 ${\Omega}/sq$ as according to the increasing of deposition time. This is reasonable because more thick metal film have better electrical characteristics. We investigated Mo change to $MoSe_2$ layer through selenization processes after Se/Mo/SLG fabrication as a function of the selenization time from 5 to 40 minutes. $MoSe_2$ thickness were changed to increase as according to the increasing of selenization time. We could find out that we have to control $MoSe_2$ thickness to get ohmic contact characteristics as controlling of proper selenization time. And we fabricated and evaluated CIGS thin film solar cell device as Al/AZO/ZnO/CdS/CIGS/Mo/SLG structures depend on Mo thickness 1.2 ${\mu}m$ and 0.6 ${\mu}m$. The efficiency of CIGS device with 0.6 ${\mu}m$ Mo thickness is batter as 9.46% because Na ion of SLG can move to CIGS layer more faster through thin Mo layer. The adhesion characteristics of Mo back electrode on SLG were improved better as plasma pre-treatment on SLG substrate before Mo deposition. And we could expect better efficiency of CIGS thin film solar cell as controlling of Mo thickness and $MoSe_2$ thickness depend on Na effect and selenization time.

• Proceedings of the Korean Vacuum Society Conference
• /
• 2011.02a
• /
• pp.368-368
• /
• 2011

최근에 보고된 양질의 고효율Cu(In,Ga)Se2 (CIGS) 태양전지는 CIGS광흡수층이 강한 (220:204) 우선배향성을 갖는 것으로 알려져 있다 [1]. 이러한 CIGS우선배향성은 Se 증착압력, Na농도, 기판온도 및 Mo후면전극의 표면상태에 영향을 받는 것으로 알려져 있지만 정확한 상호관계는 아직 명확히 알려져 있지 않으며, 특히 Mo후면전극의 영향에 대해서는 체계적인 연구결과조차 극히 드문 상황이다 [2]. 본 연구에서는 CIGS 박막의 우선배향성에 대해 Mo후면전극의 미세구조가 미치는 영향 및 이에 따른 cell특성의 변화에 대해서 연구하였다. Mo후면전극의 미세구조는 2 mTorr~16 mTorr까지 증착압력을 변화시켜 제어되었고, CIGS광흡수층은 이렇게 준비된 Mo후면전극상에 3단계 동시증밥법(3-stage process)을 사용하여 형성하였다. XRD를 통한 박막의 우선배향성 평가에서, Mo 증착압력에 대한 IGS I(300)/I(006) 및 CIGS I(220:204)/I(112)의 거동은 Mo 미세구조와 밀접한 관련이 있는 잔류응력(residual stress)의 변화 거동과 상당히 일치함을 보였다. 이에 반해, 높은 압력의 Mo위에 형성된 강한 (220:204) 우선배향성의 CIGS와 bare-glass위에서 형성된 강한 (112) 우선배향성의 CIGS내 Na농도는 서로 유사하였다. 상기의 결과는 Mo미세구조 그 자체가 CIGS 박막 우선배향성의 원인이 됨을 나타낸다. Selenized Mo시편의 XRD분석 및 IGS/Mo 시편의 TEM분석결과을 통해 MoSe2의 반응성이 잔류응력과 비례하는 Mo in-gain 밀도에 의존하는 함을 알 수 있었고, 이러한 MoSe2반응성(reactivity)과 IGS우선배향성 사이에 상당히 밀접한 관련이 있으며 이에 CIGS의 우선배향성이 결정됨을 확인하였다. 마지막으로, Mo변수에 의해 제작된 cell의 특성분석으로부터 cell의 효율이 주로 VOC의 증가에 기인하여 CIGS (220:204) 우선배향성의 정도에 비례하였다.

• Proceedings of the Korean Vacuum Society Conference
• /
• 2011.08a
• /
• pp.364-365
• /
• 2011

태양광 발전산업에서 현재 주류인 결정 실리콘 태양전지의 변환효율은 꾸준히 향상되고 있으나, 태양전지의 가격이 매년 서서히 하강되고 있는 실정에서 결정질 실리콘 가격의 상승 등으로 부가가치창출에 어려움이 있으며, 생산 원가를 낮출 수 있는 태양전지 제조기술로는 2세대 태양전지로 불리는 박막형이 현재의 대안이며, 특히 에너지 변환 효율과 생산 원가에서 장점이 있는 것이 CIGS 박막 태양전지로 판단된다. 화합물반도체 베이스인 CIGS 박막태양전지는 연구실에서는 세계적으로 20.3% 높은 효율을 보고하고 있으며, 모듈급에서도 13% 효율로 생산이 시작되고 있다. 국내에서도 연구실 규모 뿐만 아니라 대면적(모듈급) CIGS 박막 태양전지 증착용 장비, 제조공정 등의 기술개발이 진행되고 있다. CIGSe2를 광흡수층으로 하는 CIGSe2 박막 태양전지의 구조는 여러 층의 단위박막(하부전극, 광흡수층, 버퍼층, 상부투명전극)을 순차적으로 형성시켜 만든다. 이중에 하부전극은 Mo 재료을 스퍼터링 방법으로 증착하여 주로 사용한다. 하부전극은 0.24 Ohm /cm2 정도의 전기적 특성이 요구되며, 주상조직으로 성장하여야 하며, 고온 안정성 확보를 위하여 기판과의 밀착성이 좋아야하고 또한 레이저 패턴시 기판에서 잘 떨어져야 하는 특성을 동시에 가져야 한다. 그리고 CIGSe2의 광흡수층 제조시 셀렌화 공정에서 100 nm 이하의 MoSe2 두께를 갖도록 해야하며, 이는 CIGSe2 박막태양전지의 Rs 값을 줄여 Ohmic 접촉을 향상시키는데 기여한다. 본 연구에서는 CIGSe2 박막태양전지에서 요구되는 하부전극 Mo 박막의 제작과 CIGSe2 박막태양전지 전체공정에 적용후의 MoSe2/Mo 박막특성에 대해서 연구결과들을 논하고자 한다.

• Proceeding of EDISON Challenge
• /
• 2016.03a
• /
• pp.273-276
• /
• 2016

최근 single-layer $MoSe_2$와 같은 2차원의 TMD 화합물들이 물분해 광촉매로서 각광받고 있다. TMD 화합물 중 single-layer $MoSe_2$는 수소 발생 반응을 일으킬 수 있으나 산소 발생 반응은 일으킬 수 없어 산화 반응을 진행시킬 추가적인 전극이 필요하다. 이 연구에서는 strain과 doping을 통해 valence band를 아래로 이동시켜 $MoSe_2$를 더 좋은 물분해 광촉매로 변화시키는 방법을 모색하였다. 먼저 Armchair, zigzag, biaxial isotropic, z-axis direction으로 strain을 걸어줄 때 전자구조의 변화를 관찰하였다. z-axis 방향으로 -2.5% strain을 걸어주었을 때 VBM이 0.07eV만큼 감소하였다. 또한 Mo를 Nb로 치환하고 Se를 P, As로 치환한 다음 전자구조를 관찰하였다. Nb와 doping의 경우 VBM이 감소함을 확인하였으며 As doping의 경우 산화반응이 일어날 수 있고 산화력과 환원력이 비슷해짐을 알아내었다. 또한 산화반응과 환원반응이 일어나는 위치가 분리됨을 확인하였다.

• Journal of the Korean Institute of Electrical and Electronic Material Engineers
• /
• v.29 no.9
• /
• pp.576-580
• /
• 2016

Single-layered transition metal dichalcogenides (TMDs) exhibit more interesting physical properties than those of bulk TMDs owing to the indirect to direct bandgap transition occurring due to quantum confinement. In this research, we demonstrate that layer-by-layer laser etching of molybdenum diselenide ($MoSe_2$) flakes could be controlled by varying the parameters employed in laser irradiation (time, intensity, interval, etc.). We observed a dramatic increase in the photoluminescence (PL) intensity (1.54 eV peak) after etching the samples, indicating that the removal of several layers of $MoSe_2$ led to a change from indirect to direct bandgap. The laser-etched $MoSe_2$ exhibited the single $MoSe_2$ Raman vibration modes at ${\sim}239.4cm^{-1}$ and ${\sim}295cm^{-1}$, associated to out-of-plane $A_{1g}$ and in-plane ${E^1}_{2g}$ Raman modes, respectively. These results indicate that controlling the number of $MoSe_2$ layers by laser etching method could be employed for optimizing the performance of nano-electronic devices.

• Journal of Adhesion and Interface
• /
• v.24 no.1
• /
• pp.36-40
• /
• 2023

A van der Waals material refers to a material having a two-dimensional layered structure composed of van der Waals bonds with weak interlayer bonding. The research based on heterojunction structures using such van der Waals two-dimensional materials has been steadily studied since the discovery of graphene. Herein, this paper reports a van der Waals heterojunction -based field-effect transistor device based on monolayer single crystalline MoSe2 grown by atmospheric pressure chemical vapor deposition. We found that MoSe₂ grown under optimized process conditions did not have atomic-level defects and the transistor devices incorporating MoSe₂ also showed excellent characteristics.

• Proceedings of the Korean Vacuum Society Conference
• /
• 2016.02a
• /
• pp.426.2-426.2
• /
• 2016

Numerous of researches are being conducted to improve the efficiency of $Cu_2ZnSnSe_4$ (CZTSe)-based photovoltaic devices, which is one of the most promising candidates for low cost and environment-friendly solar cells. In this work, we concentrate on the back contact of the devices. A proper thickness of $MoSe_2$ in back contact structure is believed to enhance adhesion and ohmic contact between Mo back contact and absorber layer. Nevertheless, too thick $MoSe_2$ layers that are grown during high-temperature selenization process can impede the current collection, thus resulting in low cell performance. By applying molybdenum nitride as a barrier in back contact structure, we were able to control the thickness of $MoSe_2$ layer, which resulted in lower series resistance and higher fill factor of CZTSe devices. The phase transformation of Mo-N binary system was systematically studied by changing $N_2$ concentration during the sputtering process. With a proper phase of Mo-N fabricated by using an adequate partial pressure of $N_2$, the efficiency of CZTSe solar cells as high as 8.31% was achieved while the average efficiency was improved by about 2% with respect to that of the referent cells where no barrier layer was employed.

• Korean Journal of Metals and Materials
• /
• v.49 no.2
• /
• pp.187-191
• /
• 2011

In order to obtain a suitable back contacting electrode for $Cu(InGa)Se_2$-based photovoltaic devices, a molybdenum thin film was deposited using a chemical vapor transport (CVT) during the hydrogen reduction of $MoO_3$ powder. A $MoO_2$ thin film was successfully deposited on substrates by using the CVT of volatile $MoO_3(OH)_2$ at $550^{\circ}C$ for 60 min in a $H_2$ atmosphere. The Mo thin film was obtained by reduction of $MoO_2$ at $650^{\circ}C$ in a $H_2$ atmosphere. The Mo thin film on the substrate presented a low sheet resistance of approximately $1{\Omega}/sq$.