Aron Walsh
Ewha Womans University · Engineering
아론 워크 교수의 연구실은 전자구조 이론과 밀도함수이론 기반의 정밀한 양자화학 계산을 바탕으로, 태양전지 및 광촉매 등 에너지 변환 소재의 전자적 성질과 결합 구조를 규명하는 데 주력하고 있습니다. 특히 비이황화물, 페로브스카이트, 비스비스모스산화물 등의 반도체 물질에서의 비대칭 전자 구조, 비중앙대칭 배치, 그리고 고체 내 이온 결함의 영향을 깊이 있게 분석합니다. 연구는 실험과의 융합을 통해 재료 설계 원리를 제시하며, 저비용·비독성·다공성 반도체 소재의 개발에 기여하고 있습니다.
Figures are computed from collected data and may differ slightly.
The chemistry of post transition metals is dominated by the group oxidation state N and a lower N-2 oxidation state, which is associated with occupation of a metal s(2) lone pair, as found in compounds of Tl(I), Pb(II) and Bi(III). The preference of these cations for non-centrosymmetric coordination environments has previously been rationalised in terms of direct hybridisation of metal s and p valence orbitals, thus lowering the internal electronic energy of the N-2 ion. This explanation in term
We report the first-principles electronic structure of BiVO 4, a promising photocatalyst for hydrogen generation. BiVO 4 is found to be a direct band gap semiconductor, despite having band extrema away from the Brillouin zone center. Coupling between Bi 6s and O 2p forces an upward dispersion of the valence band at the zone boundary; however, a direct gap is maintained via coupling between V 3d, O 2p, and Bi 6p, which lowers the conduction band minimum. These interactions result in symmetric hol
Abstract Quaternary semiconducting materials based on the kesterite (A 2 BCX 4 ) mineral structure are the most promising candidates to overtake the current generation of light‐absorbing materials for thin‐film solar cells. Cu 2 ZnSnS 4 (CZTS), Cu 2 ZnSnSe 4 (CZTSe) and their alloy Cu 2 ZnSn(Se,S) 4 consist of abundant, low‐cost and non‐toxic elements, unlike current CdTe and Cu(In,Ga)Se 2 based technologies. Zinc‐blende related structures are formed by quaternary compounds, but the complexity a
Bulk and surface sensitive x-ray spectroscopic techniques are applied in tandem to show that the valence band edge for In2O3 is found significantly closer to the bottom of the conduction band than expected on the basis of the widely quoted bulk band gap of 3.75 eV. First-principles theory shows that the upper valence bands of In2O3 exhibit a small dispersion and the conduction band minimum is positioned at Gamma. However, direct optical transitions give a minimal dipole intensity until 0.8 eV be
Hybrid halide perovskites such as methylammonium lead iodide (CH3NH3PbI3) exhibit unusually low free-carrier concentrations despite being processed at low-temperatures from solution. We demonstrate, through quantum mechanical calculations, that an origin of this phenomenon is a prevalence of ionic over electronic disorder in stoichiometric materials. Schottky defect formation provides a mechanism to self-regulate the concentration of charge carriers through ionic compensation of charged point de
The performance of solar cells based on hybrid halide perovskites has seen an unparalleled rate of progress, while our understanding of the underlying physical chemistry of these materials trails behind. Superficially, CH<sub>3</sub>NH<sub>3</sub>PbI<sub>3</sub> is similar to other thin-film photovoltaic materials: a semiconductor with an optical band gap in the optimal region of the electromagnetic spectrum. Microscopically, the material is more unconventional. Progress in our understanding of
Degenerate $n$-type doping of semiconductors results in optical band-gap widening through occupation of the conduction band, which is partially offset by the so-called band-gap renormalization. From investigation of the magnitude and origin of these shifts through density-functional band-structure theory, we demonstrate that the key contribution to renormalization arises from the nonparabolic nature of the host conduction band but not the rigid shift of the band edges, as is the current paradigm
Open papers in the app to read, cite, and organize with AI.