이지원 교수
Jiwoon Lee
포항공과대학교 신소재공학과 · 공학
연구실 소개
이지원 교수의 연구실은 주로 태양광 및 적외선 영역의 고감도 이미징 기술을 핵심으로 하며, 콜로이드성 반도체 나노입자(특히 PbS 콜로이드 양자점)와 할라이드 퍼보스카이트를 활용한 박막 광다이오드 기반 이미징 소자를 개발하고 있습니다. CMOS 기반 읽기 회로와의 몰입적 통합을 통해 고해상도, 저비용, 유연한 SWIR(단파적외선) 및 NIR(근적외선) 이미징 솔루션을 구현하고자 하며, 특히 단일 광자 탐지 및 3D 구조 분석 기술을 접목한 고성능 센서 기술에 주력하고 있습니다. 이는 의료 영상, 자율주행, 환경 감시 등 다양한 분야에서의 응용 가능성을 열어가고 있습니다.
연구 현황
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주요 논문
15Quantum dots (QDs) have been explored for many photonic applications, both as emitters and absorbers. Thanks to the bandgap tunability and ease of processing, they are prominent candidates to disrupt the field of imaging. This review article illustrates the state of technology for infrared image sensors based on colloidal QD absorbers. Up to now, this wavelength range has been dominated by III–V and II–VI imagers realized using flip-chip bonding. Monolithic integration of QDs with the readout ch
In this letter, we present a small pixel pitch image sensor optimized for high external quantum efficiency in short-wavelength infrared (SWIR). Thin-film photodiodes based on PbS colloidal quantum dot (CQD) absorber allow us to exceed the spectral limitations of silicon’s absorption while maintaining the benefits of CMOS technology. By monolithically integrating PbS CDQ thin films with CMOS readout arrays, high-pixel density SWIR image sensors can be achieved. To overcome the remaining disadvant
Thin-film-based image sensors feature a thin-film photodiode (PD) monolithically integrated on CMOS readout circuitry. They are getting significant attention as an imaging platform for wavelengths beyond the reach of Si PDs, i.e., for photon energies lower than 1.12 eV. Among the promising candidates for converting low-energy photons to electric charge carriers, lead sulfide (PbS) colloidal quantum dot (CQD) photodetectors are particularly well suited. However, despite the dynamic research activ
A backside-illuminated (BSI) near-infrared (NIR)-enhanced silicon single-photon avalanche diode (SPAD) for time-of-flight (ToF) light detection and ranging applications is presented. The detector contains a 2- <inline-formula> <tex-math notation="LaTeX">$\boldsymbol {\mu }\text{m}$ </tex-math></inline-formula>-wide multiplication region with a spherically uniform electric field peak enforced by field-line crowding. A charge-focusing electric field extends into a 10- <inline-formula> <tex-math no
Damage to lower limb muscles requires accurate analysis of the muscular condition via objective microscopic diagnosis. However, microscopic tissue analysis may cause deformation of the tissue structure due to injury induced by external factors during tissue sectioning. To substantiate these muscle injuries, we used synchrotron X-ray imaging technology to project extremely small objects, provide three-dimensional microstructural analysis as extracted samples. In this study, we used mice as experi
Thin film photodiodes (TFPD) can supplement complementary metal-oxide-semiconductor (CMOS) image sensor vision by their exotic optoelectronic properties assisted by their monolithic processability. Halide perovskites are known to show outstanding optoelectronic properties, such as large absorption coefficient, long carrier diffusion lengths, and high carrier mobility, leading to high external quantum efficiency (EQE) and fast charge transport in photodiodes (PDs), especially compared with other
This brief presents offset and gain FPN calibrated linear-logarithmic image sensor. Offset FPN originated from threshold voltage variation of the logarithmic conversion transistor is calibrated with Two-step charge transfer operation. Remaining gain FPN is analyzed and its root cause is investigated. The subthreshold slope difference of the logarithmic conversion transistors in the shared pixel architecture is found to be responsible for the increasing FPN in the logarithmic operation region and
All-silicon highly-doped PN junction-based photodetectors, for photonic integrated circuit (PIC) calibration and power monitoring, are designed and fabricated in the C-band. The photodetector response is measured for different doping conditions. The photodetectors are integrated with an interferometric based phase-interrogator structure for a test calibration circuit. The measured devices show high responsivity (12 A/W) obtained under avalanche condition at 5.7 V reverse bias and reasonable dark
Abstract High‐performance, low‐cost, and energy‐efficient infrared (IR) photodetectors are central to next‐generation sensing technologies, but their advancement is constrained by the intrinsic limitations of conventional materials and band structure design. Here, a semimetal‐in‐oxide tellurium composite (Te‐in‐TeO x ) with an in situ‐formed gradient band structure is introduced, realized by a simple one‐step thermal evaporation process that utilizes the redox dynamics and distinct melting point
Electrical impedance tomography (EIT) has been studied to monitor lung ventilation because it is the only real-time lung imaging method without large equipment [1–2]. However, previous EIT systems just provided 2D cross-sectional image with limited spatial information of the lung and unneglectable volume detection error depending on the location of 2D EIT belt relative to the patient's lung. In spite of its importance, the 3D-EIT has not been realized in lung monitoring because it has many desig
In this article, the X-ray radiation effects on colloidal quantum dot photodiode (QDPD)-based short-wave infrared (SWIR) complementary metal-oxide semiconductor image sensors (QD-CISs) are studied. Individual QDPD, silicon readout IC (Si-ROIC), and QD-CIS are evaluated together for a comprehensive analysis. The dark current, activation energy, and external quantum efficiency (EQE) of samples are investigated before and after irradiating with 58.2 keV of X-ray radiation, which has a different tot
Quantum dot (QD) thin-film photodiodes (TFPDs) are studied extensively in the image sensor field as they can pave the way toward the cost-efficient implementation of short-wave infrared (SWIR) cameras. Interestingly, the QD TFPD image sensors can be operated in the global shutter (GS) mode by turning on the photodiode (PD) only during integration time and subsequently turning it off during the readout. This offers the substantial advantage of reducing the pixel size as it eliminates the need for
Thin-film photodiodes (TFPD) monolithically integrated on the Si Read-Out Integrated Circuitry (ROIC) are promising imaging platforms when beyond-silicon optoelectronic properties are required. Although TFPD device performance has improved significantly, the pixel development has been limited in terms of noise characteristics compared to the Si-based image sensors. Here, a thin-film-based pinned photodiode (TF-PPD) structure is presented, showing reduced kTC noise and dark current, accompanied w
This article presents a simple analytical model of the vertical pinned photodiode (PPD). In the existing pixels with relatively large sizes, the photodiode is formed byp+-n-p doping in a planar manner, and thus the vertical electric field determines the potential of the photodiode. However, as the pixel size becomes smaller, the size of the photodiode also decreases. Accordingly, the influence of the doping concentration in the periphery becomes larger and the pinning voltage is eventually predo
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