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Featured researches published by Yi-tae Kim.


international solid-state circuits conference | 2014

7.1 A 1/4-inch 8Mpixel CMOS image sensor with 3D backside-illuminated 1.12μm pixel with front-side deep-trench isolation and vertical transfer gate

Jung-Chak Ahn; Kyung-Ho Lee; Yi-tae Kim; Hee-Geun Jeong; Bum-Suk Kim; Hong-ki Kim; Jong-Eun Park; Taesub Jung; Won-Je Park; Taeheon Lee; Eun-Kyung Park; Sangjun Choi; Gyehun Choi; Haeyong Park; Yujung Choi; Seungwook Lee; Yun-kyung Kim; Y. Jay Jung; D.I. Park; Seungjoo Nah; Young-Sun Oh; Mi-Hye Kim; Yooseung Lee; Youngwoo Chung; Ihara Hisanori; Joonhyuk Im; Daniel K. J. Lee; Byung-hyun Yim; Gidoo Lee; Heesang Kown

According to the trend towards high-resolution CMOS image sensors, pixel sizes are continuously shrinking, towards and below 1.0μm, and sizes are now reaching a technological limit to meet required SNR performance [1-2]. SNR at low-light conditions, which is a key performance metric, is determined by the sensitivity and crosstalk in pixels. To improve sensitivity, pixel technology has migrated from frontside illumination (FSI) to backside illumiation (BSI) as pixel size shrinks down. In BSI technology, it is very difficult to further increase the sensitivity in a pixel of near-1.0μm size because there are no structural obstacles for incident light from micro-lens to photodiode. Therefore the only way to improve low-light SNR is to reduce crosstalk, which makes the non-diagonal elements of the color-correction matrix (CCM) close to zero and thus reduces color noise [3]. The best way to improve crosstalk is to introduce a complete physical isolation between neighboring pixels, e.g., using deep-trench isolation (DTI). So far, a few attempts using DTI have been made to suppress silicon crosstalk. A backside DTI in as small as 1.12μm-pixel, which is formed in the BSI process, is reported in [4], but it is just an intermediate step in the DTI-related technology because it cannot completely prevent silicon crosstalk, especially for long wavelengths of light. On the other hand, front-side DTIs for FSI pixels [5] and BSI pixels [6] are reported. In [5], however, DTI is present not only along the periphery of each pixel, but also invades into the pixel so that it is inefficient in terms of gathering incident light and providing sufficient amount of photodiode area. In [6], the pixel size is as large as 2.0μm and it is hard to scale down with this technology for near 1.0μm pitch because DTI width imposes a critical limit on the sufficient amount of photodiode area for full-well capacity. Thus, a new technological advance is necessary to realize the ideal front DTI in a small size pixel near 1.0μm.


international solid-state circuits conference | 2011

A 1/2.33-inch 14.6M 1.4μm-pixel backside-illuminated CMOS image sensor with floating diffusion boosting

Sangjoo Lee; Kyung-Ho Lee; Jong-Eun Park; Hyungjun Han; Young-Hwan Park; Taesub Jung; Youngheup Jang; Bum-Suk Kim; Yi-tae Kim; Shay Hamami; Uzi Hizi; Mickey Bahar; Chang-Rok Moon; Jung-Chak Ahn; Duck-Hyung Lee; Hiroshige Goto; Yun-Tae Lee

As pixel sizes continue to scale down, backside-illuminated (BSI) technology has been recently adopted as a solution to improve pixel SNR performance [1,2]. In addition, as the application of image sensors widens from digital still cameras to digital camcorders, high-resolution and high-speed operation are required. This paper presents 1/2.33-inch 14.6Mpixel CMOS image sensor employing a 1.4μm BSI pixel architecture with a floating-diffusion (FD) boosting scheme that enables high SNR and high speed read-out.


Journal of The Society for Information Display | 2001

Luminous efficacy evaluation of XeI excimer for ACPDP

Hidekazu Hatanaka; Yi-tae Kim; W. T. Lee; Y. J. Lee; Gyeongnam Kim; Hong-Sick Park; Jong-ho Hong; Seoung-jae Im; J. M. Kim

We demonstrate for the first time a luminous efficacy of a Xel excimer PDP comparable to that of a conventional Xe/Ne-mixture PDP using 6-in. ACPDPs. For the conventional PDP as a reference, a mixture of Xe:Ne = 4:96(%) with a total gas pressure of 60.0 kPa (450 torr) was used. For the Xel PDP, Ne-buffered mixtures with the same total gas pressure were tried, and a mixture of I 2 :Xe:Ne = 0.02:7.1:92.88 (%) showed an efficacy as high as that of the conventional Xe PDP.


international electron devices meeting | 2008

Advanced image sensor technology for pixel scaling down toward 1.0µm (Invited)

Jung-Chak Ahn; Chang-Rok Moon; Bum-Suk Kim; Kyung-Ho Lee; Yi-tae Kim; Moo-Sup Lim; Wook Lee; Heemin Park; Kyoung-sik Moon; Jaeryung Yoo; Yong-jei Lee; Byung-Jun Park; Sang-il Jung; June-Taeg Lee; Tae-Hun Lee; Y. J. Lee; Junghoon Jung; Jin-hak Kim; Tae-Chan Kim; Hyunwoo Cho; Duck-Hyung Lee; Yong Hee Lee

As pixel size of image sensors shrinks down rapidly, we are reaching technical barrier to get the required low light performance. In this paper, recent advanced technologies such as backside illumination, new color filter array, low F-number with extended depth of field technologies, etc. are introduced to overcome such a barrier. It is shown that the integration of these advanced sensor technologies can make pixel size shrink down toward 1.0 mum with the required performance.


Archive | 2007

CMOS image sensor and image sensing method using the same

Sung-Ho Choi; Jung-Chak Ahn; Yi-tae Kim; Young-Chan Kim; Hae-Kyung Kong


Archive | 2006

CMOS sensor array with a shared structure

Young-Chan Kim; Yi-tae Kim


Archive | 2006

CMOS active pixel sensor and active pixel sensor array using fingered type source follower transistor

Young-Chan Kim; Yi-tae Kim


Archive | 2006

Pixels for CMOS image sensors

Yi-tae Kim; Young-Chan Kim; Hae-Kyung Kong; Sung-Ho Choi


Archive | 2006

Pixel driving circuit and method of driving the same

Sung-Ho Choi; Yi-tae Kim; Young-Chan Kim; Hae-Kyung Kong


Archive | 2015

UNIT PIXEL OF IMAGE SENSOR AND IMAGE SENSOR INCLUDING THE SAME

Jun-taek Lee; Sang-il Jung; Yi-tae Kim; Woon-Phil Yang

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