20 research outputs found

    Graphene based flexible strain sensor for wearable device

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    ํ•™์œ„๋…ผ๋ฌธ (์„์‚ฌ)-- ์„œ์šธ๋Œ€ํ•™๊ต ๋Œ€ํ•™์› : ๊ณต๊ณผ๋Œ€ํ•™ ๊ธฐ๊ณ„ํ•ญ๊ณต๊ณตํ•™๋ถ€, 2019. 2. ์ด์ •ํ›ˆ.์ตœ๊ทผ ๋กœ๋ณดํ‹ฑ์Šค์™€ ์›จ์–ด๋Ÿฌ๋ธ” ๊ธฐ๊ธฐ, ํ—ฌ์Šค์ผ€์–ด ๊ด€๋ จ ๋ถ„์•ผ์—์„œ์˜ ๋†’์€ ํ™œ์šฉ ๊ฐ€๋Šฅ์„ฑ์œผ๋กœ ์ธํ•ด ๋ณ€ํ˜•๋ฅ  ์„ผ์„œ ์—ฐ๊ตฌ๊ฐ€ ํ™œ๋ฐœํžˆ ์ด๋ฃจ์–ด์ง€๊ณ  ์žˆ๋‹ค. ๋‚˜๋…ธ์™€์ด์–ด, ๋‚˜๋…ธ ์ž…์ž, ํƒ„์†Œ๋‚˜๋…ธํŠœ๋ธŒ ๋ฐ ๊ทธ๋ž˜ํ•€์„ ๋น„๋กฏํ•œ ๋‹ค์–‘ํ•œ ์†Œ์žฌ๋กœ ์œ ์—ฐํ•˜๊ณ  ๋ฏผ๊ฐํ•œ ๋ณ€ํ˜•๋ฅ  ์„ผ์„œ์— ๋Œ€ํ•œ ์—ฐ๊ตฌ๊ฐ€ ์ง„ํ–‰๋˜๊ณ  ์žˆ๋‹ค. ๊ทธ ์ค‘์—์„œ๋„ ๊ทธ๋ž˜ํ•€์€ ๋†’์€ ์ „๋„์„ฑ, ์œ ์—ฐ์„ฑ ๋ฐ ๊ธฐ๊ณ„์  ๊ฐ•๋„๋กœ ์ธํ•ด ๋งŽ์€ ์ฃผ๋ชฉ์„ ๋ฐ›๊ณ  ์žˆ๋‹ค. ๋ณธ ์—ฐ๊ตฌ์—์„œ๋Š” ๊ทธ๋ž˜ํ•€ ๊ธฐ๋ฐ˜ ์œ ์—ฐํ•œ ๋ณ€ํ˜•๋ฅ  ์„ผ์„œ์˜ ์นœํ™˜๊ฒฝ์  ๊ณต์ • ๋ฐ ํŒจํ„ฐ๋‹ ๋ฐฉ๋ฒ•์— ๋Œ€ํ•ด ๋‹ค๋ฃฌ๋‹ค. ๊ทธ๋ฆฌ๊ณ  ์ œ์ž‘๋œ ์„ผ์„œ๋ฅผ ์ด์šฉํ•˜์—ฌ ๋ฌผ์ฒด์™€์˜ ๊ฑฐ๋ฆฌ๋ฅผ ์ธ์‹ํ•˜๊ณ  ๋ฌผ์ฒด์˜ ํ‘œ๋ฉด ํ˜•์ƒ์„ ์žฌ๊ตฌ์„ฑํ•˜๋Š” ์‹คํ—˜์„ ์ˆ˜ํ–‰ํ•˜์˜€๋‹ค.Recently, strain sensors have been actively studied due to their high utilization potential in robotics, wearable devices, and health care related fields. Many researchers are working on a variety of materials including nanowires, nanoparticles, carbon nanotubes(CNTs), and graphenes to fabricate these flexible and sensitive strain sensors. Among them, graphene is attracting much attention due to its high conductivity, flexibility and mechanical strength. In this study, we tried to maximize the advantages of graphene - based strain sensor by studying human - friendly manufacturing method and easy patterning process. Experiments were carried out to recognize the distances to objects and to reconstruct the shapes of the objects by analyzing the signals using the produced graphene - based strain sensors.๊ตญ๋ฌธ์ดˆ๋ก i ๋ชฉ์ฐจ ii ๊ทธ๋ฆผ ๋ชฉ์ฐจ iii ์ œ 1 ์žฅ ์„œ๋ก  1 ์ œ 1 ์ ˆ ์—ฐ๊ตฌ๋ฐฐ๊ฒฝ 1 ์ œ 2 ์ ˆ ์ž‘๋™ ์›๋ฆฌ 5 ์ œ 2 ์žฅ Graphene coating 7 ์ œ 1 ์ ˆ Stencil method 7 ์ œ 2 ์ ˆ Layer by Layer coating method 12 ์ œ 1 ์ ˆ Inkjet printing method 14 ์ œ 3 ์žฅ Reduction process 19 ์ œ 1 ์ ˆ Flash reduction 19 ์ œ 2 ์ ˆ Chemical reduction 20 ์ œ 4 ์žฅ Discussion 21 ์ œ 1 ์ ˆ Fabrication protocol 21 ์ œ 2 ์ ˆ Result 23 ์ œ 5 ์žฅ Conclusion 26 ์ฐธ๊ณ ๋ฌธํ—Œ 27 Abstract 29Maste

    Effects of low temperature deuterium annealing on electrical properties at SiSiOโ‚‚ interface

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    ํ•™์œ„๋…ผ๋ฌธ(์„์‚ฌ) --์„œ์šธ๋Œ€ํ•™๊ต ๋Œ€ํ•™์› :์ „๊ธฐ. ์ปดํ“จํ„ฐ๊ณตํ•™๋ถ€,2007.Maste

    The Development of real-time image enlargement/ reduction module for G4 fax

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    Antitumor efficacy of hypoxia and alpha-fetoprotein-dependent oncolytic adenovirus and systemically injectable adenovirus-liposome hybrid vector

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    ์˜๊ณผํ•™๊ณผ/๋ฐ•์‚ฌ์ข…์–‘ ์„ ํƒ์  ์‚ด์ƒ adenovirus(Ad) ๋Š” ๊ธฐ์กด์˜ ๋ณต์ œ ๋ถˆ๋Šฅ Ad๋ณด๋‹ค ์น˜๋ฃŒ ํšจ๊ณผ ๋ฐ ์œ ์ „์ž ์ „๋‹ฌํšจ์œจ์ด ๋†’๊ฒŒ ๋‚˜ํƒ€๋‚จ์— ๋”ฐ๋ผ ์•” ์œ ์ „์ž ์น˜๋ฃŒ์˜ ์ƒˆ๋กœ์šด ์น˜๋ฃŒ์ œ๋กœ ์—ฐ๊ตฌ๊ฐ€ ํ™œ๋ฐœํžˆ ์ง„ํ–‰ ์ค‘์ด๋‹ค. ์ด์— ๋”ฐ๋ผ, ๋ณธ ์‹คํ—˜์‹ค์—์„œ๋Š” E1B19 kDa ์ด ์ œ๊ฑฐ๋œ ์‚ด์ƒ Ad(Ad-โˆ†E1B19)๋ฅผ ๊ฐœ๋ฐœํ•˜์—ฌ ๊ฐ•๋ ฅํ•œ ์„ธํฌ ์‚ด์ƒํšจ๊ณผ๋ฅผ ๋ณด๊ณ ํ•œ ๋ฐ” ์žˆ๋‹ค. ํ•˜์ง€๋งŒ, Ad-โˆ†E1B19๋Š” ์•”์„ธํฌ๋ฟ ๋งŒ ์•„๋‹ˆ๋ผ ์ •์ƒ์„ธํฌ๊นŒ์ง€ ์‚ด์ƒํ•˜๋Š” ํ•œ๊ณ„๊ฐ€ ๋“œ๋Ÿฌ๋‚ฌ๋‹ค. ๋”ฐ๋ผ์„œ ๋ณธ ์—ฐ๊ตฌ์—์„œ๋Š” ๊ฐ„์•” ์„ธํฌ ํŠน์ด์ ์ธ ์„ธํฌ ์‚ด์ƒ ํšจ๊ณผ๋ฅผ ํš๋“ํ•˜๊ธฐ ์œ„ํ•ด ํ–ฅ์ƒ๋œ human alpha-fetoprotein (hAFP) promoter๋ฅผ Ad์˜ ๋ณต์ œ๋ฅผ ์กฐ์ ˆํ•˜๋Š”๋ฐ ์‚ฌ์šฉํ•˜์˜€๋‹ค. ๋˜ํ•œ ์ข…์–‘ ๋‚ด์˜ ์ €์‚ฐ์†Œ ํ™˜๊ฒฝ์—์„œ promoter์˜ ํ™œ์„ฑ์„ ์ฆ๊ฐ€์‹œํ‚ค๊ธฐ ์œ„ํ•ด 6 ๋˜๋Š” 12 copies์˜ hypoxia response element(HRE)๋ฅผ ์‚ฝ์ž…ํ•˜์—ฌ hAFP promoter ๋˜๋Š” HREs/hAFP ์— ์˜ํ•ด E1A ๋ฐœํ˜„์ด ์กฐ์ ˆ๋˜๋Š” ์ข…์–‘ ์„ ํƒ์  ์‚ด์ƒ Ad๋ฅผ ์ œ์ž‘ํ•˜์˜€๋‹ค. HRE12๊ฐ€ ์‚ฝ์ž…๋œ Ad-HRE12/hAFPโˆ†19๋Š” ๋Œ€์กฐ๊ตฐ์ธ Ad-hAFPโˆ†19๊ณผ ๋น„๊ตํ•˜์—ฌ ํ–ฅ์ƒ๋œ ์ข…์–‘ ์„ ํƒ์„ฑ๊ณผ ์„ธํฌ ์‚ด์ƒ๋Šฅ์„ ๋‚˜ํƒ€๋ƒˆ๋‹ค. ๋น„์นจ์Šต์„ฑ ๋ถ„์ž ์˜์ƒ์œผ๋กœ Ad-HRE12/hAFPโˆ†19์˜ ์ข…์–‘ ์‚ด์ƒ๋Šฅ์„ ๊ด€์ฐฐํ•˜์˜€์„ ๋•Œ ํ”ผํ•˜๋ชจ๋ธ๊ณผ ์›๋ฐœ์„ฑ ๊ฐ„์•” ๋ชจ๋ธ ๋ชจ๋‘์—์„œ ์ƒ์ฒด ์™ธ ๊ฒฐ๊ณผ์™€ ์ผ์น˜ํ•˜๊ฒŒ ์ฆ๋Œ€๋œ ์ข…์–‘ ์„ ํƒ์„ฑ๊ณผ ์ข…์–‘ ์„ฑ์žฅ ์–ต์ œ๋Šฅ์„ ๋‚˜ํƒ€๋ƒˆ๋‹ค. ๋˜ํ•œ, ์ข…์–‘์˜ ์กฐ์งํ•™์  ์‹คํ—˜์„ ์ง„ํ–‰ํ•˜์˜€์„ ๋•Œ ์ €์‚ฐ์†Œ ์ง€์—ญ์—์„œ ๋ฐ”์ด๋Ÿฌ์Šค์˜ ๋ณต์ œ๊ฐ€ ํ™œ๋ฐœํžˆ ์ผ์–ด๋‚˜๋Š” ๊ฒƒ์„ ํ™•์ธํ•˜์˜€๋‹ค. ์•„์šธ๋Ÿฌ Ad-HRE12/hAFPโˆ†19๋ฅผ ์ •๋งฅ์ฃผ์‚ฌ ํ•œ ์ƒ์ฅ์—์„œ๋Š” ์‹ฌ๊ฐํ•œ ๋ฉด์—ญ๋ฐ˜์‘, ๊ฐ„ ๋…์„ฑ ๋˜๋Š” ์กฐ์ง ๋…์„ฑ์ด ๊ด€์ฐฐ๋˜์ง€ ์•Š์•˜๋‹ค. ์ด๋Ÿฌํ•œ ๊ฒฐ๊ณผ๋“ค์„ ๋ฐ”ํƒ•์œผ๋กœ ๋ณธ ์—ฐ๊ตฌ์—์„œ๋Š” hAFP promoter์™€ HREs๊ฐ€ ์‚ฝ์ž…๋œ Ad-โˆ†E1B19๋Š” ํ–ฅ์ƒ ๋œ ๊ฐ„์•” ์กฐ์ง ํŠน์ด์„ฑ๊ณผ ์ข…์–‘ ํ™˜๊ฒฝ ์„ ํƒ์„ฑ์„ ๋‚˜ํƒ€๋‚ด๋Š” ๊ฒƒ์„ ๊ฒ€์ฆํ•˜์˜€๋‹ค. ๋”ฐ๋ผ์„œ ์ฆ๋Œ€๋œ ์„ ํƒ์„ฑ๊ณผ ์ข…์–‘ ์‚ด์ƒ๋Šฅ์„ ๊ฐ€์ง„ Ad-HRE12/hAFPโˆ†19๋Š” AFP๋ฅผ ๋ฐœํ˜„ํ•˜๋Š” ๊ฐ„์•”์— ํšจ๊ณผ์ ์ธ ์น˜๋ฃŒ์ œ๊ฐ€ ๋  ๊ฒƒ์œผ๋กœ ์‚ฌ๋ฃŒ๋œ๋‹ค. ๊ทธ๋Ÿฌ๋‚˜ ์›๋ฐœ์•”์ด๋‚˜ ์ „์ด์•”์„ ์น˜๋ฃŒํ•˜๊ธฐ ์œ„ํ•œ ๋ชฉ์ ์œผ๋กœ ์ •๋งฅ ์ฃผ์‚ฌ๋ฅผ ํ†ตํ•œ Ad์˜ ์ „๋‹ฌ์€ ์ฒด๋‚ด์— ์กด์žฌํ•˜๋Š” Ad์— ๋Œ€ํ•œ ํ•ญ์ฒด์— ์˜ํ•ด ์น˜๋ฃŒํšจ๊ณผ๊ฐ€ ๋–จ์–ด์ง„๋‹ค. ๋ฟ๋งŒ ์•„๋‹ˆ๋ผ ๊ฐ„์— ๋Œ€ํ•œ ๋†’์€ ์นœํ™”๋ ฅ์œผ๋กœ ์ธํ•ด ๊ฐ„ ์ด์™ธ์˜ ์›ํ•˜๋Š” ์•” ์กฐ์ง์—๋Š” ์ „๋‹ฌ์ด ์šฉ์ดํ•˜์ง€ ์•Š์€ ๋‹จ์ ์„ ๊ฐ€์ง€๊ณ  ์žˆ๋‹ค. ์ด๋Ÿฌํ•œ ์ ์„ ๊ทน๋ณตํ•˜๊ณ ์ž ๋ณธ ์—ฐ๊ตฌ์—์„œ๋Š” ๋น„ ๋ฐ”์ด๋Ÿฌ์Šค์„ฑ ๋ฒกํ„ฐ์ธ liposome์— Ad์˜ DNA๋ฅผ ์‚ฝ์ž…ํ•˜์—ฌ hybrid ๋ฒกํ„ฐ๋ฅผ ์ œ์ž‘ํ•˜์˜€๋‹ค. ์‚ฌ์šฉ๋œ DNA๋Š” HRE์™€ ๋ณ€ํ˜•๋œ TERT promoter์— ์˜ํ•ด E1A ๋‹จ๋ฐฑ์งˆ์ด ์กฐ์ ˆ ๋˜๊ณ , ๋ถ„๋น„๋˜๋Š” TRAIL ๋‹จ๋ฐฑ์งˆ์„ ๋ฐœํ˜„ํ•จ์œผ๋กœ์„œ ์•”์„ธํฌ ์‚ด์ƒ๋Šฅ๊ณผ ์„ ํƒ์„ฑ์ด ์ฆ๋Œ€ ๋œ Ad DNA(H5mT-Rd19/stTR)์ด๋ฉฐ ํ์•”์„ ํ‘œ์ ํ™” ํ•˜๋Š” DOTAP :DOPE ๋˜๋Š” PEG:DOTAP:DOPE๋ฅผ liposome์œผ๋กœ ์ด์šฉํ•˜์—ฌ Ad DNA์™€ liposome์ด 1:6์˜ ๋น„์œจ๋กœ ํ˜ผํ•ฉ๋œ ์•ฝ 150 nm์˜ size๋ฅผ ๊ฐ–๋Š” hybrid ๋ฒกํ„ฐ๋ฅผ ์ œ์ž‘ํ•˜์˜€๋‹ค. Hybrid ๋ฒกํ„ฐ๋Š” ํ์•”์„ธํฌ์—์„œ ์„ ํƒ์ ์ธ ์„ธํฌ ์‚ด์ƒ๋Šฅ์„ ๋‚˜ํƒ€๋ƒˆ์œผ๋ฉฐ, ์ƒ์ฅ์— ์ •๋งฅ์ฃผ์‚ฌ ํ•˜์˜€์„ ๋•Œ ๋ฉด์—ญ๋ฐ˜์‘๊ณผ ๊ฐ„ ๋…์„ฑ์€ ๊ด€์ฐฐ๋˜์ง€ ์•Š์•˜๋‹ค. ์ด๋Ÿฌํ•œ ๊ฒฐ๊ณผ๋ฅผ ํ†ตํ•ด Ad DNA-liposome hybrid ๋ฒกํ„ฐ๋Š” ๊ตญ์†Œ์ ์ธ ์•” ์น˜๋ฃŒ๋ฟ ์•„๋‹ˆ๋ผ ์ „์ด ์•”์˜ ์น˜๋ฃŒ์ œ๋กœ์„œ ์œ ์šฉํ•˜๊ฒŒ ์ด์šฉ๋  ์ˆ˜ ์žˆ์„ ๊ฒƒ์œผ๋กœ ์‚ฌ๋ฃŒ๋œ๋‹ค.ope

    ๋ฏธ์„ธ ๊ฐ€๊ณต๋œ ๋Œ€๋ฅ˜์ „์ž ๊ธฐ๋ฐ˜ ํ…Œ๋ฅดํ—ค๋ฅด์ธ  ์žฅ์น˜์— ๋Œ€ํ•œ ์‹คํ—˜ ์—ฐ๊ตฌ

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    ํ•™์œ„๋…ผ๋ฌธ(๋ฐ•์‚ฌ)--์„œ์šธ๋Œ€ํ•™๊ต ๋Œ€ํ•™์› :์ž์—ฐ๊ณผํ•™๋Œ€ํ•™ ๋ฌผ๋ฆฌยท์ฒœ๋ฌธํ•™๋ถ€,2016. 8. ๋ฐ•๊ฑด์‹.For the last decade, terahertz waves have been the focus of many researches to lead to a diverse range of potential applications, such as bio-medical imaging systems, security inspection systems, material analysis systems, and high-data-rate communications systems. Though many types of terahertz components have been developed, e.g., terahertz antennas, filters, guides, and detectors, realistic terahertz applications remain rare due to the lack of powerful, efficient, practically sized, inexpensive, and stable terahertz sources which would fill the terahertz gap. While time-domain spectroscopy (TDS) systems are the main streams of terahertz sources due to the instant spectroscopic capabilities throughout the terahertz range, vacuum electronic devices (VEDs) have also garnered interest due to their high-power capabilities resulting from the high kinetic energy of their convection electrons. In this dissertation, 0.1 THz coupled cavities backward wave oscillator (CCBWO) is proposed and studied as preliminary research on terahertz VEDs, applying two-step LIGA as well as ultra nano CNC machining. The circuits are fabricated with less tolerance than a micron and the cold measurements are in excellent agreement with numerical simulation. All other components of the 0.1THz CCBWO system such as 12kV, 50mA electron gun, 2800gauss of PPM, 8% of band center frequency transmitting vacuum window, and -9kV depressed collector are designed, fabricated, and experimented and all the results match strongly to the design. All parts are assembled together and with the bias voltage at beam focusing electrode, desired perveance is observed in the beam test. 0.22THz staggered extended interaction oscillator is also investigated, focusing on the strong interaction even with relatively low voltage. In the half ฯ€ phase shifted double grating resonator, The large fraction of the fundamental TE mode is longitudinally polarized, and it excites the intense plasma-terahertz wave coupling at the shallow grating, which enables highly efficient RF generation at a relatively low operating voltage. A particle-in-cell (PIC) simulation predicts that the half-period phase-staggered grating resonator generates 0.22 THz wave with output power exceeding 100 W and interaction efficiency of more than 15 % at a low beam acceleration voltage of 5.2 kV.Chapter 1 Introduction 1 1.1 Terahertz 1 1.1.1 THz gap 2 1.1.2 Present THz sources 4 1.2 Vacuum Electronic Devices (VEDs) 6 1.3 Terahertz VEDS and problems 10 1.4 Motivation and Goal 10 1.5 Outline 11 Bibliography 13 Chapter 2 Experimental study of 0.1THz Coupled Cavities Backward Wave Oscillator (CCBWO) 19 2.1 Introduction 19 2.2 0.1THz CCBWO circuit 20 2.2.1 Design of 0.1THz CCBWO circuit 20 2.2.2 Two step LIGA fabrication 35 2.2.3 Ultra-Nano machining 37 2.2.4 Cold test of 0.1THz CCBWO circuit 42 2.3 Electron gun 45 2.3.1 Design of electron gun 45 2.3.2 Fabrication of electron gun 50 2.3.3 Beam-emission test 56 2.4 Periodic Permanent Magnet (PPM) focusing 58 2.4.1 Design of PPM 60 2.4.2 Fabrication of PPM 63 2.4.3 Measurement of PPM 65 2.5 Wide band width anti-reflecting vacuum window 67 2.5.1 Transmission analysis of pillbox window 69 2.5.2 Design of broadband width of 0.1THz vacuum window 79 2.5.3 Cold test of 0.1THz vacuum window 83 2.6 Depressed collector 85 2.6.1 Design of depressed collector 86 2.6.2 Fabrication of depressed collector 88 2.7 System assembly of 0.1THz CCBWO 92 2.7.1 RF test of 0.1THz CCBWO 98 2.8 Conclusion 99 Bibliography 100 Chapter 3 Theoretical study on 0.22 THz sheet beam staggered Extended Interaction Oscillator (sEIO) 102 3.1 Introduction 102 3.2 Design of 0.22THz sEIO 103 3.2.1 sEIO โ€“ Powerfully modified EIO 103 3.3 Particle-In-Cell (PIC) numerical hot test 108 3.4 Conclusion 119 Bibliography 120 Chapter 4 Conclusion 121 List of Publications 122 Domestic Conference proceedings and abstracts 128 ๊ตญ๋ฌธ ์ดˆ๋ก 130Docto

    ํŒŒํ˜• ์ œ์–ด๋œ 2์ฃผ๊ธฐ ๋ฏธ๋งŒ ๊ด‘ ํŽ„์Šค์— ์˜ํ•œ ๊ณ ์ฒด ๋ฐ ๊ธฐ์ฒด ๋‚ด ์ „์ž ์—ญํ•™์˜ ๊ทน์ดˆ๊ณ ์† ์ œ์–ด์™€ ๊ด€์ธก

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    DoctorMeasurement and manipulation of electron dynamics is a flourishing area of research which catches attention nowadays. Fundamental phenomena, in which electrons are involved, such as electron transition between bands in condensed matter and energy states in atoms, mostly occur at femtosecond or sub-femtosecond time scale. The observation and control of electronsโ€™ behavior has been facilitated owing to the utmost development of laser technology. In this thesis, one of the state-of-the-art light sources, waveform-controlled sub-2-cycle optical laser, was employed to explore the interaction with media in solid and gas phases. In a study with solid media, semimetallization was observed in dielectric crystals subjected to strong laser field. A current was generated and directed by the instantaneous light field. A series of theoretical calculation, based on quadruple sub-band model, showing good agreement with experiment, implies that the semimetallization was brought about by electron transition between and within valence and conduction sub-bands. Semimetallization was observed to be a general response of dielectrics to intense light field. It is accounted for by Wannier-Stark localization, a confinement of electrons in a unit cell of crystal lattice under strong field; the effect of long range crystal structure becomes less important. On the other hand, for a study with gaseous medium, an instrument for single-isolated attosecond pulse, which permits one to trace sub-femtosecond electron dynamics, was constructed. By means of high harmonics generation, a train of XUV attosecond pulses were produced and then underwent spectral filtering to select single XUV burst. The temporal profile of the XUV pulse was attained by analyzing the photoelectron kinetic energy spectrogram, ensuring the generation of a single-isolated attosecond pulse. The attosecond pulse was utilized to examine the AC Stark splitting of noble gas atom exposed to intense light field. The attosecond transient absorption spectroscopy was applied to xenon atoms exposed to an NIR intensity of ~1013W/cm2. The asymmetric AC Stark splitting (or, in other words, Autler-Townes splitting) and sub-cycle oscillation in absorption lines were revealed. Theoretical estimation relying on TDCIS, which was in accordance with experimental findings, asserted that the counter rotating wave effect is responsible for the observation

    A cyclic RGD-coated peptide nanoribbon as a selective intracellular nanocarrier

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    We have synthesized a peptide-based supramolecular building block consisting of a cyclic Arg-Gly-Asp (cRGD) peptide segment and a beta-sheet-forming peptide segment. The block peptide was shown to self-assemble into a cRGD-coated nanoribbon structure, as revealed by circular dichroism (CD), dynamic light scattering (DLS), and transmission electron microscopy (TEM) studies. We have shown that this cRGD-coated nanoribbon can encapsulate hydrophobic guest molecules and deliver them into cells. Colocalization of the nanoribbon with LysoTracker and the selective intracellular delivery results suggests that the cRGD-coated nanoribbon is likely to be internalized into the cells through integrin receptors.ope

    Ionically crosslinked Ad/chitosan nanocomplexes processed by electrospinning for targeted cancer gene therapy

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    For effective cancer gene therapy, systemic administration of tumor-targeting adenoviral (Ad) complexes is critical for delivery to both primary and metastatic lesions. Electrospinning was used to generate nanocomplexes of Ad, chitosan, poly(ethylene glycol) (PEG), and folic acid (FA) for effective FA receptor-expressing tumor-specific transduction. The chemical structure of the Ad/chitosan-PEG-FA nanocomplexes was characterized by NMR and FT-IR, and the diameter and surface charge were analyzed by dynamic light scattering and zeta potentiometry, respectively. The average size of Ad/chitosan-PEG-FA nanocomplexes was approximately 140 nm, and the surface charge was 2.1 mV compared to -4.9 mV for naked Ad. Electron microscopy showed well-dispersed, individual Ad nanocomplexes without aggregation or degradation. Ad/chitosan nanocomplexes retained biological activity without impairment of the transduction efficiency of naked Ad. The transduction efficiency of Ad/chitosan-PEG-FA was increased as a function of FA ratio in FA receptor-expressing KB cells, but not in FA receptor-negative U343 cells, demonstrating FA receptor-targeted viral transduction. In addition, the transduction efficiency of Ad/chitosan-PEG-FA was 57.2% higher than chitosan-encapsulated Ad (Ad/chitosan), showing the superiority of FA receptor-mediated endocytosis for viral transduction. The production of inflammatory cytokine, IL-6 from macrophages was significantly reduced by Ad/chitosan-PEG-FA nanocomplexes, implying the potential for use in systemic administration. These results clearly demonstrate that cancer cell-targeted viral transduction by Ad/chitosan-PEG-FA nanocomplexes can be used effectively for metastatic tumor treatment with reduced immune reaction against Ad.ope

    Enhanced delivery of adenovirus, using proteoliposomes containing wildtype or V156K apolipoprotein A-I and dimyristoylphosphatidylcholine

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    The delivery of genes or viruses via liposomes is a common approach used to enhance delivery efficiency. In the current study, to enhance delivery efficiency, proteoliposomes (PLs) containing adenovirus (Ad) were synthesized with dimyristoylphosphatidylcholine (DMPC), cholesterol, and apolipoprotein A-I (apoA-I). Wildtype apoA-I (WT) or V156K-apoA-I (V156K) was then used as an apolipoprotein to compare the structural and functional differences of the PLs. The particle diameter of V156K-PL-Ad was slightly larger than that of WT-PL-Ad, based on native gel electrophoresis. V156K showed more rapid phospholipid bilayer formation than did the WT, based on DMPC clearance. In addition, V156K exhibited maximal fluorescence that was more blue than that of WT in the PL state. Moreover, isothermal denaturation in response to the addition of guanidine hydrochloride (Gnd-HCl) revealed that V156K was more resistant, with no denaturation until 3 M Gnd-HCl was added. In addition, electron microscopy revealed that the viral particles were well associated with PL particles, which had a discoidal structure and were shaped like rouleaux. In addition, treatment of Ad in the PL state showed enhanced green fluorescent protein (GFP) expression when compared with treatment with Ad alone or with DMPC-Ad in hepatoma and brain glioma cells. Cells treated with WT-PL-Ad and V156K-PL-Ad showed approximately 50% more GFP expression than cells treated with Ad alone or with DMPC-Ad after 24 hr of incubation at 37 degrees C, indicating that viral stability was highly increased in the PL state. Furthermore, V156K-PL-Ad showed the highest expression of GFP in adult zebrafish (9 weeks old) at 5 days postinjection (10.5- and 3.8-fold more GFP expressed than by Ad only and DMPC-Ad, respectively). In conclusion, the efficiency of viral delivery and the stability of the virus were significantly enhanced when PLs containing apoA-I were used in cellular and zebrafish models.ope
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