4 research outputs found

    Laser Controlled Synthesis of Noble Metal Nanoparticle Arrays for Low Concentration Molecule Recognition

    Get PDF
    Nanostructured gold and silver thin films were grown by pulsed laser deposition. Performing the process in an ambient gas (Ar) leads to the nucleation and growth of nanoparticles in the ablation plasma and their self-organization on the substrate. The dependence of surface nanostructuring of the films on the deposition parameters is discussed considering in particular the number of laser pulses and the ambient gas nature and pressure. The performance of the deposited thin films as substrates for surface-enhanced Raman spectroscopy (SERS) was tested against the detection of molecules at a low concentration. Taking Raman maps on micrometer-sized areas, the spatial homogeneity of the substrates with respect to the SERS signal was tested

    Topographical coloured plasmonic coins

    Full text link
    The use of metal nanostructures for colourization has attracted a great deal of interest with the recent developments in plasmonics. However, the current top-down colourization methods based on plasmonic concepts are tedious and time consuming, and thus unviable for large-scale industrial applications. Here we show a bottom-up approach where, upon picosecond laser exposure, a full colour palette independent of viewing angle can be created on noble metals. We show that colours are related to a single laser processing parameter, the total accumulated fluence, which makes this process suitable for high throughput industrial applications. Statistical image analyses of the laser irradiated surfaces reveal various distributions of nanoparticle sizes which control colour. Quantitative comparisons between experiments and large-scale finite-difference time-domain computations, demonstrate that colours are produced by selective absorption phenomena in heterogeneous nanoclusters. Plasmonic cluster resonances are thus found to play the key role in colour formation.Comment: 9 pages, 5 figure

    Layer by Layer Silver Acetate based Coating on Glass and Cement Substrates to Tailor Reflectance and Conductance

    Get PDF
    Tailoring reflectance and conductance was achieved through layer by layer assembly of a silver acetate based multilayer coating. The coating was applied over glass and cement substrates by sol-gel spin coating and by brush painting, respectively. The structural, optical and electrical characteristics and the composition of the coating were studied. The diffraction peaks for all films revealed that the face-centered cubic lattice of the silver crystal structure and the films with more layers had a higher degree of crystallinity. The optical characteristics showed that having more layers leads to decreasing transmittance and increasing reflectance. The I-V characteristics of all samples showed typical ohmic contacts in a voltage range of -1 to 1ย V. The conductance increased drastically as the coating developed into multiple layers. The eight-layer coated glass and cement based substrates had very low surface resistance, at 4 รขโ€žยฆ and 2 รขโ€žยฆ at 1 V, respectively. The study also revealed that the resistance behavior of a multilayered film generally is thermally stable for annealing up to 400ย ยฐC. The coating resistance was significantly increased by further increasing the post-annealing beyond 500ย ยฐC. The studied multilayered coating can be used to tailor the reflectance and conductance of dielectric substrate surfaces for various optoelectronics and sensor device applications

    ๋ฐ”์ด์˜ค ์‘์šฉ์„ ์œ„ํ•œLSPR๊ณผ SERS ๋™์‹œ์ธก์ •๋ฐฉ๋ฒ•: ๊ด‘ํ•™ ์‹œ์Šคํ…œ๊ณผ ์„ผ์„œ ๊ธฐํŒ์— ๋Œ€ํ•ด์„œ

    Get PDF
    ๋ฐ”์ด์˜ค ๋ถ„์ž์˜ ๊ฒ€์ถœ์„ ์œ„ํ•ด, ๋‹ค์–‘ํ•œ ๋ฐฉ๋ฒ•์„ ์ด์šฉํ•œ ๋ฐ”์ด์˜ค ์„ผ์„œ๋“ค์ด ๊ฐœ๋ฐœ๋˜์–ด ์™”์œผ๋ฉฐ ๊ฐ๊ฐ์˜ ๋ฐ”์ด์˜ค ์„ผ์„œ๋“ค์€ ๊ธฐ๊ธฐ ์ ์ธ ์ธก๋ฉด์—์„œ ๋‹ค์–‘ํ•œ ์žฅ์ ๊ณผ ์ฐจ์ด์  ๋“ค์„ ๊ฐ€์ง€๊ณ  ์žˆ๋‹ค. ๊ทธ๋Ÿฌํ•œ ์—ฐ๊ตฌ ์†์—์„œ, ๋ณธ ์—ฐ๊ตฌ์—์„œ๋Š” ๊ด‘์„ฌ์œ  ๊ธฐ๋ฐ˜์˜ ๋ฐ”์ด์˜ค ์„ผ์„œ๋ฅผ ๊ฐœ๋ฐœํ•˜๊ณ ์ž ํ•œ๋‹ค. ๊ด‘์„ฌ์œ  ๊ธฐ๋ฐ˜์˜ ๋ฐ”์ด์˜ค์„ผ์„œ๋Š” ๋‹ค์–‘ํ•œ ์žฅ์ ๋“ค์„ ๊ฐ€์ง€๊ณ  ์žˆ์œผ๋ฉฐ ํŠนํžˆ ๊ด‘์„ฌ์œ  ๊ธฐ๋ฐ˜์˜ ๋ฐ”์ด์˜ค์„ผ์„œ๋Š” ํ•ญ์›-ํ•ญ์ฒด ๋ฐ˜์‘์˜ ๊ตญ์†Œ ํ‘œ๋ฉด ํ”Œ๋ผ์ฆˆ๋ชฌ (localized surface plasmon resonance, LSPR)๊ณผ ํ‘œ๋ฉด ์ฆ๊ฐ• ๋ผ๋งŒ ์‚ฐ๋ž€ (Surface-enhanced Raman scattering, SERS) ๋™์‹œ ์ธก์ • ๋ฐ ์‹ค์‹œ๊ฐ„ ์ธก์ •์ด ๊ฐ€๋Šฅํ•˜๋ฉฐ ์ด๋ฅผ ๊ธฐ๋ฐ˜์œผ๋กœ ๋ณธ ์—ฐ๊ตฌ์—์„œ๋Š” ํ‘œ์  ๋ฌผ์งˆ ์—†์ด ์ธํ„ฐํŽ˜๋ก -๊ฐ๋งˆ(IFN-ฮณ)์˜ ํ•ญ์›-ํ•ญ์ฒด ๋ฐ˜์‘์„ ๋ฐ”์ด์˜ค ๋ถ„์•ผ์˜ ์‘์šฉ์„ ์œ„ํ•œ ๊ฐœ๋… ์ฆ๋ช… ํ˜•ํƒœ๋กœ ์„ฑ๊ณต์ ์ธ ์‹คํ—˜ ์ˆ˜ํ–‰์„ ์ง„ํ–‰ํ•˜์˜€๋‹ค. ์ฑ•ํ„ฐ 1 ์—์„œ๋Š” ๋ณธ ์—ฐ๊ตฌ์˜ ๊ฐ„๋‹จํ•œ ์ด๋ก , ๊ธฐ๋ณธ ๋ฒ•์น™ ๋ฐ ์—ฐ๊ตฌ ๋ชฉ์ ์— ๋Œ€ํ•ด์„œ ๊ฐ„๋žตํ•˜๊ฒŒ ์ œ์‹œํ•˜์˜€๋‹ค. ๋˜ํ•œ ์ตœ๊ทผ ๊ธฐ์ˆ  ์ค‘์—์„œ ๋ฐ”์ด์˜ค ๋ถ„์ž ๊ฒ€์ถœ์„ ์œ„ํ•ด ๋„๋ฆฌ ์‚ฌ์šฉ๋˜๋Š” ๊ฒƒ๋“ค์— ๋Œ€ํ•œ ์˜ˆ์‹œ์™€ ํ•จ๊ป˜ ๊ฐ„๋‹จํ•œ ๋…ผ์˜๋ฅผ ์ฒจ๋ถ€ํ•˜์˜€๋‹ค. ์ฑ•ํ„ฐ 2 ์—์„œ๋Š” ๊ด‘์„ฌ์œ  ๊ธฐ๋ฐ˜์˜ ๋ฐ”์ด์˜ค ๋ถ„์ž ๊ฒ€์ถœ์„ ์œ„ํ•œ LSPR ๋ฐ SERS ๋™์‹œ ์ธก์ • ์‹œ์Šคํ…œ์˜ ๊ฐœ๋ฐœ์— ๋Œ€ํ•ด์„œ ๊ธฐ์ˆ ํ•˜์˜€๋‹ค. ์šฐ์„  ๊ด‘์„ฌ์œ  ๋ง๋‹จ ํ‘œ๋ฉด์— 50 nm ์ •๋„ ํฌ๊ธฐ๋ฅผ ๊ฐ€์ง€๋Š” ๊ธˆ ๋‚˜๋…ธ ์ž…์ž๋ฅผ ํ‘œ๋ฉด ํ™”ํ•™ ์ฒ˜๋ฆฌ๋ฅผ ์ด์šฉํ•˜์—ฌ ๊ณ ์ •์‹œ์ผฐ์œผ๋ฉฐ LSPR ๋ฐ SERS ๋™์‹œ ์ธก์ •์„ ์œ„ํ•ด ๋ถ„๊ด‘ํ•™์  ์‹œ์Šคํ…œ์„ ๊ฐœ๋ฐœํ•˜์˜€๋‹ค. ๊ฐœ๋ฐœํ•œ ์‹œ์Šคํ…œ์„ ์ด์šฉํ•˜์—ฌ ๊ธˆ ๋‚˜๋…ธ ์ž…์ž๊ฐ€ ๋„์ž…๋œ ๊ด‘์„ฌ์œ ์˜ LSPR ์‹ ํ˜ธ์˜ ๋ฏผ๊ฐ๋„ ๋ฐ ์žฌํ˜„ ๊ฐ€๋Šฅ์„ฑ์„ ์‚ดํŽด๋ณด๊ธฐ ์œ„ํ•ด ๊ตด์ ˆ๋ฅ ์— ๋”ฐ๋ฅธ ์‹ ํ˜ธ ๋ณ€ํ™”๋ฅผ ์ธก์ •ํ•˜์˜€์œผ๋ฉฐ ๋˜ํ•œ SERS ์‹ ํ˜ธ์˜ ๋ฏผ๊ฐ๋„ ๋ฐ ์žฌํ˜„ ๊ฐ€๋Šฅ์„ฑ ์—ฌ๋ถ€๋ฅผ ํ™•์ธํ•˜๊ธฐ ์œ„ํ•ด 4-aminothiophenol (4-ATP)๋ฅผ ๋„์ž…ํ•˜์—ฌ SERS ์‹ ํ˜ธ์˜ ์—ฌ๋ถ€๋ฅผ ํ™•์ธํ•˜์˜€๋‹ค. ์ด๋ฅผ ๊ธฐ๋ฐ˜์œผ๋กœ IFN-ฮณ ์˜ ์‹ค์‹œ๊ฐ„ LSPR ์‹ ํ˜ธ ๋ณ€ํ™” ๋ฐ 4-ATP์˜ SERS ์ŠคํŽ™ํŠธ๋Ÿผ์˜ ๋ณ€ํ™”๋ฅผ ๋™์‹œ ์ธก์ • ํ•˜์˜€์œผ๋ฉฐ ์ด๋ฅผ ํ†ตํ•ด ์ƒ๋ฌผํ•™์  ์‘์šฉ์˜ ๊ฐ€๋Šฅ์„ฑ์„ ํ™•์ธํ•˜์˜€๋‹ค. ๋ฐ”์ด์˜ค ๋ถ„์ž ๊ฒ€์ถœ์„ ์œ„ํ•œ SPR ๋ฐ SERS ์„ผ์„œ๋ฅผ ๊ตฌํ˜„ํ•˜๊ธฐ ์œ„ํ•ด์„œ๋Š” ์œ ๋ฆฌ ๊ธฐํŒ ํ˜น์€ ๊ด‘์„ฌ์œ  ํ‘œ๋ฉด์— ๊ท€๊ธˆ์† ๋‚˜๋…ธ ์ž…์ž๊ฐ€ ๋„์ž…๋˜์–ด์•ผ ํ•œ๋‹ค. ํ˜„์žฌ ๋Œ€๋ถ€๋ถ„์˜ ์šฉ์•ก ๊ธฐ๋ฐ˜์˜ ์—ฐ๊ตฌ์—์„œ๋Š” ๊ธฐํŒ ํ‘œ๋ฉด์˜ ๋‚˜๋…ธ ์ž…์ž ๋ฐฐ์—ด์˜ ๋ถˆ๊ท ์ผ์„ฑ์œผ๋กœ ์ธํ•ด ์‹ ํ˜ธ์˜ ๋ฏผ๊ฐ๋„๋‚˜ ์žฌํ˜„์„ฑ์ด ๋‚ฎ์€ ๊ฒฝ์šฐ๊ฐ€ ๋งŽ์œผ๋ฉฐ ์ด๋ฅผ ๊ทน๋ณตํ•˜๊ธฐ ์œ„ํ•ด ๋„์ž…ํ•˜๋Š” ์ „์ž๋น”์„ ์ด์šฉํ•œ ๋ฆฌ์†Œ๊ทธ๋ž˜ํ”ผ ๋ฐฉ๋ฒ•์ด๋‚˜ ์ง„๊ณต ์Šคํผํ„ฐ๋ง ๋“ฑ์„ ์ด์šฉํ•˜์—ฌ ๊ธฐํŒ ํ‘œ๋ฉด์„ ์ฒ˜๋ฆฌํ•˜๋Š” ๋ฐฉ๋ฒ•๋“ค์€ ๊ฐ€๊ฒฉ์ ์ธ ์ธก๋ฉด์—์„œ ๋น„์‹ธ๊ณ  ๋ณต์žกํ•œ ๊ธฐ๊ธฐ๋“ค์ด ํ•„์š”ํ•œ ๊ฒฝ์šฐ๊ฐ€ ๋Œ€๋ถ€๋ถ„์ด๋‹ค. ์ด๋Ÿฌํ•œ ํ‘œ๋ฉด ๊ธฐํŒ์˜ ๋‚˜๋…ธ ์ž…์ž์˜ ์ฒ˜๋ฆฌํ•˜๋Š” ๋ฐฉ๋ฒ•๋“ค์ด ๊ฐ€์ง€๊ณ  ์žˆ๋Š” ์—ฌ๋Ÿฌ ๋‹จ์ ์„ ๊ทน๋ณตํ•˜๋Š” ๋Œ€์•ˆ์œผ๋กœ ๊ธฐํŒ ํ‘œ๋ฉด์— ์ง์ ‘์ ์œผ๋กœ ๋‚˜๋…ธ ์ž…์ž๋ฅผ ๊ด‘ ์œ ๋„ ๋ฐ˜์‘์„ ์ด์šฉํ•ด ๋งŒ๋“œ๋Š” ๊ฒƒ์ด ์ œ์‹œ๋˜์—ˆ์œผ๋‚˜ ์ด๋Ÿฌํ•œ ๋ฐฉ๋ฒ• ์—ญ์‹œ ํ˜„์žฌ ์—ฐ๊ตฌ ์ˆ˜์ค€์—์„œ๋Š” ์—ฌ์ „ํžˆ ๊ท ์ผ๋„๊ฐ€ ๋‚ฎ์€ ๋ชจ์Šต๋“ค์„ ๋ณด์ด๊ณ  ์žˆ๋‹ค. ์ด๋ฅผ ๊ทน๋ณตํ•˜๊ธฐ ์œ„ํ•ด ์ฑ•ํ„ฐ 3 ์—์„œ๋Š” ์œ ๋ฆฌ ๊ธฐํŒ ํ‘œ๋ฉด์— ์€ ๋‚˜๋…ธ ์ž…์ž๋ฅผ ๋‹จ ๋ถ„์‚ฐ ์‹œํ‚ฌ ์ˆ˜ ์žˆ๋Š” ๊ฐ„๋‹จํ•œ ๋ฐฉ๋ฒ• ๊ฐœ๋ฐœ์— ๋Œ€ํ•ด์„œ ๊ธฐ์ˆ ํ•˜์˜€๋‹ค. ์šฐ์„  ๊ท ์ผํ•œ ์œ ๋ฆฌ ๊ธฐํŒ ํ‘œ๋ฉด์ฒ˜๋ฆฌ๋ฅผ ์œ„ํ•˜์—ฌ ์œ ๋ฆฌ ๊ธฐํŒ ํ‘œ๋ฉด์— ์•„๋ฏผ ์ž‘์šฉ๊ธฐ์™€ ์•Œํ‚ฌ ๊ทธ๋ฃน์„ ์ผ์ •ํ•œ ๋น„์œจ๋กœ ๋„์ž…ํ•˜์˜€๋‹ค. ๋˜ํ•œ ๋น›์„ ์กฐ๋ช…ํ•˜๋Š” ์‹œ๊ฐ„ ์—ญ์‹œ ์กฐ์ ˆํ•˜์˜€์œผ๋ฉฐ ์„ฑ์žฅ ์šฉ์•ก ์†์˜ ์งˆ์‚ฐ์€๊ณผ ์‹œํŠธ๋ฅด์‚ฐ ๋‚˜ํŠธ๋ฅจ์˜ ๋†๋„๋ฅผ ์กฐ์ ˆํ•˜์—ฌ ๊ธฐํŒ ํ‘œ๋ฉด์—์„œ ์„ฑ์žฅํ•˜๋Š” ๋‚˜๋…ธ ์ž…์ž์˜ ํฌ๊ธฐ ๋ฐ ๋‹จ ๋ถ„์‚ฐ์„ฑ์„ ์กฐ์ ˆํ•˜์˜€๋‹ค. ์ด๋Ÿฌํ•œ ๋‹จ ๋ถ„์‚ฐ์„ฑ์€ ์ „๊ณ„ ๋ฐฉ์ถœ ์ฃผ์‚ฌ ์ „์ž ํ˜„๋ฏธ๊ฒฝ(Field-emission scanning electron microscopy) ๊ณผ ์•”์‹œ์•ผ(Dark-field) ํ˜„๋ฏธ๊ฒฝ์„ ์ด์šฉํ•˜์—ฌ ํ™•์ธํ•˜์˜€๋‹ค. ์ด๋ฅผ ๊ธฐ๋ฐ˜์œผ๋กœ ์‹คํ—˜ ๊ฒฐ๊ณผ์— ๋Œ€ํ•œ ๊ด‘ ์œ ๋„ ๋ฐ˜์‘์— ๋Œ€ํ•œ ์ด๋ก ์ ์ธ ๋ฉ”์ปค๋‹ˆ์ฆ˜์„ ๊ทœ๋ช…ํ•˜์˜€๋‹ค.In a field of bio-molecular analysis, various kinds of biosensors have been developed extensively. Each of them has many benefits and variations in the instrument designs. In this study proposed is a fiber optic (FO) sensor which has many advantages such as utilization of localized surface Plasmon resonance (LSPR) and surface enhanced Raman scattering (SERS) simultaneously and real time detection of antibody-antigen reaction. The fiber optic sensors were successfully utilized as label-free LSPR and SERS simultaneous detection of antibody-antigen reaction interferon-gamma (IFN-ฮณ) as a proof-of-concept for bio-related applications. Chapter I, as an introductory chapter, aims to provide a brief theoretical information, basic principles and research objective of this study. Also modern techniques that are broadly used in field of bio-molecular detection and its examples are discussed. In Chapter II, fabrication of the FO LSPR and SERS sensor and its simultaneous detection system for bio-applications were described. First, an FO sensor was fabricated by immobilizing gold nanoparticles (Au NPs, ca. 50ยฑ5nm diameter) on one end of a fiber optic by chemical reaction. And simultaneous detection system of the LSPR and SERS was assembled. Then, for checking the FO sensor quality, sensitivity, and also simultaneous detection system reliability, LSPR and SERS signals were measured using various refractive indices solutions and SERS reporter molecule of 4-aminothiphenol (ATP). Finally, the sensor was applied to observe real-time LSPR sensor-gram and SERS spectra of the reporter molecule of ATP during the antibody-antigen reaction of interferon-gamma (IFN-ฮณ) as experiment of biological applications. In a variety of practical applications, including surface plasmon resonance (SPR) sensors and surface-enhanced Raman scattering (SERS) sensors for bio-detection, noble metal nanoparticles attached to a glass slide or optical fiber are required for increased sensitivity. In addition to sensitivity, reproducibility is important for practical applications. In this aspect, many approaches such as e-beam lithography, vacuum sputtering, and wet chemical methods have usually been used for deposition of NPs onto the substrate [1-3]. However, issues such as cost of e-beam method and morphological non-uniformity of wet chemical methods hindered sensitive and reproducible fabrication of the sensor substrate. Recently, several photo-induced methods have been demonstrated to grow silver or gold NPs directly on a glass substrate or fiber optic surface from their aqueous solution. Until now, the morphologies of the photo-induced grown nanoparticles on the substrate have not reached enough uniformity. In Chapter III, a simple method which grows mono-disperse and uniform silver nanoparticles (Ag NPs) directly onto a silica substrate by light irradiation of silver nitrate solution in a presence of sodium citrate was described. Changing the mixed ratio of amine and non-amine functional groups on the substrate as well as photo-illumination time and concentration of growth solutions, mono-disperse growing of Ag NPs was able to control. After photo-induced growing, substrates are characterized by field emission scanning electron microscopy (FE-SEM) and dark field (DF) microscopy. Finally, mechanism of the photo-induced growing process was described on the basis of the experimental results.Chapter 1. Introduction 1 1. Surface Plasmon Resonance Spectroscopy for Bio-detection 2 2. Surface Enhanced Raman Spectroscopy for Bio-molecular Detection 10 3. Fiber optic and its Application for Bio-detection 12 4. Noble metal Nanoparticles for Bio-molecular Detection 15 5. Photo Chemical Method of the Noble metal Nanoparticles ynthesize and Growing 18 6. Research Objective 21 Chapter 2. Fiber Optic Sensor Simultaneously Detecting Localized Surface Plasmon Resonance and Surface-Enhanced Raman Scattering 24 1. Experimental Section 25 2. Results and Discussion 42 Chapter 3. Mono-disperse Growth Control of Silver Nanoparticles on Glass Substrate using Photo-reduction and Mixed Self-assembly 52 1. Experimental Section 53 2. Results and Discussion 64 Conclusions 99 References 102 Abstract in Korean 113Docto
    corecore