4,762 research outputs found

    Trace metal analysis by laser ablation-inductively coupled plasma-mass spectrometry and x-ray K-edge densitometry of forensic samples

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    This dissertation describes a variety of studies on the determination of trace elements in samples with forensic importance. Laser ablation-inductively coupled plasma-mass spectrometry (LA-ICP-MS) was used to determine the trace element composition of numerous lipstick samples. Lipstick samples were determined to be homogeneous. Most lipstick samples of similar colors were readily distinguishable at a 95% confidence interval based on trace element composition. Numerous strands of a multi-strand speaker cable were analyzed by LA-ICP-MS. The strands in this study are spatially heterogeneous in trace element composition. In actual forensic applications, the possibility of spatial heterogeneity must be considered, especially in cases where only small samples (e.g., copper wire fragments after an explosion) are available. The effects of many unpredictable variables, such as weather, temperature, and human activity, on the retention of gunshot residue (GSR) around projectile wounds were assessed with LA-ICP-MS. Skin samples around gunshot and stab wounds and larvae feeding in and around the wounds on decomposing pig carcasses were analyzed for elements consistent with GSR (Sb, Pb, Ba, and Cu). These elements were detected at higher levels in skin and larvae samples around the gunshot wounds compared to the stab wounds for an extended period of time throughout decomposition in both a winter and summer study. After decomposition, radiographic images of the pig bones containing possible damage from bullets revealed metallic particles embedded within a number of bones. Metallic particles within the bones were analyzed with x-ray, K-edge densitometry and determined to contain lead, indicating that bullet residue can be retained throughout decomposition and detected within bones containing projectile trauma

    Laser Spectroscopy for Atmospheric and Environmental Sensing

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    Lasers and laser spectroscopic techniques have been extensively used in several applications since their advent, and the subject has been reviewed extensively in the last several decades. This review is focused on three areas of laser spectroscopic applications in atmospheric and environmental sensing; namely laser-induced fluorescence (LIF), cavity ring-down spectroscopy (CRDS), and photoluminescence (PL) techniques used in the detection of solids, liquids, aerosols, trace gases, and volatile organic compounds (VOCs)

    Three-dimensional reconstruction of the tissue-specific multielemental distribution within Ceriodaphnia dubia via multimodal registration using laser ablation ICP-mass spectrometry and X-ray spectroscopic techniques

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    In this work, the three-dimensional elemental, distribution profile within the freshwater crustacean Ceriodaphnia dubia was constructed at a spatial resolution down to S mu m via a data, fusion approach employing state-of-the-art laser ablation inductively coupled plasma-time-of-flight mass spectrometry (LAICP-TOFMS) and laboratory-based absorption microcomputed tomography (mu-CT). C. dubia was exposed to elevated Cu, Ni, and Zn concentrations, chemically fixed, dehydrated, stained, and embedded, prior to mu-CT analysis. Subsequently, the sample was cut into 5 pm thin sections that were subjected to LA-ICPTOFMS imaging. Multimodal image registration was performed to spatially align the 2D LA-ICP-TOFMS images relative to the Corresponding slices of the 3D mu-CT reconstruction. Mass channels corresponding to the isotopes of a single element were merged to improve the signal-to-noise ratios within the elemental images. In order to aid the visual interpretation of the data, LA-ICP-TOEMS data wete projected onto the mu-CT voxels representing tissue. Additionally, the image resolution and elemental sensitivity were compared to those obtained with synchrotron radiation based 3D confocal mu-X-ray fluorescence imaging upon a chemically fixed and air-dried C. dubia specimen

    Laser induced breakdown spectroscopy for heavy metal detection in a sand matrix

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    Β© The Author(s), 2016. This is the author's version of the work and is distributed under the terms of the Creative Commons Attribution License. The definitive version was published in Spectrochimica Acta Part B: Atomic Spectroscopy 125 (2016):177-183, doi:10.1016/j.sab.2016.10.001.Sediments in many locations, including harbors and coastal areas, can become contaminated and polluted, for example, from anthropogenic inputs, shipping, human activities, and poor waste management. Sampling followed by laboratory analysis has been the traditional methodology for such analysis. In order to develop rapid methodologies for eld analysis of sediment samples, especially for metals analyses, we look to Laser Induced Breakdown Spectroscopy as an option. Here through laboratory experiments, we demonstrate that dry sand samples can be rapidly analyzed for the detection of the heavy metals chromium, zinc, lead, and copper. We also demonstrate that cadmium and nickel are detectable in sand matrices at high concentrations.This work is supported by funding from the National Science Foundation (OCE-RIG: 1322704) and the Woods Hole Oceanographic Institution by The Penzance Endowed Fund in Support of Assistant Scientists and The Reuben F. and Elizabeth B. Richards Endowed Fund in Support of Scienti c Sta .2018-10-0

    Sunflower Plants as Bioindicators of Environmental Pollution with Lead (II) Ions

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    In this study, the influence of lead (II) ions on sunflower growth and biochemistry was investigated from various points of view. Sunflower plants were treated with 0, 10, 50, 100 and/or 500 ΞΌM Pb-EDTA for eight days. We observed alterations in growth in all experimental groups compared with non-treated control plants. Further we determined total content of proteins by a Bradford protein assay. By the eighth day of the experiment, total protein contents in all treated plants were much lower compared to control. Particularly noticeable was the loss of approx. 8 ΞΌg/mL or 15 ΞΌg/mL in shoots or roots of plants treated with 100 mM Pb-EDTA. We also focused our attention on the activity of alanine transaminase (ALT), aspartate transaminase (AST) and urease. Activity of the enzymes increased with increasing length of the treatment and applied concentration of lead (II) ions. This increase corresponds well with a higher metabolic activity of treated plants. Contents of cysteine, reduced glutathione (GSH), oxidized glutathione (GSSG) and phytochelatin 2 (PC2) were determined by high performance liquid chromatography with electrochemical detection. Cysteine content declined in roots of plants with the increasing time of treatment of plants with Pb-EDTA and the concentration of toxic substance. Moreover, we observed ten times higher content of cysteine in roots in comparison with shoots. The observed reduction of cysteine content probably relates with its utilization for biosynthesis of GSH and phytochelatins, because the content of GSH and PC2 was similar in roots and shoots and increased with increased treatment time and concentration of Pb-EDTA. Moreover, we observed oxidative stress caused by Pb-EDTA in roots where the GSSG/GSH ratio was about 0.66. In shoots, the oxidative stress was less distinctive, with a GSSG/GSH ratio 0.14. We also estimated the rate of phytochelatin biosynthesis from the slope of linear equations plotted with data measured in the particular experimental group. The highest rate was detected in roots treated with 100 ΞΌM of Pb-EDTA. To determine heavy metal ions many analytical instruments can be used, however, most of them are only able to quantify total content of the metals. This problem can be overcome using laser induced breakdown spectroscopy, because it is able to provide a high spatial-distribution of metal ions in different types of materials, including plant tissues. Data obtained were used to assemble 3D maps of Pb and Mg distribution. Distribution of these elements is concentrated around main vascular bundle of leaf, which means around midrib

    Laser ablation-inductively coupled plasma-mass spectrometry: Examinations of the origins of polyatomic ions and advances in the sampling of particulates

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    Ongoing issues that affect the continued maturation of laser ablation-inductively coupled plasma-mass spectrometry (LA-ICP-MS) are studied. Spectral interferences in the form of polyatomic ions can hinder the analytical abilities of this method. Differences in the origins of polyatomic ions in solution nebulization ICP-MS versus LA-ICP-MS are investigated through observation of metal oxide (MO+) ions. Conditions responsible for the measured MO+ abundances are described via the measured gas kinetic temperature (Tgas). The effect of additional gases (nitrogen and helium) on the ICP and MO+ ion abundances is also studied using this method. Tgas measurements are also used to establish the origin of metal argide (MAr+) ions during LA-ICP-MS experiments and describe conditions during the ion extraction process. The fitness of femtosecond (fs)-LA-ICP-multicollector (MC)-MS for the determination of U isotope ratios from particulates is examined. Advantages of this method over sample dissolution techniques for environmental monitoring are discussed

    ν”ŒλΌμ¦ˆλͺ¨λ‹‰ κ·€κΈˆμ† λ‚˜λ…Έκ΅¬μ‘°λ¬Όμ˜ ν•©μ„± 및 광학적 μ‘μš©

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    ν•™μœ„λ…Όλ¬Έ (박사) -- μ„œμšΈλŒ€ν•™κ΅ λŒ€ν•™μ› : μžμ—°κ³Όν•™λŒ€ν•™ ν™”ν•™λΆ€, 2020. 8. μž₯두전.In this dissertation, synthesis and optical application of plasmonic noble metal nanostructures are mainly discussed. Various methods to fabricate core-shell, nanoshells, nanospike, and nanoparticle arrays structures have been investigated. The optical and morphological properties of as-prepared nanostructures have been also studied by using UV/vis spectroscopy, Raman spectroscopy, and electron microscopy. A brief overview on preparation methods and the plasmonic resonance of noble metal nanostructures are presented in Chapter 1. Chapter 2 presents the metal-enhanced fluorescence (MEF) of gold nanoclusters adsorbed onto Ag@SiO2 core-shell nanoparticle. The static and time-resolved MEF of Au25-adsorbed Ag@SiO2 core-shell nanoparticles (NPs) has been studied systematically with variation of shell thicknesses, core sizes, and excitation wavelengths. The emission of Au25-adsorbed Ag@SiO2 NPs is blue-shifted and highly enhanced compared with that of free Au25 clusters. The photoluminescence (PL) intensity of Au25-adsorbed Ag@SiO2 NPs is higher as much as 7.4 times than that of free Au25 clusters. The increase of the radiative decay rate constant with separation is identical to that of PL enhancement, suggesting that the MEF of Au25-adsorbed Ag@SiO2 NPs arises from the increase of the radiative decay rate constant induced by the near-field enhancement of plasmonic Ag NPs. Chapter 3 describes the fabrication of hollow and bumpy Au (HBA) NSs with rough surfaces using expanded silica mesopores as templates. Because some Au seeds were located at the inner surfaces of silica mesopores, produced Au NSs have inherent inward-grown nanobumps. During seven successive reduction steps, the LSPR peak of Au nanostructures shifted progressively toward a longer wavelength as the sizes of Au seeds increased gradually. Measuring the cross-sections of HBA NSs milled by a focused ion beam, we have found that hollow and bumpy nanostructures arose from the pore structures of mSiO2 NPs. HBA NSs confine Raman-probe molecules well owing to their hollow structures and have ragged surfaces due to their inward-bumpy morphologies, exhibiting highly efficient surface-enhanced Raman scattering activity. Chapter 4 presents the fabrication of genuinely hollow Au nanourchins (HANUs) using SiO2 NPs as hard templates. Ag-SiO2 NPs were fabricated via amine-assisted reduction. Then, Au nanourchins (ANUs) were synthesized by the galvanic replacement reaction of Ag-SiO2 NPs using L-3,4-dihydroxyphenylalanine (DOPA) as a reductant and a capping agent. The silica cores of ANUs were etched using HF(aq) to produce HANUs. Measuring cross sections, we have found that HANUs have well-defined hollow morphologies. Compared with nanourchins made via DOPA-mediated reduction, HANUs hardly contain residual silver because very tiny silver seeds were used as the initiation sites of galvanic replacement. HANUs have revealed large surface-enhanced Raman scattering enhancement and a significant photothermal effect under a weak illumination. Chapter 5 describes that highly dense plasmonic silver NP arrays have been fabricated by laser-induced dewetting of commercially available silver paste as a starting bulk material. The first laser-scan mode has produced unprecedented intermediate structures, so called laser-induced fine silver nanostructures (LIFSNs) while the second laser-scan mode has transformed LIFSNs into plasmonic silver NP arrays via the dewetting of the priorly formed nanostructures. The laser-induced fabrication of silver NP arrays has been found to be very sensitive to distance from secondly irradiated laser pulses, suggesting that the fine control of laser intensity is very important. As-prepared silver NP arrays have generated numerous hot spots to show highly strong surface-enhanced Raman scattering signals.독창적이고 κΈ°λŠ₯적인 ν”ŒλΌμ¦ˆλͺ¨λ‹‰ κ·€κΈˆμ† λ‚˜λ…Έμž…μžμ˜ ν•©μ„±κ³Ό 광학적 νŠΉμ„±μ— λŒ€ν•΄ 주둜 μ—°κ΅¬ν•˜μ˜€λ‹€. λ‹€μ–‘ν•œ ν•©μ„±λ°©μ‹μœΌλ‘œ μ½”μ–΄μ‰˜, 속이 빈 껍질, λ‚˜λ…ΈμŠ€νŒŒμ΄ν¬ 그리고 λ‚˜λ…Έμž…μž μ–΄λ ˆμ΄ ꡬ쑰λ₯Ό ν•©μ„±ν•΄λ³΄μ•˜λ‹€. 뢄광광도계와 λΌλ§Œκ΄‘λ„κ³„, μ „μžν˜„λ―Έκ²½ 등을 μ΄μš©ν•˜μ—¬ μ œμž‘λœ λ‚˜λ…Έκ΅¬μ‘°λ¬Όμ˜ 광학적, ꡬ쑰적 νŠΉμ„±μ„ μ—°κ΅¬ν•΄λ³΄μ•˜λ‹€. κ·€κΈˆμ† λ‚˜λ…Έμž…μž 합성방법과 ν”ŒλΌμ¦ˆλͺ¨λ‹‰ 곡λͺ…ν˜„μƒμ„ Chapter 1에 κ°„λž΅νžˆ μ†Œκ°œν•˜μ˜€λ‹€. Chapter 2μ—μ„œλŠ” 금 ν΄λŸ¬μŠ€ν„°κ°€ 흑착된 Ag@SiO2 μ½”μ–΄μ‰˜ λ‚˜λ…Έμž…μžμ˜ κΈˆμ†-증강 ν˜•κ΄‘ (Metal-enhanced fluorescence, MEF)에 λŒ€ν•΄ μ—°κ΅¬ν•˜μ˜€λ‹€. κΈˆμ†λ‚˜λ…Έμž…μžλŠ” μž…μ‚¬ 광에 μ˜ν•΄μ„œ ν‘œλ©΄μ˜ μžμœ μ „μžλ“€μ΄ 집단적인 μ§„λ™ν•˜λŠ” ν‘œλ©΄ν”ŒλΌμ¦ˆλͺ¬κ³΅λͺ… (surface plasmon resonance, SPR)μ΄λΌλŠ” λ…νŠΉν•œ 광학적 νŠΉμ„±μ„ 가진닀. μ΄λŸ¬ν•œ ν˜„μƒμ„ 톡해 λ‚˜λ…Έμž…μž ν‘œλ©΄μ—μ„œλŠ” μž…μ‚¬λ˜λŠ” μ „μžκΈ°μž₯의 세기보닀 수천~수만 λ°° 더 큰 μ„ΈκΈ°λ‘œ 증폭될 수 있으며, μ΄λŸ¬ν•œ ν˜„μƒμ„ κ·Όμ ‘μž₯증폭이라 뢈리고 μžˆλ‹€. μ΄λŸ¬ν•œ 광학적인 κΈ°λŠ₯성을 κ°€μ§€λŠ” κΈˆμ†λ‚˜λ…Έμž…μžμ— 싀리카 κ»μ§ˆμ„ 두λ₯΄λ©΄, κΈˆμ†μž…μž ν‘œλ©΄μ΄ λ³΄ν˜Έλ˜κ±°λ‚˜ SPR ν˜„μƒμ„ λ”μš± μ¦κ°•μ‹œν‚¬ 수 μžˆλ‹€. 은 λ‚˜λ…Έμž…μžλŠ” μˆ˜μš©μ•‘μƒμ—μ„œ 은 이온의 화학적 ν™˜μ›μ„ 톡해 ꡬ ν˜•νƒœλ‘œ ν•©μ„±ν•œ λ‹€μŒ, 싀리카 물질의 전ꡬ체λ₯Ό μ΄μš©ν•œ Stober methodλ₯Ό 톡해 은 λ‚˜λ…Έμž…μž ν‘œλ©΄μ— 싀리카 κ»μ§ˆμ„ κ΅¬ν˜„ν•˜μ˜€λ‹€. TEOS 양을 달리 함에 따라 싀리카 μ‰˜ λ‘κ»˜λ₯Ό λ³€ν™”μ‹œμΌœ 각기 λ‹€λ₯Έ Ag@SiO2 μ½”μ–΄μ‰˜ λ‚˜λ…Έμž…μžλ₯Ό ν•©μ„±ν•œ λ‹€μŒ, 거리-의쑴적인 SPR ν˜„μƒμ„ κ΄€μ°°ν•˜μ˜€μŠ΅λ‹ˆλ‹€. 보톡, λ‚˜λ…Έμž…μžλŠ” μ—΄μ—­ν•™μ μœΌλ‘œ κ°€μž₯ μ•ˆμ •ν•œ ꡬ(sphere) ν˜•νƒœλ‘œ ν•©μ„±λœλ‹€. μ—΄μ—­ν•™μ μ˜ ν•œκ³„λ₯Ό λ„˜μ–΄μ„œ μ’€ 더 고차원적이고 κΈ°λŠ₯성을 κ°€μ§€λŠ” λ‚˜λ…Έμž…μž μ œμž‘μ— κ΄€ν•œ 연ꡬ가 κ΅­λ‚΄μ™Έ μ—°κ΅¬μ§„μ—μ„œ ν™œλ°œν•˜κ²Œ μ§„ν–‰λ˜κ³  μžˆλ‹€. λ‚˜λ…Έμ‰˜ (nanoshell) ν˜•νƒœμ˜ μž…μžλž€, 싀리카 같은 μœ μ „λ¬Όμ§ˆμ΄ 쀑심에 μ‘΄μž¬ν•˜κ³ , κ·Έ ν‘œλ©΄μ„ κΈˆμ†λ¬Όμ§ˆλ‘œ 껍질처럼 λ‘˜λŸ¬μ‹ΈμΈ ꡬ쑰λ₯Ό λ§ν•˜λŠ”λ°, λ‚˜λ…Έμ‰˜μž…μžλŠ” ꡬ ν˜•νƒœμ˜ μž…μžλ³΄λ‹€ SPR ν˜„μƒμ„ λ”μš± κ°•ν•˜κ²Œ λ°œν˜„μ‹œν‚€κ³ , 적외선 μ˜μ—­ μͺ½μ—μ„œ 광학적 ν™œμ„±μ„ λ³΄μ΄λŠ” κ³ κΈ°λŠ₯μ„± ꡬ쑰이닀. Chapter 3μ—μ„œλŠ” 이전에 λ³΄κ³ λ˜μ§€ μ•Šμ•˜λ˜ ꡬ쑰인, 속이 λΉ„μ–΄μžˆκ³  κ·Έ μ•ˆμͺ½μ— ν‘œλ©΄μ— κ±°μΉ κΈ°κ°€ μžˆλŠ” 금 λ‚˜λ…Έμ‰˜ μž…μžλ₯Ό 합성에 λŒ€ν•΄ μ„€λͺ…ν•˜μ˜€λ‹€. λ‚˜λ…Έμž…μžμ˜ ν‘œλ©΄μ΄ κ±°μΉ λ‹€λ©΄, λ‚˜λ…Έλ―Έν„° μŠ€μΌ€μΌμ—μ„œ μ „μžκΈ°μž₯을 μ‚°λž€μ‹œν‚¬ 수 μžˆμœΌλ―€λ‘œ SPR 효과λ₯Ό λ”μš± μ¦κ°•μ‹œν‚¬ 수 μžˆλ‹€. 속이 λΉ„μ–΄μžˆκ³  μ•ˆμͺ½μ˜ ν‘œλ©΄μ΄ 거진 λ‚˜λ…Έμ‰˜ ꡬ쑰λ₯Ό λ§Œλ“€κΈ° μœ„ν•΄ λ©”μ‘°ν¬λŸ¬μŠ€(mesoporous) 싀리카 λ‚˜λ…Έμž…μžλ₯Ό μ£Όν˜•μœΌλ‘œ μ΄μš©ν–ˆλŠ”λ°, λ©”μ‘°ν¬λŸ¬μŠ€ μ‹€λ¦¬μΉ΄λŠ” μž…μž 내에 CTAB λΆ„μžλ“€μ˜ μžκ°€μ‘°λ¦½μ— μ˜ν•΄μ„œ λ§Œλ“€μ–΄μ§„ 곡동이 무수히 μ‘΄μž¬ν•˜λŠ” 싀리카 μž…μžλ₯Ό λ§ν•œλ‹€. λ©”μ‘°ν¬λŸ¬μŠ€ 싀리카 곡동에 ν‘œλ©΄μ²˜λ¦¬λ₯Ό ν†΅ν•΄μ„œ μžκ·Έλ§ˆν•œ 금 λ‚˜λ…Έμž…μžλ₯Ό λΆ€μ°©μ‹œν‚€κ³ , 화학적 ν™˜μ›λ²•μ„ 톡해 금 λ‚˜λ…Έμž…μžλ“€μ„ μ„±μž₯μ‹œν‚¨λ‹€. μ„±μž₯λ˜λŠ” 금 λ‚˜λ…Έμž…μžλ“€μ€ μž…μžκ°€ 컀짐에 따라 싀리카 곡동ꡬ쑰λ₯Ό λΆ€λΆ„μ μœΌλ‘œ μ±„μš°κ²Œ 되고, μΆ”ν›„ 싀리카λ₯Ό HF둜 μ—μΉ­ν•¨μœΌλ‘œμ„œ 속이 λΉ„μ–΄μžˆκ³  μ•ˆμͺ½μ— 거친 ν‘œλ©΄μ„ κ°€μ§€λŠ” 금 λ‚˜λ…Έμ‰˜ (hollow and bumpy gold nanoshell, HBA NS) ν•©μ„±ν•  수 μžˆμ—ˆλ‹€. μ–΄λ– ν•œ κΈˆμ† λ‚˜λ…Έκ΅¬μ‘°λ¬Όμ— λ‚˜λ…ΈμŠ€μΌ€μΌμ˜ κ±°μΉ κΈ°λ‚˜ λ‚˜λ…ΈνŒ ν˜•νƒœλ₯Ό λΆ€μ—¬ν•˜λ©΄ λ”μš± ν–₯μƒλœ ν”ŒλΌμ¦ˆλͺ¨λ‹‰ μ„±μ§ˆμ„ 보일 수 μžˆλ‹€. 음의 μœ μ „μœ¨μ„ κ°€μ§€λŠ” κ·€κΈˆμ† λ‚˜λ…Έκ΅¬μ‘°λ¬Όμ€ μž…μ‚¬ν•˜λŠ” μ „μžκΈ°μž₯을 κ΅­λΆ€μ μœΌλ‘œ κ΅¬μ†ν•˜λŠ” λŠ₯λ ₯이 κ°€μ§€κ²Œ 되고, νŠΉνžˆλ‚˜ λ‚˜λ…ΈνŒκ³Ό 같이 ꡬ쑰체의 곑λ₯ μ΄ μ‹¬ν•˜κ²Œ λ³€ν™”ν•˜λŠ” 곳은 κ·Έ νš¨κ³Όκ°€ λ”μš± μ¦ν­λ©λ‹ˆλ‹€. Chapter 4μ—μ„œλŠ” μž…μž μ•ˆμ˜ cavityκ°€ ν™•μ‹€νžˆ μ‘΄μž¬ν•˜κ³  ν‘œλ©΄μ— λ‚˜λ…ΈνŒμ΄ λ¬΄μˆ˜ν•œ μž…μžλ₯Ό ν•©μ„±ν•˜κ³ μž λ…Έλ ₯ν•˜μ˜€λ‹€. SH-둜 ν‘œλ©΄κ°œμ§ˆλœ 싀리카 λ‚˜λ…Έμž…μžλ₯Ό ν•©μ„±ν•œ λ‹€μŒ, μ•„μ£Ό μž‘μ€ 크기의 은 λ‚˜λ…Έμž…μžλ₯Ό 싀리카 ν‘œλ©΄μ— ν•©μ„±ν•œλ‹€. 이후, 점진적인 galvanic replacement λ°˜μ‘μ„ ν†΅ν•΄μ„œ 싀리카 ν‘œλ©΄ μœ„μ— 금 λ‚˜λ…ΈνŒμ΄ λ¬΄μˆ˜ν•˜κ²Œ μ‘΄μž¬ν•˜λŠ” λ‚˜λ…Έμ„±κ²Œ μž…μž(spiky Au nanourchins, SANUs) λ₯Ό ν•©μ„±ν•œλ‹€. HAADF-STEM 츑정방식을 ν†΅ν•΄μ„œ SANUs μž…μž 쀑간에 싀리카 μž…μžκ°€ ν™•μ‹€νžˆ 보이며, galvanic replacement λ°˜μ‘μœΌλ‘œ 금 λ‚˜λ…Έκ»μ§ˆμ΄ ν™˜μ›λœ λͺ¨μŠ΅μ΄ κ΄€μ°°λœλ‹€. λ˜ν•œ EDX line-mappingκ³Ό μ›μ†ŒλΆ„μ„μ„ ν†΅ν•΄μ„œ, SANUs μž…μžλŠ” 속이 λΉ„μ–΄μžˆκ³  금 성뢄이 98 wt%둜 κ΄€μ°°λ˜λŠ” 데 λ°˜ν•΄, 은 성뢄은 0.2 wt% μ•„μ£Ό κ·Ήλ―ΈλŸ‰μœΌλ‘œ κ΅¬μ„±λ˜μ–΄μžˆμŒμ„ ν™•μΈν•˜μ˜€λ‹€. μ΅œμ’…μ μœΌλ‘œ ν•©μ„±λœ SANUs μž…μžμ— HF둜 싀리카 성뢄을 λ…Ήμ—¬μ„œ 속이 λΉ„μ–΄μžˆκ³  λ‚˜λ…ΈνŒμ΄ λ¬΄μ„±ν•œ 금 λ‚˜λ…Έμ„±κ²Œ (hollow and spiky Au nanourchins, HSANUs)λ₯Ό μ–»μ–΄λ³΄μ•˜λ‹€. FIB (focused-ion beam) κΈ°λ²•μœΌλ‘œ κ·Έ 단면을 μ‘°μ‚¬ν•˜μ—¬ HSANUs μž…μž μ•ˆμͺ½μ— ν™•μ—°ν•œ cavity ν˜•νƒœλ₯Ό ν™•μΈν•˜μ—¬, μ€‘κ΅­μ˜ 연ꡬ진듀에 μ˜ν•΄ μ œμ•ˆλœ λ‚˜λ…Έμ„±κ²Œ μž…μžμ˜ cavity의 크기가 ν™•μ—°νžˆ 비ꡐ됨을 ν™•μΈν•˜μ˜€λ‹€. λ ˆμ΄μ €λ₯Ό μ΄μš©ν•œ 미세ꡬ쑰 κ°€κ³΅κΈ°μˆ μ€ λ ˆμ΄μ € λΉ”μ˜ 고집속성 및 μ‹œκ³΅κ°„μ  μ •λ°€ν•¨μœΌλ‘œ 인해 λ°˜λ„μ²΄, μ „μž, λ©”μΉ΄νŠΈλ‘œλ‹‰μŠ€ λ“±μ˜ 첨단산업 λΆ„μ•Όμ—μ„œ ν•„μˆ˜μ μΈ κΈ°μˆ λ‘œμ„œ, μ‹  곡정 κ°œλ°œμ— κΈ°μ—¬ν•΄μ™”μŠ΅λ‹ˆλ‹€. 광열적 λΆ€μž‘μš©μ΄ μ μ–΄μ„œ 마이크둜-λ‚˜λ…Έ κΈ‰μ˜ ν˜•μƒ 가곡이 κ°€λŠ₯ν•œ κ·Ήμ΄ˆλ‹¨νŒŒ λ ˆμ΄μ €(ultrafast laser)의 λ„μž…κ³Ό 연ꡬ가 ν™œλ°œνžˆ μ§„ν–‰λ˜κ³  μžˆλŠ”λ°, chapter 5μ—μ„œλŠ” κ·Ήμ΄ˆλ‹¨νŒŒ λ ˆμ΄μ € 광원을 μ‚¬μš©ν•˜μ—¬ κΈˆμ† λ‚˜λ…Έκ΅¬μ‘°λ₯Ό μ†μ‰½κ²Œ μ œμž‘ν•œ 연ꡬλ₯Ό μ„€λͺ…ν•˜μ˜€λ‹€. λ‚˜λ…Έμ„Έμ»¨λ“œ λ ˆμ΄μ €λŠ” μ—°μ†νŒŒ λ ˆμ΄μ €μ— λΉ„ν•΄ κ°•ν•œ νŒŒμ›Œλ₯Ό 가짐과 λ™μ‹œμ— 비ꡐ적 열적 μ˜μ—­ (heat-affected zone)이 λ„“μ–΄μ„œ λ²Œν¬λ¬Όμ§ˆμ— κ·Ήμ‹¬ν•œ ν˜•νƒœλ³€ν™”λ₯Ό μœ λ„ν•  수 있기 λ•Œλ¬Έμ— top-down λ°©μ‹μ˜ μ œμž‘μ— μœ λ¦¬ν•˜λ‹€ νŒλ‹¨ν•˜μ˜€μŠ΅λ‹ˆλ‹€. 1.3 J/cm2의 νŒŒμ›Œμ™€ 50 ΞΌm/s의 μ†λ„λ‘œ λ ˆμ΄μ €λ₯Ό μ‹­μžκ°€ ν˜•νƒœλ‘œ μŠ€μΊ”ν•œ (cross-line scanning) 싀버 페이슀트 ν•„λ¦„μ—μ„œ, κ· μΌν•œ λ‚˜λ…Έμž…μžλ°°μ—΄μ΄ μ‹­μžκ°€μ˜ μ™Όμͺ½, 였λ₯Έμͺ½ 가지에 κ΄€μ°°λ˜μ—ˆκ³  μœ„, μ•„λž˜μ˜ κ°€μ§€μ—μ„œλŠ” 이전에 κ΄€μ°°λ˜μ—ˆλ˜ λ―Έμ„Έν•˜κ³  λ¬΄μˆ˜ν•œ 은 μž…μžλ“€μ΄ μ œμž‘λ˜μ—ˆλ‹€. κ°€λ‘œλ°©ν–₯의 μŠ€μΊ”μœΌλ‘œ 톡해 λ―Έμ„Έν•˜κ³  λ¬΄μˆ˜ν•œ 은 λ‚˜λ…Έμž…μžλ₯Ό μ œμž‘ν•œ λ‹€μŒ, μ„Έλ‘œλ°©ν–₯으둜 μŠ€μΊ” ν•  λ•Œ, λΆˆκ· μΌν•œ μ—λ„ˆμ§€ 뢄포 ν˜•νƒœμ˜ Gaussian form을 κ°€μ§€λŠ” λ ˆμ΄μ € 빔에 μ˜ν•΄μ„œ dewetting thresholdλ₯Ό λ„˜μ–΄κ°€λŠ” 곡간적 μ˜μ—­μ—μ„œλŠ” dewetting ν˜„μƒμ΄ μΌμ–΄λ‚˜ λ‚˜λ…Έμž…μžλ°°μ—΄μ΄ μ œμž‘λ˜λŠ” 것을 λ°œκ²¬ν•˜μ˜€λ‹€. μ‹­μžκ°€ λ ˆμ΄μ € μŠ€μΊ” λͺ¨λ“œ μ–‘μ‹μ˜ ν™•μž₯μœΌλ‘œμ„œ, κ·Έλ¬Όλͺ¨μ–‘μ˜ λ ˆμ΄μ € μŠ€μΊ”μ„ μ‹œν–‰ν•˜λ©΄ μ„Όν‹°λ―Έν„°κΈ‰μ˜ λŒ€λ©΄μ μ˜ ν”ŒλΌμ¦ˆλͺ¨λ‹‰ λ‚˜λ…Έκ΅¬μ‘°λ°°μ—΄μ„ 얻을 수 μžˆμ—ˆκ³  κ°•ν•œ μ „μžκΈ°μž₯ μ¦κ°•μœΌλ‘œ ν‘œλ©΄μ¦κ°•λΌλ§Œμ‚°λž€κΈ°λ²• (Surface-enhanced Raman scattering)을 ν†΅ν•΄μ„œ ν•˜μ—¬κΈˆ λΆ„μ„ν•˜κ³ μž ν•˜λŠ” 물질의 농도가 nM μˆ˜μ€€μœΌλ‘œ 내렀가도 μΆ©λΆ„νžˆ κ²€μΆœ κ°€λŠ₯ν•œ κΈ°λŠ₯μ„± 기판 μ œμž‘μ— μ„±κ³΅ν•˜μ˜€λ‹€.Chapter 1. General introduction 1 1.1 Preparation of noble metal nanostructures 2 1.2 Surface plasmons on noble metal nanoparticles 6 1.3 Near-field enhancement on hotspot 8 1.4 References 10 Chapter 2. Metal-enhanced fluorescence of gold nanoclusters adsorbed onto Ag@SiO2 core-shell nanoparticle 12 2.1 Abstract 13 2.2 Introduction 14 2.3 Experimental section 17 2.4 Result and discussion 21 2.5 Conclusion 45 2.6 Acknowledgements 46 2.7 References 46 Chapter 3. Hollow and inward-bumpy gold nanoshells fabricated using expanded silica mesopores as templates 50 3.1 Abstract 51 3.2 Introduction 52 3.3 Experimental section 54 3.4 Result and discussion 59 3.5 Conclusion 81 3.6 Acknowledgements 81 3.7 References 82 Chapter 4. Surface-enhanced Raman scattering and photothermal effect of hollow Au nanourchins with well-defined cavities 85 4.1 Abstract 86 4.2 Introduction 87 4.3 Experimental section 90 4.4 Result and discussion 93 4.5 Conclusion 112 4.6 Acknowledgements 113 4.7 References 113 Chapter 5. Fabrication of plasmonic silver nanoparticle arrays by laser-induced dewetting of commercial silver paste 116 5.1 Abstract 117 5.2 Introduction 118 5.3 Experimental section 122 5.4 Result and discussion 125 5.5 Conclusion 148 5.6 Acknowledgements 149 5.7 References 149 Appendices 153 A.1. List of publications 154 A.2. List of presentations 155 A.2.1. International presentations 155 A.2.2. Domestic presentations 155 Abstract (Korean) 157Docto

    Synthesis and Applications of Organic-Based Fluorescent Carbon Dots: Technical Review

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    New ways of synthesizing organic-based fluorescent carbon dots (CDs) are required in environmental application. This is crucial for mitigation and control of pollutants without increasing the risk of releasing byproduct pollutants as the case with non-organic (metallic) quantum based substrate. Notably, this study provides current research on sustainable synthesis of CDs and their applications through analytical concept of recent and advance techniques for efficient and optimized processes. New scrutinized methods of synthesis and applications of CDs are beneficial and essential to optimize the state-of-art practices. The value distilled in this study adds to the field of sustainable production and application of CDs
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