The Optimal Aspect Ratio of Gold Nanorods for Plasmonic Bio-sensing

The plasmon resonance of metal nanoparticles shifts upon refractive index changes of the surrounding medium through the binding of analytes. The use of this principle allows one to build ultra-small plasmon sensors that can detect analytes (e.g., biomolecules) in volumes down to attoliters. We use simulations based on the boundary element method to determine the sensitivity of gold nanorods of various aspect ratios for plasmonic sensors and find values between 3 and 4 to be optimal. Experiments on single particles confirm these theoretical results. We are able to explain the optimum by showing a corresponding maximum for the quality factor of the plasmon resonance.     

Live-Cell Superresolution Imaging by Pulsed STED Two-Photon Excitation Microscopy

Two-photon laser scanning microscopy (2PLSM) allows fluorescence imaging in thick biological samples where absorption and scattering typically degrade resolution and signal collection of one-photon imaging approaches. The spatial resolution of conventional 2PLSM is limited by diffraction, and the near-infrared wavelengths used for excitation in 2PLSM preclude the accurate imaging of many small subcellular compartments of neurons. Stimulated emission depletion (STED) microscopy is a superresolution imaging modality that overcomes the resolution limit imposed by diffraction and allows fluorescence imaging of nanoscale features. Here, we describe the design and operation of a superresolution two-photon microscope using pulsed excitation and STED lasers. We examine the depth dependence of STED imaging in acute tissue slices and find enhancement of 2P resolution ranging from approximately fivefold at 20 μm to approximately twofold at 90-μm deep. The depth dependence of resolution is found to be consistent with the depth dependence of depletion efficiency, suggesting resolution is limited by STED laser propagation through turbid tissue. Finally, we achieve live imaging of dendritic spines with 60-nm resolution and demonstrate that our technique allows accurate quantification of neuronal morphology up to 30-μm deep in living brain tissue.     

Far-Field Raman Imaging of Short-Wavelength Particle Plasmons on Gold Nanorods

The surface plasmon fields of gold nanorods with a diameter of 100 nm and lengths of 1–5 m are imaged by using far-field Raman scattering of methylene blue adsorbed on the rods. When optically exciting the nanorods under total internal reflection with wave vector and electric field vector orientations along the rod axis, the plasmon field intensity along this axis is observed to be periodically modulated. This modulation is attributable to a beating of the exciting light wave and the nanorod plasmon mode. The plasmon wavelength deduced from the beat frequency is 379 nm, which is considerably smaller than the exciting laser wavelength of 647 nm. In general, Raman imaging is shown to be a powerful technique to probe local plasmon fields using far-field spectroscopy.     

RGD/FA双靶纳米金棒的制备及其在肿瘤细胞协同靶向成像与光热治疗中的应用

目的:通过制备RGD/FA双靶纳米金考察其与高表达整合素与叶酸受体B16细胞的协同靶向成像与热疗作用;方法:采用功能化PEG分子将靶向小分子RGD与叶酸通过强健Au-S键连接至纳米金棒表面,利用激光共聚焦与808 nm近红外激光器评价修饰纳米金的协同靶向作用;结果:RGD与叶酸分子被成功连接于纳米金表面,且双靶纳米金对小鼠黑色素瘤细胞具有较好的协同靶向作用;结论:同时靶向同一肿瘤细胞的不同表位,可克服单一靶向功能化纳米粒子难以在肿瘤位点有效积累的问题,本研究为多功能纳米金棒在临床肿瘤早期诊断与光热治疗中的应用提供研究基础。     

Reversible Tuning the Aspect Ratio and Plasmonic Shift of Gold Nanorods in Alkaline Environment: Growth,Etching and Rebuilding

Plasmonics - The well-developed seed-mediated growth of gold nanorods (GNRs) is under the weakly acidic condition, and the aggregation of the GNRs usually takes place when the pH value is increased...     

In Vitro Identification of Gold Nanorods through Hyperspectral Imaging

Due to their unique plasmonic and optical properties, gold nanorods (GNR) have shown tremendous potential for nano-based applications extending into a variety of fields including bioimaging, sensor development, electronics, and cancer therapy. These distinctive, shape-specific properties are strongly dependent upon the GNR aspect ratio, thus producing the ability to be targeted for an application by fine-tuning their physical parameters. It is owing to their characteristic spectral signature, which is vastly different from that of a cellular setting, that GNRs are emerging as an ideal candidate for nano-based imaging applications. However, one challenge that has emerged in the field of bioimaging is the need to account for the observed plasmon coupling effect that arises from GNR agglomeration in a physiological environment. In this study, GNRs with aspect ratios of 2.5 and 6.0 were actively identified in an in vitro setting through a hyperspectral imaging (HSI) analysis; which successfully recognized and separated the light scattering pattern of these particles from that of the surrounding cells. Through inclusion of agglomerated GNR spectral patterns in the HSI spectral library, this imaging technique was able to overcome the complication of plasmon coupling, though to varying degrees. These results demonstrate the tremendous potential of GNRs coupled with HSI analysis to advance the field of nano-based sensing and imaging mechanisms.     

Subdiffraction-Limit Two-Photon Fluorescence Microscopy for GFP-Tagged Cell Imaging

We report applications of two-photon excitation fluorescence (2PEF) microscopy with subdiffraction-limit resolution for green-fluorescent-protein-tagged cell imaging. The microscope integrates 2PEF microscopy and stimulated emission depletion microscopy in one microscope that has the benefits of both techniques: intrinsic three-dimensional resolution, confined photobleaching, and subdiffraction-limit resolution. The subdiffraction-limit resolution was demonstrated by resolving green-fluorescent-protein-tagged caveolar vesicles located within a distance shorter than the diffraction limit of a regular 2PEF microscope, which is ∼250 nm even with the best optics. The full width at half-maximum of the effective point-spread function for the 2PEF microscope was estimated to be ∼54 nm.     

叶酸受体靶向的金纳米棒用于细胞内光声成像

目的 分子成像技术具有“早期检测”的特点,由于分子水平上的畸变早于解剖水平上的变化。本研究采用细胞内光声分子成像（PMI）方法,对靶向到癌细胞上的叶酸-金纳米棒（FA-AuNRs）精确定位成像。方法 本文合成了FA-AuNRs,并对其性质包括形貌、吸收光谱和生物相容性进行了研究。修饰叶酸赋予FA-AuNRs特异性靶向到叶酸受体高表达癌细胞的能力。然后,通过PMI实验研究FA-AuNRs对癌细胞的靶向特异性。结果 FA-AuNRs呈棒状,在~800 nm处有一近红外吸收峰。在癌细胞的细胞质中观察到强光声信号,而在正常细胞中只有弱光声信号,表明FA-AuNRs通过叶酸受体介导的内吞作用被癌细胞选择性摄取。这项研究证明了PMI能够实现对靶向到癌细胞上的FA-AuNRs精确定位成像。结论 借助特异性靶向作用,可以通过PMI获得癌细胞表面分子信息。该方法有望实现在细胞和分子水平上对生物过程进行可视化、表征和量化。     

Application of Gold Nanorods for Plasmonic and Magnetic Imaging of Cancer Cells

We report the use of biocompatible gold nanorods (GNRs) as multimodal (plasmonic and magnetic) probes for cancer cell labeling in vitro. These multifunctional and multimodal bioconjugates were prepared by replacing cetyltrimethylammonium bromide with a mixture of functionalized PEGylation molecules so that a variety of functionalities (e.g., magnetic resonance imaging agent gadolinium (Gd) and biorecognition molecule transferrin (Tf)) can be easily integrated using simple chemistry. It was shown that Gd incorporation did not interfere with the plasmonic properties of the GNRs and a strong T1 relaxivity was estimated (10.0 mM⁻¹ s⁻¹), which is more than twice that of the clinical MRI agent Gd-DTPA. The large observed T1 relaxivity was possibly due to the huge surface to volume ratio of GNR, which allowed huge amount of amine-terminated molecule to anchor on the surface, coupled with Gd (III) ions for the enhanced relaxation of water protons. Pancreatic cancer cell overexpressing the transferring receptor was served as the in vitro model, and the Tf-mediated uptake was demonstrated and confirmed by dark-field imaging and transmission electron microscopy. More importantly, cell viability (MTS) assay did not reveal any sign of toxicity in these treated cells, suggesting that PEGylated GNRs can serve as a biocompatible, multifunctional, and multimodal platform for variable bio-applications.     

Widefield Two-Photon Excitation without Scanning: Live Cell Microscopy with High Time Resolution and Low Photo-Bleaching

We demonstrate fluorescence imaging by two-photon excitation without scanning in biological specimens as previously described by Hwang and co-workers, but with an increased field size and with framing rates of up to 100 Hz. During recordings of synaptically-driven Ca²⁺ events in primary rat hippocampal neurone cultures loaded with the fluorescent Ca²⁺ indicator Fluo-4 AM, we have observed greatly reduced photo-bleaching in comparison with single-photon excitation. This method, which requires no costly additions to the microscope, promises to be useful for work where high time-resolution is required.     

Optimal Aspect Ratio and Excitation Spectral Region of LSPR Sensors Using Individual Au Dimmeric Nanoplates

Plasmonics - Both the excitation wavelength and aspect ratio AR are key parameters controlling the refractive index sensitivity performances of plasmonic sensors of individual Au nanoplate dimmers....     

Tuning Ultrafast Photoresponse of Gold Nanorods

Nondegenerate pump probe differential transmission experiments on gold nanorods with varying longitudinal surface plasmon resonance have revealed a new phenomenon where the polarity of the transient transmission signal can be reversibly switched between photo bleaching and photo-induced absorption by controlling probe fluence. Under the usual case where probe fluences are nominal, photo bleaching effect is observed for the nanorods with longitudinal surface plasmon resonance energy smaller than the probe photon energy. The laser-induced melting of the nanorods or change in their shape is ruled out for the observed optical switching effect. A quantitative understanding of the results is attempted by invoking a cascaded two-photon absorption dominant beyond a threshold probe fluence of ～75 μJ/cm².     

Optimized Synthesis of PEG-Encapsulated Gold Nanorods for Improved Stability and Its Application in OCT Imaging with Enhanced Contrast

Gold nanorods (GNRs) are synthesized with a surfactant template, which often poses toxicity issues for biomedical applications. In addition, blue shift of longitudinal surface plasmon resonance (LSPR) peak of GNR is an inherent problem that needs to be addressed for time-course studies. In this work, we resolve these issues by optimizing the encapsulation of GNRs with polyethylene glycol (PEG) where biocompatibility is improved by ～20 % and blue shift over a period of 8 days is reduced from 20 nm in the case of CTAB-GNR to 2 nm for PEG-encapsulated GNR. The encapsulated GNRs were then bioconjugated for targeted dark-field imaging of cancer cells. As an application, we also demonstrate the contrast-enhancing capability of GNRs in optical coherence tomography (OCT) imaging of tumor xenograft where the LSPR closely matches the OCT excitation wavelength. Our study proves that incorporating GNRs enhances the contrast of tumor tissue interfaces along with a considerable broadening in OCT depth profile by six times.     

Simultaneous Live Cell Imaging Using Dual FRET Sensors with a Single Excitation Light

Fluorescence resonance energy transfer (FRET) between fluorescent proteins is a powerful tool for visualization of signal transduction in living cells, and recently, some strategies for imaging of dual FRET pairs in a single cell have been reported. However, these necessitate alteration of excitation light between two different wavelengths to avoid the spectral overlap, resulting in sequential detection with a lag time. Thus, to follow fast signal dynamics or signal changes in highly motile cells, a single-excitation dual-FRET method should be required. Here we reported this by using four-color imaging with a single excitation light and subsequent linear unmixing to distinguish fluorescent proteins. We constructed new FRET sensors with Sapphire/RFP to combine with CFP/YFP, and accomplished simultaneous imaging of cAMP and cGMP in single cells. We confirmed that signal amplitude of our dual FRET measurement is comparable to of conventional single FRET measurement. Finally, we demonstrated to monitor both intracellular Ca²⁺ and cAMP in highly motile cardiac myocytes. To cancel out artifacts caused by the movement of the cell, this method expands the applicability of the combined use of dual FRET sensors for cell samples with high motility.     

Axial Resolution Enhancement by 4Pi Confocal Fluorescence Microscopy with Two-Photon Excitation

Confocal fluorescence microscopy and two-photon microscopy have become important techniques for the three-dimensional imaging of intact cells. Their lateral resolution is about 200–300 nm for visible light, whereas their axial resolution is significantly worse. By superimposing the spherical wave fronts from two opposing objective lenses in a coherent fashion in 4Pi microscopy, the axial resolution is greatly improved to ～100 nm. In combination with specific tagging of proteins or other cellular structures, 4Pi microscopy enables a multitude of molecular interactions in cell biology to be studied. Here, we discuss the choice of appropriate fluorescent tags for dual-color 4Pi microscopy and present applications of this technique in cellular biophysics. We employ two-color fluorescence detection of actin and tubulin networks stained with fluorescent organic dyes; mitochondrial networks are imaged using the photoactivatable fluorescent protein EosFP. A further example concerns the interaction of nanoparticles with mammalian cells.     

Surface Plasmon Dynamics of High-Aspect-Ratio Gold Nanorods

Ultrafast transient absorption studies are reported for high-aspect-ratio gold nanorods that were fabricated by electrochemical deposition in polycarbonate templates. The nanorods are 60 nm in diameter with distribution of lengths of up to 6 μm. The average aspect ratio was ∼50, resulting in a longitudinal surface plasmon resonance (SPR_L) band in the mid-IR, as well as a transverse (SPR_T) band in the visible. The rods were excited at 400 nm and probed at a range of wavelengths from the visible to the mid-IR to interrogate both SPR bands. The dynamics observed, including the electron–phonon coupling time and coherent acoustic breathing mode oscillations, closely resemble those previously reported for gold spherical nanoparticles and smaller-aspect-ratio nanorods. The electron–phonon coupling time was similarly determined to be 3.3 ± 0.2 ps for both of the SPR bands. Also, oscillations with a 32-ps period were observed for probing near the SPR_T band in the visible region due to impulsive coherent excitation of the acoustic breathing mode, which are consistent with the 60-nm diameter of the nanorods determined by scanning electron microscopy. The results demonstrate that the dynamics for long gold nanorods are similar to those for smaller nanoparticles. Gerald M. Sando is a NRL-ASEE Research Associate     

Functionalization of Gold Nanorods Toward Their Applications

The topics focusing on functionalization of gold nanorods have been reviewed with a view toward their advanced uses. In most cases, as-prepared gold nanorods are hydrophilic and protected by surfactants, since anisotropic growth of gold nanorods by chemical, electrochemical, and photo-induced methods is carried out in aqueous media in the presence of surfactants and additives. Since solvophilicity of gold nanorods predominantly affects on their optical properties, the control of dispersity of gold nanorods in matrices has been performed, without loss of their optical characters, by surface modification and hybridization with small molecules or polymers. As a result of the functionalization procedure, the capability of self-assembly of gold nanorods has been improved. Furthermore, the examples of application using gold nanorods demonstrate that gold nanorod is a promising material.     

Nonlinear Optical Properties of Large-Sized Gold Nanorods

The nonlinear optical properties of single gold nanorods (GNRs) with a large diameter of ～200 nm and a long length of ～800 nm were investigated by using a focused femtosecond (fs) laser light with tunable wavelength. While the linear and nonlinear optical properties of small-sized GNRs have been extensively studied, the nonlinear optical properties of large-sized GNRs and the effects of high-order surface plasmon resonances remain unexplored. Second harmonic generation (SHG) or/and two-photon-induced luminescence (TPL) were observed in the nonlinear response spectra, and their dependences on excitation wavelength and polarization were examined. The scattering and absorption spectra of the small- and large-sized GNRs were compared by using the discrete dipole approximation method. It was found that the extinction of large-sized GNRs is dominated by scattering rather than absorption, which is dominant in small-sized GNRs. In addition, it was revealed that the excitation wavelength-dependent SHG of a GNR is governed by the linear scattering of the GNR and the maximum SHG is achieved at the valley of the scattering spectrum. In comparison, the excitation wavelength dependence of TPL is determined by the absorption spectrum of the GNR. The polarization-dependent SHG of a GNR exhibits a strong dependence on the dimension of the GNR, and it may appear as bipolar distributions parallel or perpendicular to the long axis of the GNR or multipole distributions.     

金纳米棒的光学性质及其在生物医学领域的应用

简要介绍金纳米棒的光学性质和合成方法,重点阐述其在生物医学领域研究的最新进展,并对其今后的研究方向进行展望．金纳米棒是一种胶囊状的金纳米颗粒,具有一个横向等离子共振吸收峰和一个纵向等离子共振吸收峰,分别对应其横轴和纵轴两个特征尺寸．通过调节金纳米棒的长径比,纵向等离子共振吸收峰可由可见光区跨越至近红外光区．金纳米棒这一独特的光学性质在生物和化学传感方面有着广泛而重要的应用前景．     

Modulation of Optical Properties of Gold Nanorods on Addition of KOH

Gold nanorods are known to exhibit two distinct surface plasmon oscillations namely, transverse and longitudinal bands corresponding to oscillations of conduction electrons along width and length of gold nanorods. Considerable changes in these surface plasmon resonance peak positions occurred when KOH was added to the nanorod solution. Nanorods with initial longitudinal plasmon band at 739, 796, and 895 nm are studied with variation in KOH concentration. While the longitudinal plasmon resonance peak showed blue shift, transverse plasmon resonance peak exhibited only intensity variations. Changes could be attributed to the shape transition of gold nanorods on variation of pH in the solution. Shape transition of gold nanorods is confirmed by transmission electron microscopy images.