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A Comparison of Two Methods of Determining Transparency in Natural WatersHalicki, Phillip J. January 1957 (has links)
No description available.
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Optical properties of large U, quarter-filled band TCNQ salts/McCall, Richard Powell January 1984 (has links)
No description available.
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Growth and optical properties of ZnS and ZnSSe nanostructures. / Growth and optical properties of zinc sulfide and zinc sulfoselenide nanostructures / ZnS和ZnSSe納米結構的生長和光學性質 / CUHK electronic theses & dissertations collection / Growth and optical properties of ZnS and ZnSSe nanostructures. / ZnS he ZnSSe na mi jie gou de sheng chang he guang xue xing zhiJanuary 2009 (has links)
In addition, we have studied the growth conditions and the properties of ZnSSe alloy nano-tetrapods grown by chemical vapor deposition. Different from the ZnSSe nanowires synthesized by MOCVD, the ZnSSe nano-tetrapods are of hexagonal structure. We observed a wavelength-tunable near band gap luminescence in the UV-blue region from this nanostructurally-designed system. / Recently, semiconductor nanostructures have attracted much attention because they are potentially useful as fundamental building blocks in nanodevices. As an important member of group II-VI semiconductors, ZnS and its alloys with ZnSe are particularly important for optical applications in the UV-blue region . Thus, we concentrated on the synthesis of ZnS, ZnSe and ZnSSe nanostructures and studied their optical properties. / Vertically-aligned ZnSe nanowires were also synthesized by MOCVD using Ag and Ga nanoparticles as catalysts. In the photoluminescence spectra from Ag or Ga catalyzed ZnSe nanowires, we observed recombination of excitons bound to substitutional Ag or Ga impurities respectively, which indicates that Ag and Ga have been doped into ZnSe nanowires in our experiments. / We are among the first group to grow vertically well-aligned ZnSSe alloy nanowires of controllable composition. Most of ZnSSe nanowires were found to have a cubic structure. We also found a compositional relationship between the nanowires and precursors, which is useful for predicting the lattice constant and band-gap emission energy of ZnSSe nanowires. / ZnS nanowire arrays were fabricated on the GaAs (100), (110) (311)A and (111)B substrates by metal organic chemical vapor deposition (MOCVD) using Ag, Au and Ga particles as catalysts. Their orientation was adjusted by changing the crystallographic orientation of the substrate. Moreover, Ga was doped into ZnS nanowires, when Ga nanoparticles serve as catalysts. / Liang, Yao = ZnS和ZnSSe納米結構的生長和光學性質 / 梁瑤. / Adviser: Hank Suikong. / Source: Dissertation Abstracts International, Volume: 72-11, Section: B, page: . / Thesis (Ph.D.)--Chinese University of Hong Kong, 2009. / Includes bibliographical references. / Electronic reproduction. Hong Kong : Chinese University of Hong Kong, [2012] System requirements: Adobe Acrobat Reader. Available via World Wide Web. / Electronic reproduction. [Ann Arbor, MI] : ProQuest Information and Learning, [201-] System requirements: Adobe Acrobat Reader. Available via World Wide Web. / Abstract also in Chinese. / Liang, Yao = ZnS he ZnSSe na mi jie gou de sheng chang he guang xue xing zhi / Liang Yao.
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OPTICAL PROPERTIES OF CHEMICAL VAPOR DEPOSITED BLACK MOLYBDENUM THIN FILMS.CHAIN, ELIZABETH ELLEN. January 1983 (has links)
This dissertation reports on the study of black molybdenum, a new cermet consisting of small Mo particles embedded in MoO₂. As with most two-phase materials, the optical properties of black molybdenum are significantly different from those of either constituent, and can be adjusted within wide limits through modifications of composition and microstructure due to variations of the fabrication process parameters. The subject of this work is to understand the exact relationships, to allow reproducible production of films with chosen optical properties. Theoretical interpretation of the optical properties of two-phase materials has in the past been hampered by insufficient microstructural characterization. Recent theoretical work by others has lifted the requirements of detailed microstructural knowledge, leaving only two required parameters for characterization of cermet reflectance: the optical properties of the constituent phases and their volume fractions in the cermet. Better characterization is obtained when structural considerations, such as film topology, surface texture and the presence of a possible amorphous phase, are taken into account. We adopted this approach to the study of black molybdenum, and accomplished satisfactory agreement between theoretical and observed reflectances. Black molybdenum films were prepared using two separate chemical vapor deposition (CVD) techniques, involving deposition from either Mo(CO)₆ or MoO₂Cl₂. We found the influence of composition through a comparison of films with different Mo:MoO₂ ratios, while the influence of structure on film reflectance was determined by comparing films from these two deposition techniques. During this investigation we produced black molybdenum films which display a spectrally selective profile--low visible reflectance combined with high infrared reflectance, and which may be applied to photothermal solar energy conversion. The versatility of CVD in adjusting film composition and structure resulted in another film of interest in photothermal conversion--black tungsten, a tungsten-tungsten oxide composite material. The black molybdenum and black tungsten systems studied here establish the utility of CVD for the production of high temperature thin film optical devices.
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Excitonic optical nonlinearities in semiconductors and semiconductor microstructures.Park, Seung-Han. January 1988 (has links)
This dissertation describes the study of excitonic optical nonlinearities in semiconductors and semiconductor microstructures. The main emphasis is placed on the evolution of optical nonlinearities as one goes from bulk to quantum-confined structures. Included are experimental studies of molecular-beam-epitaxially-grown bulk GaAs and ZnSe, GaAs/AlGaAs multiple-Quantum-Wells (MQW's), and finally, quantum-confined CdSe-doped glasses. The microscopic origins and magnitudes of the optical nonlinearities of bulk GaAs and ZnSe were investigated and the exciton recovery time in ZnSe was measured. A comparison with a plasma theory indicates that in GaAs, band filling and screening of the continuum-state Coulomb enhancement are the most efficient mechanisms, while in ZnSe, exciton screening and broadening are the dominating mechanism for the nonlinearity. The maximum nonlinear index per excited electron-hole pair of ZnSe at room temperature is comparable to that of bulk GaAs and the exciton recovery times are of the order of 100 ps or less. A systematic study of the dependence of the optical nonlinearities on quantum well thickness for GaAs/AlGaAs MQWs and the results of nonlinear optical switching and gain in a 58 A GaAs/AlGaAs MQW are reported and discussed. The maximum change in the refractive index is greatest for the MQWs with the smallest well size and decreases with increasing well size, reaching a minimum for bulk GaAs. The maximum index change per photoexcited carrier increases by a factor of 3 as the well size decreases from bulk to 76 A MQW. A differential energy gain of 0.2 and the contrast of 4 are measured for a 58 MQW using 3 ns laser pulses. The linear and nonlinear optical properties of CdSe semiconductor microcrystallites grown under different heat treatments in borosilicate glasses are investigated. Pump-probe spectroscopic techniques and interferometric techniques were employed to study size quantization effects in these microcrystallites (quantum dots). Nonlinear optical properties due to the transitions between quantum confined electron and hole states are reported for low temperature and room temperature. A relatively large homogeneous linewidth is observed. Single beam saturation experiments for quantum confined samples were performed to study the optical nonlinearities as a function of microcrystallite size. Results indicate that the saturation intensity is larger for smaller size quantum dots.
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Structural inhomogeneity and anisotropy in optical filters and thin films; applications to optical storage media.Balasubramanian, Kunjithapatham. January 1988 (has links)
Optical filters and thin film optical devices play an important role in Science and Industry. Several significant applications have emerged in optics, microelectronics and computer technology. In this work, we study some aspects of their design and applications. One class of optical fibers, known as Christiansen filters, are based on scattering phenomena in suspensions of solid particles in a liquid medium. Some new scattering filters in the visible and the near UV regions and their performance characteristics are reported here. Feasibility to fabricate such optical filters in solid matrix form is established. Some applications of these scattering filters are discussed. After an introduction to the optics of homogeneous and isotropic thin films, I discuss the general design of anisotropic thin film media and a scheme implemented to calculate their performance. Optical anisotropy, produced by the growth-induced columnar microstructure in thin films and its effects on the performance of optical filters are studied. Large shifts in the peak wavelength of a typical narrow band filter are predicted. Magneto-optical (MO) thin film media of great importance to erasable optical data storage technology are studied. An approximate technique based on a 2 x 2 matrix formalism is developed to calculate the normal incidence performance of these media. To investigate anisotropic effects, to incorporate more than one magnetic film with arbitrary orientations of magnetization, and to study oblique incidence performance, a completely general 4 x 4 matrix technique is implemented in a computer program. Effects of substrate/superstrate birefringence in the read-out signal of MO media are investigated. Several optimizing design criteria, particularly, the effectiveness in employing appropriate metal or dielectric reflector layers are studied. The influence of the plasma edge of metals in enhancing the polar Kerr rotation of MO media is discussed with illustrations. A contour plot of the Kerr rotation and reflectance is developed to help in the design of these media. An explanation is given for the observation of Kerr rotation enhancement near the plasma reflection edge of the reflector layer adjacent to the active MO layer and in general, where the reflectance spectrum shows a steep gradient.
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Optical properties and mechanical stress in cubic boron nitride and diamondErasmus, Rudolph Marthinus 19 March 2013 (has links)
A thesis submitted to the Faculty of Science, University of the Witwatersrand,
Johannesburg, in fulfilment of the requirements for the degree of Doctor of
Philosophy / Raman and photoluminescence (PL) spectroscopy techniques were used to investigate the
mechanical properties of diamond and cubic boron nitride (cBN) by optical means. Both these
materials have extreme mechanical properties that make them the material of choice for many
industrial applications, ranging from cutting and grinding to wire-drawing dies. The results
obtained on single crystal diamond, polycrystalline diamond (PCD) and cBN are summarised
below.
Micro-Raman and photoluminescence (PL) spectroscopy were used to map the threedimensional
(3D) stress and deformation distributions surrounding a plastic impression made in a
synthetic, type Ib single crystal diamond. Using data from the Raman peak position, a 3D map of
the stress contours surrounding the impression was generated, while the Raman width data
yielded a map of the plastic deformation volume. The stress contours compare favorably with the
resolved shear stress contours calculated for diamond. PL intensity maps of the zero phonon line
(ZPL) associated with the [N-V]– defect centre at 1.945eV provide images of the extent of
vacancy formation and movement during the impression process. Data concerning the position
and width of the ZPL correspond well with the Raman results.
Polycrystalline diamond (PCD) tools commonly consist of a PCD layer sintered onto a
cobalt-tungsten carbide (Co-WC) substrate. These tools are used in diverse applications and both
the magnitude and distribution of the stresses in the PCD layer affect tool behavior. These
stresses in sample drillbits were investigated by means of micro-Raman spectroscopy. Cyclic
annealing of a sample drillbit to 600 oC shows that the tool properties are retained after 5 cycles,
while similar cycling to 800 oC resulted in a permanent decrease of the average surface
compressive stress. This implies a reduction in the drillbit’s ability to resist crack formation and
propagation and is thus a degradation of the tool properties.
The method of Raman mapping of stress and deformation in diamond was also applied to
single crystals of cBN. Indentations on cubic boron nitride (cBN) crystals and polycrystalline
cubic boron nitride (PcBN) composites were mapped and the shifts of the cBN Raman lines from
their unstressed positions used to quantify the residual stresses in the boron nitride due to the
deformation brought about by the indentation. These were found to be of the order of 1 GPa.
vi
These measurements illustrated for the first time the use of Raman spectroscopy to study residual
stresses in boron nitride.
Defects in cBN were studied using photoluminescence spectroscopy at low temperature
(< 10 K) of two types of cBN irradiated at ambient temperature with 1.9 MeV electrons. All the
samples were small (<1 mm diameter) single crystals of cBN. Three defect centres (with narrow
lines at 2.28 eV, 2.15 eV and 1.98 eV) were introduced in both the amber-coloured and blackbrown
coloured samples by the irradiation. The amber coloured sample also showed a defect
centre (at 1.65 eV) that is present before and after irradiation. Line shape analysis of the zero
phonon lines of all three irradiation-induced centres showed that the lines are predominantly
Gaussian in character, suggesting that linetype defects such as dislocations are a prevalent
characteristic of these crystals.
Raman spectroscopy of cBN single crystals as a function of temperature was performed
over a wide temperature range from 4 K to 1373 K. The low temperature measurements extended
the data previously reported in literature, as this data ranged from room temperature upwards. It
was concluded from the shift of Raman peak position with temperature that both linear expansion
and anharmonic effects were required to adequately account for the observed data. This is in
agreement with previously published findings. Both 3- and 4-phonon processes were required to
account for the observed linewidths as a function of temperature, again in agreement with
literature.
The results presented here and in the associated journal publications illustrate clearly
how optical spectroscopy techniques can serve as non-destructive characterisation tools for the
mechanical properties of ultra-hard materials.
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Dependence of surface plasmon polaritons on the geometry of periodic metallic nanostructures and Its application on biosensing. / 表面等離子體激元對於週期性金屬納米結構幾何形狀的依賴性及其在生物傳感中的應用 / CUHK electronic theses & dissertations collection / Dependence of surface plasmon polaritons on the geometry of periodic metallic nanostructures and Its application on biosensing. / Biao mian deng li zi ti ji yuan dui yu zhou qi xing jin shu na mi jie gou ji he xing zhuang de yi lai xing ji qi zai sheng wu chuan gan zhong de ying yongJanuary 2012 (has links)
由於表面等離子體激元可以將電磁場限制在金屬表面,從而產生強烈的場強增強效果,因此在納米光子學和生物光子學方面具有廣泛的應用價值,其中包括高性能發光二級管、光伏電池、超高分辨率光學成像和超靈敏分子檢測等。尤其在單分子和醫學診斷方面,基於表面等離子體共振的生物傳感器獲得了越來越多的青睞。本論文包括兩部份。第一部份著重討論二維週期性洞陣列的表面等離子體特性,而第二部份則是研究這種洞陣列結構在表面等離子體共振傳感方面的應用。 / 在第一部份中,表面等離子體模式被分為非簡並模式(m,O) 和簡並模式(m,±n)兩種情況分別加以討論。首先,結合實驗結果和理論模型,我們對非簡並模式的衰減壽命和激發效率進行了研究。通過光干涉光刻法和薄膜沉積技術,一系列不同幾何結構的洞陣列樣品被製備出來,且這些樣品具有很高的重複性。利用角分辨色散關係進行模式識別以及確定這些模式的衰減壽命和激發效率。通過調整起偏器和檢偏器的相對方向,表面等離子體模式的非輻射和輻射衰竭均可加以研究。結果發現,衰減壽命強烈依賴於單洞的幾何結構,而且這種行為可以用簡單的靜電模型并考慮高階修正加以解釋。從非輻射衰減和輻射衰減平衡的角度出發,激發效率對幾何結構和共振波長的依賴性也可以理解。對於簡并模式,由於存在稱合,對稱模式和反對稱模式分別被p 偏振激發和S偏振激發。它們的對稱性和對於衰減壽命和共振波長的修正可以用干涉法和模式耦合理論來理解。最後,利用多模耦合方程,我們對色散關係圖譜隨著洞深度增加而演化的情況也進行了探討。 / 第二部份對基於表面等離子體共振的生物傳感器與陣列幾何結構的關係進行了研究。結果發現,激發效率和衰減壽命對表面等離子體共振傳感器的分辨率都起到了關鍵性作用。在共振中,峰值高度和帶寬主要由表面等離子體的衰減速率控制。較低的衰減速率導致較清晰的峰值線型,從而產生較高的傳感器分辨率。因此,通過調整陣列的幾何結構以產生非常低得輻射衰減速率,表面等離于體共振傳感器的品質因數可高達104.8/RIU ,這已經超過了基於梭鏡和納米粒子對應器件的性能表現。 / Surface plasmon polaritons (SPPs) generate a strong localized electromagnetic field on metal surface and thus are promising for nano- and bio-photonics including high performing light-emitting diodes and photovoltaic cells, super-high resolution optical imaging, ultra-high sensitive bimolecular detection, etc. In particular, the application of SPPs on surface plasmon resonance (SPR) biosensor has drawn much more attention recently because of the attempt to realize single molecule detection in medical diagnosis. / This thesis contains two parts. The first part focuses on studying the basic plasmonic properties of two-dimensional periodic hole arrays while the second part concentrates on the application of hole arrays on SPR sensing. / In the first part, SPPs modes on hole arrays are classified into nondegenerate mode (m, 0) and degenerate mode (m, ±n). For nondegenerate mode, its decay lifetime and generation efficiency are studied both experimentally and theoretically. By combining interference lithography and thin film deposition, a set of arrays with a wide range of geometry has been fabricated with high reproducibility. The dispersion relations of arrays are studied by angle-dependent reflectivity for mode identification and detenninations of SPP decay lifetime and generation efficiency. In particular, through orienting the polarization of the specular reflection either parallel or orthogonal to that of the incidence, we can access both the nonradiative and radiative decays of SPPs at different resonance wavelengths. As a result, it is found that decay lifetime is strongly dependent on the geometry of single hole and its behaviors can be understood by using a simple quasi-static model taking into account of the higher order correction as well as numerical simulation deduced by finite-difference timedomain. The dependence of generation efficiency on hole geometry or resonance wavelength can be understood in tenns of trade-off between nonradiative and radiative decay rates. Once these two decay rates equals to each other, the optimum generation efficiency is realized and the field enhancement gets the maximum. And the optimum parameters can be achieved by adjusting the hole geometry or the resonance wavelength. For degenerate mode, due to the coupling between (m, +n) and (m, -n) modes, a symmetric and an anti-symmetric modes are excited under pand s-polarized excitation, respectively. Their symmetries and modifications to the decay lifetime and resonance wavelength can be understood by using the interference method and coupled mode theory. Finally, generalized coupled mode equations are employed to know about the evolution of dispersion relation as hole depth increases. / The dependence of SPR biosensor on the generation and decay of SPPs are studied in the second part. Both the generation efficiency and decay lifetime of SPPs are found to be critical in governing the resolution of SPR biosensor. In SPR, the peak height and linewidth are primarily controlled by the decay rate of SPPs. Lower decay rate leads to sharper peak profile, which results in higher SPR resolution. Therefore, by tailoring the geometry of hole arrays to achieve a very low radiative decay rate, a SPR biosensor with figure of merit (FOM) reaching l04.8/RIU can be realized, which surpasses those of prism and nanoparticle counterparts. / Detailed summary in vernacular field only. / Detailed summary in vernacular field only. / Detailed summary in vernacular field only. / Zhang, Lei = 表面等離子體激元對於週期性金屬納米結構幾何形狀的依賴性及其在生物傳感中的應用 / 張磊. / "November 2011." / Thesis (Ph.D.)--Chinese University of Hong Kong, 2012. / Includes bibliographical references (leaves 116-125). / Electronic reproduction. Hong Kong : Chinese University of Hong Kong, [2012] System requirements: Adobe Acrobat Reader. Available via World Wide Web. / Abstract also in Chinese. / Zhang, Lei = Biao mian deng li zi ti ji yuan dui yu zhou qi xing jin shu na mi jie gou ji he xing zhuang de yi lai xing ji qi zai sheng wu chuan gan zhong de ying yong / Zhang Lei. / Chapter Chapter1 --- Introduction --- p.1 / Chapter Chapter2 --- Theoretical Background --- p.7 / Chapter 2.1 --- Maxwell's equations --- p.7 / Chapter 2.2 --- Classic electromagnetic theory for dielectric properties of matter --- p.9 / Chapter 2.3 --- Surface plasmon polaritons at the dielectric/metal interface --- p.11 / Chapter 2.4 --- Excitation of surface plasmon polaritons --- p.16 / Chapter 2.4.1 --- Prism coupling --- p.17 / Chapter 2.4.2 --- Grating coupling --- p.17 / Chapter 2.5 --- lones calculus --- p.19 / Chapter 2.6 --- Finite-difference time-domain method --- p.22 / Chapter Chapter 3 --- Sample Preparation --- p.25 / Chapter 3.1 --- Interference lithography --- p.25 / Chapter 3.1.1 --- Substrate preparation --- p.26 / Chapter 3.1.2 --- Exposure --- p.27 / Chapter 3.1.3 --- Pattern development --- p.30 / Chapter 3.2 --- Thin film deposition --- p.30 / Chapter Chapter 4 --- Experimental Setups and Calibration --- p.33 / Chapter 4.1 --- Experimental setup for measuring dispersion relation --- p.33 / Chapter 4.2 --- Experimental setup calibration --- p.35 / Chapter 4.2.1 --- Calibration of spectrometer --- p.36 / Chapter 4.2.2 --- Calibration of movement stages --- p.38 / Chapter 4.3 --- Data presentation for dispersion relation --- p.40 / Chapter 4.4 --- Summary --- p.41 / Chapter Chapter 5 --- Understanding of Fundamental Properties of SPPs --- p.43 / Chapter 5.1 --- Excitation of SPPs on 2D hole arrays --- p.44 / Chapter 5.2 --- Properties of non degenerate modes and theoretical explanation --- p.53 / Chapter 5.2.1 --- Dependence of lifetime on hole geometry and theoretical explanation --- p.55 / Chapter 5.2.2 --- Dependence of generation efficiency on hole geometry and theoretical explanation --- p.63 / Chapter 5.3 --- Properties of degenerate modes and theoretical explanation --- p.70 / Chapter 5.3.1 --- Dependence of properties of degeneration modes on hole geometry by FDTD --- p.72 / Chapter 5.3.1.1 --- (0, ±l)[subscript s,a] modes --- p.72 / Chapter 5.3.l.2 --- (-1, ±l)[subscript s,a] modes --- p.76 / Chapter 5.3.2 --- Understanding of excitation of degenerate modes by using interference method --- p.79 / Chapter 5.3.3 --- Understanding of coupling between degenerate modes by using coupled mode theory --- p.85 / Chapter 5.4 --- Evolution of dispersion relation as hole depth increases --- p.90 / Chapter 5.5 --- Summary --- p.95 / Chapter Chapter 6 --- Surface Plasmon Resonance Based Label Free Biosensor --- p.98 / Chapter 6.1 --- Basics of surface plasmon resonance (SPR) based biosensor --- p.98 / Chapter 6.2 --- State-of-the-art SPR biosensor --- p.101 / Chapter 6.3 --- SPR biosensor by using 2D metallic hole arrays --- p.102 / Chapter 6.4 --- Summary --- p.111 / Chapter Chapter 7 --- Conclusions --- p.112 / References --- p.116 / Publications --- p.126
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Optical properties of metal oxide capped ZnO induced by e-beam irradiation. / 由電子束照射引起氧化金屬膜覆蓋的氧化鋅之光學特性 / Optical properties of metal oxide capped ZnO induced by e-beam irradiation. / You dian zi shu zhao she yin qi yang hua jin shu mo fu gai de yang hua xin zhi guang xue te xingJanuary 2004 (has links)
by Hui Koon-chung = 由電子束照射引起氧化金屬膜覆蓋的氧化鋅之光學特性 / 許冠中. / Thesis (M.Phil.)--Chinese University of Hong Kong, 2004. / Includes bibliographical references (leaves 87-89). / Text in English; abstracts in English and Chinese. / by Hui Koon-chung = You dian zi shu zhao she yin qi yang hua jin shu mo fu gai de yang hua xin zhi guang xue te xing / Xu Guanzhong. / ABSTRACT --- p.i / ACKNOWLEDGMENTS --- p.iii / TABLE OF CONTENTS --- p.iv / LIST OF FIGURES --- p.vi / LIST OF TABLES --- p.x / Chapter 1. --- Introduction --- p.1 / Chapter 1.1 --- Motivation --- p.1 / Chapter 1.2 --- Overview of ZnO / Chapter 1.3 --- Overview of the Thesis / Chapter 2. --- Experimental conditions and procedures --- p.11 / Chapter 2.1 --- Samples preparation / Chapter 2.2 --- Optical and electrical Characterizations of ZnO / Chapter 2.2.1 --- Setup of cathodoluminescence (CL) spectroscopy / Chapter 2.2.2 --- Setup of photoluminescence (PL) spectroscopy / Chapter 2.2.3 --- Setup of photoconductivity measurement / Chapter 2.2.4 --- Setup of atomic force microscopy AFM / Chapter 2.2.5 --- X-ray photoelectron spectroscopy (XPS) / Chapter 3. --- Experimental results and data analysis --- p.21 / Chapter 3.1 --- The luminescence of ZnO --- p.21 / Chapter 3.2 --- Effects of metal capped layer in luminescence --- p.24 / Chapter 3.3 --- Optical memory effect of A1 capped ZnO --- p.28 / Chapter 3.4 --- The XPS study ofAl capped ZnO --- p.33 / Chapter 3.5 --- Optical properties and photoconductivity studies of AlOx-capped ZnO --- p.35 / Chapter 3.6 --- Time- and Electron-dose dependent CL of AlOx capped ZnO --- p.41 / Chapter 3.7 --- Dependence of band-edge enhancement on Deep Level to band-edge emission ratio --- p.53 / Chapter 3.8 --- Temperature-dependent CL of AlOx capped ZnO --- p.56 / Chapter 3.9 --- Electrical measurement of luminescence enhanced ZnO --- p.64 / Chapter 4. --- Discussion --- p.69 / Chapter 4.1 --- General discussion --- p.69 / Chapter 4.2 --- The effect of AlOx capping on the optical properties of ZnO --- p.70 / Chapter 4.3 --- The action of e-beam irradiation on the enhancement of band-edge emission --- p.73 / Chapter 4.4 --- The function of AlOx layer when under electron irradiation --- p.83 / Chapter 5. --- Conclusions --- p.85 / Reference --- p.87
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Optical sensing and trapping based on localized surface plasmons.January 2013 (has links)
基於表面等離子體的納米器件已經在近幾十年引起了十分廣泛的興趣因為其對於半波長光子器件,光學傳感,光譜學以及光學捕獲有著廣大的應用前景。表面等離子體是一種被限定於金屬和介質介面上的一種光子-電子混合模式,而且它具有許多吸引人的特質,比如對金屬表面周圍環境極其敏感,納米尺度範圍的光學電磁場局域和場增強,以及對鄰近物體極強的場強梯度捕獲力。雖然這些特性都已經分別被廣泛的研究過,但從光學捕獲的角度去實現光學傳感的方案並還沒有引起大量的關注。很明顯,在納米尺度範圍內操縱目標的可能性將使得新的納米器件具有高的光學探測性能和多功能性。為了涉及這個論題,本項目包括新穎的等離子體納米器件的研究,這些納米器件將能夠提供獨特的功能,在光學傳感,表面增強拉曼散射,以及光學捕獲方面。 / 在第一部分設計中,構建了一種基於雙層金屬納米條陣列的耦合系統。這樣的系統具有簡單的結構,易於加工和集成於微流系統的優點。由於這個系統內的光場耦合,場強可以進一步的被加強,這樣的特點有助於提高系統的敏感特性,尤其是通過強的光場來捕獲一些金屬的納米顆粒後。這個系統的光學共振條件可以從理論上進行模式分析得到。然後二維時域有限差分法證實了理論的分析而且進一步證明了利用該系統於光學傳感和捕獲的可能性。結果表明此系統的光學敏感度約為200nm/RIU,通過光學捕獲的金屬納米顆粒引起的近場調製和場增強可以使得表面增強拉曼散射的增強因數達到10⁹ 到10¹° 的高度。 / 在第二部分的設計裡,金納米環結構被證實了可以成為一個強大的工具作為表面等離子體納米光鑷來抓獲金屬納米顆粒。首先,金屬納米環具有很多優點比如對入射光的偏振不敏感,很寬的可調的共振範圍,有環的內腔周圍和內部有著均勻的光學場增強,以及很容易製備。這裡的設計著重于納米環在入射波長為785nm 的新穎的光學捕獲特性以及表面增強拉曼散射的性能。三維的時域有限差分法被用來計算結構的光學回應,以及麥克斯韋應力張量法被用來計算光學受力分佈情況。計算結果表明對於一個有20nm 大小的金納米顆粒球,納米環結構有最大的光學捕獲勢阱約32 KgT 。由於納米環結構周圍存在多個捕獲勢阱,使得其對目標捕獲顆粒具有約10⁶nm³ 的非常之大的有效體積。而且,被捕獲的顆粒會進一步的導致一些納米間隙的形成,這些納米間隙又會使得近場增強達到約160 倍的高度,這使得在實際應用中10⁸ 的表面增強拉曼散射的增強因數成為可能。 / 在第三部分的設計裡,全光納米操縱的概念被提出並證實,因為這樣的概念拓展了等離子體光鑷的一個極其重要的功能,那就是被捕獲的分子可以在捕獲和區域內被任意的操縱和轉移,而且這個區域是納米尺度的。設計的系統由梯度形金屬納米盤組成,這些納米盤具有不同的直徑,這使得它們支援不同波長的表面等離子體共振。通過改變入射光的波長和旋轉入射光的偏振態,就可以將捕獲的目標從一個納米盤轉移到另一個納米盤。三維的時域有限差分法和麥克斯韋應力張量法被用來證實了所提出的觀點。計算結果表明被捕獲的目標感受到的捕獲勢阱深度高達5000kgT/W/μm²,最大的光學轉矩約為336pN·nm/W/μm²,而且總的有效捕獲體積可達到10⁶nm³ 。在這部分的結尾,討論了所設計的系統在光學傳感方面潛在的應用前景。 / 在最後的部分裡,展示了一個實驗的證明來說明等離子體納米光鑷對目標捕獲的觀測問題,因為這樣的觀測對往後近期的相關實驗來說是首先要關心的問題。雖然兩種途徑已經在別處被證實了,分別是通過觀測系統的透射光的強度變化和系統共振波長的改變,來監測表面等離子體納米光鑷近場捕獲行為的發生,但是在這個部分裡,等離子體納米光鑷和表面增強拉曼傳感技術被結合在了一起並且被證實了這是另一種有效的方法用於觀測捕獲行為的發生。在本實驗中兩束鐳射光束被為別用來激發等離子體納米光鑷和表面增強拉曼信號,一束是633nm 的鐳射,另一束是785nm 的鐳射。表面等離子體納米光鑷簡單地由熱蒸鍍並熱退光的金顆粒納米島墊底構成,這個墊底的共振峰被調製到緊靠633nm 的位置。目標顆粒是由光化學生長合成的銀納米十面體,這些十面體被綁定了4-巰基苯甲酸分子的單分子層,且具有遠離633nm 和785nm 的共振峰。由於當等離子體納米光鑷被激勵的時候目標顆粒會被捕獲到近場的熱點內,這時近場的光場就會被極大的增強,所以表面增強拉曼的信號就會出現。這個過程也被用數值模擬的方法(三維時域有限差分法和麥克斯韋應力張量法)闡明了。更進一步的,當等離子體納米光鑷不被激勵的時候,被捕獲的目標顆粒可以被釋放掉,那樣表面增強拉曼的信號就會消失掉。所以,本設計不僅提供了一種強有力的探測等離子體光鑷捕獲行為的方法,而且能夠成為一種在生物探測方面可重複利用的“捕獲并傳感“的平臺。 / Surface plasmons (SPs) based nanodevices have attracted much research interest in recent decades due to their powerful application potentials for subwavelength optical circuits, optical sensing, spectroscopy, and optical trapping. SPs are the hybrid photon-electron modes bound at the interface of conductors and transparent materials, and they have lots of attractive properties such as sensitive to the changes of environment around the interface, strong optical field localization and enhancement in nanoscale domain, and strong field intensity gradient forces to trap the adjacent objects. Even though these properties have been widely investigated, their application in optical sensing based on the plasmonic optical trapping strategy remains largely unexplored. Clearly, the possibility of manipulating objects within the nanometer regime will enable new nanodevices that offer high optical detection performance and multiple-functionality. With the aim to address this issue, this project involves the study of novel plasmonic nanodevices that provide unique functionality in optical sensing, surface-enhanced Raman scattering (SERS), and optical trapping. / The first design is based on a coupling system involving double-layered metal nano-strips arrays. This system has the advantages of simple geometry and direct integration with microfluidic chips. The intense optical localization due to field coupling within the system can enhance detection sensitivity of target molecules, especially by virtue of the optical trapping of plasmonic nanoparticles. The optical resonant condition is obtained theoretically through analyzing the SPs modes. Numerical modeling based on two-dimensional (2D) finite-difference time-domain (FDTD) is consistent with the theoretical analysis and demonstrates the feasibility of using this system for optical sensing and trapping. Simulation results show that the refractive index sensitivity can reach ~200 nm/RIU, and a maximum SERS enhancement factor (EF) of 10⁹-10¹° is possible because of the near-field modulation and enhancement from optically trapped metal nanoparticles. / In the second design, a gold nano-ring structure is demonstrated to be an effective approach for plasmonic nano-optical tweezers (PNOTs) for trapping metallic nanoparticles. The plasmonic nano-ring structure has many interesting merits such as polarization insensitivity, wide tunable resonance range, uniform field enhancement around and inside the ring cavity, and ease of fabrication. This design has a unique feature of having large active volume for trapping. In our demonstration example, we have optimized a device for SERS operation at the wavelength of 785 nm. Three-dimensional (3D) FDTD techniques have been employed to calculate the optical response, and the optical force distribution have been derived using the Maxwell stress tensor (MST) method. Simulation results indicate that the nano-ring produces a maximum trapping potential well of ~32 kgT on a 20 nm gold nanoparticle. The existence of multiple potential well results in a very large active trapping volume of ~10⁶ nm³ for the target particles. Furthermore, the trapped gold nanoparticles further lead to the formation of nano-gaps that offer a near-field enhancement of ~160 times, resulting in an achievable EF of 10⁸ for SERS. / In the third design, we propose a concept of all-optical nano-manipulation. We show that target molecules, after being trapped, can be transferred between the trapping sites within a linear array of PNOTs. The system consists of an array of graded plasmonic nano-disks (NDs) with individual elements coded with different resonant wavelengths according to their dimensions. Thus, by switching the wavelength and rotating the polarization of the excitation source, the target nanoparticles trapped by the device can be manipulated from one ND to another. 3D FDTD simulation and MST calculation are utilized to demonstrate the operation of this idea. Our results reveal that the target experiences a trapping potential strength as high as 5000 kgT/W/μm², maximum optical torque of ~336 pN·nm/W/μm², and the total active volume may reach ~10⁶ nm³. The potential applications in terms of optical sensing are also discussed. / In the final design, for which experimental demonstration has been conducted, we show that PNOTs are achievable with random plasmonic nano-islands. Operation of the random PNOTs can be monitored by measuring the SERS enhancement factor in real time. Two laser beams having wavelengths of 633 nm and 785 nm are utilized to stimulate the PNOTs and excite the Raman signals simultaneously. The PNOTs are formed by annealing of a thermal evaporated gold film. This so-called nano-island substrate (Au-NIS) has a resonant peak close to 633 nm. The target is photochemical synthesized silver nanodecadedrons (AgNDs) functionalized with 4-Mercaptobenzoic acid (4-MBA) and the resonant peak of these AgNDs is far away from 633 nm and 785 nm. As the target is trapped to the hot-spots when the PNOTs are active, the near-field intensity is enhanced significantly, which results in the emergence of SERS signals, i.e. confirming the expected outcome of SERS upon nanotrapping by the PNOTs. This process is also elucidated numerically through 3D FDTD simulation and MST calculation. Furthermore, the target can be released as the PNOTs become inactive, i.e. disappearance of the SERS signal. Therefore, this design offers not only a robust avenue for monitoring trapping events in PNOTs, but also a reproducible “trap-and-sense“ platform for bio-detection. / Detailed summary in vernacular field only. / Detailed summary in vernacular field only. / Detailed summary in vernacular field only. / Detailed summary in vernacular field only. / Detailed summary in vernacular field only. / Kang, Zhiwen. / Thesis (Ph.D.)--Chinese University of Hong Kong, 2013. / Includes bibliographical references (leaves 146-170). / Abstracts also in Chinese. / Abstract --- p.I / Acknowledgements --- p.VIII / List of Illustrations --- p.XIII / Chapter Chapter 1. --- Introduction --- p.1 / Chapter 1.1 --- Surface Plasmon Polaritons and Localized Surface Plasmons --- p.1 / Chapter 1.2 --- Relevant Applications Based on Surface Plasmons --- p.3 / Chapter 1.3 --- Plasmonic Nano-Optical Tweezers and Relevant Applications --- p.7 / Chapter 1.4 --- Literatures Review and Objectives of this Thesis --- p.12 / Chapter 1.5 --- Structure of this Thesis --- p.17 / Chapter Chapter 2. --- Research Methodologies --- p.20 / Chapter 2.1 --- Theoretical Background of Surface Plasmons --- p.20 / Chapter 2.2 --- Numerical Simulation Techniques for Studying Complex Nanostructures --- p.30 / Chapter 2.3 --- Optical Force Calculation with the Maxwell Stress Tensor Method --- p.38 / Chapter 2.4 --- Nanostructure Fabrication and Characterization --- p.40 / Chapter Chapter 3. --- Optical Sensing Based on Double-Layered Metal Nano-Strips --- p.43 / Chapter 3.1 --- Introduction --- p.43 / Chapter 3.2 --- Theoretical Model and Analysis --- p.46 / Chapter 3.3 --- Numerical Verification and Discussion --- p.50 / Chapter 3.4 --- Optical Sensing Evaluation --- p.54 / Chapter 3.5 --- Near-Field Modulation by Optically Trapped Metal Nanoparticles --- p.58 / Chapter 3.6 --- Discussion --- p.61 / Chapter 3.7 --- Conclusion --- p.62 / Chapter Chapter 4. --- Gold Nano-Ring as Plasmonic Nano-Optical Tweezer --- p.64 / Chapter 4.1 --- Introduction --- p.64 / Chapter 4.2 --- Design and Optical Response --- p.67 / Chapter 4.3 --- Optical Force Calculation and Evaluation of Trapping Performance --- p.73 / Chapter 4.4 --- Stable Trapping Sites and Active Trapping Volume --- p.76 / Chapter 4.5 --- Near-Field Variation and Discussion --- p.81 / Chapter 4.6 --- Conclusion --- p.84 / Chapter Chapter 5. --- Graded Plasmonic Nano-Disks for Near-Field Nano-Manipulation --- p.86 / Chapter 5.1 --- Introduction --- p.86 / Chapter 5.2 --- Modeling and Optical Response --- p.89 / Chapter 5.3 --- Optical Force Distribution in the Structure --- p.91 / Chapter 5.4 --- Optical Trapping Potential and Rotational Energy --- p.96 / Chapter 5.5 --- Optical Trapping Volume and Discussion --- p.101 / Chapter 5.6 --- Conclusion --- p.104 / Chapter Chapter 6. --- Monitoring Plasmonic Nano-Optical Trapping through Detection of Surface-Enhanced Raman Scattering --- p.106 / Chapter 6.1 --- Introduction --- p.106 / Chapter 6.2 --- Numerical Investigation --- p.110 / Chapter 6.3 --- Sample Preparation and Characterization --- p.112 / Chapter 6.4 --- Experimental Implementation and Results --- p.122 / Chapter 6.5 --- Discussion --- p.134 / Chapter 6.6 --- Conclusion --- p.137 / Chapter Chapter 7. --- Conclusion and Outlook --- p.139 / References --- p.146 / Publications from this Work --- p.171
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