Relevant bibliographies by topics / Evanescent field

Academic literature on the topic 'Evanescent field'

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Published: 4 June 2021
Last updated: 21 February 2023

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Journal articles on the topic "Evanescent field"

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CORTES, R., V. COELLO, P. SEGOVIA, C. GARCÍA, J. M. MERLO, and J. F. AGUILAR. "INTERFERENCE IN FAR-FIELD RADIATION OF EVANESCENT FIELDS." Surface Review and Letters 18, no. 06 (December 2011): 261–65. http://dx.doi.org/10.1142/s0218625x11014746.

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We investigate experimentally the interference in far-field radiation of two contra-propagating evanescent fields using a conventional optical microscope. A laser beam illuminates a glass-air interface under total internal reflection condition and through the proper setup a double evanescent illumination was produced. The evanescent fields radiate from the surface into the far-field domain due to small surface scatterers. Thus, coherent interference is produced in the far-field region which is correlated with the relative positions of the evanescent illumination sources. Finally, the above-described could be considered as a device for high accuracy micro-scale measurements as well as a direct visualization method of evanescent phenomena.
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Tortschanoff, Andreas, Marcus Baumgart, and Jaka Pribošek. "Modelling of Evanescent Field Scattering." Proceedings 56, no. 1 (December 14, 2020): 16. http://dx.doi.org/10.3390/proceedings2020056016.

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Evanescent field particle scattering is a promising method for single particle detection. In this study, we performed a detailed numerical analysis to show the possibilities and limitations of analytical models for predicting the capabilities of this sensing mechanism.
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Wang, Jinyu. "Cylindrical waveguide evanescent field ellipsometry." Optical Engineering 31, no. 7 (1992): 1432. http://dx.doi.org/10.1117/12.57699.

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Ter-Mikirtychev, Valerii V., Valery A. Kozlov, and Taiju Tsuboi. "Optical Waveguide Evanescent-Field Amplifiers." International Journal of Modern Physics B 12, no. 02 (January 20, 1998): 113–23. http://dx.doi.org/10.1142/s0217979298000089.

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We briefly describe the recent development of the optical evanescent-field amplifiers including the solid-state integrated-optic and fiber-optic devices. Application of these amplifiers to the optical communication systems is discussed.
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Oheim, Martin, and Florian Schapper. "Non-linear evanescent-field imaging." Journal of Physics D: Applied Physics 38, no. 10 (May 6, 2005): R185—R197. http://dx.doi.org/10.1088/0022-3727/38/10/r01.

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Hulst, N. F., N. P. Boer, and B. Bölger. "An evanescent-field optical microscope." Journal of Microscopy 163, no. 2 (August 1991): 117–30. http://dx.doi.org/10.1111/j.1365-2818.1991.tb03166.x.

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Xiao, Mufei. "Evanescent fields do contribute to the far field." Journal of Modern Optics 46, no. 4 (March 1999): 729–33. http://dx.doi.org/10.1080/09500349908231298.

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Chyad, Radhi M., Mohd Zubir Mat Jafri, and Kamarulazizi Ibrahim. "Nano-Optical Fiber Evanescent Field Sensors." Advanced Materials Research 626 (December 2012): 1027–32. http://dx.doi.org/10.4028/www.scientific.net/amr.626.1027.

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The nanofiber optic evanescent field sensor based on a changed cladding part as a sensor presented numerically. The influences of numerical opening, core radius of the fiber, the wavelength is effected on the light source and the submicron fiber on the sensors are promise to studied in this work. The results pointed out the sensitivity of the sensor increases when the numerical opening of the fiber is increases and the core radius is decreases. The NA of the fiber affects the sensitivity of the sensor. In the uniform core fiber, the increase in the NA increases the sensitivity of the sensor. Therefore, one should choose a fiber with high NA for the design of an evanescent-wave-absorption sensor if the core of the sensing segment uniform in diameter, so that the increase in the penetration depth or number of ray reflections or both, increases the evanescent absorption field and hence the sensitivity of the sensors. Keywords:fiber optic sensor, chemical sensors, biosensors, nanofiber optic.
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Colin, T. B., K. H. Yang, M. A. Arnold, Gary W. Small, and W. C. Stwalley. "The Effect of Length and Diameter on the Signal-to-Noise Ratio of Evanescent Field Absorption Fiber-Optic Sensors." Applied Spectroscopy 46, no. 7 (July 1992): 1129–33. http://dx.doi.org/10.1366/0003702924124240.

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This paper discusses the theoretical and experimental implications of changing the length and diameter of the evanescent field sensing region of an evanescent field sensor. Particular emphasis is placed on optimizing the intensity of the evanescent field for near-infrared sensor applications. Both theoretical and experimental results show that an optimal length and diameter must be determined experimentally for each analyte system.
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Lepeshov, S. I., and A. A. Bogdanov. "Bound states in the continuum-induced enhancement of evanescent field confinement." Journal of Physics: Conference Series 2015, no. 1 (November 1, 2021): 012083. http://dx.doi.org/10.1088/1742-6596/2015/1/012083.

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Abstract Here, the enhancement of electromagnetic field confinement in an all-dielectric metasurface is demonstrated. The enhanced confinement is achieved when the polarization singularity, corresponding to accidental bound states in the continuum, moves to the domain of evanescent fields (under the light line). Such a hybridization of the bound states and evanescent waves results in the 70-fold increase of the electric field enhancement on the top of the metasurface and boosting of the electric field localization.
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Dissertations / Theses on the topic "Evanescent field"

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Keating, Sarah Margaret. "Modelling of evanescent field immunosensors." Thesis, University College London (University of London), 2004. http://discovery.ucl.ac.uk/1446866/.

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Several factors affect the viability of biosensor design. This thesis presents the development of a computer-based model that will enable the sources and effects of noise and variations in concentrations within an evanescent field immunosensor to be analysed. The model was developed as a series of modules, each representing one aspect of the sensor, which when linked provide a simulation of the whole sensor. A complete solution of the complex biochemical reactions involved in the immunoassay module was achieved using a Markov chain approach. More traditional methods of solving sets of equations, such as optimisation, genetic algorithms and simulated annealing, all failed to produce satisfactory results. Two alternative assays, a sandwich and a competitive assay, are presented. The light module details the modelling of the coupling into a planar monomode waveguide and calculation of fluorescence excited by the resulting evanescent field using standard electromagnetic formulae. However, both beam divergence and scattering from the immobilised antibody layer were incorporated into the model. Two alternative coupling techniques were modelled, prism coupling and coupling through a "resonant mirror" multilayer. The detection system modelled the amplification of the fluorescence by a photomultiplier tube. The resulting model represents the most rigorous modelling undertaken in this area and the potential applications and benefits of such a model were detailed. Analysis of noise within the sensor allowed the impact of variation in the physical parameters defining the sensor to be determined and compared. The model was used to compare different protocols and confirmed that the sandwich assay produced the more sensitive device. A study of the kinetic response of the assay determined that measurements could be performed at half the time taken to reach equilibrium without significant loss of sensitivity. An analysis of the effect of scattering at the waveguide surface showed this to be significant noise factor. An initial study of the impact of the humectant layer illustrated that this is an issue that merits further consideration.
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Grossman, Michael. "Evanescent Field Absorption Sensing Using Sapphire Fibers." Scholar Commons, 2007. http://scholarcommons.usf.edu/etd/3814.

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This thesis explores the application of coiled sapphire multimode optical fibers for evanescent wave chemical sensing in both the visible spectrum and the near infrared. As has been suggested in the literature pertaining to silica fibers, bending converts low-order modes to high order ones, which leads to more evanescent absorption and thus a more sensitive chemical detector. By coiling the fiber many times, it was expected that even greater sensitivity would be attained. Experiments were performed to investigate the sensor response to different solutions and to characterize this response. In the first of three experiments, the large absorption peak of water at 3μm was examined in order to compare the sensitivity of a straight fiber versus a coiled one. In the second experiment, the effect of increasing the number of coils was investigated, as was the response of the sensor to varying concentrations of water in heavy water. In the third experiment, methylene blue dye was used to investigate the extent of adsorption of dye molecules on the sapphire fiber and its persistence
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Ismaeel, Rand. "Microfiber devices based on evanescent field coupling." Thesis, University of Southampton, 2015. https://eprints.soton.ac.uk/384514/.

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Microfiber (MF) devices are increasingly becoming attractive building blocks for numerous applications. This is attributed to a combinations of enabling properties including large evanescent field, compactness, low insertion loss and, most importantly, their configurability. This thesis describes the evanescent field coupling in MF devices in different forms and applications, such as microresonators for sensing, modal couplers for mode conversion and nonlinear frequency conversion. Micro-resonators are devices based on evanescent field coupling between turns of adjacent segments of the MF. Light inside these devices is confined within the resonator structure and trapped inside its cavity. Light, therefore, follows a longer path before passing to the output and this is wavelength dependent. A new type of resonator was successfully designed and manufactured: the multiport MF coil resonator. This structure has excellent features such as high extinction ratio, multiple resonance peaks and high stability. Novel modal couplers were also analysed and fabricated with high conversion efficiencies, high modal purity and low insertion loss. Modal couplers were manufactured to convert the launched input LP01 mode, into any of the higher order modes supported by the fiber. High conversion efficiencies were demonstrated for the LP11,LP21 and the LP02 modes. A MF coupler was successfully used for the detection of DNA by exploiting hybridisation on the surface of the MF coupler. The large evanescent field of the MF allows to detect the refractive index change that occurs when DNA attaches to the surface. Detection limits in the range of 10⁻⁶ per Refractive Index Unit (RIU) and sensitivities as high as 200nm=RIU were obtained. Nonlinearities were investigated both in straight MF and MF resonators, with particular stress on the second and third harmonic generation. While the conversion effciency remained relatively low for straight MFs, by using a loop resonator, the circulation of pump power (at resonance) inside the loop allowed for a conversion efficiency enhancement of 7.7 dB for the Third harmonic generation (THG) and 7.6 dB for the Second Harmonic Generation(SHG). Knot resonators were also used and provided larger enhancement of 14.2 dB for the SHG signal.
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Shah, Suhani Kiran. "Modeling scattered intensity from microspheres in evanescent field." Thesis, [College Station, Tex. : Texas A&M University, 2007. http://hdl.handle.net/1969.1/ETD-TAMU-2021.

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Delezoide, Camille. "Polymer microring resonators for optofluidic evanescent field sensors." Phd thesis, École normale supérieure de Cachan - ENS Cachan, 2012. http://tel.archives-ouvertes.fr/tel-00846193.

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Optofluidic evanescent field sensing, especially microresonator-based label-free biochemical sensing, is an emerging technology under intensive study. In this context, we demonstrate that polymeric microring resonators are excellent transducers. It is partly due to the simplicity and cost-efficiency of their fabrication and integration, and also to their robustness: a fast, repeatable and low-cost method was developed to fabricate devices with long lifetimes and state-of-the-art performances. A second advantage is the extreme sensitivity achievable to grafted molecules: a detectable signal was obtained with only a few hundreds of 5-TAMRA-cadaverine (5-TC) molecules, relatively small as compared to nucleic acids, antibodies and other biomolecules. The surface immobilization of 5-TC molecules was achieved after a simple and reproducible UV/ozone procedure for surface preparation. However, the qualities of polymer microring resonators only become apparent when coupled to high-precision instrumentation. In that respect, a measuring instrument was built to detect minute and real-time variations of the optical resonances, and thus in an optofluidic regime. The detection of absorption and desorption of 5-TC molecules on a surface functionalized with its antibody was achieved. However, truly specific responses of the instrument would only be achieved in a multiplexed configuration. Such configuration is achievable, but has yet to be developed. Meanwhile, the measuring instrument, as is, can be used for a wide variety of applications, from the measurement of dispersion coefficients to the study of local thermal effects.
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MacKenzie, Harry Straghan. "Evanescent-field devices for non-linear optical applications." Thesis, University of Cambridge, 1990. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.358807.

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McNab, Sharee J. "Evanescent near-field optical lithography : overcoming the diffraction limit." Thesis, University of Canterbury. Electrical and Electronic Engineering, 2001. http://hdl.handle.net/10092/6655.

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Concepts of optical resolution limits have been transformed in the past two decades with the development of near-field optical microscopy. Resolutions of λ/40 have been demonstrated by taking advantage of additional information present the near field of an object. These resolutions are far higher than what diffraction-limited lens-based optical systems are capable of. Attempts have been made to replicate these resolutions for lithography using a scanning probe based optical equivalent, but these systems suffer from low throughput owing to their serial nature. A desirable alternative would be replication of all the patterns within a field in a single flood exposure in a manner similar to how optical projection lithography replicates the field of a mask, but with the additional resolution available from working in the near field. This is the basis of evanescent near-field optical lithography, the subject of this thesis. Evanescent near-field optical lithography (ENFOL) brings traditional contact lithography into the near-near field using a combination of conformable masks and ultra-thin photoresists. This thesis describes a study of ENFOL both experimentally and via electromagnetic simulations to evaluate what the resolution limit might be. The fabrication of membrane masks is described, a key component for the ENFOL exposure. The characteristics of an ENFOL exposure using broad-band light are investigated from exposures into thick resist. These exposures demonstrate the trend of decreasing depth of field as the period of grating structures is reduced. ENFOL's requirement of a thin imaging photoresist for high resolution lithography complicates the pattern transfer step essential to translate the photoresist image into a useful material for devices. The development of an additive pattern transfer process is described, that utilises a trilayer resist scheme to enable lift-off metallisation. NiCr gratings with periods down to 270nm have been fabricated using this process subsequent to an ENFOL exposure. Wire-grid polarisers consisting of 270nm-period NiCr gratings on glass substrates have been fabricated and their polarisation properties measured at visible wavelengths. Simulation results of exposures of sub-wavelength grating structures are presented that investigate the fundamental limit to resolution for contact lithography techniques such as ENFOL. A full-vector, rigorous electromagnetic simulation technique, the multiple multipole program is used to provide information about the near field of subwavelength gratings. The potential for λ/20 resolution is indicated; a tantalising prospect for optical lithography and well below the diffraction limit of conventional optical projection-based lithographies. Perhaps the most critical parameter for an evanescent exposure, the depth of field, was characterised and a linear relationship shown between the depth of field and grating period. The effect of parameters such as grating duty cycle, absorber material and thickness on the exposure are observed with the intention to optimise the experimental setup. Interesting interference phenomena are observed in simulation results for exposures. where the effective exposure wavelength is equivalent to the grating period. In particular a period halving occurs in the transverse magnetic polarisation due to interference of the first diffracted orders. A novel interference technique - evanescent interference lithography is proposed that takes advantage of an enhanced period halving at an exposure wavelength corresponding to a grating resonance.
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Wong, Yuen Mei. "Optimising the plastic optical fibre evanescent field biofilm sensor." Thesis, Liverpool John Moores University, 2008. http://researchonline.ljmu.ac.uk/5906/.

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This thesis describes the development, characterisation and application of large diameter multimode plastic optical fibre (POF) sensors using evanescent field modulation. The exposed polymethylmethacrylate (PMMA) core of the POF fibre forms the sensor interface that detects refractive index changes of a measurand acting as the cladding. When a liquid measurand is used, the sensor can detect changes in refractive index, absorption and suspended particulates. It is this simple mechanism by which the evanescent field POF sensor operates. The evanescent field POF sensor has been characterised for refractive index of surrounding liquid from 1.33 to 1.49. The sensor demonstrated accuracy of ± 7x 10-3 refractive index units below 1.4 and ±2x 10-3 refractive index units above 1.4. Components have been selected and designed for this project to ruggedise the sensor, to make the sensor more self-contained and cheaper. The original design of the test conditions did not allow for optimum deployment of the sensor as it stripped out the very modes of light that were required for sensing purposes. The system was also operating under pressure, not reflecting the real conditions under which the sensor would be operating. The re-design of test conditions holds the sensor without straining the POF and operates under normal atmospheric pressure. The POF sensor was demonstrated reacting to a real measurand eg biofilm in which initial growth affects the optical properties at the core cladding interface by refractive index modulation. This sensor was capable of measuring biofouling and scaling at water interfaces. The sensor was trialled in a European Commission funded project (CLOOPT) to study biofouling and scaling in closed loop water systems such as heat exchangers in the cooling tower of an electric power plant, and as an interface sensor for water quality monitoring (AQUA-STEW) involving biofilm removal and surface cleansing with a new application for contact lens protein removal systems. Tapering multimode POF was a desirable goal as this increases the proportion of light coupled into the core available for sensing purposes, to achieve a more sensitive evanescent field POF sensor. Optically clear and consistent smooth tapering of ends and mid-lengths of POF fibre were achieved through chemical removal of material. The tapered POF sensor was characterised with a range of refractive indices, and it exhibited two distinct regions; the water/alcohol region below 1.4 refractive index units, and the oil region above 1.4 suggesting the sensor's use as an oil-in-water, or water-in-oil sensor. From 95% confidence limits, the accuracy of the POF was ±O.006 refractive index units (to 2 standard deviations) for fluids of refractive indices above 1.4. Tapered POF is sensitive to refractive index providing a cheap, easy to handle and rugged throwaway sensor for water and beverage process and quality monitoring.
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Ayachitula, Rajani. "Atom Optics Using an Optical Waveguide-Based Evanescent Field." The Ohio State University, 2010. http://rave.ohiolink.edu/etdc/view?acc_num=osu1276669685.

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Shan, Liye. "Stimulated Raman scattering in the evanescent field of nanofibers." Thesis, Paris 11, 2012. http://www.theses.fr/2012PA112421/document.

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Cette thèse porte sur les mélanges d’onde non linéaires qui peuvent avoir lieu dans le champ évanescent de nanofibres de silice. Nous nous sommes plus particulièrement intéressés à la diffusion Raman stimulée qui est obtenue par l’interaction du champ évanescent très intense et un liquide non linéaire dans lequel baigne la nanofibre. Afin de mettre en évidence la diffusion Raman stimulée« évanescente », nous avons développé un modèle de simulation non linéaire dont le but est de déterminer les caractéristiques des nanofibres à réaliser. Le gain Raman modal est calculé afin de trouver le rayon optimal des nanofibres pour chaque liquide ou mélange de liquides possible. En considérant la puissance critique et le seuil de dommage de nos nanofibres, nous avons déduit la longueur minimale d’interaction. Les conditions d’adiabacité des parties évasées menant à la nanofibre sont également discutées. Ces spécifications nous ont amenés à développer une plateforme de tirage de nanofibres spécifiquement dédiée à ces expériences de non-linéarités évanescentes. Cette palteforme nous permet de tirer des nanofibres de diamètre allant jusqu’à 200 nm sur des longueurs de 10 cm, avec plus de 90% de transmission. Avec ces nanofibres, nous avons mis en évidence le premier ordre Stokes de l’éthanol dans le champ évanescent d’une nanofibre, ainsi que les premier et second ordres Stokes du toluène. Ces premières expériences sont en très bon accord avec nos simulations et ouvrent la voie à de nombreuses expériences en optique non linéaire
The present PhD thesis explored nonlinear wave mixing with the strong evanescent field of nanofibers. The focus has been on the effect of stimulated Raman scattering which is activated by the interaction between such a strong evanescent field and the nonlinear liquid surrounding the nanofiber. In order to observe the stimulated Raman scattering, we investigated the nonlinear modeling to determine the needed characteristics of the nanofibers. The modal Raman gain was calculated to determine the optimal radius of nanofibers for each possible liquid. Considering the critical power and the damage threshold of our nanofibers, we found the minimum required interaction length. The condition of adiabacity of the tapers was also described. These specifications of nanofibers guide us towards the design of a proper pulling system. Several pulling systems and techniques are investigated for the fabrication of our specific nanofibers. We now are able to fabricate low loss uniform nanofibers of up to 10 cm long, a diameter down to 200 nm, with two identical low loss tapers by using our own designed translation stage pulling platform and implemented with the “variable heat brush” technique. With the achieved nanofibers, the Raman effect induced in the evanescent field was observed in both pure (ethanol) and binary mixture (toluene in ethanol) liquids. These first measurements are in good agreement with our simulation even without any fitting parameters in the modeling
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Books on the topic "Evanescent field"

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France, C. M. Evanescent field and surface plasmon polaritons in opticalsensors. Manchester: UMIST, 1994.

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Greffet, Jean-Jacques. Introduction to near-field optics and plasmonics. Oxford University Press, 2017. http://dx.doi.org/10.1093/oso/9780198768609.003.0002.

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A striking difference between near-field optics and far-field optics is the possibility of breaking the so-called diffraction limit, namely of confining light to subwavelength spots. The first section of this chapter introduces the concept of evanescent waves to discuss the subwavelength confinement of light. One of the key ideas put forward is that the presence of charges is required to generate highly localized fields. It is thus necessary to have a tool to compute fields in the presence of these charges. With this aim, the concept of the Green tensor is introduced in the second section. This is a powerful tool for computing electromagnetic fields in inhomogeneous environments. It is also a key quantity for discussing the local density of states and therefore controlling spontaneous emission. The final section is devoted to an introduction to surface plasmons, which are very useful for manipulating electromagnetic fields at the nanoscale.
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Book chapters on the topic "Evanescent field"

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Weik, Martin H. "evanescent field." In Computer Science and Communications Dictionary, 543. Boston, MA: Springer US, 2000. http://dx.doi.org/10.1007/1-4020-0613-6_6459.

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Weik, Martin H. "evanescent field coupling." In Computer Science and Communications Dictionary, 543. Boston, MA: Springer US, 2000. http://dx.doi.org/10.1007/1-4020-0613-6_6460.

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de Fornel, Frédärique. "Evanescent-Field Waveguide Sensors." In Springer Series in Optical Sciences, 113–29. Berlin, Heidelberg: Springer Berlin Heidelberg, 2001. http://dx.doi.org/10.1007/978-3-540-48913-9_6.

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Vigneron, J. P. "Theory of Evanescent and Radiative Fields." In Near Field Optics, 147–56. Dordrecht: Springer Netherlands, 1993. http://dx.doi.org/10.1007/978-94-011-1978-8_18.

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de Fornel, Frédärique. "Evanescent-Field Optical-Fiber Couplers." In Springer Series in Optical Sciences, 81–103. Berlin, Heidelberg: Springer Berlin Heidelberg, 2001. http://dx.doi.org/10.1007/978-3-540-48913-9_4.

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de Fornel, Frédärique. "Integrated-Optical Evanescent-Field Couplers." In Springer Series in Optical Sciences, 105–12. Berlin, Heidelberg: Springer Berlin Heidelberg, 2001. http://dx.doi.org/10.1007/978-3-540-48913-9_5.

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de Fornel, Frédärique. "The Evanescent Field in Guided Optics." In Springer Series in Optical Sciences, 51–74. Berlin, Heidelberg: Springer Berlin Heidelberg, 2001. http://dx.doi.org/10.1007/978-3-540-48913-9_3.

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Mittler, Silvia. "Waveguide Evanescent Field Fluorescence and Scattering Microscopy: The Status Quo." In Optics, Photonics and Laser Technology, 1–24. Cham: Springer International Publishing, 2018. http://dx.doi.org/10.1007/978-3-319-98548-0_1.

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Demchenko, Alexander P. "Evanescent Field Effects and Plasmonic Enhancement of Luminescence in Sensing Technologies." In Introduction to Fluorescence Sensing, 503–29. Cham: Springer International Publishing, 2020. http://dx.doi.org/10.1007/978-3-030-60155-3_13.

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Millis, Bryan A. "Evanescent-Wave Field Imaging: An Introduction to Total Internal Reflection Fluorescence Microscopy." In Methods in Molecular Biology, 295–309. Totowa, NJ: Humana Press, 2011. http://dx.doi.org/10.1007/978-1-60327-216-2_19.

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Conference papers on the topic "Evanescent field"

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Wojcik, Wieslaw, Andrzej Kotyra, Slawomir Przylucki, Andrzej Smolarz, and J. T. Szymczak. "Evanescent field absorption sensor." In Optoelectronic and Electronic Sensors II, edited by Zdzislaw Jankiewicz and Henryk Madura. SPIE, 1997. http://dx.doi.org/10.1117/12.266699.

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Willer, Ulrike, Torsten Blanke, and Wolfgang Schade. "MIR evanescent-field fiber sensors." In Environmental and Industrial Sensing, edited by Tuan Vo-Dinh and Stephanus Buettgenbach. SPIE, 2001. http://dx.doi.org/10.1117/12.417455.

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de Fornel, F., J. P. Goudonnet, L. Salomon, and E. Lesniewska. "An Evanescent Field Optical Microscope." In 1989 Intl Congress on Optical Science and Engineering, edited by Tony Wilson. SPIE, 1989. http://dx.doi.org/10.1117/12.961777.

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van Hulst, N. F., F. B. Segerink, and B. Bölger. "An Evanescent Field Optical Microscope." In Scanned probe microscopy. AIP, 1991. http://dx.doi.org/10.1063/1.41406.

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Sukharenko, Vitaly, and Roger Dorsinville. "Evanescent field scanning optical microscopy." In SPIE OPTO, edited by Michel J. F. Digonnet and Shibin Jiang. SPIE, 2014. http://dx.doi.org/10.1117/12.2035166.

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Siler, Martin, Mojmir Sery, Tomas Cizmar, and Pavel Zemanek. "Submicron particle localization using evanescent field." In Optics & Photonics 2005, edited by Kishan Dholakia and Gabriel C. Spalding. SPIE, 2005. http://dx.doi.org/10.1117/12.615741.

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Kozlov, Valery A., Alexey S. Svakhin, and Valerii V. Ter-Mikirtychev. "Evanescent field thin-film optical amplifier." In OE/LASE '94, edited by Mario N. Armenise. SPIE, 1994. http://dx.doi.org/10.1117/12.175009.

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Cohen, D. A., C. S. Wang, J. A. Nolde, D. D. Lofgreen, and L. A. Coldren. "A monolithic evanescent field spore detector." In Integrated Photonics Research. Washington, D.C.: OSA, 2004. http://dx.doi.org/10.1364/ipr.2004.ithb3.

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Cunningham, J., M. Byrne, P. C. Upadhya, C. Wood, L. Dazhang, M. Lachab, S. P. Khanna, E. H. Linfield, and A. G. Davies. "Evanescent-field Terahertz time-domain microscopy." In 2007 Joint 32nd International Conference on Infrared and Millimeter Waves and the 15th International Conference on Terahertz Electronics (IRMMW-THz). IEEE, 2007. http://dx.doi.org/10.1109/icimw.2007.4516394.

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10

Reece, Peter J., Veneranda Garcés-Chávez, and Kishan Dholakia. "Near-field optical manipulation with cavity enhanced evanescent fields." In Integrated Optoelectronic Devices 2006, edited by David L. Andrews. SPIE, 2006. http://dx.doi.org/10.1117/12.660814.

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Reports on the topic "Evanescent field"

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Yan, M., S. Oberhelman, L. Wang, W. Siekhaus, and M. Kozlowski. Characterization of surface and sub-surface defects in optical materials using the near field evanescent wave. Office of Scientific and Technical Information (OSTI), December 1998. http://dx.doi.org/10.2172/334222.

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