Academic literature on the topic 'Surface plasmon resonance sensors'

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Journal articles on the topic "Surface plasmon resonance sensors"

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Wang, Xing-Yuan, Yi-Lun Wang, Suo Wang, Bo Li, Xiao-Wei Zhang, Lun Dai, and Ren-Min Ma. "Lasing Enhanced Surface Plasmon Resonance Sensing." Nanophotonics 6, no. 2 (March 1, 2017): 472–78. http://dx.doi.org/10.1515/nanoph-2016-0006.

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AbstractThe resonance phenomena of surface plasmons has enabled development of a novel class of noncontact, real-time and label-free optical sensors, which have emerged as a prominent tool in biochemical sensing and detection. However, various forms of surface plasmon resonances occur with natively strong non-radiative Drude damping that weakens the resonance and limits the sensing performance fundamentally. Here we experimentally demonstrate the first lasing-enhanced surface plasmon resonance (LESPR) refractive index sensor. The figure of merit (FOM) of intensity sensing is ~84,000, which is about 400 times higher than state-of-the-art surface plasmon resonance (SPR) sensor. We found that the high FOM originates from three unique features of LESPR sensors: high-quality factor, nearly zero background emission and the Gaussian-shaped lasing spectra. The LESPR sensors may form the basis for a novel class of plasmonic sensors with unprecedented performance for a broad range of applications.
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Mayer, Kathryn M., and Jason H. Hafner. "Localized Surface Plasmon Resonance Sensors." Chemical Reviews 111, no. 6 (June 8, 2011): 3828–57. http://dx.doi.org/10.1021/cr100313v.

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Homola, Jiřı́, Sinclair S. Yee, and Günter Gauglitz. "Surface plasmon resonance sensors: review." Sensors and Actuators B: Chemical 54, no. 1-2 (January 25, 1999): 3–15. http://dx.doi.org/10.1016/s0925-4005(98)00321-9.

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Chung, Pei-Yu, Tzung-Hua Lin, Gregory Schultz, Christopher Batich, and Peng Jiang. "Nanopyramid surface plasmon resonance sensors." Applied Physics Letters 96, no. 26 (June 28, 2010): 261108. http://dx.doi.org/10.1063/1.3460273.

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Harris, R. D., and J. S. Wilkinson. "Waveguide surface plasmon resonance sensors." Sensors and Actuators B: Chemical 29, no. 1-3 (October 1995): 261–67. http://dx.doi.org/10.1016/0925-4005(95)01692-9.

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Mrozek, Piotr, Ewa Gorodkiewicz, Paweł Falkowski, and Bogusław Hościło. "Sensitivity Analysis of Single- and Bimetallic Surface Plasmon Resonance Biosensors." Sensors 21, no. 13 (June 25, 2021): 4348. http://dx.doi.org/10.3390/s21134348.

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Comparative analysis of the sensitivity of two surface plasmon resonance (SPR) biosensors was conducted on a single-metallic Au sensor and bimetallic Ag–Au sensor, using a cathepsin S sensor as an example. Numerically modeled resonance curves of Au and Ag–Au layers, with parameters verified by the results of experimental reflectance measurement of real-life systems, were used for the analysis of these sensors. Mutual relationships were determined between ∂Y/∂n components of sensitivity of the Y signal in the SPR measurement to change the refractive index n of the near-surface sensing layer and ∂n/∂c sensitivity of refractive index n to change the analyte’s concentration, c, for both types of sensors. Obtained results were related to experimentally determined calibration curves of both sensors. A characteristic feature arising from the comparison of calibration curves is the similar level of Au and Ag–Au biosensors’ sensitivity in the linear range, where the signal of the AgAu sensor is at a level several times greater. It was shown that the influence of sensing surface morphology on the ∂n/∂c sensitivity component had to be incorporated to explain the features of calibration curves of sensors. The shape of the sensory surface relief was proposed to increase the sensor sensitivity at low analyte concentrations.
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Amarie, Dragos, Nazanin Mosavian, Elijah L. Waters, and Dwayne G. Stupack. "Underlying Subwavelength Aperture Architecture Drives the Optical Properties of Microcavity Surface Plasmon Resonance Sensors." Sensors 20, no. 17 (August 30, 2020): 4906. http://dx.doi.org/10.3390/s20174906.

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Microcavity surface plasmon resonance sensors (MSPRSs) develop out of the classic surface plasmon resonance technologies and aim at producing novel lab-on-a-chip devices. MSPRSs generate a series of spectral resonances sensitive to minute changes in the refractive index. Related sensitivity studies and biosensing applications are published elsewhere. The goal of this work is to test the hypothesis that MSPRS resonances are standing surface plasmon waves excited at the surface of the sensor that decay back into propagating photons. Their optical properties (mean wavelength, peak width, and peak intensity) appear highly dependent on the internal morphology of the sensor and the underlying subwavelength aperture architecture in particular. Numerous optical experiments were designed to investigate trends that confirm this hypothesis. An extensive study of prior works was supportive of our findings and interpretations. A complete understanding of those mechanisms and parameters driving the formations of the MSPRS resonances would allow further improvement in sensor sensitivity, reliability, and manufacturability.
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Nenninger, G. G., P. Tobiška, J. Homola, and S. S. Yee. "Long-range surface plasmons for high-resolution surface plasmon resonance sensors." Sensors and Actuators B: Chemical 74, no. 1-3 (April 2001): 145–51. http://dx.doi.org/10.1016/s0925-4005(00)00724-3.

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Yang Peng, Yang Peng, Jing Hou Jing Hou, Zhihe Huang Zhihe Huang, Bin Zhang Bin Zhang, and Qisheng Lu Qisheng Lu. "Design of the photonic crystal f iber-based surface plasmon resonance sensors." Chinese Optics Letters 10, s1 (2012): S10607–310610. http://dx.doi.org/10.3788/col201210.s10607.

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Gryga, Michal, Dalibor Ciprian, and Petr Hlubina. "Bloch Surface Wave Resonance Based Sensors as an Alternative to Surface Plasmon Resonance Sensors." Sensors 20, no. 18 (September 8, 2020): 5119. http://dx.doi.org/10.3390/s20185119.

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We report on a highly sensitive measurement of the relative humidity (RH) of moist air using both the surface plasmon resonance (SPR) and Bloch surface wave resonance (BSWR). Both resonances are resolved in the Kretschmann configuration when the wavelength interrogation method is utilized. The SPR is revealed for a multilayer plasmonic structure of SF10/Cr/Au, while the BSWR is resolved for a multilayer dielectric structure (MDS) comprising four bilayers of TiO2/SiO2 with a rough termination layer of TiO2. The SPR effect is manifested by a dip in the reflectance of a p-polarized wave, and a shift of the dip with the change in the RH, or equivalently with the change in the refractive index of moist air is revealed, giving a sensitivity in a range of 0.042–0.072 nm/%RH. The BSWR effect is manifested by a dip in the reflectance of the spectral interference of s- and p-polarized waves, which represents an effective approach in resolving the resonance with maximum depth. For the MDS under study, the BSWRs were resolved within two band gaps, and for moist air we obtained sensitivities of 0.021–0.038 nm/%RH and 0.046–0.065 nm/%RH, respectively. We also revealed that the SPR based RH measurement is with the figure of merit (FOM) up to 4.7 × 10−4 %RH−1, while BSWR based measurements have FOMs as high as 3.0 × 10−3 %RH−1 and 1.1 × 10−3 %RH−1, respectively. The obtained spectral interferometry based results demonstrate that the BSWR based sensor employing the available MDS has a similar sensitivity as the SPR based sensor, but outperforms it in the FOM. BSW based sensors employing dielectrics thus represent an effective alternative with a number of advantages, including better mechanical and chemical stability than metal films used in SPR sensing.
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Dissertations / Theses on the topic "Surface plasmon resonance sensors"

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Vukusic, Peter. "Sensing thin layers using surface plasmon resonance." Thesis, University of Exeter, 1993. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.358142.

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Guo, Jing. "MULTI-MODE SELF-REFERENCING SURFACE PLASMON RESONANCE SENSORS." UKnowledge, 2013. http://uknowledge.uky.edu/ece_etds/13.

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Surface-plasmon-resonance (SPR) sensors are widely used in biological, chemical, medical, and environmental sensing. This dissertation describes the design and development of dual-mode, self-referencing SPR sensors supporting two surface-plasmon modes (long- and short-range) which can differentiate surface binding interactions from bulk index changes at a single sensing location. Dual-mode SPR sensors have been optimized for surface limit of detection (LOD). In a wavelength interrogated optical setup, both surface plasmons are simultaneously excited at the same location and incident angle but at different wavelengths. To improve the sensor performance, a new approach to dual-mode SPR sensing is presented that offers improved differentiation between surface and bulk effects. By using an angular interrogation, both surface plasmons are simultaneously excited at the same location and wavelength but at different angles. Angular interrogation offers at least a factor of 3.6 improvement in surface and bulk cross-sensitivity compared to wavelength-interrogated dual-mode SPR sensors. Multi-mode SPR sensors supporting at least three surface-plasmon modes can differentiate a target surface effect from interfering surface effects and bulk index changes. This dissertation describes a tri-mode SPR sensor which supports three surface plasmon resonance modes at one single sensing position, where each mode is excited at a different wavelength. The tri-mode SPR sensor can successfully differentiate specific binding from the non-specific binding and bulk index changes.
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Nehru, Neha. "Reference Compensation for Localized Surface-Plasmon Resonance Sensors." UKnowledge, 2014. http://uknowledge.uky.edu/ece_etds/41.

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Noble metal nanoparticles supporting localized surface plasmon resonances (LSPR) have been extensively investigated for label free detection of various biological and chemical interactions. When compared to other optical sensing techniques, LSPR sensors offer label-free detection of biomolecular interactions in localized sensing volume solutions. However, these sensors also suffer from a major disadvantage – LSPR sensors remain highly susceptible to interference because they respond to both solution refractive index change and non-specific binding as well as specific binding of the target analyte. These interactions can severely compromise the measurement of the target analyte in a complex unknown media and hence limit the applicability and impact of the sensor. In spite of the extensive amount of work done in this field, there has been a clear absence of efforts to make LSPR sensors immune to interfering effects. The work presented in this document investigates, both experimentally and numerically, dual- and tri-mode LSPR sensors that utilize the multiple surface plasmon modes of gold nanostructures to distinguish target analyte from interfering bulk and non-specific binding effects. Finally, a series of biosensing experiments are performed to examine various regeneration assays for LSPR sensors built on indium tin oxide coated glass substrate.
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Badjatya, Vaibhav. "TUNABLE LASER INTERROGATION OF SURFACE PLASMON RESONANCE SENSORS." UKnowledge, 2009. http://uknowledge.uky.edu/gradschool_theses/588.

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Surface plasmons are bound TM polarized electromagnetic waves that propagate along the interface of two materials with real dielectric constants of opposite signs. Surface plasmon resonance (SPR) sensors make use of the surface plasmon waves to detect refractive index changes occurring near this interface. For sensing purposes, this interface typically consists of a metal layer, usually gold or silver, and a liquid dielectric. SPR sensors usually measure the shift in resonance wavelength or resonance angle due to index changes adjacent to the metal layer. However this restricts the limit of detection (LOD), as the regions of low slope (intensity vs. wavelength or angle) in the SPR curve contain little information about the resonance. This work presents the technique of tunable laser interrogation of SPR sensors. A semiconductor laser with a typical lasing wavelength of 650nm was used. A 45nm gold layer sputtered on a BK7 glass substrate served as the sensor. The laser wavelength is tuned to always operate in the region of highest slope by using a custom-designed LabVIEW program. It is shown that the sensitivity is maximized and LOD is minimized by operating around the region of high slope on the SPR curve.
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Johnston, Kyle S. "Planar substrate surface plasmon resonance probe with multivariant calibration /." Thesis, Connect to this title online; UW restricted, 1996. http://hdl.handle.net/1773/6069.

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Jorgenson, Ralph Corleissen. "Surface plasmon resonance based bulk optic and fiber optic sensors /." Thesis, Connect to this title online; UW restricted, 1993. http://hdl.handle.net/1773/5996.

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Matcheswala, Akil Mannan. "GOLD NANOSPHERES AND GOLD NANORODS AS LOCALIZED SURFACE PLASMON RESONANCE SENSORS." UKnowledge, 2010. http://uknowledge.uky.edu/gradschool_theses/60.

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A novel localized surface plasmon resonance (LSPR) sensor that differentiates between background refractive index changes and surface-binding of a target analyte (e.g. a target molecule, protein, or bacterium) is presented. Standard, single channel LSPR sensors cannot differentiate these two effects as their design allows only one mode to be coupled. This novel technique uses two surface plasmon modes to simultaneously measure surface binding and solution refractive index changes. This increases the sensitivity of the sensor. Different channels or modes can be created in sensors with the introduction of gold nanospheres or gold nanorods that act as receptor mechanisms. Once immobilization was achieved on gold nanospheres, the technique was optimized to achieve the same immobilization for gold nanorods to get the expected dual mode spectrum. Intricate fabrication methods are illustrated with using chemically terminated self assembled monolayers. Then the fabrication process advances from chemically silanized nanoparticles, on to specific and systematic patterns generated with the use of Electron Beam Lithography. Comparisons are made within the different methods used, and guidelines are set to create possible room for improvement. Some methods implemented failed, but there was a lot to learn from these unsuccessful outcomes. Finally, the applications of the dual mode sensor are introduced, and current venues where the sensors can be used in chemical and biological settings are discussed.
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Keathley, Phillip Donald. "DESIGN AND ANALYSIS OF NANO-GAP ENHANCED SURFACE PLASMON RESONANCE SENSORS." UKnowledge, 2009. http://uknowledge.uky.edu/gradschool_theses/643.

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Surface plasmon resonance (SPR) sensors are advantageous to other techniques of sensing chemical binding, offering quantitative, real-time, label-free results. Previous work has demonstrated the effectiveness of using dual-mode SPR sensors to differentiate between surface and background effects, making the sensors more robust to dynamic environments. This work demonstrates a technique that improves upon a previously optimized planar film dual-mode SPR sensor’s LOD by introducing a periodic array of subwavelength nano-gaps throughout the plasmon supporting material. First, general figures of merit for a sensor having an arbitrary number of modes are studied. Next, the mode effective index dispersion and magnetic field profiles of the two strongly bound modes found using a gap width of 20nm are analyzed. Qualitative analysis of the results demonstrates how such a design can enable better LODs in terms of each figure of merit. By optimizing a nano-gap enhanced sensor containing 20nm gaps, it is quantitatively demonstrated that the resulting modes improve upon almost every figure of merit, especially with respect to the orthogonality and magnitude of the sensitivity vectors, resulting in LODs approximately a factor of five less than the optimal planar design.
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Sommers, Daniel R. "Design and verification of a surface plasmon resonance biosensor." Thesis, Georgia Institute of Technology, 2004. http://hdl.handle.net/1853/6967.

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The Microelectronics Group has been researching sensors useful for detecting and quantifying events in biological molecular chemistry, for example, binding events. Our previous research has been based primarily on quartz resonators. This thesis describes the results of our initial research of Surface Plasmon Resonance (SPR) based technology. This study contains the design and implementation of a fully functional SPR biosensor with detailed disclosure of monolayer construction, digital hardware interfaces and software algorithms for process the SPR sensors output. An antibody monolayer was constructed on the biosensor surface with the goal of setting the strengths, weaknesses and limitation of measuring molecular events with SPR technology. We documented several characteristics of molecular chemistry that directly effect any measurements made using Surface Plasmon Resonance technology including pH, free ions, viscosity and temperature. Furthermore, the component used in our study introduced additional limitations due to wide variations amongst parts, the constraint of a liquid medium and the large surface area used for molecular interrogation. We have identified viable applications for this sensor by either eliminating or compensating for the factors that affect the measured results. This research has been published at the inaugural IEEE sensors conference and to our knowledge is the first time a biosensor has been constructed by attaching a sensor to a PDA and performing all signal processing, waveform analysis and display in the PDAs core processor.
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Watkins, William L. "Study and development of localised surface plasmon resonance based sensors using anisotropic spectroscopy." Electronic Thesis or Diss., Sorbonne université, 2018. https://accesdistant.sorbonne-universite.fr/login?url=https://theses-intra.sorbonne-universite.fr/2018SORUS505.pdf.

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La résonance de plasmon de surface localisée (LSPR) est définie comme l’oscillation collective du nuage d’électrons de conduction induite par un champ électrique externe. Dans le cas de nanoparticules composé de métaux nobles tels que l’or, l’argent, ou le cuivre,la résonance est localisée dans le visible ou le proche UV. La polarisabilité d’une nanoparticule est directement proportionnelle à quatre paramètres clefs : son volume, sa composition, sa forme et son milieu environnant. Ce sont ces propriétés qui font que la LSPR peut être utilisée à des fin de capteur. Dans le cas d’une particule isotrope, tel que la sphère, le spectre LSPR montre un seul pic d’absorption. Dans le cas d’une particule anisotrope, tel qu’une ellipsoïde, le spectre d’absorption a deux maxima distincts. Si on calcule la section efficace d’absorption en considérant une lumière non polarisée, on obtient deux maxima. Le point clef de ce type de système est la possibilité de découpler les deux résonances en utilisant une lumière polarisée. Dans cette description le système anisotrope est considéré comme microscopique, c’est à dire qu’il ne s’agit que d’une ou deux particules. Dans le cas d’un échantillon macroscopique, tel qu’une solution colloïdale d’ellipsoïdes ou nanotiges, le spectre d’absorption aura toujours deux maxima d’absorption, mais ceux-ci ne pourront pas être découplés car l’échantillon n’est pas globalement anisotrope. En revanche, si l’échantillon présente une anisotropie globale telle que des nanotiges alignés, ou des nanosphères organisées en ligne, il est possible d’avoir un spectre de plasmon dépendant de la polarisation de la lumière. Être capable de découpler les résonances d’un échantillon anisotrope permet de mesurer un spectre différentiel en prenant la différence des deux spectres d’absorption. Cela est expérimentalement possible en utilisant la spectroscopie de transmis- sion anisotrope qui permet la mesure de l’anisotropie optique. L’avantage est d’obtenir un spectre relative et différentiel donc plus stable et reproductible. De plus il est maintenant possible de suivre l’évolution de la réponse optique des particules plasmoniques, non plus en mesurant un déplacement spectral, mais en mesurant le changement d’intensité du signal à une longueur d’onde fixe. Cette méthode est utilisée pour deux cas d’études qui sont la mesure de l’interaction du dihydrogène avec des nanoparticules d’or, ainsi que la détection de faible pression partielle de dihydrogène dans un gaz porteur (argon, et air) à l’aide de palladium, pour des applications de capteur d’hydrogène
Localised surface plasmon resonance (LSPR) is defined as the collective oscillation of the conduction electron cloud induced by an external electric field. In the case of nanoparticles composed of noble metals such as gold, silver, or copper, the resonance is located in the visible or near UV range. The polarisability of a nanoparticle is directly proportional to four key parameters: its volume, its composition, its shape and its surrounding environment. It is these properties that make LSPR useful for sensor applications. In the case of isotropic particles, such as spheres, the LSPR spectrum shows only one absorption peak. In the case of an anisotropic particle, such as an ellipsoid, the absorption spectrum has two or more distinct peaks. If the absorption cross-section is measured with unpolarised light, multiple maxima are obtained. The key point for these type of systems is the possibility to decouple the resonances using polarised light. In this description the anisotropic system is considered microscopic, i.e. it is only made of one or two particles. In the case of a macroscopic sample, such as a colloidal solution of ellipsoids or nanorods, the absorption spectrum will always have multiple absorption maxima, and they cannot be decoupled because the sample is not globally anisotropic.On the other hand, if the sample has a global anisotropy such as aligned nanorods, or nanosphere organised in lines, it is possible to have a plasmon spectrum dependent on the light polarisation. Being able to decouple the resonances of an anisotropic sample makes it possible to measure a differential spectrum by taking the difference of the two absorption spectra. This is experimentally possible by using anisotropic transmission spectroscopy which measures the optical anisotropy. The advantage is to obtain a relative and differential spectrum more stable and reproducible. Moreover, it is now possible to follow the evolution of the optical response of the plasmonic particles no longer by measuring a spectral shift but by measuring the change in intensity of the signal at a fixed wavelength. This method is used on two case studies which are the measurement of the interaction of dihydrogen with gold nanoparticles, as well as the detection of low partial pressure of dihydrogen in a carrier gas (argon, and air) using palladium nanoparticles, for hydrogen sensing applications
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Books on the topic "Surface plasmon resonance sensors"

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Oliveira, Leiva Casemiro, Antonio Marcus Nogueira Lima, Carsten Thirstrup, and Helmut Franz Neff. Surface Plasmon Resonance Sensors. Cham: Springer International Publishing, 2015. http://dx.doi.org/10.1007/978-3-319-14926-4.

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Oliveira, Leiva Casemiro, Antonio Marcus Nogueira Lima, Carsten Thirstrup, and Helmut Franz Neff. Surface Plasmon Resonance Sensors. Cham: Springer International Publishing, 2019. http://dx.doi.org/10.1007/978-3-030-17486-6.

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Homola, Jiří, ed. Surface Plasmon Resonance Based Sensors. Berlin, Heidelberg: Springer Berlin Heidelberg, 2006. http://dx.doi.org/10.1007/b100321.

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Mol, Nico J., and Marcel J. E. Fischer, eds. Surface Plasmon Resonance. Totowa, NJ: Humana Press, 2010. http://dx.doi.org/10.1007/978-1-60761-670-2.

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Schasfoort, Richard B. M., ed. Handbook of Surface Plasmon Resonance. Cambridge: Royal Society of Chemistry, 2017. http://dx.doi.org/10.1039/9781788010283.

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Schasfoort, Richard B. M., and Anna J. Tudos, eds. Handbook of Surface Plasmon Resonance. Cambridge: Royal Society of Chemistry, 2008. http://dx.doi.org/10.1039/9781847558220.

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Surface plasmon resonance: Methods and protocols. New York: Humana Press, 2010.

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Long, Yi-Tao, and Chao Jing. Localized Surface Plasmon Resonance Based Nanobiosensors. Berlin, Heidelberg: Springer Berlin Heidelberg, 2014. http://dx.doi.org/10.1007/978-3-642-54795-9.

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Stepanov, Andrey L. Surface plasmon polariton nanooptics. Hauppauge, N.Y: Nova Science Publishers, 2011.

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Zaheer, Sameer Mahmood, and Ramachandraiah Gosu, eds. Methods for Fragments Screening Using Surface Plasmon Resonance. Singapore: Springer Singapore, 2021. http://dx.doi.org/10.1007/978-981-16-1536-8.

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Book chapters on the topic "Surface plasmon resonance sensors"

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Erickson, David. "Surface Plasmon Resonance Sensors." In Encyclopedia of Microfluidics and Nanofluidics, 3123–31. New York, NY: Springer New York, 2015. http://dx.doi.org/10.1007/978-1-4614-5491-5_1504.

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Erickson, David. "Surface Plasmon Resonance Sensors." In Encyclopedia of Microfluidics and Nanofluidics, 1–9. Boston, MA: Springer US, 2014. http://dx.doi.org/10.1007/978-3-642-27758-0_1504-2.

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Oliveira, Leiva Casemiro, Antonio Marcus Nogueira Lima, Carsten Thirstrup, and Helmut Franz Neff. "Introduction and Background Information." In Surface Plasmon Resonance Sensors, 1–9. Cham: Springer International Publishing, 2019. http://dx.doi.org/10.1007/978-3-030-17486-6_1.

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Oliveira, Leiva Casemiro, Antonio Marcus Nogueira Lima, Carsten Thirstrup, and Helmut Franz Neff. "Active Metal-Type Compounds." In Surface Plasmon Resonance Sensors, 257–72. Cham: Springer International Publishing, 2019. http://dx.doi.org/10.1007/978-3-030-17486-6_10.

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Oliveira, Leiva Casemiro, Antonio Marcus Nogueira Lima, Carsten Thirstrup, and Helmut Franz Neff. "Heavy Metals." In Surface Plasmon Resonance Sensors, 273–83. Cham: Springer International Publishing, 2019. http://dx.doi.org/10.1007/978-3-030-17486-6_11.

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Oliveira, Leiva Casemiro, Antonio Marcus Nogueira Lima, Carsten Thirstrup, and Helmut Franz Neff. "Artificial Metal-Insulator Multi-layer Structures." In Surface Plasmon Resonance Sensors, 285–88. Cham: Springer International Publishing, 2019. http://dx.doi.org/10.1007/978-3-030-17486-6_12.

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Oliveira, Leiva Casemiro, Antonio Marcus Nogueira Lima, Carsten Thirstrup, and Helmut Franz Neff. "Practical Applications." In Surface Plasmon Resonance Sensors, 289–314. Cham: Springer International Publishing, 2019. http://dx.doi.org/10.1007/978-3-030-17486-6_13.

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Oliveira, Leiva Casemiro, Antonio Marcus Nogueira Lima, Carsten Thirstrup, and Helmut Franz Neff. "Conclusions." In Surface Plasmon Resonance Sensors, 315–19. Cham: Springer International Publishing, 2019. http://dx.doi.org/10.1007/978-3-030-17486-6_14.

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Oliveira, Leiva Casemiro, Antonio Marcus Nogueira Lima, Carsten Thirstrup, and Helmut Franz Neff. "Physical Features of the Surface Plasmon Polariton." In Surface Plasmon Resonance Sensors, 11–21. Cham: Springer International Publishing, 2019. http://dx.doi.org/10.1007/978-3-030-17486-6_2.

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Oliveira, Leiva Casemiro, Antonio Marcus Nogueira Lima, Carsten Thirstrup, and Helmut Franz Neff. "Design Features of Surface Plasmon Resonance Sensors." In Surface Plasmon Resonance Sensors, 23–30. Cham: Springer International Publishing, 2019. http://dx.doi.org/10.1007/978-3-030-17486-6_3.

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Conference papers on the topic "Surface plasmon resonance sensors"

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Homola, Jirí, Marek Piliarik, and Pavel Kvasnicka. "Surface plasmon resonance biosensors." In Third European Workshop on Optical Fibre Sensors. SPIE, 2007. http://dx.doi.org/10.1117/12.738340.

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Pollet, Jeroen, Filip Delport, Dinh Tran Thi, Martine Wevers, and Jeroen Lammertyn. "Aptamer-based surface plasmon resonance probe." In 2008 IEEE Sensors. IEEE, 2008. http://dx.doi.org/10.1109/icsens.2008.4716654.

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Graham, David J. L., and Lionel R. Watkins. "Surface plasmon resonance imaging with polarisation modulation." In 2009 IEEE Sensors. IEEE, 2009. http://dx.doi.org/10.1109/icsens.2009.5398306.

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Kim, Jongdeog, and Yo Han Choi. "Differential Angle Scanning Surface Plasmon Resonance Detection." In 2018 IEEE Sensors. IEEE, 2018. http://dx.doi.org/10.1109/icsens.2018.8589578.

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5

Špašková, Barbora, Nicholas S. Lynn, Jiří Slabý, Markéta Bocková, and Jiří Homola. "Nanostructure-enhanced surface plasmon resonance imaging (Conference Presentation)." In Optical Sensors, edited by Robert A. Lieberman, Francesco Baldini, and Jiri Homola. SPIE, 2017. http://dx.doi.org/10.1117/12.2268269.

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6

Schuster, Tobias, Niels Neumann, and Christian Schäffer. "A Fiber-Optic Surface-Plasmon-Resonance Bio-Sensor." In Optical Sensors. Washington, D.C.: OSA, 2010. http://dx.doi.org/10.1364/sensors.2010.swb6.

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Wilson, Denise, and Brian Ferguson. "Optimization of surface plasmon resonance for environmental monitoring." In 2010 Ninth IEEE Sensors Conference (SENSORS 2010). IEEE, 2010. http://dx.doi.org/10.1109/icsens.2010.5690814.

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8

Jung, Chuck C. "Surface plasmon resonance fiber optic sensors." In Third Pacific Northwest Fiber Optic Sensor Workshop, edited by Eric Udd and Chuck C. Jung. SPIE, 1997. http://dx.doi.org/10.1117/12.285592.

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Wilkop, Thomas, Anil S. Ramlogan, Ian L. Alberts, Joost D. de Bruijn, and Asim K. Ray. "Surface plasmon resonance imaging for medical and biosensing." In 2009 IEEE Sensors. IEEE, 2009. http://dx.doi.org/10.1109/icsens.2009.5398485.

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Harris, R. D., B. J. Luff, J. S. Wilkinson, R. Wilson, D. J. Schiffrin, J. Piehler, A. Brecht, G. Gauglitz, R. A. Abuknesha, and C. Mouvet. "Waveguide Surface Plasmon Resonance Biosensor For Simazine Analysis." In Optical Fiber Sensors. Washington, D.C.: OSA, 1996. http://dx.doi.org/10.1364/ofs.1996.th21.

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Reports on the topic "Surface plasmon resonance sensors"

1

McWhorter, C. S. Surface Plasmon Resonance Spectroscopy-Based Process Sensors. Office of Scientific and Technical Information (OSTI), September 2003. http://dx.doi.org/10.2172/815565.

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2

Anderson, B. B. Feasibility Study for the Development of a Surface Plasmon Resonance spectroscopy-based Sensor for the BNFL-Hanford. Office of Scientific and Technical Information (OSTI), July 2000. http://dx.doi.org/10.2172/759145.

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3

Zheng, Junwei. Surface plasmon enhanced interfacial electron transfer and resonance Raman, surface-enhanced resonance Raman studies of cytochrome C mutants. Office of Scientific and Technical Information (OSTI), November 1999. http://dx.doi.org/10.2172/754842.

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4

Sanchez, Erik. Modeling of the Surface Plasmon Resonance (SPR) Effect for a Metal-Semiconductor (M-S) Junction at Elevated Temperatures. Portland State University Library, January 2000. http://dx.doi.org/10.15760/etd.6508.

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