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And evanescent waves

A very specific surface structure is observed after the annealing of a PS/polybuta-diene (PB) diblock copolymer, PS-b-PB, shown in Fig. 7 b. The surface is very smooth directly after preparation of the film from solution (similar to Fig. 7 a). By annealing at 120 °C the surface structure shown in Fig. 7 b evolves, which we believe is due to the formation of layers of PS and PB parallel to the surface. The outermost layer might not be completely filled due to lack of material leading to steps at the surface. Similar behavior is observed with other diblock copolymers such as PS-b-PMMA [61]. Enrichment of one component is also observed at the surface of a polymer solution [115,116] by X-ray fluorescene and evanescent wave techniques. [Pg.382]

PLANAR OPTICAL SENSORS AND EVANESCENT WAVE EFFECTS... [Pg.193]

Planar Optical Sensors and Evanescent Wave Effects... [Pg.195]

The pH measurement can by realized using sol-gel films and evanescent-wave sensors method74. To incorporate a near-infrared pH sensitive fluorescent dye, a thin-film coating on the core of a multimode fiber was used. By evanescent wave excitation an absorption or fluorescent based sensor can be realized for use in high pH regions. [Pg.370]

P. Kumar, R.C. Willson, J.J. Valdes and J.P. Chambers, Monitoring of oligonucleotide hybridization using light-addressable potentiometric and evanescent wave fluorescence sensing, Mater. Sci. Eng. C, 1(3) (1994) 187-192. [Pg.122]

Another feature that has not been systematically covered concerns additional means of determining properties of adsorbates. Examples here are the classical spectroscopies, with their surface variants (secs. 1.7.10-12), reflection methods, including elllpsometry, reflectometry and evanescent wave studies, NMR. X-ray analysis, neutron diffraction and dielectric spectroscopy. The theory of the last mentioned phenomenon for bulk phases has been discussed in sec. I.4.5f if applied to adsorbates, the technique can give information on the various degrees of freedom that polar molecules may have, say, for water adsorbed on oxides. For thicker water layers containing ions, measurement of the surface conductivity may yield additional information see also sec. I.6.6d. The reason for not systematizing these techniques is that we do not consider them typically "surface methods, but rather surface variants of bulk methods. [Pg.143]

Fig. 3 Propagation of guided modes in the core and evanescent waves in the cladding... Fig. 3 Propagation of guided modes in the core and evanescent waves in the cladding...
Fig. 23 Concentration calibration for the three opto/fluid connectors Tl, T2 and T3. Each data point is averaged over three runs with two cycles per run. Tl - direct excitation, T2 - combination of direct and evanescent wave, and T3 - evanescent wave excitation only. (Reprinted from Dhadwal et al. [2], with permission of Elsevier)... Fig. 23 Concentration calibration for the three opto/fluid connectors Tl, T2 and T3. Each data point is averaged over three runs with two cycles per run. Tl - direct excitation, T2 - combination of direct and evanescent wave, and T3 - evanescent wave excitation only. (Reprinted from Dhadwal et al. [2], with permission of Elsevier)...
Complementary operators, on the other hand, comprise an efficient boundary procedure that improves the absorption of numerical reflections by using previously developed ABCs [13]. Their competence is based on the implementation of two boundary operators that are complementary in their action. In this manner, new ABCs that produce prespecified reflection coefficients are derived. By solving the problem with each of the two operators and then averaging the two solutions, the technique annihilates the first-order artificial reflections of both obliquely propagating and evanescent waves, irrespective of their wave number. More specifically, absorption of the latter occurs even if the original ABC reflects them totally. The modified higher order development of COM starts from a well-posed and stable ABC that can be expressed by a single differential equation, defined as J-. If nonstandard operator [.] is... [Pg.97]

J. Fang and Z. Wu, Generalized perfectly matched layer for the absorption of propagating and evanescent waves in lossless and lossy media, IEEE Trans. Microvu. Theory Tech., vol. 44, no. 12, pp. 2216-2222, Dec. 1996.doi 10.1109/22.556449... [Pg.118]

For the dispersion relation, the analysis of Section 6.4.3 is employed. Likewise, in the solution both propagating and evanescent waves are superimposed to allow a precise approximation. So, it is derived that... [Pg.162]

Optical fibres are useful accessories in a variety of photophysical measurements. The current status and prospects for their further use in chemical analysis are assessed in an article by Norris. Luminescence spectroscopy and evanescent wave devices are topics highlighted in this review. By way of example of this developing technology a device described for luminescence examination of inorganic semiconductors may be cited. [Pg.8]

Fig. 6. Internal reflection and evanescent wave at an interface at which there is an intervening layer of medium 2. Fig. 6. Internal reflection and evanescent wave at an interface at which there is an intervening layer of medium 2.
Laue M (1960) Roentgenstrahl-Interferenzen, Akademische-Verlagsgeslellschaft, Frankfurt Lee TL, Qian Y, Lyman PF, Woicik JC, Pellegrino JG, Bedzyk MJ (1996) The use of X-ray standing waves and evanescent-wave emission to study buried strained-layer heterostractures. Physica 221 437-440... [Pg.265]

Chabay, I. Optical Waveguides. Photon Plumbing for the Chemistry Lab Fiber Optics, Waveguides, and Evanescent Waves as Tools for Chemical Analysis. Anal. Chem. 54(9) 1071A-1080A (1982)... [Pg.193]

Thus, the transition between propagating and evanescent waves is determined by = 0 that is, from (4.2) we have... [Pg.88]

Table 3.1 Critical angles of total Internal reflection and evanescent wave penetration depths... Table 3.1 Critical angles of total Internal reflection and evanescent wave penetration depths...
The flow velocity of a fluid at submicrometric distances from a solid wall is investigated using a novel optical technique based on fluorescence recovery after photobleaching and evanescent wave induced fluorescence. For a polymer melt, three different friction regimes, all characterized by slip at the wall, are identified and modeled at the molecular level. For a simple fluid (alkane), slip at the wall is put into evidence and factors influencing the extend of slip are identified. [Pg.154]

Fluorescence measurements and detection can either be made under steady-state or time-resolved conditions. Some of the commonly used measurement techniques focus on changes in optical properties such as fluorescence intensity quenching, phase fluorometry (lifetime), polarization, surface plasmon resonance (SPR), and evanescent waves. Here, we will present detector systems based for (a) fluorescence intensity quenching and (b) phase fluorometry in detail. A few example references of integrated optical sensor systems based on the various optical measurement techniques are given in Table 1 and the reader is encourage to review those papers if more details are desired. [Pg.34]

In this chapter we shall consider the optical response of a gas in the close vicinity of a solid surface. We shall become aware of different optical techniques which allow us to study various aspects of interactions between gas atoms or molecules and a surface. They are based on reflection of light from a gas-solid interface. Depending on whether the incidence angle is less or greater than the critical angle, one distinguishes between selective reflection spectroscopy (SRS) and evanescent wave spectroscopy (EWS). [Pg.173]


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