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When an incident beam couples with the evanescent field of a surface plasmon, an excited fluorophore will couple to the surface plasmon throughout an outgoing (emissive) beam.
The oscillating piezoelectric field of a surface acoustic wave (SAW) is employed to transport photoexcited electrons and holes in GaAs nanowires deposited on a SAW delay line on a LiNbO3 crystal.
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The calculation of traction forces is based on the Boussinesq solution for the displacement field on a surface of a semi-infinite solid [37].
The field drains of a surface system may be arranged in many patterns.
As an example of the first type of data, we consider discrete samples of a scalar function f : R 2 → R, which represents a height field of a terrain surface as shown in Figure 1.
The mitotic index was determined according to the number of mitoses per 10 high power fields (each field corresponded to a surface of 3.3 mm), as low when <11, moderate when (11 22) and high when >22 (Vincent-Salomon et al, 2004).
Contrary to eq 1, the above expression describes a genuinely nonlocal self-interaction process where the electron first induces a field (through excitation of a surface plasmon) and then performs work against the induced field.
This paper presents a high frequency micro-magnetic field sensor composed of a surface acoustic wave (SAW) transponder and a giant magnetoimpedance (GMI) sensitive element.
The correlation between the stress field of a MD and surface profile for a CS-GaInP is shown in Fig. 4a.
The amplitude of the scattered field from a surface element is (8).
To achieve this, it is possible to write the following expression for the amplitude of the scattered field from a surface element: (9).
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