The methods assume that the interface has a fixed width in which the incoming and outgoing components are distributed in a way that moves the interface while maintaining local equilibrium.
But for reflections from boundaries between two materials, the inner one of which has a negative refractive index and the outer one a positive refractive index, the Goos-Hänchen effect instead narrows the width in which the light ray can bounce about.
Fruit netting was scored by both netting density and netting width in which the same QTLs in LG 2, 4, 6, and 7 were identified for both traits.
Assuming hindlimb proportions common to basal ornithischians [28] [34], a hip height of 1.2 m, and taking into account differences in foot posture, we estimate that limb abduction angle ranged between 22° at maximum gauge width (46 cm) and −9° at minimum gauge width (−4 cm), in which the feet stepped across the midline (Fig. 4B).
Unlike conventional transverse width (CTW) mode in which the resonating direction and the acoustic beam direction are identical, in the TROB mode, the active material is set in resonance in half-wavelength mode in one transverse direction and the acoustic beam is generated in the CTW beam direction, the latter being orthogonal to the resonating transverse direction.
In order to allow a direct comparison between measurements made in different experiments where small variations in hyphal width occur (and to facilitate comparison with other organisms), we normalize all measurement of σ to the width of the hypha in which the measurement was made, and we express the results in hyphal width units (hwu).
As is shown in [13], such an observation leads to the conclusion that the width of the dislocation core is equal or less than the width of the ledge in which the dislocation emerged calculated from the tip radius.
In order to allow a direct comparison between measurements made in different experiments where small variations in hyphal width occur (and to facilitate comparison with other organisms), we normalized all measurements of σ to the width of the hypha in which the measurement was made.
The experimental results and their treatment by the developed model showed that the electrolyte concentration generally affects parameters such as the weight and porosity of the film, the pore base hemispherical surface area, the time at which the pore external diameter approaches cell width, the time interval in which the model applies, the parameters involved in the developed kinetic model, etc.
Here, δ denotes the width of the region in which the potential switches its sign in each layer.
The other is the width > 1 μm region, in which the MTF shows a strong width dependence.
