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But in any case there is local or global maximum of the electric field intensity at the metal interface with Bragg mirror for p-modes.
It is well known that metal-InP interfaces are usually subjected to a strong "Fermi level pinning" with the consequence of small barrier height on the metal interface with n-type InP [6].
Thus, the electric field intensity is maximal on the metal interface with Bragg mirror for the lower mode (Fig. 4 a, b and d), whereas the electric field intensity is maximal at the boundary of Bragg mirror with the environment for the second (Fig. 4 c) and third (Fig. 4 f) modes.
When ∈ m < − ∈ d (this condition defines the so-called SPP resonance), it turns out that k x > k0 and, thus, SPPs are trapped at the metal interface, with its intensity exponentially decaying from the interface.
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We have demonstrated that at transition metal interfaces with strong DM interaction it is in particular the exchange interaction that can be tuned by interface composition and structure.
Longevity of cemented hip reconstruction may be achieved by either (1) enhancing fixation and minimizing motion at the cement-metal interface with rougher surfaced implants or (2) minimizing cement abrasion in the presence of motion at the cement-metal interface with smoother surfaced implants.
To date, there is no information on how these porous metals interface with bone cement.
As for [Hg II)]S[Zn II)(H2O/OH–)]N TRIL9CL23H 3 n +, the rate of hydrolysis is pH-dependent, increasing with an increase in pH and MID1-Zn (metal interface design with zinc) has a kinetic p Ka of 8.2 ± 0.1 and a maximal efficiency of 630 ± 90 M–1 s–1.
The catalytic activity and selectivity of metals interfaced with solid electrolytes can be altered dramatically and reversibly via potential application.
As shown by numerical simulations, the hybrid mode for p-polarized light is characterized by low broadening due to the redistribution of the electric field intensity between the metal interface and Bragg mirror with concentration of electric field in the optically less dense layers of Bragg mirror.
The insulating layers of the structure consist in SiO2 on the bottom with the unique Ti metal interface, and Si3N4 on the top with both Ti/TiN and Au interfaces.
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