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Equation (1) is a (3N times 3N) linear system of equations where N is the number of cavities of the system.
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The option of cooling is composed of valves and ports necessary to direct a gas of cooling (nitrogen or clean air) towards the containers in the cavity of the system.
Proteins can interact with biological surfaces such as cell membrane, chaperones, cornea, bone, arteries, veins, and heart cavities of the cardiovascular system and also with non-biological surfaces including dialysis membranes and tubing, catheters, invasive surgical instruments, needles, and artificial implants.
Adding another cavity to the system, the PIT window appears which is attributed to the additional cavity-cavity coupling.
Based on the transmission characteristics of the graphene waveguide with one cavity, we investigate the properties of the system with multi-cavities.
Here we stress that, because of the arrangement of our 1D array [see Figure 1(a)] and of the asymmetric coupling between the atom and its right/left cavity, the antiferromagnetic symmetry of the system is spontaneously broken.
The surface plasmon resonance and the spherical cavity resonance in the system of a layer of periodically arranged dielectric spheres laid on outside of a metal slab or embedded in the metal substrate are investigated by observing the absorption spectrum.
In this case, Eq. (1) becomes an eigenvalue problem sum_{i' neq i} mathbf{G}_{i i'}( omega_{0}) mathbf{P}_{i'}= Omega mathbf{P}_{i}, (2) where F has been absorbed within the definition of (mathbf{G}_{i i'} omega_{0})) and we have set (mathbf{E}^{inc}=mathbf{0}) in Eq. (1) as we seek the eigenmodes of the system of cavities.
In addition, the unsteady characteristics of the system composed of cavity and vehicle generate time-varying longitudinal loads that are sources of parametric resonances.
Contrary to those RF systems, the cavities of the CYCIAE230 cyclotron connect two opposite dees.
Figure 13 Interpretation of transient dynamics of the system in the Fabry-Pérot cavity considered.
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