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In general, the quality of the entanglement between the two modes is affected by the losses of the JPA.
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Our results show that chemical enhanced b2-type modes are affected differently relative to electromagnetic enhanced a1-type modes and to the continuum emission background.
This suggests that the lower order normal modes are affected by entanglement effects but the higher order modes are not, for semidilute solutions.
Since any TEn0 mode wave can be decomposed into two TEM mode waves travelling in different diagonal directions, all TEn0 modes are affected nearly equally.
The X-mode is affected more by absorption and group retardation in an ionized atmosphere in comparison with the O-mode (see, e.g., Tsutsumi and Aso 2005).
The steady-state resonator mode is affected by the complex, non-linear electron beam evolution as well as the resonator design.
The resonator mode is affected by a Brownian stochastic force with zero mean value, and ξ ̂ ( t ) has the correlation function ξ ̂ + ( t ) ξ ̂ ( t ′ ) = γ m ω m ∫ dω 2 π ω e - iω ( t - t ′ ) [ 1 + coth ( ℏω 2 κ B T ) ], where k B and T are the Boltzmann constant and the temperature of the reservoir, respectively.
The proliferation mode is affected by the dynamic balance between the positive and negative feedback loops.
In the case of the perpendicular alignment, the momentum transfer from the fluid flow to the graphene (out-of-plane phonon mode) was affected by the decreased flow velocity and increased vorticity, causing the voltage generation to drop.
Change of the allocation mode was affected by worst physical functioning.
Travel behaviour and market research studies have shown that mode choice is affected by three classes of factors: the quantity and relative quality of competing transportation services; characteristics of the trips people take; and attributes of the people themselves and their households.
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