“…where κ is the bound state wave number, then such a potential is unique and its scattering amplitude can be analytically continued into the bound state pole [25]. Thus the ambiguity in the two-body potential calls for more thorough selection of the potential because eventually the adopted potential for the bound state will determine the overall normalization of the astrophysical factor for peripheral direct radiative capture processes.…”
Section: Inverse Scattering Problem Bound-state Potential and Ancmentioning
“…where κ is the bound state wave number, then such a potential is unique and its scattering amplitude can be analytically continued into the bound state pole [25]. Thus the ambiguity in the two-body potential calls for more thorough selection of the potential because eventually the adopted potential for the bound state will determine the overall normalization of the astrophysical factor for peripheral direct radiative capture processes.…”
Section: Inverse Scattering Problem Bound-state Potential and Ancmentioning
“…There is an analogue of the Friedel sum rule in scattering theory. Known as Levinson's theorem [40], it relates the number of bound states in a scattering region to the sum of the scattering phase shifts at zero energy. Employing the Friedel sum rule, Levy Yeyati and Büttiker argued that the addition of a charge ∆Q to a conducting region Ω should change the phase of the transmission amplitude t through that region according to ∆Q/e = ∆arg(t)/π.…”
This is a review of the phase coherent transmission through interacting mesoscopic conductors. As a paradigm we study the transmission amplitude and the dephasing rate for electron transport through a quantum dot in the Coulomb blockade regime. We summarize experimental and theoretical work devoted to the phase of the transmission amplitude. It is shown that the evolution of the transmission phase may be dominated by non-universal features in the short-time dynamics of the quantum dot. The controlled dephasing in Coulomb coupled conductors is investigated. Examples comprise a single or multiple quantum dots in close vicinity to a quantum point contact. The current through the quantum point contact "measures" the state of the dots and causes dephasing. The dephasing rate is derived using widely different theoretical approaches. The Coulomb coupling between mesoscopic conductors may prove useful for future work on electron coherence and quantum computing.
“…Using the well-known Rayleigh-Gans approximation [26,27], we compute the elements of the scattering amplitude matrix and the scattering cross section.…”
Section: Light Scattering and Optical Transmittancementioning
confidence: 99%
“…Following the standard procedure [26,27], the undisturbed incident wave is assumed to be a harmonic plane wave with the frequency ω and the wavenumber k = n m ω/c. The wave is propagating through the effective medium along the direction specified by a unit vector k inc and the wave vector k inc = kk inc .…”
Section: Scattering Amplitude Matrix In Rayleigh-gans Approximationmentioning
confidence: 99%
“…[Throughout the paper summation over repeated indices will be assumed.] Asymptotic behavior of the scattered outgoing wave in the far field region (kr ≫ 1) is known [26,27]:…”
Section: Scattering Amplitude Matrix In Rayleigh-gans Approximationmentioning
We study the effects of droplet ordering in initial optical transmittance through polymer dispersed liquid crystal (PDLC) films prepared in the presence of an electrical field. The experimental data are interpreted by using a theoretical approach to light scattering in PDLC films that explicitly relates optical transmittance and the order parameters characterizing both the orientational structures inside bipolar droplets and orientational distribution of the droplets. The theory relies on the Rayleigh-Gans approximation and uses the Percus-Yevick approximation to take into account the effects due to droplet positional correlations.
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