“…The Green functions are multipolar [10][11][12][13][14], since the denominator is a polynomial D N +1 of order N +1. Therefore, we must use the factorization of prime poles…”
Section: Exciton Statesmentioning
confidence: 99%
“…To determine the crystalline film dynamic permittivity, as in [10][11][12][13][14], we will use formula of DzyaloshinskiPitaevski [18]:…”
Section: Ultrathin Films Permittivitymentioning
confidence: 99%
“…Analyses were done using the innovated method of Green functions, adapted for investigation of quantum structures [10][11][12][13][14]. Due to adequately incorporated statistics, this method is successfully applied in calculating both microscopic and macroscopic, balanced and imbalanced, properties of crystals.…”
This paper presents a model of molecular ultrathin crystalline film and analysis of dielectric properties of these spatially very restricted structures. Using the two-time dependent Green functions the energy spectrum and possible exciton states were determined and the dynamic permittivity was calculated. It was shown that the appearance of localized states in the boundary layers of the film depend on the thickness and the changing values of parameters in the border areas of the film. These localized states define schedule and determine the number of resonant absorption lines in the infrared area of the external electromagnetic radiation.
“…The Green functions are multipolar [10][11][12][13][14], since the denominator is a polynomial D N +1 of order N +1. Therefore, we must use the factorization of prime poles…”
Section: Exciton Statesmentioning
confidence: 99%
“…To determine the crystalline film dynamic permittivity, as in [10][11][12][13][14], we will use formula of DzyaloshinskiPitaevski [18]:…”
Section: Ultrathin Films Permittivitymentioning
confidence: 99%
“…Analyses were done using the innovated method of Green functions, adapted for investigation of quantum structures [10][11][12][13][14]. Due to adequately incorporated statistics, this method is successfully applied in calculating both microscopic and macroscopic, balanced and imbalanced, properties of crystals.…”
This paper presents a model of molecular ultrathin crystalline film and analysis of dielectric properties of these spatially very restricted structures. Using the two-time dependent Green functions the energy spectrum and possible exciton states were determined and the dynamic permittivity was calculated. It was shown that the appearance of localized states in the boundary layers of the film depend on the thickness and the changing values of parameters in the border areas of the film. These localized states define schedule and determine the number of resonant absorption lines in the infrared area of the external electromagnetic radiation.
“…[31][32][33][34][35] Differentiating (39) with respect to time and using equations of motion for operator B n t , we obtain the following equation …”
Section: Magnetization Of Ultrathin Film In Bloch's (Harmonic) Approxmentioning
The problem of the analysis of low temperature magnetization is exposed in detail. The application of exact Bose representation of spin operators to the bulk ferromagnets is justified. By means of this representation the magnetization of ultrathin films was analysed. It turned out that thin films magnetization contains exponentially small terms characterized by Dyson's functions even in harmonical approximation. The main conclusions of this work are that magnetic lattice of thin film is more rigid than the macroscopic lattice and that the autoreduction process (the three layer film divides onto three two layer subfilms) takes place in the film.
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