2007
DOI: 10.1557/proc-1017-dd08-50
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Phonon Spectra and Thermodynamic Properties Of Crystalline Nanowires

Abstract: Phonon spectra and allowed phonon states, as well as thermodynamic characteristics of nanowires of simple cubic crystalline structure, are analyzed using the method of two-time dependent Green's functions, adjusted to bounded crystalline structures. Poles of Green's functions, defining phonon spectra, can be found by solving of the secular equation. For different boundary parameters, this problem is presented graphically. The presence of boundaries as well as the change of boundary parameters leads to appearan… Show more

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Cited by 7 publications
(8 citation statements)
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“…Starting point of our theoretical approach is the standard Hamiltonian of the phonon subsystem for bulk structures [5][6][7][8], written in the harmonic as well as in the nearest neighbor approximations, which is adapted to the model-structure of quantum wire presented in Fig. 1b:…”
Section: Theoretical Analysismentioning
confidence: 99%
“…Starting point of our theoretical approach is the standard Hamiltonian of the phonon subsystem for bulk structures [5][6][7][8], written in the harmonic as well as in the nearest neighbor approximations, which is adapted to the model-structure of quantum wire presented in Fig. 1b:…”
Section: Theoretical Analysismentioning
confidence: 99%
“…Phonon participation in thermodynamic properties (or heat capacitance temperature behavior, i.e. generallyin heat transferring) in thin film was found in our previous paper (Lazarev et al, 2000;Jaćimovski et al, 2004;Šetrajčić et al, 2007;Ilić et al, 2007;Šetrajčić et al, 2009). Getting that, when k → 0 (in long-wave approximation: 4 sin 2 (ak x /2) + sin 2 ak y /2 ≈ a 2 k 2 , k 2 = k 2 x + k 2 y ), energies of all three phonon branches have non-zero values, it can be utilized dispersion relations 22, 49 and 64, in somewhat simplified form:…”
Section: Phonon Thermodynamics Of Thin Film-structuresmentioning
confidence: 58%
“…The most significant results that we have achieved in our previous researches [32][33][34][35], concerning the formation and the analysis of the core-shell crystalline nanomodel and its potential application in nanomedicine, can be briefly defined in the following way: on bordering surfaces of the nanofilm (here it is a nanoshell), due to extreme localization of elementary excitations, all the physical properties of the material change, therefore: − Small, thermally or mechanically stimulated disturbances can become surface waves of great amplitude, i.e. energies that can imply the braking up of crystallographic connections between the atoms of bordering planes and the decomposition of the bordering layer, and then of all the other atoms; − Heat can be more easily absorbed and surface conducted, which allows the nanolayer to be supplied with additional energy which is necessary to melt the material on bordering layers first, and the other layers afterwards;…”
Section: Ultrathin Shell-model Of Molecular Crystalsmentioning
confidence: 76%