1993
DOI: 10.1103/physrevb.47.16597
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Interaction Hamiltonian between an electron and polar surface vibrations in a symmetrical three-layer structure

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Cited by 13 publications
(11 citation statements)
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“…Furthermore, we consider quantum wells of much larger thickness than the lattice constant. As a consequence, we neglect interface phonon modes, whose amplitude decreases exponentially away from the interface [28,29]. The phonon dispersion is also neglected because we consider only phonons with small in-plane wave vectors.…”
Section: Interaction Between Phonons and Intersubband Excitationsmentioning
confidence: 99%
“…Furthermore, we consider quantum wells of much larger thickness than the lattice constant. As a consequence, we neglect interface phonon modes, whose amplitude decreases exponentially away from the interface [28,29]. The phonon dispersion is also neglected because we consider only phonons with small in-plane wave vectors.…”
Section: Interaction Between Phonons and Intersubband Excitationsmentioning
confidence: 99%
“…The first term in (7) corresponds to the influence of all layers on the potential in the n-th one, whereas the second part describes intralayer potential modulation transfer. The functions F,"(z) are solutions of the Laplace equation having definite symmetry,…”
Section: Equations Of Motion For the Inertial Polarization Vectormentioning
confidence: 99%
“…It was shown that the spectrum of polar vibrations consists of surface modes and transverse and longitudinal bulk-like ones, called "the slab modes". In the following a great number of works appeared being performed within this model for various structures: the slab in vacuum [2,31, the two-layer slab in vacuum [4], multilayer structures of arbitrary number of layers [5], three-layer symmetrical structures with external layers of infinite [6] and finite thickness [7], and superlattices [5, 8, 91. In these works polar eigenmodes were investigated and the Hamiltonians of the electron-phonon interaction were deduced.…”
Section: Introductionmentioning
confidence: 99%
“…Spatial confinement of acoustic and optical phonons in semiconductor thin films, superlattices and nanowires changes their properties in comparison with bulk materials [1][2][3][4][5][6][7][8][9][10][11][12][13][14][15]. Phonon confinement in nanostructures leads to emergence of the quantized energy subbands with corresponding modification of the phonon density of states [1][2][3][4][10][11][12][13][14][15].…”
Section: Introductionmentioning
confidence: 99%
“…Spatial confinement of acoustic and optical phonons in semiconductor thin films, superlattices and nanowires changes their properties in comparison with bulk materials [1][2][3][4][5][6][7][8][9][10][11][12][13][14][15]. Phonon confinement in nanostructures leads to emergence of the quantized energy subbands with corresponding modification of the phonon density of states [1][2][3][4][10][11][12][13][14][15]. The changes in the phonon dispersion give rise to changes in the electron-phonon scattering rates [15][16][17][18][19][20][21], optical properties of the nanostructured materials [5,[22][23][24][25][26][27][28], and phonon scattering on defects, boundaries and other phonons [10,12,13,[29][30][31].…”
Section: Introductionmentioning
confidence: 99%