2014
DOI: 10.4213/tmf8642
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Волновые Функции И Собственные Значения Носителей Заряда В Нанотрубке В Окрестности Точки Дирака При Наличии Продольного Электрического Поля

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Cited by 4 publications
(3 citation statements)
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“…This model almost coincides with the model used in [31,42]. In [40] as distinct from [39] the array of chiral nanotubes is viewed. In [35] A, B chains correspond to gA and gB chains from [43] when g is odd; if g is even, C and D from our paper chains correspond to gA and gB.…”
Section: B Narrow Nanoribbonssupporting
confidence: 57%
See 1 more Smart Citation
“…This model almost coincides with the model used in [31,42]. In [40] as distinct from [39] the array of chiral nanotubes is viewed. In [35] A, B chains correspond to gA and gB chains from [43] when g is odd; if g is even, C and D from our paper chains correspond to gA and gB.…”
Section: B Narrow Nanoribbonssupporting
confidence: 57%
“…In [39] on account of an elementary phase cell, which contains sublattice A and sublattice B, the wave functions, equidistant energy levels and dipole matrix elements of laser transition in the presence of a longitudinal electric field are analytically obtained. In [40] as distinct from [39] the array of chiral nanotubes is viewed. We write the Liouville equation for the considered multilevel system for the density matrix…”
Section: A Nanotubesmentioning
confidence: 99%
“…2 Theory 2.1 The polarization equation Sadykov and Skorkin (2013) and Sadykov (2014) showed that in the random metallic CNT energy levels are independent from the longitudinal electric field value [the case of zigzag CNT type is considered by Sadykov and Skorkin (2013)] if they meet the conditions ao 2ã =oz 2 ( oã=oz, ao 2b =oz 2 ( ob=oz forã andb coefficients at the atomic orbitals in the case of two-point elementary cell near Fermi surface…”
Section: Introductionmentioning
confidence: 99%