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Negative differential resistance in n-type noncompensated silicon at low temperature of the NDR. We attribute this effect to the delocalization of the D- states in the upper Hubbard band due

Negative differential resistance in n-type noncompensated silicon at low temperature of the NDR. We attribute this effect to the delocalization of the D- states in the upper Hubbard band due

Анализ приведенных модификаций уравнения состояния Пенга-Робинсона в рамках процесса Джоуля-Томсона. In the framework of thermodynamic method the modifications of the Peng – Robinson equations of state are considered

Universal DV-CV interaction mechanism for deterministic generation of entangled hybridity of the entangled hybrid states consisting of continuous variable (CV) and discrete variable (DV) states

Уровни генетической изменчивости и зараженности гельминтами в популяциях мелких млекопитающихOn the basis of the analysis of the state of the gene structure and parasitological situation

МОДЕЛЬ СТАТИСТИЧЕСКОГО И АВТОКОРРЕЛЯЦИОННОГО АНАЛИЗА И ЭКОНОМИЧЕСКАЯ МОДЕЛЬ ВАРИАБЕЛЬНОСТИ КАРДИОПЕРИОДОВ, ПРИМЕНЯЕМАЯ ПРИ ОРТОСТАТИЧЕСКОЙ ПРОБЕ В УСЛОВИЯХ ИЗМЕНЯЮЩЕГОСЯ КЛИМАТА У РАЗНЫХ ЭТНОСОВ В СИСТЕМЕ ЧЕЛОВЕК-МАШИНА when using variable methods to identify the physiological state of seafarers

Особенности комплекса параметров гемодинамики и их вариабельность у лиц юношеского возраста с разными типами кровообращенияResearches of typological features of blood circulation and their variabilities of youth were held

The nature of the unique precataclysmic variable V664 Cas with two-peaked balmer lines in its spectrum the characteristics of its radiation are consistent with the star being a cataclysmic variable with powerful

A search for periodic and quasi-periodic photometric behavior in the cataclysmic variable TT arietis out to study optical variability on timescales from minutes to weeks. The best-fit primary photometric

On describing bound states for a spin 1 particle in the external Coulomb field states. With the use of the Lorentz generalized condition in presence of the Coulomb field, we prove

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