391 research outputs found

    Atomistic Simulations of the Efficiencies of Ge and Pt Ion Implantation into Graphene

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    Recent success in the direct implantation of 74Ge+ ion, the heaviest atomic impurity to date, into monolayer graphene presents a general question of the efficiency of low-energy ion implantation technique for heavy atoms. A comparative computational study, using classical molecular dynamics, of low-energy Ge and Pt ions implantation into single- and double-layer graphene is presented. It confirms that the highest probability for the perfect substitutional doping of single-layer graphene, i.e., direct implanting of ion into monovacancy, can be achieved 80 eV and it reaches the value of 64% for Ge ions directed at 45Β° angle to graphene plane and 21% for Pt ion beam perpendicular to graphene. Implantation efficiency is strongly dependent on the angle of ion beam. The sputtering yield of carbon atoms is found to be lower for double layer of graphene, which has better protective properties against low-energy ion irradiation damage than a single graphene layer. In double-layer graphene, incident ions traveling in the direction perpendicular to graphene can be trapped between the layers with the highest efficiency above or equal to 80% in the energy range of 40–90 eV for Ge ions and above 90% in the energy range of 40–70 eV for Pt ions. The energy range corresponding to the efficient trapping of ions in double-layer graphene is shifted toward higher energies upon tilting of the angle of incident ion beam

    ΠŸΠžΠ’Π«Π¨Π•ΠΠ˜Π• Π­Π€Π€Π•ΠšΠ’Π˜Π’ΠΠžΠ‘Π’Π˜ ΠŸΠžΠ”ΠΠ’Π›Π•ΠΠ˜Π― ΠΠšΠ’Π˜Π’ΠΠ«Π₯ ΠŸΠžΠœΠ•Π₯ Π’ Π Π›Π‘ ΠŸΠ•Π Π•Π₯ВАВА Π’ΠžΠ—Π”Π£Π¨ΠΠ«Π₯ Π¦Π•Π›Π•Π™ Π’ Π Π•Π–Π˜ΠœΠ• ΠžΠ‘Π—ΠžΠ Π

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    The modified algorithm of the adaptive compensating of the active noise jamming, based on usage of the recurrence estimation of inverse covariance matrix of jamming in the course of an self-tuning is considered. The matrix estimation is formed by a method of a serial regression (SRM), a consequence application of a lemma about inversing of a matrix to differential – to the difference equation for a rounded estimation of direct covariance matrix of jamming (CMJ). The single estimation of straight line CMJ is formed as result dyad products of the instant vectors of noises in handling channels. In partial channels the adaptive transversal filters with the self-tuning on value of a signal of an aggregate error are implemented.In article skeleton diagrams of devices of the compensating implemented by various methods are resulted. Mathematical modeling of operation of the algorithms, implemented by a method of the least squares (criterion of a minimum RMS error) and a method of a serial regression is performed.Results of mathematical modeling of operation of the device of compensating of active noises jamming in the conditions of the active radio-electronic counteraction at multipath propagation of signals both non-identical amplitude and phase characteristics of channels of handling are resulted. Optimal values of technical parameters of devices of compensating of the active noises jamming providing obtaining of demanded values of coefficient of suppression are given. The comparative analysis of indexes of efficiency of classical and offered algorithms of compensating is made. Advantage of algorithm of compensating of the active noises jamming, using the recurrence estimation of a inverse covariance matrix of jamming is shown.The algorithm of functioning on the basis of SRM allows to lower essentially requirements to specialized VLSI (FPGA) at implementation is hardware – program complexes for preprocessing of the radar, radio communication and radio – navigation information in the conditions of influence of the active noises jamming in the presence of effects of multipath propagation of signals, in the presence of delay of signals on an antenna system aperture, and also at unremovable technological dispersion amplitude and phase characteristics of the microwave of channels of handling.РассматриваСтся ΠΌΠΎΠ΄ΠΈΡ„ΠΈΡ†ΠΈΡ€ΠΎΠ²Π°Π½Π½Ρ‹ΠΉ Π°Π»Π³ΠΎΡ€ΠΈΡ‚ΠΌ Π°Π΄Π°ΠΏΡ‚ΠΈΠ²Π½ΠΎΠΉ компСнсации Π°ΠΊΡ‚ΠΈΠ²Π½Ρ‹Ρ… ΡˆΡƒΠΌΠΎΠ²Ρ‹Ρ… ΠΏΠΎΠΌΠ΅Ρ…, основанный Π½Π° использовании Ρ€Π΅ΠΊΡƒΡ€Ρ€Π΅Π½Ρ‚Π½ΠΎΠΉ ΠΎΡ†Π΅Π½ΠΊΠΈ ΠΎΠ±Ρ€Π°Ρ‚Π½ΠΎΠΉ ΠΊΠΎΠ²Π°Ρ€ΠΈΠ°Ρ†ΠΈΠΎΠ½Π½ΠΎΠΉ ΠΌΠ°Ρ‚Ρ€ΠΈΡ†Ρ‹ ΠΏΠΎΠΌΠ΅Ρ… Π² процСссС самонастройки. ΠžΡ†Π΅Π½ΠΊΠ° ΠΌΠ°Ρ‚Ρ€ΠΈΡ†Ρ‹ формируСтся ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΎΠΌ ΠΏΠΎΡΠ»Π΅Π΄ΠΎΠ²Π°Ρ‚Π΅Π»ΡŒΠ½ΠΎΠΉ рСгрСссии (МПР), ΡΠ²Π»ΡΡŽΡ‰Π΅Π³ΠΎΡΡ слСдствиСм примСнСния Π»Π΅ΠΌΠΌΡ‹ ΠΎΠ± ΠΎΠ±Ρ€Π°Ρ‰Π΅Π½ΠΈΠΈ ΠΌΠ°Ρ‚Ρ€ΠΈΡ†Ρ‹ ΠΊ Π΄ΠΈΡ„Ρ„Π΅Ρ€Π΅Π½Ρ†ΠΈΠ°Π»ΡŒΠ½ΠΎ-разностному ΡƒΡ€Π°Π²Π½Π΅Π½ΠΈΡŽ для сглаТСнной ΠΎΡ†Π΅Π½ΠΊΠΈ прямой ΠΊΠΎΠ²Π°Ρ€ΠΈΠ°Ρ†ΠΈΠΎΠ½Π½ΠΎΠΉ ΠΌΠ°Ρ‚Ρ€ΠΈΡ†Ρ‹ ΠΏΠΎΠΌΠ΅Ρ… (КМП). Разовая ΠΎΡ†Π΅Π½ΠΊΠ° прямой КМП формируСтся ΠΊΠ°ΠΊ Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚ Π΄ΠΈΠ°Π΄Π½ΠΎΠ³ΠΎ произвСдСния ΠΌΠ³Π½ΠΎΠ²Π΅Π½Π½Ρ‹Ρ… Π²Π΅ΠΊΡ‚ΠΎΡ€ΠΎΠ² ΠΏΠΎΠΌΠ΅Ρ… Π² ΠΊΠ°Π½Π°Π»Π°Ρ… ΠΎΠ±Ρ€Π°Π±ΠΎΡ‚ΠΊΠΈ. Π’ ΠΏΠ°Ρ€Ρ†ΠΈΠ°Π»ΡŒΠ½Ρ‹Ρ… ΠΊΠ°Π½Π°Π»Π°Ρ… Ρ€Π΅Π°Π»ΠΈΠ·ΡƒΡŽΡ‚ΡΡ Π°Π΄Π°ΠΏΡ‚ΠΈΠ²Π½Ρ‹Π΅ Ρ‚Ρ€Π°Π½ΡΠ²Π΅Ρ€ΡΠ°Π»ΡŒΠ½Ρ‹Π΅ Ρ„ΠΈΠ»ΡŒΡ‚Ρ€Ρ‹ с самонастройкой ΠΏΠΎ Π²Π΅Π»ΠΈΡ‡ΠΈΠ½Π΅ сигнала суммарной ошибки. Π’ ΡΡ‚Π°Ρ‚ΡŒΠ΅ ΠΏΡ€ΠΈΠ²Π΅Π΄Π΅Π½Ρ‹ структурныС схСмы устройств компСнсации, Ρ€Π΅Π°Π»ΠΈΠ·ΠΎΠ²Π°Π½Π½Ρ‹Ρ… Ρ€Π°Π·Π»ΠΈΡ‡Π½Ρ‹ΠΌΠΈ способами.Π’Ρ‹ΠΏΠΎΠ»Π½Π΅Π½ΠΎ матСматичСскоС ΠΌΠΎΠ΄Π΅Π»ΠΈΡ€ΠΎΠ²Π°Π½ΠΈΠ΅ Ρ€Π°Π±ΠΎΡ‚Ρ‹ Π°Π»Π³ΠΎΡ€ΠΈΡ‚ΠΌΠΎΠ², Ρ€Π΅Π°Π»ΠΈΠ·ΠΎΠ²Π°Π½Π½ΠΎΠ³ΠΎ ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΎΠΌ Π½Π°ΠΈΠΌΠ΅Π½ΡŒΡˆΠΈΡ… ΠΊΠ²Π°Π΄Ρ€Π°Ρ‚ΠΎΠ² (ΠΊΡ€ΠΈΡ‚Π΅Ρ€ΠΈΠΉ ΠΌΠΈΠ½ΠΈΠΌΡƒΠΌΠ° срСднСквадратичСской ошибки) ΠΈ ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΎΠΌ ΠΏΠΎΡΠ»Π΅Π΄ΠΎΠ²Π°Ρ‚Π΅Π»ΡŒΠ½ΠΎΠΉ рСгрСссии.ΠŸΡ€ΠΈΠ²ΠΎΠ΄ΡΡ‚ΡΡ Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹ матСматичСского модСлирования Ρ€Π°Π±ΠΎΡ‚Ρ‹ устройства компСнсации ΠΏΠΎΠΌΠ΅Ρ… Π² условиях Π°ΠΊΡ‚ΠΈΠ²Π½ΠΎΠ³ΠΎ радиоэлСктронного противодСйствия ΠΏΡ€ΠΈ ΠΌΠ½ΠΎΠ³ΠΎΠ»ΡƒΡ‡Π΅Π²ΠΎΠΌ распространСнии сигналов ΠΈ Π½Π΅ΠΈΠ΄Π΅Π½Ρ‚ΠΈΡ‡Π½Ρ‹Ρ… Π°ΠΌΠΏΠ»ΠΈΡ‚ΡƒΠ΄Π½Ρ‹Ρ… ΠΈ Ρ„Π°Π·ΠΎΠ²Ρ‹Ρ… характСристиках ΠΊΠ°Π½Π°Π»ΠΎΠ² ΠΎΠ±Ρ€Π°Π±ΠΎΡ‚ΠΊΠΈ. Π”Π°Π½Ρ‹ ΠΎΠΏΡ‚ΠΈΠΌΠ°Π»ΡŒΠ½Ρ‹Π΅ значСния тСхничСских ΠΏΠ°Ρ€Π°ΠΌΠ΅Ρ‚Ρ€ΠΎΠ² устройств компСнсации ΠΏΠΎΠΌΠ΅Ρ…, ΠΎΠ±Π΅ΡΠΏΠ΅Ρ‡ΠΈΠ²Π°ΡŽΡ‰ΠΈΡ… ΠΏΠΎΠ»ΡƒΡ‡Π΅Π½ΠΈΠ΅ Ρ‚Ρ€Π΅Π±ΡƒΠ΅ΠΌΡ‹Ρ… Π²Π΅Π»ΠΈΡ‡ΠΈΠ½ коэффициСнта подавлСния. Π’Ρ‹ΠΏΠΎΠ»Π½Π΅Π½ ΡΡ€Π°Π²Π½ΠΈΡ‚Π΅Π»ΡŒΠ½Ρ‹ΠΉ Π°Π½Π°Π»ΠΈΠ· ΠΏΠΎΠΊΠ°Π·Π°Ρ‚Π΅Π»Π΅ΠΉ эффСктивности классичСского ΠΈ ΠΏΡ€Π΅Π΄Π»Π°Π³Π°Π΅ΠΌΠΎΠ³ΠΎ Π°Π»Π³ΠΎΡ€ΠΈΡ‚ΠΌΠΎΠ² компСнсации. Показано прСимущСство Π°Π»Π³ΠΎΡ€ΠΈΡ‚ΠΌΠ° компСнсации Π°ΠΊΡ‚ΠΈΠ²Π½Ρ‹Ρ… ΠΏΠΎΠΌΠ΅Ρ…, ΠΈΡΠΏΠΎΠ»ΡŒΠ·ΡƒΡŽΡ‰Π΅Π³ΠΎ Ρ€Π΅ΠΊΡƒΡ€Ρ€Π΅Π½Ρ‚Π½ΡƒΡŽ ΠΎΡ†Π΅Π½ΠΊΡƒ ΠΎΠ±Ρ€Π°Ρ‚Π½ΠΎΠΉ ΠΊΠΎΠ²Π°Ρ€ΠΈΠ°Ρ†ΠΈΠΎΠ½Π½ΠΎΠΉ ΠΌΠ°Ρ‚Ρ€ΠΈΡ†Ρ‹ ΠΏΠΎΠΌΠ΅Ρ….Алгоритм функционирования Π½Π° основС МПР позволяСт сущСствСнно ΡΠ½ΠΈΠ·ΠΈΡ‚ΡŒ трСбования ΠΊ спСциализированным Π‘Π‘Π˜Π‘ (ΠŸΠ›Π˜Π‘) ΠΏΡ€ΠΈ Ρ€Π΅Π°Π»ΠΈΠ·Π°Ρ†ΠΈΠΈ Π°ΠΏΠΏΠ°Ρ€Π°Ρ‚Π½ΠΎ-ΠΏΡ€ΠΎΠ³Ρ€Π°ΠΌΠΌΠ½Ρ‹Ρ… комплСксов для ΠΏΠ΅Ρ€Π²ΠΈΡ‡Π½ΠΎΠΉ ΠΎΠ±Ρ€Π°Π±ΠΎΡ‚ΠΊΠΈ Ρ€Π°Π΄ΠΈΠΎΠ»ΠΎΠΊΠ°Ρ†ΠΈΠΎΠ½Π½ΠΎΠΉ, радиосвязной ΠΈ Ρ€Π°Π΄ΠΈΠΎΠ½Π°Π²ΠΈΠ³Π°Ρ†ΠΈΠΎΠ½Π½ΠΎΠΉ ΠΈΠ½Ρ„ΠΎΡ€ΠΌΠ°Ρ†ΠΈΠΈ Π² условиях воздСйствия Π°ΠΊΡ‚ΠΈΠ²Π½Ρ‹Ρ… ΡˆΡƒΠΌΠΎΠ²Ρ‹Ρ… ΠΏΠΎΠΌΠ΅Ρ… ΠΏΡ€ΠΈ Π½Π°Π»ΠΈΡ‡ΠΈΠΈ эффСктов ΠΌΠ½ΠΎΠ³ΠΎΠ»ΡƒΡ‡Π΅Π²ΠΎΠ³ΠΎ распространСния сигналов, ΠΏΡ€ΠΈ Π½Π°Π»ΠΈΡ‡ΠΈΠΈ запаздывания сигналов ΠΏΠΎ раскрыву Π°Π½Ρ‚Π΅Π½Π½ΠΎΠΉ систСмы, Π° Ρ‚Π°ΠΊΠΆΠ΅ ΠΏΡ€ΠΈ нСустранимом тСхнологичСском разбросС Π°ΠΌΠΏΠ»ΠΈΡ‚ΡƒΠ΄Π½ΠΎ-Ρ„Π°Π·ΠΎΠ²Ρ‹Ρ… характСристик Π‘Π’Π§-Ρ‚Ρ€Π°ΠΊΡ‚Π° ΠΊΠ°Π½Π°Π»ΠΎΠ² ΠΎΠ±Ρ€Π°Π±ΠΎΡ‚ΠΊΠΈ

    Termination Reaction in the Anionic Polymerization of Methacrylonitrile

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    The anionic polymerization of methacrylonitrile initiated by triethylphosphine in dimethylformamide was studied. Experimental evidence for two mechanisms of termination reaction was obtained. By addition of water or alcohol in polymerizing system the rate of polymerization and molecular weight of polymethacrylon1itrile decrease, which proves the termination reaction to be bimolecular and proceed by interaction of the active carbanion with water or alcohol. The rate constant for termination of free anions with water was determined, k~,0 = 2.2 x 102 dm3 moP s-1β€’ The termination reaction could not be excluded by purification and prolonged drying of all components of the system, which indicates that the second mechanism of termination is operative as well. Conductivity measurements gave evidence for a monomolecular spontaneous reaction leading to deactivation of the anion

    ΠΠΠΠ›Π˜Π’Π˜Π§Π•Π‘ΠšΠ˜Π™ Π‘Π˜ΠΠ’Π•Π— ΠœΠ•Π’ΠžΠ”Π ΠΠΠ’Π•Π”Π•ΠΠ˜Π― Π‘Π’Π•Π Π₯Π—Π’Π£ΠšΠžΠ’ΠžΠ“Πž Π‘Π•Π‘ΠŸΠ˜Π›ΠžΠ’ΠΠžΠ“Πž Π›Π•Π’ΠΠ’Π•Π›Π¬ΠΠžΠ“Πž АППАРАВА НА ΠžΠ‘ΠΠžΠ’Π• ΠœΠΠžΠ“ΠžΠœΠ•Π ΠΠžΠ™ ΠΠ•Π›Π˜ΠΠ•Π™ΠΠžΠ™ Π”Π˜ΠΠΠœΠ˜Π§Π•Π‘ΠšΠžΠ™ ΠœΠžΠ”Π•Π›Π˜

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    A method of analytical synthesis of an optimal controller for the terminal control task of supersonic unmanned aerial vehicles based on synergetic approach to the design of control systems for nonlinear multidimensional dynamic objects is considered.The article provides analytical expressions describing the algorithm for control the velocity vector position of a supersonic UAV, the simulation results and the comparative analysis of the proposed control algorithm with the modified method of proportional navigation.РассматриваСтся аналитичСский синтСз ΠΌΠ΅Ρ‚ΠΎΠ΄Π° навСдСния для Ρ‚Π΅Ρ€ΠΌΠΈΠ½Π°Π»ΡŒΠ½ΠΎΠΉ Π·Π°Π΄Π°Ρ‡ΠΈ управлСния свСрхзвуковыми бСспилотными Π»Π΅Ρ‚Π°Ρ‚Π΅Π»ΡŒΠ½Ρ‹ΠΌΠΈ Π°ΠΏΠΏΠ°Ρ€Π°Ρ‚Π°ΠΌΠΈ Π½Π° основС синСргСтичСского ΠΏΠΎΠ΄Ρ…ΠΎΠ΄Π° ΠΊ ΠΏΡ€ΠΎΠ΅ΠΊΡ‚ΠΈΡ€ΠΎΠ²Π°Π½ΠΈΡŽ систСм управлСния Π½Π΅Π»ΠΈΠ½Π΅ΠΉΠ½Ρ‹ΠΌΠΈ ΠΌΠ½ΠΎΠ³ΠΎΠΌΠ΅Ρ€Π½Ρ‹ΠΌΠΈ динамичСскими ΠΎΠ±ΡŠΠ΅ΠΊΡ‚Π°ΠΌΠΈ. ΠœΠ΅Ρ‚ΠΎΠ΄ основан Π½Π° Π²Π²Π΅Π΄Π΅Π½ΠΈΠΈ Π² пространствС состояний синтСзируСмых систСм ΠΎΠΏΡ‚ΠΈΠΌΠ°Π»ΡŒΠ½Ρ‹Ρ… ΠΈΠ½Π²Π°Ρ€ΠΈΠ°Π½Ρ‚Π½Ρ‹Ρ… ΠΌΠ½ΠΎΠ³ΠΎΠΎΠ±Ρ€Π°Π·ΠΈΠΉ – Π°Ρ‚Ρ‚Ρ€Π°ΠΊΡ‚ΠΎΡ€ΠΎΠ², Π½Π° ΠΊΠΎΡ‚ΠΎΡ€Ρ‹Ρ… Π½Π°ΠΈΠ»ΡƒΡ‡ΡˆΠΈΠΌ ΠΎΠ±Ρ€Π°Π·ΠΎΠΌ ΡΠΎΠ³Π»Π°ΡΡƒΡŽΡ‚ΡΡ ΠΎΠ±Ρ‰ΠΈΠ΅ СстСствСнныС (энСргСтичСскиС, мСханичСскиС, баллистичСскиС ΠΈ Π΄Ρ€.) свойства ΠΎΠ±ΡŠΠ΅ΠΊΡ‚Π° ΠΈ частныС трСбования ΠΊΠΎΠ½ΠΊΡ€Π΅Ρ‚Π½ΠΎΠΉ тСхнологичСской Π·Π°Π΄Π°Ρ‡ΠΈ. ΠŸΡ€ΠΈ этом ΠΎΠ±Π΅ΡΠΏΠ΅Ρ‡ΠΈΠ²Π°ΡŽΡ‚ΡΡ ΠΆΠ΅Π»Π°Π΅ΠΌΡ‹Π΅ динамичСскиС характСристики ΠΈ гарантируСтся асимптотичСская ΡƒΡΡ‚ΠΎΠΉΡ‡ΠΈΠ²ΠΎΡΡ‚ΡŒ двиТСния систСмы ΠΎΠΏΡ‚ΠΈΠΌΠ°Π»ΡŒΠ½Ρ‹ΠΉ рСгулятор – ΠΎΠ±ΡŠΠ΅ΠΊΡ‚ управлСния.ΠŸΡ€ΠΈΠ²ΠΎΠ΄ΡΡ‚ΡΡ аналитичСскиС выраТСния, ΠΎΠΏΠΈΡΡ‹Π²Π°ΡŽΡ‰ΠΈΠ΅ Π°Π»Π³ΠΎΡ€ΠΈΡ‚ΠΌ управлСния ΠΏΠΎΠ»ΠΎΠΆΠ΅Π½ΠΈΠ΅ΠΌΠ²Π΅ΠΊΡ‚ΠΎΡ€Π° скорости свСрхзвукового бСспилотного Π»Π΅Ρ‚Π°Ρ‚Π΅Π»ΡŒΠ½ΠΎΠ³ΠΎ Π°ΠΏΠΏΠ°Ρ€Π°Ρ‚Π°, Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹ матСматичСского модСлирования ΠΈ ΡΡ€Π°Π²Π½ΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎΠ³ΠΎ Π°Π½Π°Π»ΠΈΠ·Π° ΠΏΡ€Π΅Π΄Π»Π°Π³Π°Π΅ΠΌΠΎΠ³ΠΎ Π°Π»Π³ΠΎΡ€ΠΈΡ‚ΠΌΠ° управлСния с ΠΌΠΎΠ΄ΠΈΡ„ΠΈΡ†ΠΈΡ€ΠΎΠ²Π°Π½Π½Ρ‹ΠΌ ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΎΠΌ ΠΏΡ€ΠΎΠΏΠΎΡ€Ρ†ΠΈΠΎΠ½Π°Π»ΡŒΠ½ΠΎΠΉ Π½Π°Π²ΠΈΠ³Π°Ρ†ΠΈΠΈ

    Permanent annihilation of thermally activated defects which limit the lifetime of float-zone silicon

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    We have observed very large changes in the minority carrier lifetime when high purity float-zone (FZ) silicon wafers are subject to heat-treatments in the range of 200– 1100˚C. Recombination centres were found to become activated upon annealing at 450–700˚C, causing significant reductions in the bulk lifetime, detrimental for high efficiency solar cells and stable high powered devices. Photoluminescence imaging of wafers annealed at 500˚C revealed concentric circular patterns, with lower lifetimes occurring in the centre, and higher lifetimes around the periphery. Deep level transient spectroscopy measurements on samples extracted from the centre of an n-type FZ silicon wafer annealed at 500˚C revealed a large variety of defects with activation energies ranging between 0.16– 0.36eV. Our measurements indicate that vacancy related defects are causing the severe degradation in lifetime when FZ wafers are annealed at 450–700˚C. Upon annealing FZ silicon at temperatures >800Β°C, the lifetime is completely recovered, whereby the defect-rich regions vanish and do not reappear (permanently annihilated). Our results indicate that, in general, as-grown FZ silicon should not be assumed to be defect lean, nor can it be assumed that the bulk lifetime will remain stable during thermal processing, unless annealed at temperatures >1000Β°C

    The Dynamics of Zeroth-Order Ultrasensitivity: A Critical Phenomenon in Cell Biology

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    It is well known since the pioneering work of Goldbeter and Koshland [Proc. Natl. Acad. Sci. USA, vol. 78, pp. 6840-6844 (1981)] that cellular phosphorylation- dephosphorylation cycle (PdPC), catalyzed by kinase and phosphatase under saturated condition with zeroth order enzyme kinetics, exhibits ultrasensitivity, sharp transition. We analyse the dynamics aspects of the zeroth order PdPC kinetics and show a critical slowdown akin to the phase transition in condensed matter physics. We demonstrate that an extremely simple, though somewhat mathematically "singular" model is a faithful representation of the ultrasentivity phenomenon. The simplified mathematical model will be valuable, as a component, in developing complex cellular signaling network theory as well as having a pedagogic value.Comment: 8 pages, 3 figure

    90 Years to the Society of Anatomists, Histologists and Embryologists

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    Scientific research of the members of society in 90 years are diverse and they are numerous, they dedicated to questions of ethnic and integrative anthropology, to study of versions and anomalies in different systems of the organs of man, to study of cardiovascular and nervous systems in the aspect dependent on age and with the pathology, to development and the regeneration of the cardiovascular system, to questions of anatomical and anthropological equipment, comparative and veterinary anatomy. The members of society actively participated in the work of the forums of morphologists and clinicians. Was formed the sufficiently authoritative Rostov school of morphologists, whose representatives led departments in Russia cities and abroad

    Energy state distributions of the P(b) centers at the (100), (110), and (111) Si/SiO(2) interfaces investigated by Laplace deep level transient spectroscopy

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    The energy distribution of the P(b) centers at the Si/SiO(2) interface has been determined using isothermal laplace deep level transient spectroscopy. For the (111) and (110) interface orientations, the distributions are similar and centered at 0.38 eV below the silicon conduction band. This is consistent with only P(b0) states being present. For the (100) orientation, two types of the interface states are observed: one similar to the (111) and (110) orientations while the other has a negative-U character in which the emission rate versus surface potential dependence is qualitatively different from that observed for P(b0) and is presumed to be P(b1). (C) 2008 American Institute of Physics. (DOI: 10.1063/1.2939001

    ΠŸΠžΠ’Π«Π¨Π•ΠΠ˜Π• ВОЧНОБВИ ΠžΠ¦Π•ΠΠ˜Π’ΠΠΠ˜Π― ΠšΠžΠžΠ Π”Π˜ΠΠΠ’ ΠžΠ‘ΠͺΠ•ΠšΠ’Π Π’ ΠœΠΠžΠ“ΠžΠŸΠžΠ—Π˜Π¦Π˜ΠžΠΠΠžΠ™ Π ΠΠ”Π˜ΠžΠ›ΠžΠšΠΠ¦Π˜ΠžΠΠΠžΠ™ Π‘Π˜Π‘Π’Π•ΠœΠ• Π‘ ΠŸΠ Π˜Π•ΠœΠΠ«Πœ ПУНКВОМ Π’ΠžΠ—Π”Π£Π¨ΠΠžΠ“Πž Π‘ΠΠ—Π˜Π ΠžΠ’ΠΠΠ˜Π―

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    The dependence of the accuracy of the object's coordinates estimation on the relative position of transmitting and receiving points of the multi-position radar system was studied. A way to increase of the accuracy of the object's coordinates estimation for small elevation angles by placement of the one receiving positions on the aerial vehicle was proposed.ИсслСдована Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡ‚ΡŒ точности ΠΎΡ†Π΅Π½ΠΊΠΈ ΠΊΠΎΠΎΡ€Π΄ΠΈΠ½Π°Ρ‚ ΠΎΠ±ΡŠΠ΅ΠΊΡ‚Π° ΠΎΡ‚ Π²Π·Π°ΠΈΠΌΠ½ΠΎΠ³ΠΎ располоТСния ΠΏΠ΅Ρ€Π΅Π΄Π°ΡŽΡ‰Π΅Π³ΠΎ ΠΈ ΠΏΡ€ΠΈΠ΅ΠΌΠ½Ρ‹Ρ… ΠΏΡƒΠ½ΠΊΡ‚ΠΎΠ² суммарно-разностно-Π΄Π°Π»ΡŒΠ½ΠΎΠΌΠ΅Ρ€Π½ΠΎΠΉ ΠΌΠ½ΠΎΠ³ΠΎΠΏΠΎΠ·ΠΈΡ†ΠΈΠΎΠ½Π½ΠΎΠΉ Ρ€Π°Π΄ΠΈΠΎΠ»ΠΎΠΊΠ°Ρ†ΠΈΠΎΠ½Π½ΠΎΠΉ систСмы (ΠœΠŸΠ Π›Π‘). ΠŸΡ€Π΅Π΄Π»ΠΎΠΆΠ΅Π½ способ ΠΏΠΎΠ²Ρ‹ΡˆΠ΅Π½ΠΈΡ точности оцСнивания ΠΊΠΎΠΎΡ€Π΄ΠΈΠ½Π°Ρ‚ для ΠΌΠ°Π»Ρ‹Ρ… ΡƒΠ³Π»ΠΎΠ² мСста Π·Π° счСт располоТСния ΠΎΠ΄Π½ΠΎΠΉ ΠΈΠ· ΠΏΠΎΠ·ΠΈΡ†ΠΈΠΉ Π½Π° Π»Π΅Ρ‚Π°Ρ‚Π΅Π»ΡŒΠ½ΠΎΠΌ срСдствС
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