151 research outputs found

    Implementation of Fault-tolerant Quantum Logic Gates via Optimal Control

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    The implementation of fault-tolerant quantum gates on encoded logic qubits is considered. It is shown that transversal implementation of logic gates based on simple geometric control ideas is problematic for realistic physical systems suffering from imperfections such as qubit inhomogeneity or uncontrollable interactions between qubits. However, this problem can be overcome by formulating the task as an optimal control problem and designing efficient algorithms to solve it. In particular, we can find solutions that implement all of the elementary logic gates in a fixed amount of time with limited control resources for the five-qubit stabilizer code. Most importantly, logic gates that are extremely difficult to implement using conventional techniques even for ideal systems, such as the T-gate for the five-qubit stabilizer code, do not appear to pose a problem for optimal control.Comment: 18 pages, ioptex, many figure

    Photon storage in Lambda-type optically dense atomic media. II. Free-space model

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    In a recent paper [Gorshkov et al., Phys. Rev. Lett. 98, 123601 (2007)], we presented a universal physical picture for describing a wide range of techniques for storage and retrieval of photon wave packets in Lambda-type atomic media in free space, including the adiabatic reduction of the photon group velocity, pulse-propagation control via off-resonant Raman techniques, and photon-echo based techniques. This universal picture produced an optimal control strategy for photon storage and retrieval applicable to all approaches and yielded identical maximum efficiencies for all of them. In the present paper, we present the full details of this analysis as well some of its extensions, including the discussion of the effects of non-degeneracy of the two lower levels of the Lambda system. The analysis in the present paper is based on the intuition obtained from the study of photon storage in the cavity model in the preceding paper [Gorshkov et al., Phys. Rev. A 76, 033804 (2007)].Comment: 26 pages, 8 figures. V2: significant changes in presentation, new references, higher resolution of figure

    Quantum control theory for coupled 2-electron dynamics in quantum dots

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    We investigate optimal control strategies for state to state transitions in a model of a quantum dot molecule containing two active strongly interacting electrons. The Schrodinger equation is solved nonperturbatively in conjunction with several quantum control strategies. This results in optimized electric pulses in the THz regime which can populate combinations of states with very short transition times. The speedup compared to intuitively constructed pulses is an order of magnitude. We furthermore make use of optimized pulse control in the simulation of an experimental preparation of the molecular quantum dot system. It is shown that exclusive population of certain excited states leads to a complete suppression of spin dephasing, as was indicated in Nepstad et al. [Phys. Rev. B 77, 125315 (2008)].Comment: 24 pages, 9 figure

    Π§Π˜Π‘Π›Π•ΠΠΠžΠ• И ΠΠΠΠ›Π˜Π’Π˜Π§Π•Π‘ΠšΠžΠ• Π Π•Π¨Π•ΠΠ˜Π― ΠšΠ ΠΠ•Π’ΠžΠ™ Π—ΠΠ”ΠΠ§Π˜ Π”Π›Π― Π£Π ΠΠ’ΠΠ•ΠΠ˜Π― ΠŸΠΠ ΠΠ‘ΠžΠ›Π˜Π§Π•Π‘ΠšΠžΠ“Πž ВИПА Π’ ΠΠ•Π¦Π˜Π›Π˜ΠΠ”Π Π˜Π§Π•Π‘ΠšΠžΠ™ ΠžΠ‘Π›ΠΠ‘Π’Π˜

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    The article presents comparative analysis of the non-steady heat transfer problem solutions in the area of the border moving according to the law t under the conditions of temperature heating. The solutions were obtained using the method of difference schemes and analytically.Π’ настоящСй ΡΡ‚Π°Ρ‚ΡŒΠ΅ ΠΏΡ€ΠΎΠ²Π΅Π΄Π΅Π½ ΡΡ€Π°Π²Π½ΠΈΡ‚Π΅Π»ΡŒΠ½Ρ‹ΠΉ Π°Π½Π°Π»ΠΈΠ· Ρ€Π΅ΡˆΠ΅Π½ΠΈΠΉ Π·Π°Π΄Π°Ρ‡ΠΈ нСстационарной Ρ‚Π΅ΠΏ-лопроводности Π² области с Π³Ρ€Π°Π½ΠΈΡ†Π΅ΠΉ, двиТущСйся ΠΏΠΎ Π·Π°ΠΊΠΎΠ½Ρƒ , Π² условиях Ρ‚Π΅ΠΌΠΏΠ΅Ρ€Π°Ρ‚ΡƒΡ€Π½ΠΎΠ³ΠΎ Π½Π°Π³Ρ€Π΅Π²Π°. РСшСния ΠΏΠΎΠ»ΡƒΡ‡Π΅Π½Ρ‹ с ΠΏΠΎΠΌΠΎΡ‰ΡŒΡŽ ΠΌΠ΅Ρ‚ΠΎΠ΄Π° разностных схСм ΠΈ аналитичСски

    Mother-fetus immunogenetic dialogue as a factor of progeny immune system development

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    Despite the advances in medicine, about 4 million children under the age of 6 months die annually around the world due to infection, which is 450 deaths per hour (UNISEF, 2009). The degree of development of the immune system of children born in time is determined by many factors, including the immunogenetic similarity or difference of mother and fetus organisms, which, in turn, is due to the genotypes of mating pairs, as well as the selection of surrogate mothers during in vitro fertilization. From our review of the literature, it follows that immunogenetic interactions of mother and fetus organisms, which occur at all stages of pre- and postnatal development, have a signifcant effect on the resistance of offspring to infections and allergens. Before implantation, the mother’s immune responses are formed under the influence of semen fluid antigens, leukocytes and cytokines, as well as under the influence of the genes of the major histocompatibility complex, which are expressed in embryos at the stage of two cells. After implantation, transplacental transfer of immunoglobulins and immunocompetent cells becomes of immunomodulating importance. It is important to emphasize that, although substances with a high molecular weight usually do not pass through the placenta, this rule does not apply to immunoglobulin G (IgG), which, with a molecular weight of about 160 kDa, overcomes the transplacental barrier due to binding to the fetal Fc receptor. The level of IgG in newborns usually correlates with the level of maternal antibodies. During the period of natural feeding, the immune protection of newborns is provided by the mechanisms of innate immunity and the factors of humoral immunity of mothers. It has been shown that immunoglobulins from the milk of many animal species are transferred through the neonatal intestinal epithelium to the blood. Since breast milk contains large amounts of various immunoactive components, including proteins, cytokines, hormones, immunoglobulins, exosomes containing micro-RNA, and viable immune cells, the immunomodulating effects of breast milk persist even after elimination of maternal immunoglobulins from the blood of the offspring, up to maturation. Analysis of a large body of experimental data shows that the study of mechanisms of β€œmotherfetus” and β€œmother-newborn” interactions are the basis of a knowledge base needed to fnd means of life-long directed modulation of the descendants’ immune status

    The termal deformation reducing in sheet metal at manufacturing parts by CNC cutting machines

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    In various industries for the manufacturing of parts (workpieces) from sheet metal the CNC machines for thermal cutting (laser/plasma/gas cutting) are used. During process of thermal cutting, various deformations of the metal can occur, that cause the distortion of the geometric forms and sizes of the cut parts. These distortions are caused both by the uneven distribution of temperature in the sheet, and by certain geometric characteristics of the cutting process. Geometric characteristics are determined by the set sequence (order) of cutting of figured parts, as well as by selecting the piercing points of sheet material, i.e. the places of inserting the tool into the material. Previously, the authors formulated heuristic geometric rules, that allow reducing the value of geometric deformations of parts produced by the CNC cutting machines. To comply with these rules, users of Computer-Aided Design (CAM) systems that are used to generate NC programs, have to use interactive design methods. One of these rules (so-called "Part Hardness Rule") refers to the selecting the location of points for inserting (piercing) a CNC machine tool into the material. The paper describes a model based on the use of the heat conduction equation, which makes it possible to calculate the temperature of the sheet material at each moment of cutting process. The computational experiments showed that the points, which according to the "Part Hardness Rule" can't be used for piercing, have a higher material temperature than the points that satisfy this rule. In the paper the results of the computational experiments are given. Another rule (socalled "Sheet Hardness Rule"), which also reduces the deformation of the material during thermal cutting, refers to the order of parts cutting from the sheet. A heuristic algorithm that automatically generates the order of cutting parts that satisfy the rules of "Part Hardness" and of "Sheet Hardness" is developed. Developed software allows us to abandon the interactive methods of the NC programs generation for the thermal cutting of figured parts on CNC machines. Β© 2019 IOP Publishing Ltd. All rights reserved.Russian Foundation for Basic Research,Β RFBRThe work was supported by the Russian Foundation for Basic Research (grant 19-01-00573)

    Π Π°Π·Ρ€Π°Π±ΠΎΡ‚ΠΊΠ° микронасосной систСмы для ΠΏΠΎΠ΄Π΄Π΅Ρ€ΠΆΠΊΠΈ кровообращСния

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    Introduction. Support systems currently used in modern cardiac surgery to provide partial or complete, permanent or temporary replacement of cardiac function are frequently characterized by large dimensions, thus requiring major surgical interventions. Low invasiveness can be ensured by reducing the size of the implanted part of such systems, allowing these devices to be inserted through the femoral artery.Aim. Development of a minimally invasive micropump system to support blood circulation.Materials and methods. Based on the analysis of implementation of micropump circulatory support systems (MCSS), the configuration, operational principles and main components of such a system were determined. When designing a micropump, as a unit defining the weight and size parameters of the entire system, numerical and experimental methods were used to optimize its flow path based on the condition of minimizing blood injury and thrombus formation. The lubrication and cooling system was developed by solving the thermodynamic problem of heat removal. The electronic control unit was developed on the basis of accumulated experience in the design and operation of control units for circulatory support systems.Results. A micropump with a diameter of 6.5 mm and a length of 43 mm with the required hydro- and hemodynamic parameters was designed. The device ensures minimal trauma and thrombus formation. The main MCSS parameters, as well as its main components (electric drives, lubrication and cooling systems), were defined. The configuration and operational principles of the electronic control unit (ECU), consisting in a microprocessor-based control system with feedback, were developed. The ECU built-in software manages the rotational speed of the electric drives of the micropump and coolant supply pump in the required range. In addition, the software is used to measure, display and register the MCSS operational parameters, as well as to monitor their operation in the required ranges and to exchange data between the ECU and the PC.Conclusion. All the necessary documentation for the MCSS nodes and components was prepared. These nodes and components ensure the hydro- and hemodynamic parameters required for the use of the developed minimally invasive micropump system. Future work will address the stages of MCSS assembly and debugging.Π’Π²Π΅Π΄Π΅Π½ΠΈΠ΅. Π’ соврСмСнной ΠΊΠ°Ρ€Π΄ΠΈΠΎΡ…ΠΈΡ€ΡƒΡ€Π³ΠΈΠΈ для обСспСчСния частичной ΠΈΠ»ΠΈ ΠΏΠΎΠ»Π½ΠΎΠΉ, постоянной ΠΈΠ»ΠΈ Π²Ρ€Π΅ΠΌΠ΅Π½Π½ΠΎΠΉ Π·Π°ΠΌΠ΅Π½Ρ‹ Ρ„ΡƒΠ½ΠΊΡ†ΠΈΠΈ сСрдца ΠΏΡ€ΠΈΠΌΠ΅Π½ΡΡŽΡ‚ΡΡ систСмы ΠΏΠΎΠ΄Π΄Π΅Ρ€ΠΆΠΊΠΈ, ΠΈΠΌΠ΅ΡŽΡ‰ΠΈΠ΅ Ρ€Π°Π·ΠΌΠ΅Ρ€Ρ‹, Ρ‚Ρ€Π΅Π±ΡƒΡŽΡ‰ΠΈΠ΅ провСдСния ΡΠ΅Ρ€ΡŒΠ΅Π·Π½ΠΎΠΉ хирургичСской ΠΎΠΏΠ΅Ρ€Π°Ρ†ΠΈΠΈ. Для обСспСчСния ΠΌΠ°Π»ΠΎΠΉ инвазивности трСбуСтся сущСствСнно ΡƒΠΌΠ΅Π½ΡŒΡˆΠΈΡ‚ΡŒ Ρ€Π°Π·ΠΌΠ΅Ρ€Ρ‹ ΠΈΠΌΠΏΠ»Π°Π½Ρ‚ΠΈΡ€ΡƒΠ΅ΠΌΠΎΠΉ части систСмы, Ρ‡Ρ‚ΠΎ ΠΏΠΎΠ·Π²ΠΎΠ»ΠΈΡ‚ Π²Π²ΠΎΠ΄ΠΈΡ‚ΡŒ эти устройства Ρ‡Π΅Ρ€Π΅Π· Π±Π΅Π΄Ρ€Π΅Π½Π½ΡƒΡŽ Π°Ρ€Ρ‚Π΅Ρ€ΠΈΡŽ.ЦСль Ρ€Π°Π±ΠΎΡ‚Ρ‹. Π Π°Π·Ρ€Π°Π±ΠΎΡ‚ΠΊΠ° ΠΌΠ°Π»ΠΎΠΈΠ½Π²Π°Π·ΠΈΠ²Π½ΠΎΠΉ микронасосной систСмы для ΠΏΠΎΠ΄Π΄Π΅Ρ€ΠΆΠΊΠΈ кровообращСния.ΠœΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π»Ρ‹ ΠΈ ΠΌΠ΅Ρ‚ΠΎΠ΄Ρ‹. На основС Π°Π½Π°Π»ΠΈΠ·Π° Ρ‚Π΅Ρ…Π½ΠΎΠ»ΠΎΠ³ΠΈΠΈ примСнСния систСмы ΠΏΠΎΠ΄Π΄Π΅Ρ€ΠΆΠΊΠΈ кровообращСния (МБПК) Ρ€Π°Π·Ρ€Π°Π±ΠΎΡ‚Π°Π½ Π΅Π΅ состав, ΠΏΡ€ΠΈΠ½Ρ†ΠΈΠΏ Ρ€Π°Π±ΠΎΡ‚Ρ‹, спроСктированы основныС Π΅Π΅ ΡƒΠ·Π»Ρ‹ ΠΈ элСмСнты. ΠŸΡ€ΠΈ ΠΏΡ€ΠΎΠ΅ΠΊΡ‚ΠΈΡ€ΠΎΠ²Π°Π½ΠΈΠΈ микронасоса ΠΊΠ°ΠΊ ΡƒΠ·Π»Π°, ΠΎΠΏΡ€Π΅Π΄Π΅Π»ΡΡŽΡ‰Π΅Π³ΠΎ массогабаритныС ΠΏΠ°Ρ€Π°ΠΌΠ΅Ρ‚Ρ€Ρ‹ всСй систСмы, ΠΈΡΠΏΠΎΠ»ΡŒΠ·ΡƒΡŽΡ‚ΡΡ числСнныС ΠΈ ΡΠΊΡΠΏΠ΅Ρ€ΠΈΠΌΠ΅Π½Ρ‚Π°Π»ΡŒΠ½Ρ‹Π΅ ΠΌΠ΅Ρ‚ΠΎΠ΄Ρ‹ ΠΎΠΏΡ‚ΠΈΠΌΠΈΠ·Π°Ρ†ΠΈΠΈ Π΅Π³ΠΎ ΠΏΡ€ΠΎΡ‚ΠΎΡ‡Π½ΠΎΠΉ части ΠΈΠ· условия ΠΌΠΈΠ½ΠΈΠΌΠΈΠ·Π°Ρ†ΠΈΠΈ Ρ‚Ρ€Π°Π²ΠΌΡ‹ ΠΊΡ€ΠΎΠ²ΠΈ ΠΈ тромбообразования. ΠŸΡ€ΠΈ Ρ€Π°Π·Ρ€Π°Π±ΠΎΡ‚ΠΊΠ΅ систСмы смазки ΠΈ охлаТдСния Ρ€Π΅ΡˆΠ°Π»Π°ΡΡŒ тСрмодинамичСская Π·Π°Π΄Π°Ρ‡Π° ΠΏΠΎ ΠΎΠ±Π΅ΡΠΏΠ΅Ρ‡Π΅Π½ΠΈΡŽ ΠΎΡ‚Π²ΠΎΠ΄Π° Ρ‚Π΅ΠΏΠ»Π°. Π­Π»Π΅ΠΊΡ‚Ρ€ΠΎΠ½Π½Ρ‹ΠΉ Π±Π»ΠΎΠΊ управлСния Ρ€Π°Π·Ρ€Π°Π±ΠΎΡ‚Π°Π½ Π½Π° основании Π½Π°ΠΊΠΎΠΏΠ»Π΅Π½Π½ΠΎΠ³ΠΎ ΠΎΠΏΡ‹Ρ‚Π° проСктирования ΠΈ эксплуатации Π±Π»ΠΎΠΊΠΎΠ² управлСния клиничСски примСняСмых систСм Π²ΡΠΏΠΎΠΌΠΎΠ³Π°Ρ‚Π΅Π»ΡŒΠ½ΠΎΠ³ΠΎ кровообращСния.Π Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹. Π‘ΠΏΡ€ΠΎΠ΅ΠΊΡ‚ΠΈΡ€ΠΎΠ²Π°Π½ микронасос Π΄ΠΈΠ°ΠΌΠ΅Ρ‚Ρ€ΠΎΠΌ 6,5 ΠΌΠΌ ΠΈ Π΄Π»ΠΈΠ½ΠΎΠΉ 43 ΠΌΠΌ с Ρ‚Ρ€Π΅Π±ΡƒΠ΅ΠΌΡ‹ΠΌΠΈ Π³Π΅ΠΌΠΎ- ΠΈ гидродинамичСскими ΠΏΠ°Ρ€Π°ΠΌΠ΅Ρ‚Ρ€Π°ΠΌΠΈ, ΠΎΠ±Π΅ΡΠΏΠ΅Ρ‡ΠΈΠ²Π°ΡŽΡ‰ΠΈΠΉ ΠΌΠΈΠ½ΠΈΠΌΠ°Π»ΡŒΠ½ΡƒΡŽ Ρ‚Ρ€Π°Π²ΠΌΡƒ ΠΈ Ρ‚Ρ€ΠΎΠΌΠ±ΠΎΠΎΠ±Ρ€Π°Π·ΠΎΠ²Π°Π½ΠΈΠ΅. ΠžΠΏΡ€Π΅Π΄Π΅Π»Π΅Π½Ρ‹ основныС ΠΏΠ°Ρ€Π°ΠΌΠ΅Ρ‚Ρ€Ρ‹ ΠΈ спроСктированы ΡƒΠ·Π»Ρ‹ ΠΈ элСмСнты МБПК (элСктроприводы, систСма смазки ΠΈ охлаТдСния). Π Π°Π·Ρ€Π°Π±ΠΎΡ‚Π°Π½ состав ΠΈ ΠΏΡ€ΠΈΠ½Ρ†ΠΈΠΏ Ρ€Π°Π±ΠΎΡ‚Ρ‹ элСктронного Π±Π»ΠΎΠΊΠ° управлСния (Π­Π‘Π£), ΠΊΠΎΡ‚ΠΎΡ€Ρ‹ΠΉ прСдставляСт собой ΠΌΠΈΠΊΡ€ΠΎΠΏΡ€ΠΎΡ†Π΅ΡΡΠΎΡ€Π½ΡƒΡŽ систСму управлСния МБПК с ΠΎΠ±Ρ€Π°Ρ‚Π½ΠΎΠΉ связью. ВстроСнноС ΠΏΡ€ΠΎΠ³Ρ€Π°ΠΌΠΌΠ½ΠΎΠ΅ обСспСчСниС Π­Π‘Π£ позволяСт ΡƒΠΏΡ€Π°Π²Π»ΡΡ‚ΡŒ частотой вращСния элСктроприводов микронасоса ΠΈ насоса ΠΏΠΎΠ΄Π°Ρ‡ΠΈ ΠΎΡ…Π»Π°ΠΆΠ΄Π°ΡŽΡ‰Π΅ΠΉ Тидкости Π² Ρ‚Ρ€Π΅Π±ΡƒΠ΅ΠΌΠΎΠΌ Π΄ΠΈΠ°ΠΏΠ°Π·ΠΎΠ½Π΅, ΠΈΠ·ΠΌΠ΅Ρ€ΡΡ‚ΡŒ, ΠΎΡ‚ΠΎΠ±Ρ€Π°ΠΆΠ°Ρ‚ΡŒ, Ρ€Π΅Π³ΠΈΡΡ‚Ρ€ΠΈΡ€ΠΎΠ²Π°Ρ‚ΡŒ Ρ€Π΅ΠΆΠΈΠΌΠ½Ρ‹Π΅ ΠΏΠ°Ρ€Π°ΠΌΠ΅Ρ‚Ρ€Ρ‹ Ρ€Π°Π±ΠΎΡ‚Ρ‹ МБПК, Π° Ρ‚Π°ΠΊΠΆΠ΅ ΠΎΡΡƒΡ‰Π΅ΡΡ‚Π²Π»ΡΡ‚ΡŒ ΠΊΠΎΠ½Ρ‚Ρ€ΠΎΠ»ΡŒ ΠΈΡ… Ρ€Π°Π±ΠΎΡ‚Ρ‹ Π² Ρ‚Ρ€Π΅Π±ΡƒΠ΅ΠΌΡ‹Ρ… Π΄ΠΈΠ°ΠΏΠ°Π·ΠΎΠ½Π°Ρ…, ΠΎΠ±ΠΌΠ΅Π½ΠΈΠ²Π°Ρ‚ΡŒΡΡ Π΄Π°Π½Π½Ρ‹ΠΌΠΈ ΠΌΠ΅ΠΆΠ΄Ρƒ Π­Π‘Π£ ΠΈ ΠΊΠΎΠΌΠΏΡŒΡŽΡ‚Π΅Ρ€ΠΎΠΌ.Π—Π°ΠΊΠ»ΡŽΡ‡Π΅Π½ΠΈΠ΅. ΠŸΠΎΠ΄Π³ΠΎΡ‚ΠΎΠ²Π»Π΅Π½Π° докумСнтация Π½Π° ΡƒΠ·Π»Ρ‹ ΠΈ элСмСнты МБПК, ΠΎΠ±Π΅ΡΠΏΠ΅Ρ‡ΠΈΠ²Π°ΡŽΡ‰ΠΈΠ΅ Ρ‚Ρ€Π΅Π±ΡƒΠ΅ΠΌΡ‹Π΅ Π³ΠΈΠ΄Ρ€ΠΎ- ΠΈ гСмодинамичСскиС ΠΏΠ°Ρ€Π°ΠΌΠ΅Ρ‚Ρ€Ρ‹, Π½Π΅ΠΎΠ±Ρ…ΠΎΠ΄ΠΈΠΌΡ‹Π΅ для примСнСния микронасосной ΠΌΠ°Π»ΠΎΠΈΠ½Π²Π°Π·ΠΈΠ²Π½ΠΎΠΉ систСмы, Ρ‡Ρ‚ΠΎ позволяСт ΠΏΠ΅Ρ€Π΅ΠΉΡ‚ΠΈ ΠΊ сборкС ΠΈ ΠΎΡ‚Π»Π°Π΄ΠΊΠ΅ ΡƒΠ·Π»ΠΎΠ² ΠΈ элСмСнтов МБПК Π² Ρ†Π΅Π»ΠΎΠΌ

    The dynamic model of enterprise revenue management

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    The article presents the dynamic model of enterprise revenue management. This model is based on the quadratic criterion and linear control law. The model is founded on multiple regression that links revenues with the financial performance of the enterprise. As a result, optimal management is obtained so as to provide the given enterprise revenue, namely, the values of financial indicators that ensure the planned profit of the organization are acquired

    Stripes in Doped Antiferromagnets: Single-Particle Spectral Weight

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    Recent photoemission (ARPES) experiments on cuprate superconductors provide important guidelines for a theory of electronic excitations in the stripe phase. Using a cluster perturbation theory, where short-distance effects are accounted for by exact cluster diagonalization and long-distance effects by perturbation (in the hopping), we calculate the single-particle Green's function for a striped t-J model. The data obtained quantitatively reproduce salient (ARPES-) features and may serve to rule out "bond-centered" in favor of "site-centered" stripes.Comment: final version as appeared in PRL; (c) 2000 The American Physical Society; 4 pages, 4 figure

    Carbon nanotube-based quantum pump in the presence of superconducting lead

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    Parametric electron pump through superconductor-carbon-nanotube based molecular devices was investigated. It is found that a dc current, which is assisted by resonant Andreev reflection, can be pumped out from such molecular device by a cyclic variation of two gate voltages near the nanotube. The pumped current can be either positive or negative under different system parameters. Due to the Andreev reflection, the pumped current has the double peak structure around the resonant point. The ratio of pumped current of N-SWNT-S system to that of N-SWNT-N system (I^{NS}/I^N) is found to approach four in the weak pumping regime near the resonance when there is exactly one resonant level at Fermi energy inside the energy gap. Numerical results confirm that in the weak pumping regime the pumped current is proportional to the square of the pumping amplitude V_p, but in the strong pumping regime the pumped current has the linear relation with V_p. Our numerical results also predict that pumped current can be obtained more easily by using zigzag tube than by using armchair tube
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