Artículos de revistas: "Mesoscopics"

1

Galperin, Yu y V. I. Kozub. "Classical Mesoscopics". Europhysics Letters (EPL) 15, n.º 6 (15 de julio de 1991): 631–35. http://dx.doi.org/10.1209/0295-5075/15/6/012.

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2

GREEN, FREDERICK y MUKUNDA P. DAS. "NOISE AND TRANSPORT IN MESOSCOPICS: PHYSICS BEYOND THE LANDAUER–BÜTTIKER FORMALISM". Fluctuation and Noise Letters 05, n.º 01 (marzo de 2005): C1—C14. http://dx.doi.org/10.1142/s0219477505002355.

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The standard physical model of contemporary mesoscopic noise and transport consists in a phenomenologically based approach, proposed originally by Landauer and since continued and amplified by Büttiker, Imry and others. Throughout all the years of its gestation and growth, it is surprising that the Landauer–Büttiker approach to mesoscopics has matured with scant attention to the conserving properties lying at its roots: that is, at the level of actual microscopic principles. We systematically apply the sum rules for the electron gas to clarify the issue of conservation within the standard model of mesoscopic conduction. Noise, as observed in quantum point contacts, provides the vital clue.

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3

Kroy, Klaus y Erwin Frey. "Focus on soft mesoscopics: physics for biology at a mesoscopic scale". New Journal of Physics 17, n.º 11 (27 de noviembre de 2015): 110203. http://dx.doi.org/10.1088/1367-2630/17/11/110203.

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4

Jauho, A. P. "Photon side-bands in mesoscopics". Superlattices and Microstructures 23, n.º 3-4 (marzo de 1998): 843–51. http://dx.doi.org/10.1006/spmi.1997.0545.

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5

Andreev, Aleksandr F. "Superfluidity, superconductivity and magnetism in mesoscopics". Physics-Uspekhi 41, n.º 6 (30 de junio de 1998): 581–88. http://dx.doi.org/10.1070/pu1998v041n06abeh000408.

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6

Flórez, F. Durán, E. D. V-Niño y J. Barba-Ortega. "Frozen magnetic response in mesoscopics superconductors". Journal of Physics: Conference Series 743 (agosto de 2016): 012012. http://dx.doi.org/10.1088/1742-6596/743/1/012012.

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7

Feigel'man, M. V., V. V. Ryazanov y V. B. Timofeev. "The current state of quantum mesoscopics". Physics-Uspekhi 44, n.º 10S (1 de enero de 2001): 5–19. http://dx.doi.org/10.1070/1063-7869/44/10s/s01.

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8

Andreev, Aleksandr F. "Superfluidity, superconductivity and magnetism in mesoscopics". Uspekhi Fizicheskih Nauk 168, n.º 06 (junio de 1998): 655–64. http://dx.doi.org/10.3367/ufnr.0168.199806f.0655.

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9

Feigel'man, Mikhail V., Valerii V. Ryazanov y Vladislav B. Timofeev. "Chernogolovka 2000: Mesoscopic and strongly correlated electron systems The current state of quantum mesoscopics". Physics-Uspekhi 44, n.º 10 (31 de octubre de 2001): 1045–59. http://dx.doi.org/10.1070/pu2001v044n10abeh001013.

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10

Andreev, Alexander F. "Mesoscopics and fundamental properties of space-time". Physica B: Condensed Matter 280, n.º 1-4 (mayo de 2000): 440–41. http://dx.doi.org/10.1016/s0921-4526(99)01825-6.

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11

Khmelnitskii, D. E. y M. Yosefin. "Mesoscopics in a strong perpendicular magnetic field". Physica A: Statistical Mechanics and its Applications 200, n.º 1-4 (noviembre de 1993): 525–29. http://dx.doi.org/10.1016/0378-4371(93)90556-j.

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12

Feigel'man, M. V., Valerii V. Ryazanov y Vladislav B. Timofeev. "Chernogolovka 2000: Mesoscopic and strongly correlated electron systems The current state of quantum mesoscopics". Uspekhi Fizicheskih Nauk 171, n.º 10 (2001): 1099. http://dx.doi.org/10.3367/ufnr.0171.200110k.1099.

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13

Weaver, Richard. "Localization and mesoscopics in structures and rooms I". Journal of the Acoustical Society of America 123, n.º 5 (mayo de 2008): 3059. http://dx.doi.org/10.1121/1.2932786.

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14

Andreev, Alexander F. "Mesoscopics, superconductivity, and fundamental properties of space-time". Physica C: Superconductivity 352, n.º 1-4 (abril de 2001): 1–3. http://dx.doi.org/10.1016/s0921-4534(00)01665-8.

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15

Weaver, Richard. "Localization and mesoscopics in structures and rooms II". Journal of the Acoustical Society of America 123, n.º 5 (mayo de 2008): 3762. http://dx.doi.org/10.1121/1.2935350.

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16

Das, Mukunda P. y Frederick Green. "What is novel in quantum transport for mesoscopics?" Pramana 67, n.º 1 (julio de 2006): 73–83. http://dx.doi.org/10.1007/s12043-006-0038-5.

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17

Skvortsov, M. A. y M. V. Feigel'man. "Mesoscopics in vortex core: level statistics and transport properties". Physica C: Superconductivity 332, n.º 1-4 (mayo de 2000): 432–36. http://dx.doi.org/10.1016/s0921-4534(99)00718-2.

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18

Giazotto, Francesco, Tero T. Heikkilä, Arttu Luukanen, Alexander M. Savin y Jukka P. Pekola. "Opportunities for mesoscopics in thermometry and refrigeration: Physics and applications". Reviews of Modern Physics 78, n.º 1 (17 de marzo de 2006): 217–74. http://dx.doi.org/10.1103/revmodphys.78.217.

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19

Harris, J. G. E., N. Argaman y S. J. Allen. "Absence of Shapiro-Like Steps in Certain MesoscopicS-N-Sjunctions". Physical Review Letters 78, n.º 13 (31 de marzo de 1997): 2678. http://dx.doi.org/10.1103/physrevlett.78.2678.

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20

Barba-Ortega, J., J. D. Gonzalez y Miryam R. Joya. "Computational simulation of vortex matter in Type-II mesoscopics superconductors". Journal of Physics: Conference Series 410 (8 de febrero de 2013): 012009. http://dx.doi.org/10.1088/1742-6596/410/1/012009.

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21

Larose, É. "Mesoscopics of ultrasound and seismic waves: application to passive imaging". Annales de Physique 31, n.º 3 (mayo de 2006): 1–126. http://dx.doi.org/10.1051/anphys:2007001.

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22

Nikolenko, A. N. "Mesoscopics of the concept of a hierarchical structure of materials". Powder Metallurgy and Metal Ceramics 37, n.º 1-2 (enero de 1998): 72–78. http://dx.doi.org/10.1007/bf02677233.

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23

Vagner, I. D., A. S. Rozhavsky, P. Wyder y A. Yu Zyuzin. "Is the Magnetic Field Necessary for the Aharonov-Bohm Effect in Mesoscopics?" Physical Review Letters 80, n.º 11 (16 de marzo de 1998): 2417–20. http://dx.doi.org/10.1103/physrevlett.80.2417.

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24

Vladimir Ivanovitch, Kodolov, Kodolova-Chukhontzeva Vera Vladimirovna y Mustakimov Rostislav Valer’evitch. "Mini Review: Some Peculiarities of Chemical Mesoscopics and This Scientific Trend Development Perspective". Science Journal of Chemistry 9, n.º 4 (2021): 97. http://dx.doi.org/10.11648/j.sjc.20210904.12.

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25

Bezborodov, Viktor, Luca Di Persio, Tyll Krueger y Pasha Tkachov. "Spatial growth processes with long range dispersion: Microscopics, mesoscopics and discrepancy in spread rate". Annals of Applied Probability 30, n.º 3 (junio de 2020): 1091–129. http://dx.doi.org/10.1214/19-aap1524.

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26

Zhu, Jian-Xin, Z. D. Wang y H. X. Tang. "Bound states and Josephson current in mesoscopics-wave superconductor–normal-metal–d-wave superconductor junctions". Physical Review B 54, n.º 10 (1 de septiembre de 1996): 7354–59. http://dx.doi.org/10.1103/physrevb.54.7354.

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27

Giazotto, Francesco, Tero T. Heikkilä, Arttu Luukanen, Alexander M. Savin y Jukka P. Pekola. "Erratum: Opportunities for mesoscopics in thermometry and refrigeration: Physics and applications [Rev. Mod. Phys. 78, 217 (2006)]". Reviews of Modern Physics 81, n.º 3 (29 de septiembre de 2009): 1351. http://dx.doi.org/10.1103/revmodphys.81.1351.

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28

Fedotov, V. V. "Review of Theory of Mesocopic Systems". Фізика і хімія твердого тіла 18, n.º 3 (15 de septiembre de 2017): 282–87. http://dx.doi.org/10.15330/pcss.18.3.282-287.

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In the framework of this work an overview of the theory of mesoscopic systems is made. The main effects of mesoscopic systems are noted. It is determined that the macroscopic characteristics of the system are significantly fluctuating within the mesoscopic level. The basic indicators of coherence of the quantum phase are determined and the mechanisms of influence are outlined. Six effects of mesoscopic systems are characterized with detailed justification. The theory of mesoscopic systems is based on the following mesoscopic effects: the Aaronov-Bohm effect; the effect of the integral quantum output; fractional quantum Hall effect; universal fluctuations of conduction; quantum conductivity quantum dot contact; DC currents in mesoscopic rings.Prospects for further developments in this area of research are based on a detailed study of mesoscopic effects based on the growing tendency for the production and research of materials containing the smallest structures and have low-dimensional features, which leads to the mesoscopic regime.

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29

Xu, Hui Ning, Jin Xu y Zhong Hong Li. "Rock Mesoscopic Structural Plane, Mesoscopic Anisotropy and Mesoscopic Anisotropy Index". Advanced Materials Research 594-597 (noviembre de 2012): 230–36. http://dx.doi.org/10.4028/www.scientific.net/amr.594-597.230.

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In this article, we define rock structural planes caused by mineral orientation and layering distribution of some rock ingredients which is different from both rock mass scale structural planes and micro structural plane at crystal scale, as rock mesoscopic structural plane, and the rock anisotropy caused by the existence of these structural planes as rock mesoscopic anisotropy. Rock mesoscopic scale anisotropy index is introduced and its simple but efficient testing method is suggested. With the rock mesoscopic anisotropy index, the degree of rock mesoscopic anisotropy can be quantified easily and the process in simplified.

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30

Chen, Kuo-Ching. "On the macroscopic–mesoscopic mixture of a magnetorheological fluid". Proceedings of the Royal Society A: Mathematical, Physical and Engineering Sciences 462, n.º 2068 (17 de enero de 2006): 1123–44. http://dx.doi.org/10.1098/rspa.2005.1609.

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This paper is concerned with the modelling of a magnetorheological (MR) fluid in the presence of an applied magnetic field as a twofolded mixture—a macroscopic fluid continuum and mesoscopic multi-solid continua. By assigning to each solid particle a vectorial mesoscopic variable, which is defined as the nearest relative position vector with respect to other particles, the solid medium of the MR fluid is further treated as a mixture consisting of different components, specified by these mesoscopic variables. The treatment of multi-solid continua is similar to that in the mesoscopic theory of liquid crystals. However, the key difference lies in the fact that the time-discontinuity of the defined vectorial mesoscopic variable will give rise to a ‘pseudo’ chemical reaction in the solid continuum. The equation of the phenomenological mesoscopic distribution function of the solid continuum then has an additional production term from the pseudo chemical reaction, analogous to the collision term appearing in the Boltzmann equation. The mesoscopic and macroscopic balance equations are then derived and by assuming the special constitutive relations the macroscopic equation for the second moment of the distribution function can be obtained.

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31

Pahlavani, Hassan. "The persistent current and energy spectrum on a driven mesoscopic LC-circuit with Josephson junction". International Journal of Modern Physics B 32, n.º 06 (26 de febrero de 2018): 1850066. http://dx.doi.org/10.1142/s0217979218500662.

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The quantum theory for a mesoscopic electric circuit including a Josephson junction with charge discreteness is studied. By considering coupling energy of the mesoscopic capacitor in Josephson junction device, a Hamiltonian describing the dynamics of a quantum mesoscopic electric LC-circuit with charge discreteness is introduced. We first calculate the persistent current on a quantum driven ring including Josephson junction. Then we obtain the persistent current and energy spectrum of a quantum mesoscopic electrical circuit which includes capacitor, inductor, time-dependent external source and Josephson junction.

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32

Ren, Jiaolong, Zhe Liu, Jinshun Xue y Yinshan Xu. "Influence of the Mesoscopic Viscoelastic Contact Model on Characterizing the Rheological Behavior of Asphalt Concrete in the DEM Simulation". Advances in Civil Engineering 2020 (8 de febrero de 2020): 1–14. http://dx.doi.org/10.1155/2020/5248267.

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The numerical simulation based on the discrete element method (DEM) is popular to analyze the material behavior of asphalt concrete in recent years because of the advantage of the DEM in characterizing the heterogeneous microstructures. As a type of viscoelastic material, the rheological behavior of asphalt concrete is represented depending on the mesoscopic viscoelastic contact model between two particles in a contact in DEM simulations. However, what is missing in the existing literature studies is analysis of the influence of the mesoscopic viscoelastic contact models. Hence, the existing mesoscopic viscoelastic contact models are employed to build different types of DEM numerical samples of asphalt concrete in this study. Laboratory tests and the corresponding numerical tests at different temperatures and frequencies are implemented to investigate the difference in simulation precision in the case of using different mesoscopic viscoelastic contact models via the rheological index of dynamic modulus and phase angle. The results show the following: (1) the mesoscopic generalized Maxwell contact model provides the best simulation precision at low temperatures; (2) the mesoscopic generalized Kelvin contact model shows an improved precision at high temperatures; and (3) although the mesoscopic Burgers contact model has the simplest mathematical structure, the simulation precisions are obviously lower than those of the other two contact models, particularly when simulating the phase angle at low temperatures and frequencies. The results will be beneficial to select the appropriate mesoscopic contact model for the DEM modeling of asphalt concrete according to the loading conditions.

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33

Lachowicz, Mirosław y Mateusz Dȩbowski. "Diauxic Growth at the Mesoscopic Scale". Entropy 22, n.º 11 (12 de noviembre de 2020): 1280. http://dx.doi.org/10.3390/e22111280.

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In the present paper, we study a diauxic growth that can be generated by a class of model at the mesoscopic scale. Although the diauxic growth can be related to the macroscopic scale, similarly to the logistic scale, one may ask whether models on mesoscopic or microscopic scales may lead to such a behavior. The present paper is the first step towards the developing of the mesoscopic models that lead to a diauxic growth at the macroscopic scale. We propose various nonlinear mesoscopic models conservative or not that lead directly to some diauxic growths.

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34

Freeman, Walter J. y Robert Kozma. "Local-global interactions and the role of mesoscopic (intermediate-range) elements in brain dynamics". Behavioral and Brain Sciences 23, n.º 3 (junio de 2000): 401. http://dx.doi.org/10.1017/s0140525x00243252.

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A unifing theory of spatiotemporal brain dynamics should incorporate multiple spatial and temporal scales. Between the microscopic (local) and macroscopic (global) components proposed by Nunez, mesoscopic (intermediate-range) elements should be integral parts of models. The corresponding mathematical formalism requires tools of nonlinear dynamics and the use of aperiodic (chaotic) attractors. Some relations between local-mesoscopic and mesoscopic-global components are outlined.

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35

PAHLAVANI, H. "THE PERSISTENT CURRENT ON A DRIVEN MESOSCOPIC RLC CIRCUIT". International Journal of Modern Physics B 25, n.º 23n24 (30 de septiembre de 2011): 3225–36. http://dx.doi.org/10.1142/s0217979211101788.

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The quantum theory for mesoscopic electric LC circuits with charge discreteness is briefly described. We take into account a resistance element (R) as an environment of the discrete-charge mesoscopic quantum LC circuit which is modeled by a Hamiltonian consisting of oscillators with continuous range of frequencies. Using a minimal coupling method, we investigate the quantum dynamics of this system. Hereby, the persistent current on a quantum damped L-design under the external potential source is obtained. Then, we write Heisenberg equations for a driven mesoscopic quantum RLC circuit with a dissipative term proportional to Ohmic damping and obtain persistent current on such a mesoscopic electric circuit.

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36

KIWATA, H., T. KIHARA, K. ONO, M. OSHIMA, T. OKUDA, A. HARASAWA, T. KINOSHITA y A. YOKOO. "DOMAIN IMAGING OF MESOSCOPIC MAGNETIC STRUCTURES BY PHOTOELECTRON EMISSION MICROSCOPY". Surface Review and Letters 09, n.º 01 (febrero de 2002): 365–69. http://dx.doi.org/10.1142/s0218625x02002336.

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We have observed magnetic domains of mesoscopic magnetic structures of Ni by synchrotron radiation photoelectron emission microscopy using circularly polarized soft X-rays from the bending magnet. The mesoscopic magnetic structures of Ni were fabricated by electron beam lithography combined with a chemical liftoff process. The geometries of the Ni mesoscopic samples were square, triangular and hexagonal with the sizes of 5 and 10 μm. The magnetic domains structures were clearly observed by dividing the images measured at the Ni L3-edge by the images measured at the Ni L2-edge. The magnetic domains of the Ni mesoscopic structures are discussed with the results of magnetic force microscopy and micromagnetic simulation.

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37

Sow, Libasse, Fabrice Bernard, Siham Kamali-Bernard y Cheikh Mouhamed Fadel Kébé. "Experiment-based modelling of the mechanical behaviour of non-hazardous waste incineration bottom ashes treated by hydraulic binder". MATEC Web of Conferences 149 (2018): 01038. http://dx.doi.org/10.1051/matecconf/201814901038.

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Instrumented indentation tests have been carried out on an isolated 25 mm diameter particle of Non-Hazardous Waste Incineration bottom ash. These tests have enabled one to assess the intrinsic mean reduced modulus of elasticity “Er” of the particles. This result is used as input data for a 3D numerical model of Representative Elementary Volumes (REV) of a road gravel made with this kind of by-products. This numerical model is based on a multi-scale hierarchical modelling strategy. The aggregates treated with cement have been decomposed into two REV at the sub-mesoscopic and mesoscopic scales. The numerical simulations campaign (“virtual laboratory”) lead to the following results. At the sub-mesoscopic scale, we determined the input parameters for the Concrete Damaged Plasticity Model (CDPM) used at the mesoscopic scale. At the mesoscopic scale, the mechanical characteristics of the road aggregates usually determined through experiments have been found. The non-hazardous waste incineration bottom ashes treated by hydraulic binder was classified into mechanical classe 3.

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38

Grmela, Miroslav. "Role of thermodynamics in extensions of mesoscopic dynamical theories". Communications in Applied and Industrial Mathematics 7, n.º 2 (1 de junio de 2016): 56–80. http://dx.doi.org/10.1515/caim-2016-0006.

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AbstractComplex macroscopic systems (like for instance those encountered in nanotechnology and biology) need to be investigated in a family of mesoscopic theories involving varying amount of details. In this paper we formulate a general thermodynamics providing a universal framework for such multiscale viewpoint of mesoscopic dynamics. We then discuss its role in making extensions (i.e. in lifting a mesoscopic theory to a more microscopic level that involves more details).

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39

Domínguez, D., A. R. Bishop y N. Grønbech-Jensen. "Coherence and Complexity in Condensed Matter: Josephson Junction Arrays". International Journal of Bifurcation and Chaos 07, n.º 05 (mayo de 1997): 979–88. http://dx.doi.org/10.1142/s0218127497000790.

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The importance of the mesoscopic bridge between microscopic and mesoscopic descriptions of complex, nonlinear-nonequilibrium extended dynamical systems is illustrated in a condensed matter context through three-dimensional Josephson junction arrays. Large-scale Langevin molecular dynamics is used to study novel transformer and melting effects, emphasizing the central roles of topological excitations (flux vortex lines) in determining mesoscopic patterns and dynamics — through flux line creation, annihilation, interaction and statistical mechanics.

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40

Moussa, M. H. Y. y B. Baseia. "Teleporting the Schrödinger Cat State". Modern Physics Letters B 12, n.º 29n30 (30 de diciembre de 1998): 1209–16. http://dx.doi.org/10.1142/s0217984998001438.

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We present a scheme for the teleportation of a coherent state or a mesoscopic superposition of coherent states — the Schrödinger-cat state. The proposal involves a mesoscopic-correlated state as the quantum channel which is generated through an adaptation of a quantum switch scheme. The required joint measurement performed in a mesoscopic Bell basis is accomplished through a technique for detection of a Schrödinger-cat state "trapped" in a cavity.

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41

Kiss, Tamás y Péter Érdi. "Mesoscopic neurodynamics". Biosystems 64, n.º 1-3 (enero de 2002): 119–26. http://dx.doi.org/10.1016/s0303-2647(01)00180-0.

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42

Weitz, D. A. "Mesoscopic Disorder". MRS Bulletin 19, n.º 5 (mayo de 1994): 11–13. http://dx.doi.org/10.1557/s0883769400036502.

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Disorder characterizes most of the materials that surround us in nature. Despite their great technological importance, materials with ordered crystalline structures are relatively rare. Examples of disordered materials, however, abound, and their forms can be as varied as their number. The paper on which these words are printed has a disordered structure composed of a highly interconnected network of fibers. It has also been coated with particulate materials to improve its properties and the visibility of the ink. The reading glasses you may require to focus on these words are composed of a glass or polymer material that is disordered on a molecular level. Even the structure of your hand holding this magazine is disordered. These and virtually all other disordered materials are typically parameterized by a characteristic length scale. Above this length scale, the material is homogeneous and the effects of the disorder are not directly manifest; below this characteristic length the disorder of the structure dominates, directly affecting the properties.The range of characteristic length scales for the disordered materials around us is immense. For the glass or polymer of your reading glasses, it is microscopic; the disorder is apparent only at the molecular level, while above this level the material is homogeneous. For the paper on which this magazine is printed, the scale is larger; the paper is white partly because the disordered fiber network has within it structures that are comparable in size to the wavelength of light, resulting in strong scattering of the light.

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43

Harding, John H. "Mesoscopic modelling". Current Opinion in Solid State and Materials Science 2, n.º 6 (diciembre de 1997): 728–32. http://dx.doi.org/10.1016/s1359-0286(97)80017-4.

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44

Nikolić, K. y R. Šordan. "Mesoscopic diode". Microelectronic Engineering 43-44 (agosto de 1998): 527–32. http://dx.doi.org/10.1016/s0167-9317(98)00214-7.

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45

Gantmakher, Vsevolod F. y Mikhail V. Feigel'man. "Mesoscopic unification". Physics-Uspekhi 41, n.º 2 (28 de febrero de 1998): 105–8. http://dx.doi.org/10.1070/pu1998v041n02abeh000337.

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46

Sowa, Artur. "Mesoscopic mechanics". Journal of Physics and Chemistry of Solids 65, n.º 8-9 (agosto de 2004): 1507–15. http://dx.doi.org/10.1016/j.jpcs.2003.12.012.

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47

Sigrist, Manfred. "Mesoscopic magnetism". Nature 396, n.º 6707 (noviembre de 1998): 110–11. http://dx.doi.org/10.1038/24033.

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48

Goodman, Maurice. "Mesoscopic mapping". Physics World 21, n.º 12 (diciembre de 2008): 19. http://dx.doi.org/10.1088/2058-7058/21/12/30.

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49

Thornton, T. J. "Mesoscopic devices". Reports on Progress in Physics 58, n.º 3 (1 de marzo de 1995): 311–64. http://dx.doi.org/10.1088/0034-4885/58/3/002.

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50

Scott, J. F. "Mesoscopic Dielectrics". Australian Journal of Physics 52, n.º 5 (1999): 903. http://dx.doi.org/10.1071/ph98094.

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This paper describes four unsolved theoretical problems in ferroelectrics and related dielectrics with high permittivities: (1) finite size effects in thin films and small particles, and their relationship to depolarisation fields; (2) nucleation and growth kinetics, and especially the recently discovered coherent nucleation of small domains in front of advancing walls; (3) low-temperature quantum effects in ferroelectrics and the process of ‘freeze-out’, in which domain wall mobilities suddenly drop to zero; (4) self-patterning of nanoscale assemblies on the surfaces of substrates, and the consideration of lateral finite size effects.

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Artículos de revistas sobre el tema "Mesoscopics"

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