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Auteur : Grafiati
Publié le 10 mars 2023

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1

Sadatian, Seyed Davood. « Orderly Disorder in Modern Physics ». International Letters of Chemistry, Physics and Astronomy 48 (mars 2015) : 163–72. http://dx.doi.org/10.18052/www.scipress.com/ilcpa.48.163.

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Fractal structures in various subjects are taken into consideration. In this article, we study fractal structures in physics which could be found or might be existent. Basically, fractals are important because they CHANGE the most basic ways we analyze and understand physics and experimental data.
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Sadatian, Seyed Davood. « Orderly Disorder in Modern Physics ». International Letters of Chemistry, Physics and Astronomy 48 (25 mars 2015) : 163–72. http://dx.doi.org/10.56431/p-43z834.

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Fractal structures in various subjects are taken into consideration. In this article, we study fractal structures in physics which could be found or might be existent. Basically, fractals are important because they CHANGE the most basic ways we analyze and understand physics and experimental data.
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3

Voss, D. « APPLIED PHYSICS : Light amid Disorder ». Science 319, no 5864 (8 février 2008) : 699c. http://dx.doi.org/10.1126/science.319.5864.699c.

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4

Cho, A. « STATISTICAL PHYSICS : A Fresh Take on Disorder, Or Disorderly Science ? » Science 297, no 5585 (23 août 2002) : 1268–69. http://dx.doi.org/10.1126/science.297.5585.1268.

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5

Beavers, Christine M., et Theocharis Stamatatos. « Disorder ! Disorder ! Disorder ! » Acta Crystallographica Section A Foundations and Advances 73, a1 (26 mai 2017) : a301. http://dx.doi.org/10.1107/s0108767317097057.

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6

Yu, Sunkyu, Xianji Piao, Jiho Hong et Namkyoo Park. « Metadisorder for designer light in random systems ». Science Advances 2, no 10 (octobre 2016) : e1501851. http://dx.doi.org/10.1126/sciadv.1501851.

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Disorder plays a critical role in signal transport by controlling the correlation of a system, as demonstrated in various complex networks. In wave physics, disordered potentials suppress wave transport, because of their localized eigenstates, from the interference between multiple scattering paths. Although the variation of localization with tunable disorder has been intensively studied as a bridge between ordered and disordered media, the general trend of disorder-enhanced localization has remained unchanged, and the existence of complete delocalization in highly disordered potentials has not been explored. We propose the concept of “metadisorder”: randomly coupled optical systems in which eigenstates can be engineered to achieve unusual localization. We demonstrate that one of the eigenstates in a randomly coupled system can always be arbitrarily molded, regardless of the degree of disorder, by adjusting the self-energy of each element. Ordered waves with the desired form are then achieved in randomly coupled systems, including plane waves and globally collective resonances. We also devise counterintuitive functionalities in disordered systems, such as “small-world–like” transport from non–Anderson-type localization, phase-conserving disorder, and phase-controlled beam steering.
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7

Ziegler, K. « Disorder physics in mixtures of fermionic atoms ». Laser Physics 16, no 4 (avril 2006) : 699–706. http://dx.doi.org/10.1134/s1054660x06040268.

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8

Gaskell, P. H. « Solid state physics : Unravelling disorder in glass ». Nature 317, no 6035 (septembre 1985) : 285–86. http://dx.doi.org/10.1038/317285a0.

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9

Tyutyunnik, Vyacheslav M. « Disorder and fluctuations in complex physical systems : Nobel Prize winner in physics 2021 Giorgio Parisi ». Image Journal of Advanced Materials and Technologies 6, no 4 (2021) : 243–46. http://dx.doi.org/10.17277/jamt.2021.04.pp.243-246.

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In 2021, the Nobel Prize in Physics was awarded “for innovative contributions to our understanding of complex systems,” with half awarded jointly to Shukuro Manabe and Klaus Hasselmann “for the physical modelling of Earth’s climate, quantifying variability and reliably predicting global warming”, and the other half to Giorgio Parisi “for the discovery of the interplay of disorder and fluctuations in physical systems from atomic to planetary scales”. Parisi discovered hidden patterns in disordered, complex materials. His discoveries are one of the most important contributions to the theory of complex systems. He proved that equilibrium is never achieved in spin glasses, because frustrations do not allow all limitations to be satisfied. In reality, there are an infinite number of practically equilibrium states in which frustrations tend to a minimum. Parisi’s research interests cover 14 different directions.
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10

Ray, Purusattam. « Statistical physics perspective of fracture in brittle and quasi-brittle materials ». Philosophical Transactions of the Royal Society A : Mathematical, Physical and Engineering Sciences 377, no 2136 (26 novembre 2018) : 20170396. http://dx.doi.org/10.1098/rsta.2017.0396.

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We discuss the physics of fracture in terms of the statistical physics associated with the failure of elastic media under applied stresses in presence of quenched disorder. We show that the development and the propagation of fracture are largely determined by the strength of the disorder and the stress field around them. Disorder acts as nucleation centres for fracture. We discuss Griffith's law for a single crack-like defect as a source for fracture nucleation and subsequently consider two situations: (i) low disorder concentration of the defects, where the failure is determined by the extreme value statistics of the most vulnerable defect (nucleation regime) and (ii) high disorder concentration of the defects, where the scaling theory near percolation transition is applicable. In this regime, the development of fracture takes place through avalanches of a large number of tiny microfractures with universal statistical features. We discuss the transition from brittle to quasi-brittle behaviour of fracture with the strength of disorder in the mean-field fibre bundle model. We also discuss how the nucleation or percolation mode of growth of fracture depends on the stress distribution range around a defect. We discuss the corresponding numerical simulation results on random resistor and spring networks. This article is part of the theme issue ‘Statistical physics of fracture and earthquakes’.
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11

Sinova, Jairo, Allan H. MacDonald et S. M. Girvin. « Disorder and interactions in quantum Hall ferromagnets : effects of disorder in Skyrmion physics ». Physica E : Low-dimensional Systems and Nanostructures 12, no 1-4 (janvier 2002) : 16–19. http://dx.doi.org/10.1016/s1386-9477(01)00263-6.

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12

Deressa, Zeleke, et P. Singh. « Disorder-Induced Superconductor-Insulator Transition ». Advances in Condensed Matter Physics 2020 (15 juillet 2020) : 1–5. http://dx.doi.org/10.1155/2020/2021576.

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In this paper, we report the results of our theoretical investigation on the interplay of superconductivity and disorder in two-dimensional (2D) systems. The effect of disorder on superconductivity of 2D systems was found analytically using Green’s function formalism. The results of our calculation revealed that disorder induced due to randomly distributed superconducting islands enhances decoherence of Cooper pairs and suppresses superconductivity. We have also determined the critical value of disorder at which the 2D system completely loses its superconducting properties. Below this critical value of disorder, the system acts as a superconductor, a system with zero electrical resistance. Above the critical value, it acts as an insulator, a system with infinite electric resistance. This is a fascinating result because a direct transition from the state of the infinite conductivity to the opposite extreme of infinite resistivity is unexpected in the theory of condensed matter physics.
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13

Ashton, Christopher, et Denise Duffie. « Crossed wires : the hall effect in substance use disorder ». MOJ Addiction Medicine & ; Therapy 7, no 1 (3 octobre 2022) : 1–2. http://dx.doi.org/10.15406/mojamt.2022.07.00150.

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The underlying neuroscience of substance use disorder is becoming well elaborated. Nonetheless, some of the more subtle symptomatology is not well matched with underlying organic processes identified to date. The ability to explain mental phenomena with underlying brain processes is a strong part of the literature and valuable to those caring for persons. This article draws on current knowledge of the fundamentals of substance use disorder and expands on current literature surrounding axonal demyelination to suggest a likely mechanism for thought disorders commonly experienced by persons in recovery. Viewing demyelination and conduction through an analogue lens is more likely to represent the physics involved more accurately than an ‘on or off’ signalling model as associated with action potentials. Additionally, this approach is thought to better enunciate the underlying physiology behind the mental features characteristic to the disorder.
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14

Chen, Guihua, Zhihong Huang et Zhijie Mai. « Two-dimensional discrete Anderson location in waveguide matrix ». Journal of Nonlinear Optical Physics & ; Materials 23, no 03 (septembre 2014) : 1450033. http://dx.doi.org/10.1142/s0218863514500337.

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Anderson location is an important wave phenomenon when the system contains disorder. Anderson location of light is a significant topic in optical science. Arrays of evanescently coupled waveguides made of nonlinear materials are the fundamental model of discrete nonlinear optics. Guided propagation of light in such arrays emulates electronic wave functions in fundamental periodic and disordered potentials of solid state physics. In this work, the Anderson location effect in a two-dimensional waveguide matrix is studied, and the influence of the nonlinearity on the localized effect induced by the disorder of the system is considered.
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15

QI, LIMEI, ZIQIANG YANG et XI GAO. « DISORDERED ONE-DIMENSIONAL METALLIC-DIELECTRIC PHOTONIC CRYSTAL REFLECTOR ». Modern Physics Letters B 23, no 05 (20 février 2009) : 715–22. http://dx.doi.org/10.1142/s0217984909018941.

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The reflected properties of one-dimensional frequency-dependent metallic-dielectric photonic crystals are investigated when disorders are introduced for the first time. It is demonstrated that disordered metallic-dielectric photonic crystal provides remarkably high reflection range compared with the corresponding period metallic-dielectric one when the degree of disorder is moderately chosen, and a wider stop band will be obtained with the increasing of periods. At last, the reflected properties influenced by incident angle for different polarizations are also calculated and discussed.
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16

Hern�ndez-Garc�a, E., L. Pesquera, M. A. Rodr�guez et M. San Miguel. « Random walk in dynamically disordered chains : Poisson white noise disorder ». Journal of Statistical Physics 55, no 5-6 (juin 1989) : 1027–52. http://dx.doi.org/10.1007/bf01041077.

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17

SÁNCHEZ, ANGEL, et LUIS VÁZQUEZ. « NONLINEAR WAVE PROPAGATION IN DISORDERED MEDIA ». International Journal of Modern Physics B 05, no 18 (10 novembre 1991) : 2825–82. http://dx.doi.org/10.1142/s0217979291001115.

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We briefly review the state-of-the-art of research on nonlinear wave propagation in disordered media. The paper is intended to provide the non-specialist reader with a flavor of this active field of physics. Firstly, a general introduction to the subject is made. We describe the basic models and the ways to study disorder in connection with them. Secondly, analytical and numerical techniques suitable for this purpose are outlined. We summarize their features and comment on their respective advantages, drawbacks and applicability conditions. Thirdly, the Nonlinear Klein-Gordon and Schrödinger equations are chosen as specific examples. We collect a number of results that are representative of the phenomena arising from the competition between nonlinearity and disorder. The review is concluded with some remarks on open questions, main current trends and possible further developments.
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18

Pető, T., F. Iglói et I. A. Kovács. « Random Ising chain in transverse and longitudinal fields : Strong disorder RG study ». Condensed Matter Physics 26, no 1 (2023) : 13102. http://dx.doi.org/10.5488/cmp.26.13102.

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Motivated by the compound LiHoxY1-xF4, we consider the Ising chain with random couplings and in the presence of simultaneous random transverse and longitudinal fields, and study its low-energy properties at zero temperature by the strong disorder renormalization group approach. In the absence of longitudinal fields, the system exhibits a quantum-ordered and a quantum-disordered phase separated by a critical point of infinite disorder. When the longitudinal random field is switched on, the ordered phase vanishes and the trajectories of the renormalization group are attracted to two disordered fixed points: one is characteristic of the classical random field Ising chain, the other describes the quantum disordered phase. The two disordered phases are separated by a separatrix that starts at the infinite disorder fixed point and near which there are strong quantum fluctuations.
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19

SOTO-PUEBLA, DIEGO, FELIPE RAMOS-MENDIETA et MUFEI XIAO. « DISORDER-TUNABLE PHOTONIC PROPERTIES OF PERIODIC DIELECTRIC/METAL SUPERLATTICES ». International Journal of Modern Physics B 18, no 01 (10 janvier 2004) : 125–35. http://dx.doi.org/10.1142/s0217979204023763.

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Influences of perturbative disorders to the photonic properties of one-dimensional periodic dielectric/metal superlattices have been numerically studied. In the calculations, two different disorders were considered, i.e. the disorder in position and in thickness of the metallic layers. Significant modifications induced by the disorders have been found in the photonic band structures. The modifications vary according to the type as well as the degree of the disorders. Both enhanced and attenuated transmissions have been observed in the photonic band gap. Detailed discussions on the calculated photonic band structures would provide useful information on how to obtain desired photonic band structures by introducing certain disorders.
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20

Faizabadi, Edris, et Mahboubeh Omidi. « Disorder-averaged currents in edged topological disordered mesoscopic cylinder ». Physics Letters A 373, no 16 (avril 2009) : 1469–77. http://dx.doi.org/10.1016/j.physleta.2009.02.057.

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21

Beeby, John. « Structured disorder ». Physics World 1, no 12 (décembre 1988) : 40. http://dx.doi.org/10.1088/2058-7058/1/12/30.

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22

Ne'eman, Yuval. « Evolving disorder ». Physics World 16, no 7 (juillet 2003) : 17. http://dx.doi.org/10.1088/2058-7058/16/7/22.

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23

XIE, X. C., D. Z. LIU et J. K. JAIN. « STUDY OF SCALING IN THE FRACTIONAL QUANTUM HALL EFFECT ». Modern Physics Letters B 10, no 17 (20 juillet 1996) : 801–8. http://dx.doi.org/10.1142/s0217984996000900.

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In the composite fermion model of the fractional quantum Hall effect, composite fermions experience, in addition to the usual potential disorder, also a magnetic flux disorder. Motivated by this, we investigate the localization properties of a single fermion in two dimensions, moving in the presence of both static potential and static magnetic flux disorders, but with a non-zero average magnetic field. It is found that the exponent characterizing the divergence of the localization length is not changed upon the addition of the flux disorder, provided it is not too large.
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24

Photiadis, Douglas M. « Fluid Loaded Structures With One Dimensional Disorder ». Applied Mechanics Reviews 49, no 2 (1 février 1996) : 100–125. http://dx.doi.org/10.1115/1.3101885.

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This paper reviews the problem of the vibration of fluid loaded structures with one dimensional disorder. There are two aspects which are important in understanding the behavior of such systems: the nature of the fluid loading and the effects arising from irregularity. These two areas of investigation have been pursued simultaneously by the structural acoustics and condensed matter physics communities, and only recently have attempts been made to use the results from both fields. The key results from these areas which have been employed in the analysis of disordered fluid loaded structures are reviewed, and the recent research results in this area are described.
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25

Gupta, Sanjay, et Tribikram Gupta. « Physics of metal–correlated barrier with disorder–metal heterostructure ». Solid State Communications 152, no 10 (mai 2012) : 878–82. http://dx.doi.org/10.1016/j.ssc.2012.02.014.

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26

Frieden, B. Roy. « Fisher information, disorder, and the equilibrium distributions of physics ». Physical Review A 41, no 8 (1 avril 1990) : 4265–76. http://dx.doi.org/10.1103/physreva.41.4265.

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27

PANG, XIAO-FENG, JIA-FENG YU et YU-HUI LAO. « COMBINATION EFFECTS OF STRUCTURE NONUNIFORMITY OF PROTEINS ON THE SOLITON TRANSPORTED BIO-ENERGY ». International Journal of Modern Physics B 21, no 01 (10 janvier 2007) : 13–42. http://dx.doi.org/10.1142/s021797920703659x.

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Combination effects of structure disorder of protein molecules containing the fluctuations of spring constant, dipole-dipole interaction constant and exciton-phonon coupling constant and diagonal disorder, resulting from nonuniform distribution of masses of amino acid residues and impurities, on the soliton transported the bio-energy in the proteins have been numerically simulated by fourth-order Runge–Kutta method in the improved model. The results obtained show that these structure disorders can change the states of solitons but as the solitons are quite robust against these disorder effects, they can only be dispersed or disrupted in the cases of quite large structure disorders. From these results and the properties of molecular structure of biological proteins we can conclude that the new soliton in the improved model is quite stable in normal conditions. Thus the soliton is possibly a carrier of bio-energy transport in the protein molecules.
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28

Kudrnovsky, J., Vaclav Drchal, Ilja Turek, David Wagenknecht et Sergii Khmelevskyi. « The Spin-Disorder Resistivity : The Disordered Local Moment Approach ». Solid State Phenomena 289 (avril 2019) : 185–91. http://dx.doi.org/10.4028/www.scientific.net/ssp.289.185.

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The spin-disorder resistivity (SDR) of a broad range of magneticmaterials, both ordered and disordered, is reviewed.We identify the SDR at the critical temperature with the residualresistivity of the corresponding system evaluated in the frameworkof the disordered local moment (DLM) model.The underlying electronic structure is determined in the frameworkof the tight-binding linear muffin-tin orbital method which employsthe coherent potential approximation to describe the DLM stateand chemical disorder.The DLM fixed-spin moment method is used in the case when the DLMmoment collapses.The Kubo-Greenwood approach is employed to estimate the resistivityof the DLM state.Formalism is applied to Fe and Ni and its alloys, Heusler alloys,and ordered ferromagnetic and antiferromagnetic alloys.Finally, the SDR of the Earth's core will be studied using thesame formalism.Calculations are compared with available experimental data.
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29

Unruh, Davis, Alberto Camjayi, Chase Hansen, Joel Bobadilla, Marcelo J. Rozenberg et Gergely T. Zimanyi. « Disordered Mott–Hubbard Physics in Nanoparticle Solids : Transitions Driven by Disorder, Interactions, and Their Interplay ». Nano Letters 20, no 12 (18 novembre 2020) : 8569–75. http://dx.doi.org/10.1021/acs.nanolett.0c03141.

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Rodríguez Andrés, L., T. Ballesta Casanova, M. S. Hernández García, C. Noval Canga, L. Gallardo Borge et J. A. Espina Barrio. « Autistic spectrum disorder masked by mental retardation and impulse control disorder ». European Psychiatry 33, S1 (mars 2016) : S639. http://dx.doi.org/10.1016/j.eurpsy.2016.01.2404.

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Clinical case reportA 48-year-old male, diagnosed with impulsive control disorder, sex addiction disorder and mental retardation was followed-up by different psychiatrists for the last 20 years. He consults because of presenting depressive symptoms and behavioural disturbances related to the death of his mother two years before. The patient reports to experimenting depressed mood, irritability, insomnia and trends to cry. He has lost motivation for his job and hobbies (he used to show interest in topics such as physics, philosophy, maths, and medicine). He has feelings of loneliness, which make him look for social interaction and support through continuous calls to telephone sex lines. This act has made him spend large amounts of cash, thus, making him be in deep debts. He does not feel integrate in society.Mental status examinationIntrovert, limited social skills, coherent language, echolalic, monotone, tangential speech, depressed mood, feelings of guilt and futility, dysphoria, partial anhedonia, ideas of hopelessness, structured death ideation, unconsciousness of his own acts, with trend to impulsiveness and compulsive behaviour and insomnia.Complementary testWais test: no mental retardation found.DiagnosisAutistic spectrum disorder (F84.0); major depressive disorder (F32.1); bereavement (V62.82).DiscussionThe patient showed classic diagnostic criteria DSM 5 associated with autistic spectrum disorder (Asperger's disorder in DSM-IV); the permanent inability for social interactions and repetitive, restricted and stereotypic behavioural patterns.Disclosure of interestThe authors have not supplied their declaration of competing interest.
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31

Frank, T. D. « Strongly Nonlinear Stochastic Processes in Physics and the Life Sciences ». ISRN Mathematical Physics 2013 (28 mars 2013) : 1–28. http://dx.doi.org/10.1155/2013/149169.

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Strongly nonlinear stochastic processes can be found in many applications in physics and the life sciences. In particular, in physics, strongly nonlinear stochastic processes play an important role in understanding nonlinear Markov diffusion processes and have frequently been used to describe order-disorder phase transitions of equilibrium and nonequilibrium systems. However, diffusion processes represent only one class of strongly nonlinear stochastic processes out of four fundamental classes of time-discrete and time-continuous processes evolving on discrete and continuous state spaces. Moreover, strongly nonlinear stochastic processes appear both as Markov and non-Markovian processes. In this paper the full spectrum of strongly nonlinear stochastic processes is presented. Not only are processes presented that are defined by nonlinear diffusion and nonlinear Fokker-Planck equations but also processes are discussed that are defined by nonlinear Markov chains, nonlinear master equations, and strongly nonlinear stochastic iterative maps. Markovian as well as non-Markovian processes are considered. Applications range from classical fields of physics such as astrophysics, accelerator physics, order-disorder phase transitions of liquids, material physics of porous media, quantum mechanical descriptions, and synchronization phenomena in equilibrium and nonequilibrium systems to problems in mathematics, engineering sciences, biology, psychology, social sciences, finance, and economics.
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32

Sherrington, David. « Physics and complexity ». Philosophical Transactions of the Royal Society A : Mathematical, Physical and Engineering Sciences 368, no 1914 (13 mars 2010) : 1175–89. http://dx.doi.org/10.1098/rsta.2009.0208.

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This paper is concerned with complex macroscopic behaviour arising in many-body systems through the combinations of competitive interactions and disorder, even with simple ingredients at the microscopic level. It attempts to indicate and illustrate the richness that has arisen, in conceptual understanding, in methodology and in application, across a large range of scientific disciplines, together with a hint of some of the further opportunities that remain to be tapped. In doing so, it takes the perspective of physics and tries to show, albeit rather briefly, how physics has contributed and been stimulated.
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33

Csahok, Z., et T. Vicsek. « Traffic models with disorder ». Journal of Physics A : Mathematical and General 27, no 16 (21 août 1994) : L591—L596. http://dx.doi.org/10.1088/0305-4470/27/16/005.

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34

Stishov, Sergei M. « Entropy, disorder, melting ». Uspekhi Fizicheskih Nauk 154, no 1 (1988) : 93. http://dx.doi.org/10.3367/ufnr.0154.198801c.0093.

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35

Benini, Leonardo. « Inspired by disorder ». Nature Physics 18, no 10 (octobre 2022) : 1149. http://dx.doi.org/10.1038/s41567-022-01801-x.

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36

Hicks, Trevor J., et David L. Huber. « Magnetism in Disorder ». Physics Today 49, no 7 (juillet 1996) : 64. http://dx.doi.org/10.1063/1.2807696.

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37

Marshall, Joe. « Devices in disorder ? » Physics World 2, no 2 (février 1989) : 47. http://dx.doi.org/10.1088/2058-7058/2/2/28.

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38

Sherrington, David. « Complexity and disorder ». Physics World 4, no 8 (août 1991) : 62. http://dx.doi.org/10.1088/2058-7058/4/8/38.

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39

Wright, Alison. « Disorder for localization ». Nature Physics 9, no 2 (février 2013) : 64. http://dx.doi.org/10.1038/nphys2552.

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40

Baierlein, Ralph, et Clayton A. Gearhart. « The disorder metaphor ». American Journal of Physics 71, no 2 (février 2003) : 103. http://dx.doi.org/10.1119/1.1516199.

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41

Eisenberg, E., et R. Berkovits. « Disorder induced ferromagnetism ». Annalen der Physik 8, no 7-9 (novembre 1999) : 707–10. http://dx.doi.org/10.1002/(sici)1521-3889(199911)8:7/9<707 ::aid-andp707>3.0.co;2-r.

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42

Hulin, J. P. « Porous media : A model system for the physics of disorder ». Advances in Colloid and Interface Science 49 (avril 1994) : 47–84. http://dx.doi.org/10.1016/0001-8686(94)80012-x.

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43

Kun, Ferenc, Gergő Pál, Imre Varga et Ian G. Main. « Effect of disorder on the spatial structure of damage in slowly compressed porous rocks ». Philosophical Transactions of the Royal Society A : Mathematical, Physical and Engineering Sciences 377, no 2136 (26 novembre 2018) : 20170393. http://dx.doi.org/10.1098/rsta.2017.0393.

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Faults and damage zone properties control a range of important phenomena, from the hydraulic properties of underground reservoirs to the physics of earthquakes on a larger scale. Here, we investigate the effect of disorder of porous rocks on the spatial structure of damage emerging under compression. Model rock samples are numerically generated by sedimenting particles where the amount of disorder is controlled by the particle size distribution. To obtain damage bands with a sufficiently large length along axis, we performed simulations of ‘Brazilian’-type compression tests of cylindrical samples. As failure is approached, damage localization leads to the formation of two conjugate shear bands. The orientation angle of bands to the loading direction increases with disorder, implying a decrease in the internal coefficient of friction. The width of the damage band scales as a power law of the degree of disorder. Inside the damage band, the sample is crushed into a large number of pieces with a power law mass distribution. The shape of fragments undergoes a crossover at a disorder-dependent size from the isotropy of small pieces to the anisotropic flattened form of the large ones. The results provide important constraints in understanding the role of disorder in geological fractures. This article is part of the theme issue ‘Statistical physics of fracture and earthquakes’.
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Gerbaldo, R., G. Ghigo, L. Gozzelino, E. Mezzetti, B. Minetti et R. Cherubini. « Pinning and confinement of vortices : Random disorder and correlated disorder ». Il Nuovo Cimento D 19, no 8-9 (août 1997) : 1323–28. http://dx.doi.org/10.1007/bf03185427.

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Bellier-Castella, L., M. JP Gingras, P. CW Holdsworth et R. Moessner. « Frustrated order by disorder : The pyrochlore anti-ferromagnet with bond disorder ». Canadian Journal of Physics 79, no 11-12 (1 décembre 2001) : 1365–71. http://dx.doi.org/10.1139/p01-098.

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The classical Heisenberg anti-ferromagnet on the pyrochlore lattice is macroscopically and continuously degenerate and the system remains disordered at all temperatures, even in the presence of weak dilution with nonmagnetic ions. We show that, in contrast, weak-bond disorder lifts the ground-state degeneracy in favour of locally collinear spin configurations. We present a proof that for a single tetrahedron the ground state is perfectly collinear but identify two mechanisms that preclude the establishment of a globally collinear state; one due to frustration and the other due to higher order effects. We thus obtain a rugged energy landscape, which is necessary to account for the glassy phenomena found in real systems such as the pyrochlore Y2Mo2O7 recently reported by Booth et al. (Phys. Rev. B: Condens. Matter Mater. Phys. 62, R755 (2000).) to contain a substantial degree of bond disorder. PACS Nos.: 75.10.Hk, 75.40.Mg, 75.40.Gb
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PUSEP, Y. A., M. B. RIBEIRO, H. ARAKAKI, C. A. DE SOUZA, S. MALZER et G. H. DÖHLER. « DISORDER INDUCED COHERENCE-INCOHERENCE CROSSOVER IN RANDOM GaAs/AlGaAs SUPERLATTICES ». International Journal of Modern Physics B 18, no 27n29 (30 novembre 2004) : 3629–32. http://dx.doi.org/10.1142/s0217979204027165.

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The coherence of electrons was studied in intentionally disordered GaAs / AlGaAs superlattices as a function of the vertical interlayer coupling. Depending on the relation of the disorder energy and the Fermi energy the coherent and incoherent diffusive transport regimes were distinguished. New features of weakly coupled layered electron systems such as the vertical coupling energy and the in-plane phase-breaking time were observed by magnetoresistance measurements in the coherent and incoherent regimes respectively. Both of them were found to decrease with increasing disorder strength. This demonstrates the disorder induced break-down of the interlayer coherence of quasi-particles which drastically affected their intralayer coherence.
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Nield, V. M., J. C. Li, D. K. Ross et R. W. Whitworth. « Disorder in ice Ih ». Physica Scripta T57 (1 janvier 1995) : 179–83. http://dx.doi.org/10.1088/0031-8949/1995/t57/031.

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Laubie, Hadrien, Siavash Monfared, Farhang Radjaï, Roland Pellenq et Franz-Josef Ulm. « Disorder-induced stiffness degradation of highly disordered porous materials ». Journal of the Mechanics and Physics of Solids 106 (septembre 2017) : 207–28. http://dx.doi.org/10.1016/j.jmps.2017.05.008.

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Brezini, A. « Effects of Disorder and Electron Correlation in Disordered Systems ». physica status solidi (b) 166, no 1 (1 juillet 1991) : 125–34. http://dx.doi.org/10.1002/pssb.2221660113.

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Dittrich, Birger, Christoph Sever et Jens Lübben. « Disappearing disorder ». CrystEngComm 22, no 43 (2020) : 7432–46. http://dx.doi.org/10.1039/d0ce00300j.

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