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Автор: Grafiati
Опубліковано: 7 липня 2024

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Статті в журналах з теми "Ising mode":

1

Kokshenev, V. B., and P. R. Silva. "To Critical Dynamics Near Structural Phase Transitions in Ferroelectrics: Central-Mode And Soft-Mode Behavior." Modern Physics Letters B 12, no. 08 (April 10, 1998): 265–69. http://dx.doi.org/10.1142/s0217984998000342.

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We analyze the critical dynamics of the order-disorder phase transition through the pseudo-spin quantum and classical Ising models. The findings derived by the Green-function equation-motion method and realized through Tyablikov's and Tserkovnikov's schemes, on the one hand, and the Thompson–Silva renormalization group approach, on the other hand are discussed. The slowing-down Δ and the dynamical z critical exponents are predicted for the relaxation (Δ=5/4, z=2) and resonant (Δ=5/16, z=1/2) motion regimes for three-dimensional Ising models. The results obtained give support to the idea that the classical and quantum d=2, 3 Ising models at nonzero critical temperature belong to the same universality class.
2

Albanese, Claudio. "A goldstone mode in the Kawasaki-Ising model." Journal of Statistical Physics 77, no. 1-2 (October 1994): 77–87. http://dx.doi.org/10.1007/bf02186833.

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3

Deshmukh, Ankosh D., Nitesh D. Shambharkar, and Prashant M. Gade. "Effect of a Mode of Update on Universality Class for Coupled Logistic Maps: Directed Ising to Ising Class." International Journal of Bifurcation and Chaos 31, no. 03 (March 15, 2021): 2150042. http://dx.doi.org/10.1142/s0218127421500425.

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Ising model at zero temperature leads to a ferromagnetic state asymptotically. There are two such possible states linked by symmetry, and Glauber–Ising dynamics are employed to reach them. In some stochastic or deterministic dynamical systems, the same absorbing state with [Formula: see text] symmetry is reached. This transition often belongs to the directed Ising (DI) class where dynamic exponents and persistence exponent are different. In asymmetrically coupled sequentially updated logistic maps, the transition belongs to the DI class. We study changes in the nature of transition with an update scheme. Even with the synchronous update, the transition still belongs to the DI class. We also study a synchronous probabilistic update scheme in which each site is updated with the probability [Formula: see text]. The order parameter decays with an exponent [Formula: see text] in this scheme. Nevertheless, the dynamic exponent [Formula: see text] is less than [Formula: see text] even for small values of [Formula: see text] indicating a very slow crossover to the Ising class. However, with a random asynchronous update, we recover [Formula: see text]. In the presence of feedback, synchronous update leads to a transition in the DI universality class which changes to Ising class for synchronous probabilistic update.
4

Mahboob, Imran, Hajime Okamoto, and Hiroshi Yamaguchi. "An electromechanical Ising Hamiltonian." Science Advances 2, no. 6 (June 2016): e1600236. http://dx.doi.org/10.1126/sciadv.1600236.

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Solving intractable mathematical problems in simulators composed of atoms, ions, photons, or electrons has recently emerged as a subject of intense interest. We extend this concept to phonons that are localized in spectrally pure resonances in an electromechanical system that enables their interactions to be exquisitely fashioned via electrical means. We harness this platform to emulate the Ising Hamiltonian whose spin 1/2 particles are replicated by the phase bistable vibrations from the parametric resonances of multiple modes. The coupling between the mechanical spins is created by generating two-mode squeezed states, which impart correlations between modes that can imitate a random, ferromagnetic state or an antiferromagnetic state on demand. These results suggest that an electromechanical simulator could be built for the Ising Hamiltonian in a nontrivial configuration, namely, for a large number of spins with multiple degrees of coupling.
5

Semenov, A. G. "Pairing and Collective Excitations in Ising Superconductors." JETP Letters 119, no. 1 (January 2024): 46–52. http://dx.doi.org/10.1134/s0021364023603810.

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Two-dimensional Ising superconductivity formed in NbSe2, MoS2, WS2, etc. transition-metal dichalcogenides is considered. For the superconducting state, the effective low-energy action for phases of the order parameters has been obtained and collective modes in the system have been studied. It has been shown that the system contains not only the Goldstone mode but also the Leggett mode with a mass related to the difference between the singlet and triplet pairing constants. The effect of a low magnetic field parallel to the plane of the system has also been discussed.
6

Einax, Mario, and Michael Schulz. "Mode-coupling approach for spin-facilitated kinetic Ising models." Journal of Chemical Physics 115, no. 5 (August 2001): 2282–96. http://dx.doi.org/10.1063/1.1383053.

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7

Gebril, Mohamed Atef Mohamed. "Some Proposition that Links Ferromagnetic Models with Cantorian Set Theory." Applied Physics Research 8, no. 6 (October 21, 2016): 1. http://dx.doi.org/10.5539/apr.v8n6p1.

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<p class="1Body">In this paper, we established a link between ferromagnetic models and set theory. Three dimension spins "S<sub>X</sub>, S<sub>y</sub>, S<sub>z</sub>" are considered in Heisenberg model but it is restricted to z_ axis<strong><em> </em></strong>" S<sub>z</sub>" in Ising mode. By using Brouwer theory, fractal motion of magnetic domains is predicted theoretically in the materials that their magnetism are explained by Ising model. In addition, we achieved that the experimental data of the fractal motion of magnetic domains in the thin films are agreement with the theoretical assumptions that are proposed.</p>
8

Zalesky, Boris A. "Network flow optimization for restoration of images." Journal of Applied Mathematics 2, no. 4 (2002): 199–218. http://dx.doi.org/10.1155/s1110757x02110035.

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The network flow optimization approach is offered for restoration of gray-scale and color images corrupted by noise. The Ising models are used as a statistical background of the proposed method. We present the new multiresolution network flow minimum cut algorithm, which is especially efficient in identification of the maximum a posteriori (MAP) estimates of corrupted images. The algorithm is able to compute the MAP estimates of large-size images and can be used in a concurrent mode. We also consider the problem of integer minimization of two functions,U1(x)=λ∑i|yi−xi|+∑i,j βi,j|xi−xj|andU2(x)=∑i λi (yi−xi)2+∑i,j βi,j (xi−xj)2, with parametersλ,λi,βi,j>0and vectorsx=(x1,…,xn),y=(y1,…,yn)∈{0,…,L−1}n. Those functions constitute the energy ones for the Ising model of color and gray-scale images. In the caseL=2, they coincide, determining the energy function of the Ising model of binary images, and their minimization becomes equivalent to the network flow minimum cut problem. The efficient integer minimization ofU1(x),U2(x)by the network flow algorithms is described.
9

SIRE, CLÉMENT. "ISING CHAIN IN A QUASIPERIODIC MAGNETIC FIELD." International Journal of Modern Physics B 07, no. 06n07 (March 1993): 1551–67. http://dx.doi.org/10.1142/s0217979293002481.

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This paper is devoted to the study of the ground state properties of an Ising chain in a magnetic Held of the form hi=h sin (ki+ϕ). The ground state energy is exactly computed in various situations. For a given h>2, the ground state energy E(h, k, ϕ) presents local minima as a function of k. This is a mode locking. If h<2, and only for k close enough. to π, the ground state is purely ferromagnetic, the transition being of the first order. As a general feature, the various physical quantities (magnetization, ground state energy…) are shown to be discontinuous at any rational value of k when the ground state is not ferromagnetic. Finally, the rigidity of the ground state under small displacement is also studied. All these results are compared to the ones obtained in a quite similar model: the Frenkel-Kontorova (FK) model. For instance, in our model which is shown to reduce to a constrained FK model, one can observe a lock-in transition, and the critical magnetic field hc(k) is computed, as opposed to the critical potential for the defectible/undefectible transition in the FK case. The hull function is also exactly computed. All these results are illustrated by means of numerical simulations.
10

TANG, BING, DE-JUN LI, KE HU, and YI TANG. "INTRINSIC LOCALIZED MODES IN QUANTUM FERROMAGNETIC ISING–HEISENBERG CHAINS WITH SINGLE-ION UNIAXIAL ANISOTROPY." International Journal of Modern Physics B 27, no. 25 (September 12, 2013): 1350139. http://dx.doi.org/10.1142/s0217979213501397.

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Based on the coherent-state method combined with the Dyson–Maleev representation of spin operators, the existence and properties of intrinsic localized spin-wave modes in quantum ferromagnetic Ising–Heisenberg chains with single-ion uniaxial anisotropy are investigated analytically in the semiclassical limit. With the help of the multiple-scale method combined with semidiscrete approximation, the equation of motion for the coherent-state amplitude is reduced to the nonlinear Schrödinger equation. It is found that, at the center of the Brillouin zone, a bright type intrinsic localized spin-wave mode can exist below the bottom of the linear spin-wave spectrum. Besides, we show that, at the boundary of the Brillouin zone, a dark type intrinsic localized spin-wave mode appears above the top of the linear spin-wave spectrum, which is different from the resonant nonpropagating kink mode.
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Статті в журналах Дисертації Книги

Дисертації з теми "Ising mode":

1

Kamenetsky, Dmitry, and dkamen@rsise anu edu au. "Ising Graphical Model." The Australian National University. ANU College of Engineering and Computer Science, 2010. http://thesis.anu.edu.au./public/adt-ANU20100727.221031.

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The Ising model is an important model in statistical physics, with over 10,000 papers published on the topic. This model assumes binary variables and only local pairwise interactions between neighbouring nodes. Inference for the general Ising model is NP-hard; this includes tasks such as calculating the partition function, finding a lowest-energy (ground) state and computing marginal probabilities. Past approaches have proceeded by working with classes of tractable Ising models, such as Ising models defined on a planar graph. For such models, the partition function and ground state can be computed exactly in polynomial time by establishing a correspondence with perfect matchings in a related graph. In this thesis we continue this line of research. In particular we simplify previous inference algorithms for the planar Ising model. The key to our construction is the complementary correspondence between graph cuts of the model graph and perfect matchings of its expanded dual. We show that our exact algorithms are effective and efficient on a number of real-world machine learning problems. We also investigate heuristic methods for approximating ground states of non-planar Ising models. We show that in this setting our approximative algorithms are superior than current state-of-the-art methods.
2

Li, Chengshu. "Tricritical Ising edge modes in a Majorana-Ising ladder." Thesis, University of British Columbia, 2017. http://hdl.handle.net/2429/62467.

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While Majorana fermions remain at large as fundamental particles, they emerge in condensed matter systems with peculiar properties. Grover et al. proposed a Majorana-Ising chain model, or the GSV model, where the system undergoes a tricritical Ising transition by tuning just one parameter. In this work, we generalize this model to a ladder with inter-chain Majorana couplings. From a mean field analysis, we argue that the tricritical Ising transition will also occur with inter-chain couplings that allow the system to be gapless in the non-interacting case. More crucially, based on analysis of the interacting chain model and the non-interacting ladder model, we expect the tricritical Ising modes to appear on the edges, a feature that might persist when going to 2d. We carry out extensive DMRG calculations to verify the theory in the ladder model. Finally, we discuss possible numerical probes of a 2d model.
Science, Faculty of
Physics and Astronomy, Department of
Graduate
3

Pugh, Mathew. "Ising model and beyond." Thesis, Cardiff University, 2008. http://orca.cf.ac.uk/54791/.

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We study the SU(3) AVE graphs, which appear in the classification of modular in variant partition functions from numerous viewpoints, including determination of their Boltzmann weights, representations of Hecke algebras, a new notion of A2 planar algebras and their modules, various Hilbert series of dimensions and spectral measures, and the K-theory of associated Cuntz-Krieger algebras. We compute the K-theory of the of the Cuntz-Krieger algebras associated to the SU(3) AVE graphs. We compute the numerical values of the Ocneanu cells, and consequently representations of the Hecke algebra, for the AVE graphs. Some such representations have appeared in the literature and we compare our results. We use these cells to define an SU(3) analogue of the Goodman-de la Harpe-Jones construction of a subfactor, where we embed the j42-Temperley-Lieb algebra in an AF path-algebra of the SU(3) AVE graphs. Using this construction, we realize all SU(3) modular invariants by subfactors previously announced by Ocneanu. We give a diagrammatic representation of the i42-Temperley-Lieb algebra, and show that it is isomorphic to Wenzl's representation of a Hecke algebra. Generalizing Jones's notion of a planar algebra, we construct an 42-planar algebra which captures the structure contained in the SU(3) AVE subfactors. We show that the subfactor for an AVE graph with a flat connection has a description as a flat >12-planar algebra. We introduce the notion of modules over an 42-planar algebra, and describe certain irreducible Hilbert A2- Temperley-Lieb-modules. A partial decomposition of the ,42-planar algebras for the AVE graphs is achieved. We compare various Hilbert series of dimensions associated to ADE models for SU(2), and the Hilbert series of certain Calabi-Yau algebras of dimension 3. We also consider spectral measures for the ADE graphs and generalize to SU(3), and in particular obtain spectral measures for the infinite SU(3) graphs.
4

Marsolais, Annette M. "The Equivalence Between the Kitaev, the Transverse Quantum Ising Model and the Classical Ising Model." University of Akron / OhioLINK, 2021. http://rave.ohiolink.edu/etdc/view?acc_num=akron1619792923386843.

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5

Silva, Romero Tavares da. "ALEATORIEDADE EM MODELOS DE ISING." Universidade de São Paulo, 1993. http://www.teses.usp.br/teses/disponiveis/43/43133/tde-22052012-133450/.

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Na primeira parte deste trabalho propomos uma aproximacão de campo médio dinâmico para analisar modelos de Ising com elementos e aleatoriedade definidos por distribuicões de probabilidades discretas. Analisamos o modelo com campo aleatório (S = 1/2), com interações aleatórias (S = 1/2), com diluição de sítios (S = 1/2) e com anisotropia aleatória (S = 1), obtendo  os respectivos diagramas de fases.   Na segunda parte analisamos modelos de vidros de spin (S= 3/2) com anisotropia de campo cristalino. Estudamos o modelo de van Hemmen, e o modelo clássico à la Sherrington e Kirkpatrick dentro do esquema de réplicas simétricas, obtendo os  diagramas de fases correspondentes.
In the first part of this work we propose a dynamical mean field approximation to analyse Ising models with elements of randomnss, defined by discret probability functions. We have analysed the random field model (S = 1/2); the random bond model (S = 1/2); the site diluted model (S = 3/2) and the random crystal field model (S = 1), obtaining the respective phase diagrams.   In the second part we have analysed spinglass models (S = 3/2) in the presence of a crystal field. We have studied the van Hemmen and the classic spin glass model à la Sherrington and Kirkpatrick, using replica symmetric scheme, to obtain the corresponding phase diagrams.
6

Ridderstolpe, Ludwig. "Exact Solutions of the Ising Model." Thesis, Uppsala universitet, Teoretisk astrofysik, 2017. http://urn.kb.se/resolve?urn=urn:nbn:se:uu:diva-329081.

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This report presents the general Ising model and its basic assumptions. This study aims to, from diagonalization of the Transfer Matrix, obtain the Helmholtz free energy and the exclusion of a phase transition for the one-dimensional Ising model under an external magnetic field. Furthermore from establishing the commutation relations of the Transfer matrices and using the Kramers-Wannier duality one finds the free energy and the presence of a phase transition for the square-lattice Ising model.
7

Smith, Thomas H. R. "Driven interfaces in the Ising model." Thesis, University of Bristol, 2010. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.535182.

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8

Gray, Sean. "Bootstrapping the Three-dimensional Ising Model." Thesis, Uppsala universitet, Teoretisk fysik, 2017. http://urn.kb.se/resolve?urn=urn:nbn:se:uu:diva-322146.

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This thesis begins with the fundamentals of conformal field theory in three dimensions. The general properties of the conformal bootstrap are then reviewed. The three-dimensional Ising model is presented from the perspective of the renormalization group, after which the conformal field theory aspect at the critical point is discussed. Finally, the bootstrap programme is applied to the three-dimensional Ising model using numerical techniques, and the results analysed.
9

Tamashiro, Mário Noboru. "Modelos de Ising com Competição." Universidade de São Paulo, 1996. http://www.teses.usp.br/teses/disponiveis/43/43133/tde-28022014-163442/.

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Neste trabalho consideramos três modelos de Ising com competição: que é gerada por acoplamentos dinâmicos de caráter antagônicos, pela própria geometria da rede subjacente ou através de interações de periodicidades uniaxiais competitivas e elementos de desordem. O primeiro modelo, no qual as técnicas de mecânica estatística de equilíbrio não se aplicam, consiste numa rede neural atratora completamente conectada com acoplamentos assimétricos armazenando p = 2 padrões, cuja evolução temporal pode ser descrita (no caso de atualização síncrona) por um mapeamento dissipativo bidimensional. O segundo modelo se refere ao problema clássico do antiferromagneto de Ising na rede triangular na presença de um campo magnético uniforme, investigado através de diversas aproximações - em particular, através de uma aproximação de Bethe-Peierls considerando três sub-redes interpenetrantes equivalentes. O terceiro modelo, introduzido para investigar o efeito de uma desordem congelada em um sistema magnético modulado, é definido pelo modelo ANNNI em um campo aleatório. Inicialmente consideramos um análogo deste modelo na árvore de Cayley, no limite de coordenação infinita, que pode ser formulado em termos de um mapeamento dissipativo bidimensional. A seguir, consideramos uma versão de campo médio em uma rede cúbica simples. que permite uma análise das superfícies de transição de primeira ordem e das linhas tricriticas.
In this work we consider three Ising models with competition: which is generated by dynamical couplings of antagonistic character, by the geometry of the underlying lattice, or by interactions of competitive uniaxial periodicities and disorder elements. The first model, for which equilibrium statistical mechanics techniques do not apply, consists in a fully connected attractor neural network storing p = 2 patterns, whose temporal evolution can be described (in the case of synchronous updating) by a two-dimensional dissipative mapping. The second model refers to the classic problem of the Ising antiferromagnet on the triangular lattice in the presence of a uniform magnetic field, which is investigated by various approximations - in particular, by a Bethe-Peierls approximation considering three interpenetrating equivalent sublattices. The third model, introduced to investigate the effects of quenched disorder in a modulated magnetic system, is defined by the ANNNI model in a random field. Initially we consider an analogous of this model on a Cayley tree, in the infinite-coordination limit, which can be formulated in terms of a two-dimensional dissipative mapping. Next, we consider a mean-field version on a simple cubic lattice, which allows for an analysis of the first-order transition surfaces and tricritical lines.
10

Hystad, Grethe. "Periodic Ising Correlations." Diss., The University of Arizona, 2009. http://hdl.handle.net/10150/196130.

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We consider the finite two-dimensional Ising model on a lattice with periodic boundaryconditions. Kaufman determined the spectrum of the transfer matrix on the finite,periodic lattice, and her derivation was a simplification of Onsager's famous result onsolving the two-dimensional Ising model. We derive and rework Kaufman's resultsby applying representation theory, which give us a more direct approach to computethe spectrum of the transfer matrix. We determine formulas for the spin correlationfunction that depend on the matrix elements of the induced rotation associated withthe spin operator. The representation of the spin matrix elements is obtained byconsidering the spin operator as an intertwining map. We wrap the lattice aroundthe cylinder taking the semi-infinite volume limit. We control the scaling limit of themulti-spin Ising correlations on the cylinder as the temperature approaches the criticaltemperature from below in terms of a Bugrij-Lisovyy conjecture for the spin matrixelements on the finite, periodic lattice. Finally, we compute the matrix representationof the spin operator for temperatures below the critical temperature in the infinite-volume limit in the pure state defined by plus boundary conditions.
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Книги з теми "Ising mode":

1

Chakrabarti, B. K. Quantum ising phases and transitions in transverse ising models. New York: Springer, 1996.

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2

Liebmann, R. Statistical mechanics of periodic frustrated Ising systems. Berlin: Springer-Verlag, 1986.

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3

Kremer, Sebastian. Oberflächendynamik im Q2R-Ising-Modell. Aachen: Verlag Shaker, 1992.

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4

MacFarland, T. Parallel simulation of the Ising model. Ithaca, N.Y: Cornell Theory Center, Cornell University, 1994.

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5

Baxter, Rodney J. Exactly solved models in statistical mechanics. London: Academic, 1989.

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6

Rychkov, Slava. Lectures on the Random Field Ising Model. Cham: Springer Nature Switzerland, 2023. http://dx.doi.org/10.1007/978-3-031-42000-9.

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7

Handrick, Klaus. Modelle zur Beschreibung magnetischer Wechselwirkungen zwischen paramagnetischen Zentren in niedrigdimensionalen Systemen. Aachen [Germany]: Shaker, 1992.

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8

Cerf, Raphaël. The Wulff crystal in Ising and percolation models: Ecole d'Ete de Probabilites de Saint-Flour XXXIV, 2004. Edited by Picard Jean. Berlin: Springer, 2006.

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9

Jerrum, Mark. Polynomial-time approximation algorithms for the Ising model. Edinburgh: University of Edinburgh Department of Computer Science, 1990.

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10

A, Jackson Kenneth. Monte Carlo simulation of the rapid crystallization of bismuth-doped silicon. [Washington, D.C: National Aeronautics and Space Administration, 1997.

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Частини книг з теми "Ising mode":

1

Strocchi, Franco. "11 Symmetry Breaking in the Ising Mode." In Symmetry Breaking, 131–38. Berlin, Heidelberg: Springer Berlin Heidelberg, 2005. http://dx.doi.org/10.1007/10981788_23.

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2

Nolting, Wolfgang, and Anupuru Ramakanth. "Ising Model." In Quantum Theory of Magnetism, 233–71. Berlin, Heidelberg: Springer Berlin Heidelberg, 2009. http://dx.doi.org/10.1007/978-3-540-85416-6_6.

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3

Stauffer, Dietrich, Friedrich W. Hehl, Nobuyasu Ito, Volker Winkelmann, and John G. Zabolitzky. "Ising Model." In Computer Simulation and Computer Algebra, 79–84. Berlin, Heidelberg: Springer Berlin Heidelberg, 1993. http://dx.doi.org/10.1007/978-3-642-78117-9_9.

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4

Eynard, Bertrand. "Ising Model." In Counting Surfaces, 365–407. Basel: Springer Basel, 2016. http://dx.doi.org/10.1007/978-3-7643-8797-6_8.

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5

Binek, Christian. "Ising-type Antiferromagnets: Model Systems in Statistical Physics." In Ising-type Antiferromagnets, 5–40. Berlin, Heidelberg: Springer Berlin Heidelberg, 2003. http://dx.doi.org/10.1007/978-3-540-45001-6_2.

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Suzuki, Sei, Jun-ichi Inoue, and Bikas K. Chakrabarti. "ANNNI Model in Transverse Field." In Quantum Ising Phases and Transitions in Transverse Ising Models, 73–103. Berlin, Heidelberg: Springer Berlin Heidelberg, 2013. http://dx.doi.org/10.1007/978-3-642-33039-1_4.

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7

Abaimov, Sergey G. "The Ising Model." In Springer Series in Synergetics, 149–223. Cham: Springer International Publishing, 2015. http://dx.doi.org/10.1007/978-3-319-12469-8_3.

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8

Salinas, Silvio R. A. "The Ising Model." In Graduate Texts in Contemporary Physics, 257–76. New York, NY: Springer New York, 2001. http://dx.doi.org/10.1007/978-1-4757-3508-6_13.

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9

Lévy, Laurent-Patrick. "The Ising Model." In Magnetism and Superconductivity, 117–31. Berlin, Heidelberg: Springer Berlin Heidelberg, 2000. http://dx.doi.org/10.1007/978-3-662-04271-7_6.

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10

Mattis, Daniel C. "The Ising Model." In Springer Series in Solid-State Sciences, 89–163. Berlin, Heidelberg: Springer Berlin Heidelberg, 1985. http://dx.doi.org/10.1007/978-3-642-82405-0_3.

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Тези доповідей конференцій з теми "Ising mode":

1

Legrady, George. "The Ising model." In SA '18: SIGGRAPH Asia 2018. New York, NY, USA: ACM, 2018. http://dx.doi.org/10.1145/3282805.3282812.

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2

Takesue, Hiroki, Takahiro Inagaki, Kensuke Inaba, Takuya Ikuta, Yasuhiro Yamada, Yuya Yonezu, and Toshimori Honjo. "Computation with degenerate optical parametric oscillator networks." In Optical Fiber Communication Conference. Washington, D.C.: Optica Publishing Group, 2024. http://dx.doi.org/10.1364/ofc.2024.w1f.2.

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Анотація:
We report the recent progress of a coherent Ising machine, which simulates the Ising model using a network of degenerate optical parametric oscillators (DOPO). We also describe a spiking neural network realized with DOPOs.
3

Chalupnik, Michelle, Anshuman Singh, James Leatham, Marko Lončar, and Mo Soltani. "Photonic Integrated Circuit Phased Array XY/Ising Model Solver." In Frontiers in Optics. Washington, D.C.: Optica Publishing Group, 2022. http://dx.doi.org/10.1364/fio.2022.jtu7b.6.

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4

Takesue, Hiroki, Yasuhiro Yamada, Kensuke Inaba, Takuya Ikuta, Yuya Yonezu, Takahiro Inagaki, Toshimori Honjo, et al. "Simulating Phase Transition in Two-Dimensional Ising Model on Coherent Ising Machine." In CLEO: Science and Innovations. Washington, D.C.: Optica Publishing Group, 2022. http://dx.doi.org/10.1364/cleo_si.2022.sf4f.4.

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We show that two-dimensionally coupled optical parametric oscillator pulses capture the signature of the exact phase transition of the two-dimensional Ising model rather than that of a mean-field one.
5

Yoshimura, Natsuhito, Masashi Tawada, Shu Tanaka, Junya Arai, Satoshi Yagi, Hiroyuki Uchiyama, and Nozomu Togawa. "Efficient Ising Model Mapping for Induced Subgraph Isomorphism Problems Using Ising Machines." In 2019 IEEE 9th International Conference on Consumer Electronics (ICCE-Berlin). IEEE, 2019. http://dx.doi.org/10.1109/icce-berlin47944.2019.8966218.

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6

Someya, Kenta, Ryoto Ono, and Takayuki Kawahara. "Novel Ising model using dimension-control for high-speed solver for Ising machines." In 2016 14th IEEE International New Circuits and Systems Conference (NEWCAS). IEEE, 2016. http://dx.doi.org/10.1109/newcas.2016.7604797.

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7

Li, Jinyu, Yu Pan, Hongfeng Yu, and Qi Zhang. "Prediction Approach for Ising Model Estimation." In 2019 International Conference on Data Mining Workshops (ICDMW). IEEE, 2019. http://dx.doi.org/10.1109/icdmw.2019.00106.

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Mondal, Ankit, and Ankur Srivastava. "Spintronics-based Reconfigurable Ising Model Architecture." In 2020 21st International Symposium on Quality Electronic Design (ISQED). IEEE, 2020. http://dx.doi.org/10.1109/isqed48828.2020.9137043.

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9

Kendon, V., D. Gunlycke, V. Vedral, and S. Bose. "Entanglement in a 1D Ising model." In International Conference on Quantum Information. Washington, D.C.: OSA, 2001. http://dx.doi.org/10.1364/icqi.2001.pa16.

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10

Nagao, Tomonori, Mayumi Ohmiya, Theodore E. Simos, George Psihoyios та Ch Tsitouras. "Networked Ising-Sznajd AR-β Model". У NUMERICAL ANALYSIS AND APPLIED MATHEMATICS: International Conference on Numerical Analysis and Applied Mathematics 2009: Volume 1 and Volume 2. AIP, 2009. http://dx.doi.org/10.1063/1.3241433.

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Звіти організацій з теми "Ising mode":

1

Gupta, R., and P. Tamayo. Critical exponents for the 3D Ising model. Office of Scientific and Technical Information (OSTI), March 1996. http://dx.doi.org/10.2172/251352.

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2

Ball, Justin R., and James B. Elliott. Simulating the Rayleigh-Taylor instability with the Ising model. Office of Scientific and Technical Information (OSTI), August 2011. http://dx.doi.org/10.2172/1113469.

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3

David P. Belanger. The random-field Ising model at high magnetic concentration. Office of Scientific and Technical Information (OSTI), April 2005. http://dx.doi.org/10.2172/838773.

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4

Parlett, Beresford, and Wee-Liang Heng. Implementation of Minimal Representations in 2d Ising Model Calculations. Fort Belvoir, VA: Defense Technical Information Center, May 1992. http://dx.doi.org/10.21236/ada256580.

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5

Parlett, Beresford, and Wee-Liang Heng. The Method of Minimal Representations in 2d Ising Model Calculations. Fort Belvoir, VA: Defense Technical Information Center, May 1992. http://dx.doi.org/10.21236/ada256581.

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6

Kepner, J. Canonical vs. micro-canonical sampling methods in a 2D Ising model. Office of Scientific and Technical Information (OSTI), December 1990. http://dx.doi.org/10.2172/6095623.

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