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Статті в журналах з теми "Mott-Hubbard transition"

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Bang, Y., C. Castellani, M. Grilli, G. Kotliar, R. Raimondi, and Z. Wang. "SINGLE PARTICLE AND OPTICAL GAPS IN CHARGE-TRANSFER INSULATORS." International Journal of Modern Physics B 06, no. 05n06 (March 1992): 531–45. http://dx.doi.org/10.1142/s0217979292000311.

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We analyze the collective excitations near a Mott-Hubbard and a metal charge transfer insulator transition, using the slave boson technique. We show that the Mott transition can be viewed as an excitonic softening, which takes place when the bound state between the lower and upper Hubbard bands reaches zero energy. The exciton energy is related to the jump of the chemical potential at zero doping. In a charge transfer insulator this mode describes a p-d charge fluctuation, i.e. it is a charge transfer exciton. In the single band Hubbard model the excitonic resonance describes virtual transitions between the lower and the upper Hubbard band. Finally we contrast the behaviour of the collective modes near the Mott transition with and near the Charge Transfer Instability. In the former the exciton energy and the charge compressibility go to zero. In the latter the exciton energy remains finite and the charge susceptibility diverges, causing phase separation.
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Montorsi, A., and M. Rasetti. "Mott-hubbard metal-insulator transition." Il Nuovo Cimento D 16, no. 10-11 (October 1994): 1649–57. http://dx.doi.org/10.1007/bf02462155.

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Le, Duc-Anh. "Mott transition in the dynamic Hubbard model within slave boson mean-field approach." Modern Physics Letters B 28, no. 10 (April 20, 2014): 1450078. http://dx.doi.org/10.1142/s021798491450078x.

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At zero temperature, the Kotliar–Ruckenstein slave boson mean-field approach is applied to the dynamic Hubbard model. In this paper, the influences of the dynamics of the auxiliary boson field on the Mott transition are investigated. At finite boson frequency, the Mott-type features of the Hubbard model is found to be enhanced by increasing the pseudospin coupling parameter g. For sufficiently large pseudospin coupling g, the Mott transition occurs even for modest values of the bare Hubbard interaction U. The lack of electron–hole symmetry is highlighted through the quasiparticle weight. Our results are in good agreement with the ones obtained by two-site dynamical mean-field theory and determinant quantum Monte Carlo simulation.
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Rozenberg, M. J., X. Y. Zhang, and G. Kotliar. "Mott-Hubbard transition in infinite dimensions." Physical Review Letters 69, no. 8 (August 24, 1992): 1236–39. http://dx.doi.org/10.1103/physrevlett.69.1236.

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SHASTRY, B. SRIRAM. "MOTT TRANSITION IN THE HUBBARD MODEL." Modern Physics Letters B 06, no. 23 (October 10, 1992): 1427–38. http://dx.doi.org/10.1142/s0217984992001137.

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In this article, I discuss W. Kohn’s criterion for a metal insulator transition, within the framework of a one-band Hubbard model. This and related ideas are applied to 1-dimensional Hubbard systems, and some interesting.miscellaneous results discussed. The Jordan-Wigner transformation converting the two species of fermions to two species of hardcore bosons is performed in detail, and the “extra phases” arising from odd-even effects are explicitly derived. Bosons are shown to prefer zero flux (i.e., diamagnetism), and the corresponding “happy fluxes” for the fermions identified. A curious result following from the interplay between orbital diamagnetism and spin polarization is highlighted. A“spin-statistics” like theorem, showing that the anticommutation relations between fermions of opposite spin are crucial to obtain the SU(2) invariance is pointed out.
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Noack, R. M., and F. Gebhard. "Mott-Hubbard Transition in Infinite Dimensions." Physical Review Letters 82, no. 9 (March 1, 1999): 1915–18. http://dx.doi.org/10.1103/physrevlett.82.1915.

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Lundin, Urban, Igor Sandalov, and Börje Johansson. "Mott–Hubbard transition in the N-orbital Hubbard model." Physica B: Condensed Matter 281-282 (June 2000): 836–37. http://dx.doi.org/10.1016/s0921-4526(99)00980-1.

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LE, DUC-ANH, and ANH-TUAN HOANG. "PHASE TRANSITION IN THE HALF-FILLED IONIC HUBBARD MODEL: MEAN-FIELD SLAVE BOSON STUDY." Modern Physics Letters B 26, no. 03 (January 30, 2012): 1150016. http://dx.doi.org/10.1142/s0217984911500163.

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We study electronic phase transitions in the half-filled ionic Hubbard model with an on-site Coulomb repulsion U and an ionic energy Δ by using the Kotliar–Ruckenstein slave-boson theory. Assuming a paramagnetic solution, we show that for any non-zero values of Δ, with increasing U the system undergoes a transition from band-insulator to Mott-insulator. Our results have implied the absence of a metallic phase between the band and the Mott insulator phases.
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Bao, An. "Mott transition in ruby lattice Hubbard model." Chinese Physics B 28, no. 5 (May 2019): 057101. http://dx.doi.org/10.1088/1674-1056/28/5/057101.

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Takenobu, T., T. Muro, Y. Iwasa, and T. Mitani. "Mott-Hubbard transition in alkali ammonia fullerides." Synthetic Metals 121, no. 1-3 (March 2001): 1173–74. http://dx.doi.org/10.1016/s0379-6779(00)01234-0.

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Дисертації з теми "Mott-Hubbard transition"

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Sordi, Giovanni. "Mott-Hubbard transition in strongly correlated electron systems." Paris 11, 2008. http://www.theses.fr/2008PA112160.

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J’ai étudié la transition méta-isolant avec la théorie du champ moyen dynamique appliquée à deux Hamiltoniens largement employés pour décrire les systèmes d’électrons fortement corrélés : le modèle de Hubbard et le modèle d’Anderson périodique. Le scénario pour la transition dans le modèle de Hubbard a été passé en revue et l’analyse du spectre de photoémission près de la transition a été présentée en détail. La transition de Mott induite par le dopage dans le modèle d’Anderson périodique a été discutée par rapport à celle réalisée dans le modèle de Hubbard. Le résultat principal nous conduit à établir un scénario qualitativement différent pour les transitions induites par dopage avec des électrons ou avec des trous. Dans le premier cas, la transition est, comme attendue, similaire à la transition du premier ordre du modèle de Hubbard. Toutefois, dans le dernier cas, une transition du deuxième ordre a été trouvée. J’ai donc démontré que le scénario pour la transition de Mott du modèle de Hubbard n’est pas générique pour le modèle d’Anderson périodique
I study the Mott metal-insulator transition within the dynamical mean-field theory in two schematic Hamiltonians widely used to describe the strongly correlated electron systems : the Hubbard model and the periodic Anderson model. The scenario for the transition in the Hubbard model is reviewed and the analysis of the photoemission spectra near the transition is presented in detail. The doping driven Mott transition in the periodic Anderson model is discussed with respect to the one realized in the Hubbard model. The main finding is a qualitatively different scenario for electron or hole driven transitions. In the former case the transition is expectedly similar to the first order transition of the Hubbard model. However, in the latter case, a second order transition is found. Thus I demonstrate that the transition scenario of the Hubbard model is not generic for the periodic Anderson model
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Capone, Massimo. "The Mott Transition: Role of Frustration and Orbital Degeneracy." Doctoral thesis, SISSA, 2000. http://hdl.handle.net/20.500.11767/4230.

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Pai, R. V., A. Punnoose, and R. A. Römer. "The Mott-Anderson transition in the disordered one-dimensional Hubbard model." Universitätsbibliothek Chemnitz, 1998. http://nbn-resolving.de/urn:nbn:de:bsz:ch1-199801405.

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We use the density matrix renormalization group to study the quantum transitions that occur in the half-filled one-dimensional fermionic Hubbard model with onsite potential disorder. We find a transition from the gapped Mott phase with algebraic spin correlations to a gapless spin-disordered phase beyond a critical strength of the disorder 1 c ss U= 2. Both the transitions in the charge and spin sectors are shown to be coincident. We also establish the finite-size corrections to the charge gap and the spin-spin correlation length in the presence of disorder and using a finite-size-scaling analysis we obtain the zero temperature phase diagram of the various quantum phase transitions that occur in the disorder-interaction plane.
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Blümer, Nils [Verfasser]. "Mott-Hubbard Metal-Insulator Transition and Optical Conductivity in High Dimensions / Nils Blümer." Aachen : Shaker, 2003. http://d-nb.info/1172609020/34.

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Bourassa, Louis. "Transition de Mott et supraconductivité dans les matériaux organiques." Mémoire, Université de Sherbrooke, 2017. http://hdl.handle.net/11143/10610.

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Dans ces travaux, nous avons étudié la rigidité superfluide en CDMFT (théorie du champ moyen dynamique sur amas) dans les matériaux organiques supraconducteurs. Ceux-ci appartiennent à la catégorie des supraconducteurs à haute température. Nous obtenons des résultats, en accord qualitatif avec l'expérience, qui suivent la tendance suggérée par la loi dite de Homes. La température critique et la masse effective ont donc également été calculées à des fins d'analyses. Ces dernières quantités sont également en accord avec l'expérience et les travaux antérieurs.
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Liu, Qinyong [Verfasser]. "Emergent Disorder : Nano-Domain Formation Near the First-Order Mott-Hubbard Transition / Qinyong Liu." Bonn : Universitäts- und Landesbibliothek Bonn, 2012. http://d-nb.info/1044081848/34.

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Winograd, Emilio. "Orbital-selectivity in strongly correlated fermionic systems. From materials to cold-atoms." Thesis, Paris 11, 2013. http://www.theses.fr/2013PA112031.

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Анотація:
Cette thèse se concentre sur des aspects multiorbitales des systèmes fermioniques fortement corrélés. En particulier, sur l'existence d'une différentiation orbitale dans laquelle la coexistence de caractère itinérant et localisé peut être associée à différentes orbitales. Cette problématique est examinée dans le contexte des atomes froids et des matériaux, offrant un pont entre les deux communautés.Dans la première partie de la thèse, nous donnons un aperçu du problème des corrélations fortes dans les matériaux, et nous introduisons le concept de 'transition de Mott sélective en orbitales'. Nous fournissons également les principaux outils pour comprendre comment les matériaux peuvent être simulés avec des atomes froids, et nous présentons des résultats importants liés à la transition métal-isolant de Mott. Les aspects techniques, basées sur la théorie du champ moyen dynamique sont également discutés, et la solution de deux principaux modèles de systèmes fermioniques fortement corrélés, à savoir le modèle d'Hubbard (HM) et le modèle de Falicov-Kimball (FKM), sont passés en revue.Ensuite, nous étudions en détail la physique de deux espèces fermioniques en interaction forte avec des masses différentes dans un réseau optique. Nous établissons les différentes phases (avec et sans ordre à longue portée) en termes de la force des interactions (U), du rapport des masses et de la température (T), et aussi nous discutons les variables thermodynamiques, qui sont pertinentes pour les expériences d'atomes froids. Nous montrons que dans la phase métallique (U inférieure à une valeur critique) et avec un certain degré de différence de masses, un 'crossover' apparaît entre un état métallique du type de liquide de Fermi à basse T, et un état avec différentiation orbital à haute T, où les fermions lourds se localisent tandis que les fermions légers restent itinérant. Par conséquent, nous proposons ce modèle minimal pour étudier la physique des systèmes qui présentent une différentiation orbitale avec des expériences d'atomes froids.Basé sur les propriétés du modèle étudié, nous proposons la 'chromatographie entropique' comme une nouvelle méthode pour refroidir des atomes fermioniques dans les réseaux optiques. Nous discutons son efficacité et ses limites, et fournissons quelques idées afin de les surmonter.Dans la dernière partie de la thèse, nous généralisons le modèle précédent aux matériaux corrélés à plusieurs bandes qui permet d'afficher la différentiation orbitale. Nous montrons que l'état de Mott sélectif en orbital peut être stable sous les distorsions du réseau, modélisées par une hybridation locale entre les orbitales. Cependant, l'état de Mott est caractérisé par un pseudo-gap, où les fluctuations de charge sont brusquement réduites, mais l'état reste compressible. En relation au modèle précédent, nous discutons le 'crossover' entre l'état métallique et l'état sélectif induit par des effets température, nous comparons nos résultats avec les expériences de photoémission, et nous prédisons ce qui se passerait dans les matériaux qui présentent une hybridation locale entre les bandes
This thesis focuses on multiorbital aspects of strongly correlated fermionic systems. In particular, it focuses on the existence of orbital differentiation in which coexistence of itinerant and localized character can be associated to different orbitals. This subject is discussed in the context of cold atoms and materials, providing a bridge between both communities.In the first part of the thesis, we give an insight into the problem of strong correlations in materials, and we introduce the concept of 'orbital-selective Mott transition'. We also provide the main tools to understand how materials can be simulated with cold atoms experiments, and we present important related results in the context of the metal-Mott insulator transition. The technical aspects, based on dynamical mean-field theory are also discussed, and the solution of two key models of strongly correlated fermionic systems, i.e., the Hubbard model (HM) and the Falicov-Kimball model (FKM), are reviewed.Then we study in detail the physics of two interacting fermionic species with different masses in an optical lattice. We establish the different phases (with and without long-range order) in terms of the interactions strength (U), mass ratio and temperature (T), and also discuss the thermodynamic variables, which are relevant in cold atoms experiments. We show that in the metallic phase (U below a critical value) and for some degree of mass imbalance, a crossover appears between a Fermi-liquid metallic state at low T, and an 'orbital-selective' state at higher T, where the heavy fermions effectively localize while the light species remain itinerant. Hence, we propose this minimal model for addressing orbital-selective physics with cold atoms experiments.Based on the properties of the studied model, we propose the 'entropic chromatography' as a new method for cooling fermionic atoms in optical lattices. We discuss its efficiency and limitations, and provide some ideas in order to overcome them.In the last part of the thesis we generalize the previous model to a model relevant for multiband correlated materials that can display orbital differentiation. We show that the orbital-selective Mott state can be stable under lattice distortions modeled by local hybridization between the orbitals. However, the Mott state is characterized by a pseudogap, where charge fluctuations abruptly reduce, but the state remains compressible. In connection with the previous model, we discuss the temperature-induced orbital-selective crossover in this problem, we compare our results with photoemission experiments, and predict what would happen in materials that display local hybridization between the bands
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Costa, Karine Piacentini Coelho da. "Estudo do modelo de Bose-Hubbard usando o algoritmo Worm." Universidade de São Paulo, 2011. http://www.teses.usp.br/teses/disponiveis/43/43134/tde-27022012-085711/.

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Nesta dissertação estudaremos sistemas de bósons ultrafrios armadilhados em uma rede ótica quadrada bidimensional sem levar em consideração o confinamento harmônico. A dinâmica desses sistemas é bem descrita pelo modelo de Bose-Hubbard, que prevê uma transição de fase quântica de um superfluido para um isolante de Mott a temperaturas baixas, e pode ser induzida variando a profundidade do potencial da rede ótica. Apresentaremos o diagrama de fases dessa transição construído a partir de uma aproximação de campo médio e também com um cálculo numérico usando um algoritmo de Monte Carlo Quântico, denominado algoritmo Worm. Encontramos o ponto crítico para o primeiro lobo de Mott em ambos os casos, concordando com trabalhos anteriores.
This work study the two-dimensional ultracold bosonic atoms loaded in a square optical lattice, without harmonic confinement. The dynamics of this system is described by the Bose-Hubbard model, which predicts a quantum phase transition from a superfluid to a Mott-insulator at low temperatures that can be induced by varying the depth of the optical potential. We present here the phase diagram of this transition built from a mean field approach and from a numerical calculation using a Quantum Monte Carlo algorithm, namely the Worm algorithm. We found the critical transition point for the first Mott lobe in both cases, in agreement with the standard literature.
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Suárez, Villagrán Martha Yolima 1984. "Estudos do modelo de Hubbard desordenado em duas dimensões." [s.n.], 2013. http://repositorio.unicamp.br/jspui/handle/REPOSIP/276990.

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Анотація:
Orientador: Eduardo Miranda
Tese (doutorado) - Universidade Estadual de Campinas, Instituto de Física Gleb Wataghin
Made available in DSpace on 2018-08-23T18:51:04Z (GMT). No. of bitstreams: 1 SuarezVillagran_MarthaYolima_D.pdf: 7321255 bytes, checksum: d76479a0e0c1143207cb4ee380a8034d (MD5) Previous issue date: 2013
Resumo: Estudamos nesta tese alguns aspectos da transição metal-isolante de Mott no caso desordenado. O modelo no qual baseamos nosso estudo é o modelo de Hubbard desordenado, que é o modelo mais simples a apresentar a transição metal-isolante de Mott. Analisamos esse modelo através da Teoria Dinâmica de Campo Médio Estatística (StatDMFT). Essa teoria é uma extensão natural da Teoria Dinâmica de Campo Médio (DMFT), que foi usada com relativo sucesso nos últimos anos para analisar a transição de Mott no caso limpo. Como no caso dessa última, a StatDMFT incorpora os efeitos de correlação eletrônica apenas nos seus aspetos locais. A desordem é tratada de maneira a incorporar todos os efeitos de localização de Anderson. Com essa técnica, analisamos a transição de Mott desordenada no caso bi-dimensional, usando o Monte Carlo quântico para resolver os problemas de impureza única de Anderson requeridos pela StatDMFT. Encontramos as linhas espinodais nas quais o metal e o isolante deixam de ser meta-estáveis. Também estudamos os padrões espaciais das flutuações de quantidades locais, como a auto-energia e a função de Green local, e mostramos como há o aparecimento de regiões metálicas dentro do isolante e viceversa. Analisamos efeitos de tamanho finito e mostramos que, em consonância com os teoremas de Imry e Ma, a transição de primeira ordem desaparece no limite termodinâmico. Analisamos as propriedades de transporte desse sistema através de um mapeamento a um sistema de resistores aleatórios clássicos e calculamos a corrente média e sua distribuição através da transição metal-isolante. Finalmente, estudamos o comportamento da parede de domínio que se forma entre o isolante e o metal no caso limpo. Isso foi feito através de um modelo de uma cadeia unidimensional conectada a reservatórios, um metálico e um isolante, cada um em uma de suas extremidades. Nesse caso, utilizamos o método da Teoria de Perturbação Iterada para a solução dos modelos de impureza única. Encontramos o comportamento da parede como função da temperatura e das interações
Abstract: In this thesis, we studied some aspects of the Mott metal-insulator transition in the disordered case. The model on which we based our analysis is the disordered Hubbard model, which is the simplest model capable of capturing the Mott metal-insulator transition. We investigated this model through the Statistical Dynamical Mean-Field Theory (statDMFT). This theory is a natural extension of the Dynamical Mean-Field Theory (DMFT), which has been used with relative success in the last several years with the purpose of describing the Mott transition in the clean case. As is the case for the latter theory, the statDMFT incorporates the electronic correlation effects only incorporate Anderson localization effects.. With this technique, we analyzed the disordered two-dimensional Mott transition, using Quantum Monte Carlo to solve the associated single-impurity problems. We found the spinodal lines at which metal and insulator cease to be meta-stable. We also studied the spatial fluctuations of local quantities, such as the self-energy and the local Green¿s function, and showed the appearance of metallic regions within the insulator and vice-versa. We carried out an analysis of finite-size effects and showed that, in agreement with the theorems of Imry and Ma, the first-order transition is smeared in the thermodynamic limit. We analyzed transport properties by means of a mapping to a random classical resistor network and calculated both the average current and its distribution across the metalinsulator transition. Finally, we studied the behavior of the domain wall which forms between the metal and the insulator in the clean case. This was done by means of a model of a one-dimensional chain connected to two reservoirs, one metallic and the other insulating, each attached to one of the chain¿s ends. In this case, we used the Iterated Perturbation Theory technique in order to solve the associated singleimpurity problems. We then established the behavior of the domain wall width as a function of temperature and interactions
Doutorado
Física
Doutora em Ciências
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Schäfer, Steffen. "Approximation des Phases Aléatoires Self-Consistante dans le Modèle de Hubbard." Phd thesis, Université Joseph Fourier (Grenoble), 1998. http://tel.archives-ouvertes.fr/tel-00002990.

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La RPA Self-Consistante (SCRPA) est appliquée aux fonctions de corrélation particule-trou dans le Modèle de Hubbard.

Pour une fonction de Green générale à $n$ corps cette méthode se dérive à partir de l'Equation de Dyson où seules sont retenues les contributions instantanées de l'opérateur de masse. La fonction de Green est alors donnée par un système d'équations intégrales non-linéaires que l'on cherchera à résoudre de façon self-consistante. Elle satisfait, parmi d'autres théorèmes, la règle de somme pondérée par l'énergie. Pour les fonctions de Green à une et à deux particules, la SCRPA obéit à un principe variationnel. Dans le Modèle de Hubbard les fonctions de corrélation de charge et de spin sont calculées en SCRPA. En négligeant les densités connectées à deux corps, nous obtenons une théorie self-consistante plus simple, la RPA renormalisée. Les deux méthodes sont étudiées et comparées à la RPA standard.

Nous établissons et résolvons numériquement les équations de la RPA renormalisée pour les fonctions de corrélations de densité de charge dans le Modèle de Hubbard à une dimension. Les susceptibilités de charge et de spin longitudinal, la distribution des impulsions et plusieurs propriétés du fondamental sont évaluées et comparées aux résultats exacts. Dans la limite du couplage fort de la bande à moitié remplie, la RPA renormalisée possède une solution analytique qui est, à un facteur près, en accord avec le développement pour fortes interactions de l'ansatz de Bethe. Comme prévu, des particularités liées à la dimension spatiale $1$, par exemple un comportement de liquide de Luttinger, n'ont pas pu être retrouvées. Or, la description fournie par notre méthode pourrait être assez réaliste en dimensions plus élevées.

Une partie de ces travaux a été publié dans
"Dyson Equation Approach to Many-Body Greens Functions and
Self-Consistent RPA, First Application to the Hubbard Model"
Steffen Schäfer, Peter Schuck, Phys. Rev. B 59, 1712-1733 (1999).
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Книги з теми "Mott-Hubbard transition"

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mer, Nils Blu. Mott-Hubbard metal-insulator transition and optical conductivity in high dimensions. Aachen: Shaker, 2003.

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1953-, Fujimori A., Tokura Y. 1954-, and Taniguchi International Symposium on the Theory of Condensed Matter (17th : 1994 : Kashikojima, Japan), eds. Spectroscopy of mott insulators and correlated metals: Proceedings of the 17th Taniguchi Symposium, Kashikojima, Japan, October 24-28, 1994. Berlin: Springer, 1995.

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3

Gebhard, Florian. The mott metal-insulator transition: Models and methods. New York: Springer, 1997.

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Fujimori, Atsushi, and Yoshinori Tokura. Spectroscopy of Mott Insulators and Correlated Metals: Proceedings of the 17th Taniguchi Symposium, Kashikojima, Japan, October 24 - 28, 1994 (Springer Series in Solid-State Sciences). Springer, 1995.

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Частини книг з теми "Mott-Hubbard transition"

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Brune, Ph, and A. P. Kampf. "Band to Mott Insulator Transition in the Ionic Hubbard Model." In High Performance Computing in Science and Engineering ’01, 167–77. Berlin, Heidelberg: Springer Berlin Heidelberg, 2002. http://dx.doi.org/10.1007/978-3-642-56034-7_15.

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Noack, R. M., C. Aebischer, D. Baeriswyl, and F. Gebhard. "Studies of the Mott-Hubbard Transition in one and Infinite Dimensions." In Open Problems in Strongly Correlated Electron Systems, 347–59. Dordrecht: Springer Netherlands, 2001. http://dx.doi.org/10.1007/978-94-010-0771-9_36.

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3

Kim, Changman, Tomoya Ohool, Takeshi Tamura, Yasushi Oikawa, Jae-Soo Shin, and Hajime Ozaki. "The Relation Between Peierls and Mott-Hubbard Transition in VO2, by Tunneling Spectroscopy." In Advanced Processing and Manufacturing Technologies for Structural and Multifunctional Materials II, 147–54. Hoboken, NJ, USA: John Wiley & Sons, Inc., 2009. http://dx.doi.org/10.1002/9780470456224.ch15.

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4

Goodenough, J. B., and J. S. Zhou. "Vibronic Phenomena At Localized-Itinerant and Mott-Hubbard Transitions." In Supermaterials, 37–47. Dordrecht: Springer Netherlands, 2000. http://dx.doi.org/10.1007/978-94-010-0912-6_4.

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5

Spałek, J., and W. Wójcik. "Almost Localized Fermions and Mott-Hubbard Transitions at Non-Zero Temperature." In Spectroscopy of Mott Insulators and Correlated Metals, 41–65. Berlin, Heidelberg: Springer Berlin Heidelberg, 1995. http://dx.doi.org/10.1007/978-3-642-57834-2_5.

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6

"Mott Transition and Hubbard Model." In Lecture Notes on Electron Correlation and Magnetism, 147–97. WORLD SCIENTIFIC, 1999. http://dx.doi.org/10.1142/9789812386274_0004.

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7

SRIRAM SHASTRY, B. "MOTT TRANSITION IN THE HUBBARD MODEL." In Selected Topics in Superconductivity, 153–63. WORLD SCIENTIFIC, 1993. http://dx.doi.org/10.1142/9789814354660_0007.

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8

"The Mott Transition and the Hubbard Model." In Quantum Electron Liquids and High-T c Superconductivity, 151–73. Berlin, Heidelberg: Springer Berlin Heidelberg, 1995. http://dx.doi.org/10.1007/978-3-540-47678-8_7.

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9

"Band Structures of Mott–Hubbard Materials and the Transition Metal Ionic Compounds, and Polaron." In Elements of Structures and Defects of Crystalline Materials, 201–5. Elsevier, 2018. http://dx.doi.org/10.1016/b978-0-12-814268-4.00019-9.

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10

Byczuk, Krzysztof, Walter Hofstetter, and Dieter Vollhardty. "ANDERSON LOCALIZATION VS. MOTT–HUBBARD METAL–INSULATOR TRANSITION IN DISORDERED, INTERACTING LATTICE FERMION SYSTEMS." In 50 Years of Anderson Localization, 473–501. WORLD SCIENTIFIC, 2010. http://dx.doi.org/10.1142/9789814299084_0020.

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Тези доповідей конференцій з теми "Mott-Hubbard transition"

1

Takenobu, T. "Mott-Hubbard transition and antiferromagnetism in ammoniated alkali fullerides." In The 14th international winterschool on electronic properties of novel materials - molecular nanostructures. AIP, 2000. http://dx.doi.org/10.1063/1.1342462.

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2

Otsuka, Yuichi, Seiji Yunoki та Sandro Sorella. "Mott Transition in the 2D Hubbard Model with π-Flux". У Proceedings of the International Conference on Strongly Correlated Electron Systems (SCES2013). Journal of the Physical Society of Japan, 2014. http://dx.doi.org/10.7566/jpscp.3.013021.

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3

Ostmeyer, Johann, Evan Berkowitz, Stefan Krieg, Timo Lahde, Thomas Luu, and Carsten Urbach. "The Semimetal-Antiferromagnetic Mott Insulator Quantum Phase Transition of the Hubbard Model on the Honeycomb Lattice." In The 38th International Symposium on Lattice Field Theory. Trieste, Italy: Sissa Medialab, 2022. http://dx.doi.org/10.22323/1.396.0303.

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4

Wada, Y., T. Furuta, and M. Yamashita. "Optical, magnetic, and electrical studies of the metal-insulator transition in the mott-hubbard MMX-chain system." In International Conference on Science and Technology of Synthetic Metals. IEEE, 1994. http://dx.doi.org/10.1109/stsm.1994.835971.

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5

Watanabe, Tsutomu, Hisatoshi Yokoyama, and Kenji Kobayashi. "Impurity Effect on Magnetism and Mott Transitions in Hubbard Model on Anisotropic Triangular Lattice." In Proceedings of the International Conference on Strongly Correlated Electron Systems (SCES2019). Journal of the Physical Society of Japan, 2020. http://dx.doi.org/10.7566/jpscp.30.011004.

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