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Journal articles on the topic 'Condensed matter systems'

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1

Wölfle, Peter. "Quasiparticles in condensed matter systems." Reports on Progress in Physics 81, no. 3 (January 22, 2018): 032501. http://dx.doi.org/10.1088/1361-6633/aa9bc4.

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2

Kobes, R., and G. Semenoff. "Cutkosky rules for condensed-matter systems." Physical Review B 34, no. 6 (September 15, 1986): 4338–41. http://dx.doi.org/10.1103/physrevb.34.4338.

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3

Slusher, R. E., and C. Weisbuch. "Optical microcavities in condensed matter systems." Solid State Communications 92, no. 1-2 (October 1994): 149–58. http://dx.doi.org/10.1016/0038-1098(94)90868-0.

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4

Laflorencie, Nicolas. "Quantum entanglement in condensed matter systems." Physics Reports 646 (August 2016): 1–59. http://dx.doi.org/10.1016/j.physrep.2016.06.008.

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5

Zurek, W. H. "Cosmological experiments in condensed matter systems." Physics Reports 276, no. 4 (November 1996): 177–221. http://dx.doi.org/10.1016/s0370-1573(96)00009-9.

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6

Nenno, Dennis M., Christina A. C. Garcia, Johannes Gooth, Claudia Felser, and Prineha Narang. "Axion physics in condensed-matter systems." Nature Reviews Physics 2, no. 12 (September 30, 2020): 682–96. http://dx.doi.org/10.1038/s42254-020-0240-2.

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7

LEV, B. I. "CELLULAR STRUCTURE IN CONDENSED MATTER." Modern Physics Letters B 27, no. 28 (October 24, 2013): 1330020. http://dx.doi.org/10.1142/s0217984913300202.

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In this paper, general description of a cellular structure formation in a system of interacting particles has been proposed. Analytical results are presented for such structures in colloids, systems of particles immersed into a liquid crystal and gravitational systems. It is shown that physical nature of formation of cellular structures in all systems of interacting particles is identical. In all cases, a characteristic of the cellular structure, depending on strength of the interaction, concentration of particles and temperature, can be obtained.
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8

Li, Qiang, and Dmitri E. Kharzeev. "Chiral magnetic effect in condensed matter systems." Nuclear Physics A 956 (December 2016): 107–11. http://dx.doi.org/10.1016/j.nuclphysa.2016.03.055.

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9

Fayer, Michael D. "Picosecond FEL experiments on condensed matter systems." Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment 304, no. 1-3 (July 1991): 797. http://dx.doi.org/10.1016/0168-9002(91)90979-z.

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10

Ma, Chen-Te. "A duality web in condensed matter systems." Annals of Physics 390 (March 2018): 107–30. http://dx.doi.org/10.1016/j.aop.2018.01.008.

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11

Hutter, Jürg, Marcella Iannuzzi, Florian Schiffmann, and Joost VandeVondele. "cp2k: atomistic simulations of condensed matter systems." Wiley Interdisciplinary Reviews: Computational Molecular Science 4, no. 1 (June 13, 2013): 15–25. http://dx.doi.org/10.1002/wcms.1159.

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12

Singleton, Douglas, and Jerzy Dryzek. "Electromagnetic-field angular momentum in condensed matter systems." Physical Review B 62, no. 19 (November 15, 2000): 13070–75. http://dx.doi.org/10.1103/physrevb.62.13070.

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13

Bishop, A. R. "Mesoscopic phenomena in two-dimensional condensed matter systems." Physica Scripta T49B (January 1, 1993): 667–71. http://dx.doi.org/10.1088/0031-8949/1993/t49b/049.

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14

Mosseri, Rémy. "Geometrical frustration and defects in condensed matter systems." Comptes Rendus Chimie 11, no. 3 (March 2008): 192–97. http://dx.doi.org/10.1016/j.crci.2007.03.019.

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15

Gay-Balmaz, François, Michael Monastyrsky, and Tudor S. Ratiu. "Lagrangian Reductions and Integrable Systems in Condensed Matter." Communications in Mathematical Physics 335, no. 2 (February 22, 2015): 609–36. http://dx.doi.org/10.1007/s00220-015-2317-9.

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16

Spagnolo, Bernardo, Claudio Guarcello, Luca Magazzù, Angelo Carollo, Dominique Persano Adorno, and Davide Valenti. "Nonlinear Relaxation Phenomena in Metastable Condensed Matter Systems." Entropy 19, no. 1 (December 31, 2016): 20. http://dx.doi.org/10.3390/e19010020.

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17

Hofstetter, W., and T. Qin. "Quantum simulation of strongly correlated condensed matter systems." Journal of Physics B: Atomic, Molecular and Optical Physics 51, no. 8 (March 29, 2018): 082001. http://dx.doi.org/10.1088/1361-6455/aaa31b.

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18

Isaacs, Eric D., and Phil Platzman. "Inelastic X‐Ray Scattering in Condensed Matter Systems." Physics Today 49, no. 2 (February 1996): 40–45. http://dx.doi.org/10.1063/1.881488.

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19

Shi, Yu. "Quantum entanglement in second-quantized condensed matter systems." Journal of Physics A: Mathematical and General 37, no. 26 (June 17, 2004): 6807–22. http://dx.doi.org/10.1088/0305-4470/37/26/014.

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20

Mehlig, B., D. W. Heermann, and B. M. Forrest. "Hybrid Monte Carlo method for condensed-matter systems." Physical Review B 45, no. 2 (January 1, 1992): 679–85. http://dx.doi.org/10.1103/physrevb.45.679.

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21

Ammon, M. "Gauge/gravity duality applied to condensed matter systems." Fortschritte der Physik 58, no. 11-12 (October 11, 2010): 1123–250. http://dx.doi.org/10.1002/prop.201000080.

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22

Lang, M. "Condensed Matter Systems with Variable Many‐Body Interactions." physica status solidi (b) 256, no. 9 (September 2019): 1900505. http://dx.doi.org/10.1002/pssb.201900505.

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23

Fernando, Gayanath W., R. Matthias Geilhufe, Adil-Gerai Kussow, and W. Wasanthi P. De Silva. "Driven emergent phases in small interacting condensed-matter systems." EPL (Europhysics Letters) 134, no. 3 (May 1, 2021): 37004. http://dx.doi.org/10.1209/0295-5075/134/37004.

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24

Baumgratz, Tillmann, and Martin B. Plenio. "Lower bounds for ground states of condensed matter systems." New Journal of Physics 14, no. 2 (February 13, 2012): 023027. http://dx.doi.org/10.1088/1367-2630/14/2/023027.

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25

Lang, Peter. "Surface induced ordering effects in soft condensed matter systems." Journal of Physics: Condensed Matter 16, no. 23 (May 29, 2004): R699—R720. http://dx.doi.org/10.1088/0953-8984/16/23/r02.

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26

Melnikov, G. "The quasicrystal model of cluster systems in condensed matter." IOP Conference Series: Materials Science and Engineering 168 (January 2017): 012020. http://dx.doi.org/10.1088/1757-899x/168/1/012020.

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27

Buividovich, P. V., and M. V. Ulybyshev. "Applications of lattice QCD techniques for condensed matter systems." International Journal of Modern Physics A 31, no. 22 (August 9, 2016): 1643008. http://dx.doi.org/10.1142/s0217751x16430089.

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We review the application of lattice QCD techniques, most notably the Hybrid Monte Carlo (HMC) simulations, to first-principle study of tight-binding models of crystalline solids with strong inter-electron interactions. After providing a basic introduction into the HMC algorithm as applied to condensed matter systems, we review HMC simulations of graphene, which in the recent years have helped to understand the semimetal behavior of clean suspended graphene at the quantitative level. We also briefly summarize other novel physical results obtained in these simulations. Then we comment on the applicability of hybrid Monte Carlo to topological insulators and Dirac and Weyl semimetals and highlight some of the relevant open physical problems. Finally, we also touch upon the lattice strong-coupling expansion technique as applied to condensed matter systems.
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28

Srivastava, Ajit Mohan. "String defects in condensed-matter systems as optical fibers." Physical Review B 50, no. 9 (September 1, 1994): 5829–33. http://dx.doi.org/10.1103/physrevb.50.5829.

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29

Scalapino, D. J. "Simulations: A tool for studying quantum condensed matter systems." Journal of Statistical Physics 43, no. 5-6 (June 1986): 757–70. http://dx.doi.org/10.1007/bf02628303.

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30

Selke, Walter. "Monte Carlo and molecular dynamics of condensed matter systems." Journal of Statistical Physics 87, no. 3-4 (May 1997): 959–60. http://dx.doi.org/10.1007/bf02181259.

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31

Sarkar, Tapobrata, Hernando Quevedo, and Rong-Gen Cai. "Information Geometry: From Black Holes to Condensed Matter Systems." Advances in High Energy Physics 2013 (2013): 1–2. http://dx.doi.org/10.1155/2013/465957.

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32

Swain, John, Allan Widom, and Yogendra N. Srivastava. "Low Energy Standard Model Interactions in Condensed Matter." Key Engineering Materials 644 (May 2015): 57–60. http://dx.doi.org/10.4028/www.scientific.net/kem.644.57.

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This paper briey reviews the current status of Standard Model (weak and strong nuclear) interactions induced in condensed matter systems via the excitation of collective de-grees of freedom to provide the necessary energies. The central point is that a variety of low energy systems can accelerate electrons to several MeV, making it possible to produce neutrons via collisions with protons and to photodissociate nuclei via giant dipole resonances allowing a wide variety of nuclear transmutations to occur. Some sample systems are discussed as well as some of their implications.
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33

Cartwright, Julyan H. E. "Nonlinear dynamics determines the thermodynamic instability of condensed matter in vacuo." Philosophical Transactions of the Royal Society A: Mathematical, Physical and Engineering Sciences 378, no. 2174 (June 8, 2020): 20190534. http://dx.doi.org/10.1098/rsta.2019.0534.

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Condensed matter is thermodynamically unstable in a vacuum. That is what thermodynamics tells us through the relation showing that condensed matter at temperatures above absolute zero always has non-zero vapour pressure. This instability implies that at low temperatures energy must not be distributed equally among atoms in the crystal lattice but must be concentrated. In dynamical systems such concentrations of energy in localized excitations are well known in the form of discrete breathers, solitons and related nonlinear phenomena. It follows that to satisfy thermodynamics such localized excitations must exist in systems of condensed matter at arbitrarily low temperature and as such the nonlinear dynamics of condensed matter is crucial for its thermodynamics. This article is part of the theme issue ‘Stokes at 200 (Part 1)’.
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34

Lazar, Emanuel A., Jian Han, and David J. Srolovitz. "Topological framework for local structure analysis in condensed matter." Proceedings of the National Academy of Sciences 112, no. 43 (October 12, 2015): E5769—E5776. http://dx.doi.org/10.1073/pnas.1505788112.

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Physical systems are frequently modeled as sets of points in space, each representing the position of an atom, molecule, or mesoscale particle. As many properties of such systems depend on the underlying ordering of their constituent particles, understanding that structure is a primary objective of condensed matter research. Although perfect crystals are fully described by a set of translation and basis vectors, real-world materials are never perfect, as thermal vibrations and defects introduce significant deviation from ideal order. Meanwhile, liquids and glasses present yet more complexity. A complete understanding of structure thus remains a central, open problem. Here we propose a unified mathematical framework, based on the topology of the Voronoi cell of a particle, for classifying local structure in ordered and disordered systems that is powerful and practical. We explain the underlying reason why this topological description of local structure is better suited for structural analysis than continuous descriptions. We demonstrate the connection of this approach to the behavior of physical systems and explore how crystalline structure is compromised at elevated temperatures. We also illustrate potential applications to identifying defects in plastically deformed polycrystals at high temperatures, automating analysis of complex structures, and characterizing general disordered systems.
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35

Bhatnagar, Neha. "Some Applications of Holography to Study Strongly Correlated Systems." EPJ Web of Conferences 177 (2018): 09002. http://dx.doi.org/10.1051/epjconf/201817709002.

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In this work, we study the transport coefficients of strongly coupled condensed matter systems using gauge/gravity duality (holography). We consider examples from the real world and evaluate the conductivities from their gravity duals. Adopting the bottom-up approach of holography, we obtain the frequency response of the conductivity for (1+1)-dimensional systems. We also evaluate the DC conductivities for non-relativistic condensed matter systems with hyperscaling violating geometry.
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36

MATSUURA, HIROYUKI. "RELATIVISTIC QUANTUM FIELD THEORY FOR CONDENSED SYSTEMS-(I): (GENERAL FORMALISM)." International Journal of Modern Physics B 17, no. 25 (October 10, 2003): 4477–90. http://dx.doi.org/10.1142/s0217979203023069.

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We proposed Atomic Schwinger–Dyson method (ASD method) in this paper, which was the nonperturbative and finite relativistic quantum field theory, and we treat many electron system and electronic matter. The ASD formalism consists of coupled Dyson equations of electrons and photons. Since, it includes self-energies in a nonperturbative way, higher-order correlations beyond Hartee–Fock approximation are taken into account. Some important differences between the ASD formalism for the system of finite electron density and SD formalism of zero electron density are shown. The main difference is due to the existence of condensed photon field, symmetry breaking, and what we call, Coulomb's potential. By paying special attention to the treatment of the condensed photon fields, the coupled Dyson equations of electron and photon are derived based on functional propagator method. It is shown that this treatment of the condensed fields naturally leads to tadpole energy, which cancels the Hartree energy. By using these photon propagators, explicit expression of ASD coupled equations and the energy density of matters are derived for numerical calculations in a subsequent paper. Similarities and differences between ASD and traditional methods such as the mean field theory or the Hartree–Fock method are discussed; it is shown that these traditional methods were included in our ASD formalism.
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37

Suzuki, Michi-To, Hiroaki Ikeda, and Peter M. Oppeneer. "First-principles Theory of Magnetic Multipoles in Condensed Matter Systems." Journal of the Physical Society of Japan 87, no. 4 (April 15, 2018): 041008. http://dx.doi.org/10.7566/jpsj.87.041008.

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38

Prezhdo, Oleg V. "Modeling Non-adiabatic Dynamics in Nanoscale and Condensed Matter Systems." Accounts of Chemical Research 54, no. 23 (November 10, 2021): 4239–49. http://dx.doi.org/10.1021/acs.accounts.1c00525.

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39

EBELING, WERNER, and BERNARDO SPAGNOLO. "GUEST EDITORS' EDITORIAL: NOISE IN CONDENSED MATTER AND COMPLEX SYSTEMS." Fluctuation and Noise Letters 05, no. 02 (June 2005): L159—L161. http://dx.doi.org/10.1142/s0219477505002495.

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40

Cazalilla, M. A., R. Citro, T. Giamarchi, E. Orignac, and M. Rigol. "One dimensional bosons: From condensed matter systems to ultracold gases." Reviews of Modern Physics 83, no. 4 (December 1, 2011): 1405–66. http://dx.doi.org/10.1103/revmodphys.83.1405.

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41

Slichter, C. P. "The Knight shift—a powerful probe of condensed-matter systems." Philosophical Magazine B 79, no. 9 (September 1999): 1253–61. http://dx.doi.org/10.1080/13642819908216968.

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42

Salmhofer, Manfred. "Renormalization in condensed matter: Fermionic systems – from mathematics to materials." Nuclear Physics B 941 (April 2019): 868–99. http://dx.doi.org/10.1016/j.nuclphysb.2018.07.004.

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43

Bravo-Prieto, Carlos, Josep Lumbreras-Zarapico, Luca Tagliacozzo, and José I. Latorre. "Scaling of variational quantum circuit depth for condensed matter systems." Quantum 4 (May 28, 2020): 272. http://dx.doi.org/10.22331/q-2020-05-28-272.

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We benchmark the accuracy of a variational quantum eigensolver based on a finite-depth quantum circuit encoding ground state of local Hamiltonians. We show that in gapped phases, the accuracy improves exponentially with the depth of the circuit. When trying to encode the ground state of conformally invariant Hamiltonians, we observe two regimes. A finite-depth regime, where the accuracy improves slowly with the number of layers, and a finite-size regime where it improves again exponentially. The cross-over between the two regimes happens at a critical number of layers whose value increases linearly with the size of the system. We discuss the implication of these observations in the context of comparing different variational ansatz and their effectiveness in describing critical ground states.
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44

Spagnolo, B., D. Valenti, C. Guarcello, A. Carollo, D. Persano Adorno, S. Spezia, N. Pizzolato, and B. Di Paola. "Noise-induced effects in nonlinear relaxation of condensed matter systems." Chaos, Solitons & Fractals 81 (December 2015): 412–24. http://dx.doi.org/10.1016/j.chaos.2015.07.023.

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45

Marchetti, P. A. "Path-integral approach to bosonization of planar condensed matter systems." Nuclear Physics B - Proceedings Supplements 33, no. 3 (November 1993): 134–44. http://dx.doi.org/10.1016/0920-5632(93)90378-j.

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46

Fröhlich, Jürg. "Gauge invariance and anomalies in condensed matter physics." Journal of Mathematical Physics 64, no. 3 (March 1, 2023): 031903. http://dx.doi.org/10.1063/5.0135142.

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This paper begins with a summary of a powerful formalism for the study of electronic states in condensed matter physics called “gauge theory of states/phases of matter.” The chiral anomaly, which plays quite a prominent role in that formalism, is recalled. I then sketch an application of the chiral anomaly in 1 + 1 dimensions to quantum wires. Subsequently, some elements of the quantum Hall effect in two-dimensional (2D) gapped (“incompressible”) electron liquids are reviewed. In particular, I discuss the role of anomalous chiral edge currents and of the anomaly inflow in 2D gapped electron liquids with explicitly or spontaneously broken time reversal, i.e., in Hall and Chern insulators. The topological Chern–Simons action yielding transport equations valid in the bulk of such systems and the associated anomalous edge action are derived. The results of a general classification of “Abelian” Hall insulators are outlined. After some remarks on induced Chern–Simons actions, I sketch results on certain 2D chiral photonic wave guides. I then continue with an analysis of chiral edge spin-currents and bulk response equations in time-reversal invariant 2D topological insulators of electron gases with spin–orbit interactions. The “chiral magnetic effect” in 3D systems and axion-electrodynamics are reviewed next. This prepares the ground for an outline of a general theory of 3D topological insulators, including “axionic insulators.” Some remarks on Weyl semi-metals, which exhibit the chiral magnetic effect, and on Mott transitions in 3D systems with dynamical axion-like degrees of freedom conclude this review.
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47

Gadomski, Adam. "Dissipative, Entropy Production Systems across Condensed Matter and Interdisciplinary Classical vs. Quantum Physics." Entropy 24, no. 8 (August 9, 2022): 1094. http://dx.doi.org/10.3390/e24081094.

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48

Yoshii, Ryosuke, and Muneto Nitta. "Nambu-Jona Lasinio and Nonlinear Sigma Models in Condensed Matter Systems." Symmetry 11, no. 5 (May 6, 2019): 636. http://dx.doi.org/10.3390/sym11050636.

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We review various connections between condensed matter systems with the Nambu–Jona-Lasinio model and nonlinear sigma models. The field theoretical description of interacting systems offers a systematic framework to describe the dynamical generation of condensates. Recent findings of a duality between the Nambu–Jona-Lasinio model and nonlinear sigma models enables us to investigate various properties underlying both theories. In this review, we mainly focus on inhomogeneous condensations in static situations. The various methods developed in the Nambu–Jona-Lasinio model reveal the inhomogeneous phase structures and also yield new inhomogeneous solutions in nonlinear sigma models owing to the duality. The recent progress on interacting systems in finite systems is also reviewed.
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49

SUGAR, R. L. "NUMERICAL STUDIES OF MANY ELECTRON SYSTEMS." International Journal of Modern Physics C 01, no. 02n03 (September 1990): 215–32. http://dx.doi.org/10.1142/s0129183190000128.

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The numerical simulation of many electron systems in condensed matter physics is described. Numerical algorithms are discussed in detail, and results are presented from simulations of the Hubbard model in two and three dimensions.
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50

Scalapino, D. J. "Numerical Simulations of Quantum Condensed Matter Systems—What Can We Learn?" Physica Scripta T9 (January 1, 1985): 203–8. http://dx.doi.org/10.1088/0031-8949/1985/t9/034.

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