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1

Ronning, Filip, and Cristian Batista. "Strongly correlated electron systems." Journal of Physics: Condensed Matter 23, no. 9 (February 16, 2011): 090201. http://dx.doi.org/10.1088/0953-8984/23/9/090201.

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2

Saxena, Siddharth S., and P. B. Littlewood. "Strongly correlated electron systems." Journal of Physics: Condensed Matter 24, no. 29 (July 6, 2012): 290301. http://dx.doi.org/10.1088/0953-8984/24/29/290301.

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3

Avella, Mancini, and Plekhanov. "Ergodicity in strongly correlated systems." Condensed Matter Physics 9, no. 3 (2006): 485. http://dx.doi.org/10.5488/cmp.9.3.485.

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4

Lebowitz, Joel L., and H. Saleur. "Percolation in strongly correlated systems." Physica A: Statistical Mechanics and its Applications 138, no. 1-2 (September 1986): 194–205. http://dx.doi.org/10.1016/0378-4371(86)90180-9.

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5

Yanagisawa, T., M. Miyazaki, and K. Yamaji. "Strongly correlated superconductivity." International Journal of Modern Physics B 32, no. 17 (July 9, 2018): 1840023. http://dx.doi.org/10.1142/s0217979218400234.

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We investigate the electronic properties of the ground state of strongly correlated electron systems. We use an optimization variational Monte Carlo method for the two-dimensional Hubbard model and the three-band d-p model. The many-body wavefunction is improved and optimized by introducing variational parameters that control the correlation between electrons. The on-site repulsive Coulomb interaction U induces strong antiferromagnetic (AF) correlation. There is a crossover from weakly to strongly correlated regions as U increases. We show an idea that high-temperature superconductivity occurs as a result of this crossover in the strongly correlated region where U is greater than the bandwidth.
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6

Fulde, P., and F. Pollmann. "Strings in strongly correlated electron systems." Annalen der Physik 520, no. 7 (June 13, 2008): 441–49. http://dx.doi.org/10.1002/andp.20085200703.

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7

Gunnarsson, O. "Resonance Photoemission in Strongly Correlated Systems." Physica Scripta T41 (January 1, 1992): 12–18. http://dx.doi.org/10.1088/0031-8949/1992/t41/002.

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8

Antonov, V. N., L. V. Bekenov, and A. N. Yaresko. "Electronic Structure of Strongly Correlated Systems." Advances in Condensed Matter Physics 2011 (2011): 1–107. http://dx.doi.org/10.1155/2011/298928.

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The article reviews the rich phenomena of metal-insulator transitions, anomalous metalicity, taking as examples iron and titanium oxides. The diverse phenomena include strong spin and orbital fluctuations, incoherence of charge dynamics, and phase transitions under control of key parameters such as band filling, bandwidth, and dimensionality. Another important phenomena presented in the article is a valence fluctuation which occur often in rare-earth compounds. We consider some Ce, Sm, Eu, Tm, and Yb compounds such as Ce, Sm and Tm monochalcogenides, Sm and Yb borides, mixed-valent and charge-ordered Sm, Eu and Yb pnictides and chalcogenides R4X3and R3X4(R = Sm, Eu, Yb; X = As, Sb, Bi), intermediate-valence YbInCu4and heavy-fermion compounds YbMCu4(M = Cu, Ag, Au, Pd). Issues addressed include the nature of the electronic ground states, the metal-insulator transition, the electronic and magnetic structures. The discussion includes key experiments, such as optical and magneto-optical spectroscopic measurements, x-ray photoemission and x-ray absorption, bremsstrahlung isochromat spectroscopy measurements as well as x-ray magnetic circular dichroism.
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9

Fukuyama, Hidetoshi. "Strongly Correlated Electrons in Molecular Systems." Progress of Theoretical Physics Supplement 176 (2008): 44–49. http://dx.doi.org/10.1143/ptps.176.44.

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10

Dagotto, E. "Complexity in Strongly Correlated Electronic Systems." Science 309, no. 5732 (July 8, 2005): 257–62. http://dx.doi.org/10.1126/science.1107559.

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11

Lee, Mu-Kun, Tsung-Sheng Huang, and Chyh-Hong Chern. "Fluctuations in strongly correlated electron systems." Results in Physics 10 (September 2018): 444–48. http://dx.doi.org/10.1016/j.rinp.2018.06.045.

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12

Monien, H. "Spectral properties of strongly correlated systems." Physica B: Condensed Matter 244 (January 1998): 81–85. http://dx.doi.org/10.1016/s0921-4526(97)00466-3.

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13

Couch, Vernon, and Alexei Stuchebrukhov. "Proteins as strongly correlated protonic systems." FEBS Letters 586, no. 5 (October 4, 2011): 519–25. http://dx.doi.org/10.1016/j.febslet.2011.09.036.

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14

Allen, J. W. "Electron spectroscopy of strongly correlated systems." Physica B: Condensed Matter 171, no. 1-4 (May 1991): 175–84. http://dx.doi.org/10.1016/0921-4526(91)90513-e.

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15

LIU, YU-LIANG. "UNIVERSAL DESCRIPTION OF STRONGLY CORRELATED SYSTEMS." International Journal of Modern Physics B 16, no. 05 (February 20, 2002): 773–802. http://dx.doi.org/10.1142/s0217979202009949.

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In the eigen-functional theoretical framework, exact/accurate treatment of high-dimensional strongly correlated electron systems may be realized. The two key steps of this method are that under the path integral formulation we first change a D-dimensional quantum many-particle system into an (D+1)-dimensional (time-dependent) effective "single-particle" problem, then by solving the eigen-equation of the propagator operator of the particles, we can obtain the ground state energy functional and action, respectively. Under the eigen-functional theory, the problems of quantum many-particle systems end in to solve the equation of phase fields that are completely determined by the electron interaction. In practice this equation of the phase fields can be numerically solved for large lattice sites. After replacing the real time by the imaginary time, this method can also be applied for finite temperature cases.
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16

RICE, T. M., and F. C. ZHANG. "ELECTRONIC PROPERTIES OF STRONGLY CORRELATED SYSTEMS." International Journal of Modern Physics B 02, no. 05 (October 1988): 627–29. http://dx.doi.org/10.1142/s0217979288000457.

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The observation that the energy scale of the magnetic excitations determined by the Heisenberg coupling constant ( J ≈ 0.1eV ) is much smaller than the charge excitation energies (≳ 2eV ) places the stoichiomatic Cu-oxides with formal valence Cu 2+ in the class of Mott insulators. Holes introduced into the CuO 2 layers can therefore be described by an effective Hamiltonian which contains a hopping term for holes between nearest neighbor CuO 4-squares (matrix element, t ) in addition to the Heisenberg term1). This effective Hamiltonian is restricted to the Hilbert subspace with one or less electrons in the Wannier orbital on each CuO 4 square. The Wannier orbital is made up from the [Formula: see text] Cu-orbital and a combination of the 2p O-orbitals with the same symmetry. The hybridization energy is maximized for a hole by forming a spin singlet combination of these orbitals so that the form of the effective Hamiltonian does not differ in form2) from that of a single band Hubbard model in the strongly correlated limit. The inclusion of O-O hopping does not change this conclusion3). Estimates of the parameter t , give a value t ≈ 0.5eV so that the ratio J/t ≪ l .
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17

Perakis, I. E. "Ultrafast dephasing in strongly correlated systems." physica status solidi (b) 238, no. 3 (August 2003): 502–8. http://dx.doi.org/10.1002/pssb.200303170.

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18

Fulde, P., and F. Pollmann. "Strings in strongly correlated electron systems." Annalen der Physik 17, no. 7 (July 1, 2008): 441–49. http://dx.doi.org/10.1002/andp.200810309.

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19

Izyumov, Yurii A. "Magnetism and superconductivity in strongly correlated systems." Uspekhi Fizicheskih Nauk 161, no. 11 (1991): 1. http://dx.doi.org/10.3367/ufnr.0161.199111a.0001.

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20

Protogenov, A. P. "Anyon superconductivity in strongly-correlated spin systems." Uspekhi Fizicheskih Nauk 162, no. 7 (1992): 1. http://dx.doi.org/10.3367/ufnr.0162.199207a.0001.

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21

Pagliuso, Pascoal J. G., Cris Adriano, and Eduardo Miranda. "The 2020 Strongly Correlated Electron Systems Conference." Journal of Physics: Conference Series 2164, no. 1 (March 1, 2022): 011001. http://dx.doi.org/10.1088/1742-6596/2164/1/011001.

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The International Conference on Strongly Correlated Electrons systems (SCES) is one of the most traditional conferences in Condensed Matter Physics worldwide. SCES continues to bring together, in every edition, outstanding scientists working in the frontiers of the complex and advanced phenomena of this area. The SCES 2020 Edition was planned to be an in-person event in Guaruja, SP, Brazil in September of 2020 as a continuation of the successful series of the SCES conferences: Sendai (’92), San Diego (’93), Amsterdam (’94), Goa (’95), Zurich (’96), Paris (’98), Nagano (’99), Ann Arbor (’01), Krakow (’02), Karlsruhe (’04), Vienna (’05), Houston (’07), Buzios (’08), Santa Fe (’10), Cambridge (’11), Tokyo (’13), Grenoble (’14), Hangzhou (’16), Prague (’17) and Okayama (’19). Additionally, every three years since 1997, SCES has been joining the International Conference on Magnetism (ICM) held in: Cairns (’97), Recife (’00), Rome (’03), Kyoto (’06), Karlsruhe (’09), Busan (’12), Barcelona (’15), and San Francisco (’18). List of The international advisory committee, The prize committee, The publication Committee, The organizing committee, The local committee are available in this pdf.
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22

Freericks and Strečka. "Strongly correlated electron systems and quantum magnetism." Condensed Matter Physics 23, no. 4 (December 2020): 40101. http://dx.doi.org/10.5488/cmp.23.40101.

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23

Domanski, Krawiec, Michalik, and Wysokinski. "TRANSPORT PROPERTIES OF THE STRONGLY CORRELATED SYSTEMS." Condensed Matter Physics 7, no. 2 (2004): 331. http://dx.doi.org/10.5488/cmp.7.2.331.

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24

Tung, Nguen Dan, and Nikolay Plakida. "Charge dynamics in strongly-correlated electronic systems." International Journal of Modern Physics B 32, no. 29 (November 20, 2018): 1850327. http://dx.doi.org/10.1142/s0217979218503277.

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We consider the dynamic charge susceptibility and the charge density waves in strongly-correlated electronic systems within the two-dimensional t-J-V model. Using the equation of motion method for the relaxation functions in terms of the Hubbard operators, we calculate the static susceptibility and the spectrum of charge fluctuations as functions of doped hole concentrations and temperature. Charge density waves emerge for a sufficiently strong intersite Coulomb interaction. Calculation of the dynamic charge susceptibility reveals a strong damping of charge density waves for a small hole doping and propagating high-energy charge excitations at large doping.
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25

Fazekas, P. "Variational Studies of Strongly Correlated Electron Systems." Physica Scripta T29 (January 1, 1989): 125–29. http://dx.doi.org/10.1088/0031-8949/1989/t29/023.

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26

Shaginyan, V. R., A. Z. Msezane, V. A. Stephanovich, G. S. Japaridze, and E. V. Kirichenko. "Flat bands and strongly correlated Fermi systems." Physica Scripta 94, no. 6 (April 2, 2019): 065801. http://dx.doi.org/10.1088/1402-4896/ab10b4.

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27

Seibold, G. "Charge instabilities in strongly correlated bilayer systems." European Physical Journal B - Condensed Matter 35, no. 2 (September 1, 2003): 177–89. http://dx.doi.org/10.1140/epjb/e2003-00267-3.

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28

Zverev, M. V., V. A. Khodel, and M. Baldo. "Phase diagram of strongly correlated Fermi systems." Journal of Experimental and Theoretical Physics Letters 72, no. 3 (August 2000): 126–30. http://dx.doi.org/10.1134/1.1316814.

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29

Izyumov, Yurii A. "Magnetism and superconductivity in strongly correlated systems." Soviet Physics Uspekhi 34, no. 11 (November 30, 1991): 935–57. http://dx.doi.org/10.1070/pu1991v034n11abeh002481.

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30

Protogenov, Aleksandr P. "Anyon superconductivity in strongly-correlated spin systems." Soviet Physics Uspekhi 35, no. 7 (July 31, 1992): 535–71. http://dx.doi.org/10.1070/pu1992v035n07abeh002247.

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31

Boyarsky, L. A. "Pseudogap effects in strongly correlated electron systems." Low Temperature Physics 32, no. 8 (August 2006): 819–23. http://dx.doi.org/10.1063/1.2219503.

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32

Dagotto, E., and J. R. Schrieffer. "Constructing quasiparticle operators in strongly correlated systems." Physical Review B 43, no. 10 (April 1, 1991): 8705–8. http://dx.doi.org/10.1103/physrevb.43.8705.

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33

Di Ciolo, Andrea, and Adolfo Avella. "Strongly Correlated Electron Systems: An Operatorial Perspective." Physica B: Condensed Matter 536 (May 2018): 359–63. http://dx.doi.org/10.1016/j.physb.2017.10.006.

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34

Tian, D. P., and H. Keiter. "Hall effect in strongly correlated Fermi systems." Physics Letters A 244, no. 1-3 (July 1998): 144–48. http://dx.doi.org/10.1016/s0375-9601(98)00226-6.

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35

Edelstein, Alan S. "An overview of strongly correlated electron systems." Journal of Magnetism and Magnetic Materials 256, no. 1-3 (January 2003): 430–48. http://dx.doi.org/10.1016/s0304-8853(02)00697-2.

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36

Ueda, Kazuo, and Yasufumi Yamashita. "Magnetism in strongly correlated and frustrated systems." Physica B: Condensed Matter 359-361 (April 2005): 626–32. http://dx.doi.org/10.1016/j.physb.2005.01.185.

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37

Capone, M., C. Castellani, and M. Grilli. "Electron-Phonon Interaction in Strongly Correlated Systems." Advances in Condensed Matter Physics 2010 (2010): 1–18. http://dx.doi.org/10.1155/2010/920860.

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The Hubbard-Holstein model is a simple model including both electron-phonon interaction and electron-electron correlations. We review a body of theoretical work investigating, the effects of strong correlations on the electron-phonon interaction. We focus on the regime, relevant to high-Tcsuperconductors, in which the electron correlations are dominant. We find that electron-phonon interaction can still have important signatures, even if many anomalies appear, and the overall effect is far from conventional. In particular in the paramagnetic phase the effects of phonons are much reduced in the low-energy properties, while the high-energy physics can still be affected by phonons. Moreover, the electron-phonon interaction can give rise to important effects, like phase separation and charge-ordering, and it assumes a predominance of forward scattering even if the bare interaction is assumed to be local (momentum independent). Antiferromagnetic correlations reduce the screening effects due to electron-electron interactions and revive the electron-phonon effects.
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38

Ferraz, A., and E. A. Kochetov. "Effective action for strongly correlated electron systems." Nuclear Physics B 853, no. 3 (December 2011): 710–38. http://dx.doi.org/10.1016/j.nuclphysb.2011.08.011.

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39

Kitaoka, Y., H. Tou, G. q. Zheng, K. Ishida, K. Asayama, T. C. Kobayashi, A. Kohda, et al. "NMR study of strongly correlated electron systems." Physica B: Condensed Matter 206-207 (February 1995): 55–61. http://dx.doi.org/10.1016/0921-4526(94)00365-3.

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40

Murthy, M. V. N., and R. Shankar. "Exclusion statistics and strongly correlated electron systems." Physica B: Condensed Matter 212, no. 3 (August 1995): 315–19. http://dx.doi.org/10.1016/0921-4526(95)00048-e.

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41

Capponi, Sylvain. "Effective Hamiltonian Approach for Strongly Correlated Systems." Theoretical Chemistry Accounts 116, no. 4-5 (February 14, 2006): 524–34. http://dx.doi.org/10.1007/s00214-006-0090-8.

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42

Gonçalves, L. L. "Spin systems in strongly correlated random fields." Journal of Magnetism and Magnetic Materials 140-144 (February 1995): 265–66. http://dx.doi.org/10.1016/0304-8853(94)01328-4.

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43

Moskalenko, V. A. "Electron-phonon interaction in strongly correlated systems." Theoretical and Mathematical Physics 111, no. 3 (June 1997): 744–53. http://dx.doi.org/10.1007/bf02634062.

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44

SHERMAN, A., and M. SCHREIBER. "SPIN DYNAMICS IN STRONGLY CORRELATED ELECTRON SYSTEMS." International Journal of Modern Physics B 21, no. 05 (February 20, 2007): 669–90. http://dx.doi.org/10.1142/s0217979207036692.

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Magnetic properties of the two-dimensional t-J model are reviewed. Some of these properties are close to those observed in cuprate perovskites. In particular, the magnetic response of the model is characterized by the intensive peak at the antiferromagnetic wave vector and at some transfer frequency. The peak splits into several incommensurate maxima for lower and higher frequencies. We discuss mechanisms which are responsible for these peculiarities in the model, which might also refer to cuprates.
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45

Asensio, M. "Angle-resolved photoemission from strongly correlated systems." Acta Crystallographica Section A Foundations of Crystallography 58, s1 (August 6, 2002): c222. http://dx.doi.org/10.1107/s0108767302093881.

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46

Huaiyu, Wang, Han Rushan, and Chen Nanxian. "Density-functional formula for strongly correlated systems*." Progress in Natural Science 15, no. 5 (May 1, 2005): 395–401. http://dx.doi.org/10.1080/10020070512331342290.

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47

Miura, Kazuo, Tamifusa Matsuura, and Yoshihiro Kuroda. "Quasi-particle interaction in strongly correlated systems." Physica C: Superconductivity 179, no. 4-6 (September 1991): 411–29. http://dx.doi.org/10.1016/0921-4534(91)92190-m.

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48

Steglich, Frank, Christoph Geibel, Robert Modler, Michael Lang, Peter Hellmann, and Philipp Gegenwart. "Classification of strongly correlated f-electron systems." Journal of Low Temperature Physics 99, no. 3-4 (May 1995): 267–81. http://dx.doi.org/10.1007/bf00752293.

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49

J. Ohkawa, Fusayoshi. "Auxiliary-Particle Theory of Strongly Correlated Systems." Journal of the Physical Society of Japan 58, no. 11 (November 15, 1989): 4156–67. http://dx.doi.org/10.1143/jpsj.58.4156.

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50

Citro, R., and M. Marinaro. "Charge susceptibility in strongly correlated electron systems." Journal of Physical Studies 2, no. 2 (1998): 236–40. http://dx.doi.org/10.30970/jps.02.236.

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