Abstract.
We present a model example of a quantum critical behavior of the renormalized single-particle Wannier function composed of Slater s-orbitals and represented in an adjustable Gaussian STO-7G basis, which is calculated for cubic lattices in the Gutzwiller correlated state near the metal-insulator transition (MIT). The discussion is carried out within the extended Hubbard model and using the method of approach proposed earlier [Eur. Phys. J. B 66, 385 (2008)]. The component atomic-wave-function size, the Wannier function maximum, as well as the system energy, all scale with the increasing lattice parameter R as [ (R-Rc)/Rc] s with s in the interval [0.9, 1.0]. Such scaling law is interpreted as the evidence of a dominant role of the interparticle Coulomb repulsion, which for R > Rc is of intersite character. Relation of the insulator-metal transition critical value of the lattice-parameter R = Rc to the original Mott criterion is also obtained. The method feasibility is tested by comparing our results with the exact approach for the Hubbard chain, for which the Mott-Hubbard transition is absent. In view of unique features of our results, an extensive discussion in qualitative terms is also provided.
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References
N.F. Mott, Metal-Insulator Transitions (Taylor & Francis, London, 1990)
M. Imada, A. Fujimori, Y. Tokura, Rev. Mod. Phys. 70, 1039 (1998)
F. Gebhardt, The Mott Metal-Insulator Transition (Springer Vg., Berlin, 1997)
For cold atomic gasses see: M. Greiner, O. Mandel, T. Esslinger, T.W. Häsch, I. Bloch, Nature 415, 39 (2002)
F. Gerbier, Phys. Rev. Lett. 99, 120405 (2007)
The situation in hadronic matter is recently reviewed in: P. Braun-Munzinger, J. Wambach, Rev. Mod. Phys. 81, 1031 (2009)
J. Hubbard, Proc. Roy. Soc. (London) A 281, 401 (1964)
W.F. Brinkman, T.M. Rice, Phys. Rev. B 2, 4302 (1970)
For recent review see e.g.: G. Kotliar, D. Vollhardt, Phys. Today 53 (2004)
J. Spałek, A. Datta, J.M. Honig, Phys. Rev. Lett. 49, 728 (1987)
A. Georges, G. Kotliar, W. Krauth, M.J. Rozenberg, Rev. Mod. Phys. 68, 13 (1996)
J. Spałek, in Encyclopedia of Condensed Matter Physics, edited by F. Bassani et al. (Elsevier, Amsterdam, 2005), Vol. 3, pp. 126–36
For a didactical review see: J. Spałek, Eur. J. Phys. 21, 511 (2000)
P. Limelette, A. Georges, D. Jérome, P. Wzietek, P. Metcalf, J.M. Honig, Science 302, 89 (2003)
In the case of quasi-two-dimensional system see: F. Kagawa, K. Miyagawa, K. Kanoda, Nature 436, 534 (2005)
E.g. the case of NiS2-xSex, for review see: J.M. Honig, J. Spałek, Chem. Mater. 10, 2910 (1998)
On theoretical side, see e.g. P. Korbel et al., Eur. Phys. J. B 32, 315 (2003). In these cases the antiferromagnetic itinerant state (of Slater type) transition into the same state of Mott type, which can be described by an effective Heisenberg model
See e.g. T. Misawa, M. Imada, Phys. Rev. B 75, 115121 (2007)
Experiment: I. Kézsmárki et al., Phys. Rev. Lett. 93, 266401 (2004)
J. Spałek, R. Podsiadły, W. Wójcik, A. Rycerz, Phys. Rev. B 61, 15676 (2000)
A. Rycerz, J. Spałek, Eur. Phys. J. B 40, 153 (2004)
For review see: J. Spałek, E.M. Görlich, A. Rycerz, R. Zahorbeński, J. Phys.: Condens. Matter 19, 255212 (2007), pp. 1–43
G. Kotliar et al., Rev. Mod. Phys. 78, 866 (2006), and references therein
V.I. Anisimov, J. Zaanen, O.K. Andersen, Phys. Rev. B 44, 993 (1991)
V.I. Anisimov, F. Aryasetiawa, A.I. Lichtenstein, J. Phys.: Condens. Matter 9, 767 (1997)
J. Kurzyk, W. Wójcik, J. Spałek, Eur. Phys. J. B 66, 385 (2008), this paper is regarded as Part I
J. Kurzyk, J. Spałek, W. Wójcik, Acta Phys. Polon. A 111, 603 (2007), cf. [arXiv:0706.1266] (2007)
E.H. Lieb, F.Y. Wu, Phys. Rev. Lett. 20, 1445 (1968)
E.H. Lieb, Physica A 321, 1 (2003)
For review see: M. Takahashi, Thermodynamics of onedimensional solvable models (Cambridge University Press, 1999), Chap. 6
W. Metzner, D. Vollhardt, Phys. Rev. B 37, 7382 (1988)
W. Metzner, D. Vollhardt, Phys. Rev. Lett. 62, 324 (1989)
M.C. Gutzwiller, Phys. Rev. 137, A1726 (2005)
A. Houghton, J.B. Marston, Phys. Rev. B 48, 7790 (1993)
A. Houghton, J.B. Marston, Phys. Rev. B 50, 1351 (1994)
A. Houghton, J.B. Marston, Phys. Rev. Lett. 72, 284 (1994)
K. Byczuk, J. Spałek, Phys. Rev. B 51, 7934 (1995)
Strictly speaking, the Gutzwiller-ansatz approach may be regarded as equivalent with the saddle-point approximation of the slave-boson approach when discussed in the nonmagnetic case; see e.g. J. Spałek, W. Wójcik, in Spectroscopy of Mott Insulator and Correlated Metals, edited by A. Fujimori, Y. Tokura (Springer Verlag, Berlin, 1995), pp. 41–65
For a simple treatment of orbitally degenerate system within GA approach see e.g.: A. Klejnberg, J. Spałek, Phys. Rev. B 57, 12041 (1998), particularly Section IV
The results of which can be related to LDA+U approach along the line discussed in: E.R. Ylvisaker, W.E. Picket, K. Koepernik, Phys. Rev. B 79, 035103 (2009)
For LDA+Gutzwiller see: J. Bünemann et al., Europhys. Lett. 61, 667 (2003)
G.-T. Wang, Z. Fang, Phys. Rev. Lett. 101, 066403 (2008)
R.P. Feynman, Statistical Physics; A Set of Lectures (W.A. Benjamin, Inc. Reading, MA, 1972), Chap. 6.6
V.A. Fock, Raboty po kvantovoi teorii pola (in Russian) (Izdatelstvo Leningradskogo Universiteta, 1957), Chap. 2
V.A. Fock, Z. Phys. 75, 622, (1932)
S.S. Schweber, An Introduction to Relativistic Quantum Field Theory (Peterson and Co., Evanston, IL, 1961)
Even the original Schrödinger single-particle wave equation can be determined variationally, from Hamiltonian variational principle encompassing the compromise between the kinetic and the potential energies; see: E. Schrödinger, Ann. Phys. (Leipzig) 79, 1 (1926), particularly the Appendix
H.A. Bethe, E.E. Salpeter, Quantum Mechanics of Oneand Two-Electron Atoms (Academic Press, New York, 1957), pp. 154–156
For overview of LDA approach see e.g. P.C. Hohenberg, W. Kohn, L.J. Sham, The Beginnings and Some Thoughts on the Future, in Advances in Quantum Chemistry, edited by S.B. Trickey (Academic Press Inc., San Diego, 1990), Vol. 21, pp. 7–20
W. Kohn, in Proc. 1966 Midwest Conf. Theoret. Phys. (Indiana University, Bloomington, IN, 1966), pp. 13–23
D. Vollhardt, P. Wölfle, in Electronic Phase Transitions, edited by W. Hanke, Yu.V. Kopaev (Elsevier, Amsterdam, 1992), cf. Chap. 1, particularly p. 41
F. Wegner, Z. Phys. B 32, 207 (1979)
For definition of Landau-Gutzwiller quasiparticles see e.g. J. Bünemann, F. Gebhard, R. Thul, Phys. Rev. B 67, 075103 (2003)
Those quasiparticles have been defined on a phenomenological basis in: J. Spałek, A. Datta, J.M. Honig, Phys. Rev. B 33, 4891 (1986)
The above papers follow the approach presented in: D. Vollhardt, Rev. Mod. Phys. 56, 99 (1984)
For DFT+Gutzwiller application to ferromagnetic Ni see: W. Weber, J. Bünemann, F. Gebhard, in Bandferromagnetism, edited by K. Baberschke, M. Donath, W. Nolting (Springer Verlag, 2001), p. 9. The present proposal extends their approach to the MIT regime, as well as avoids the double counting problem
For recent extension of statistical (Landau-Gutzwiller) quasiparticles concept going beyond the Landau- Gutzwiller concept (cf. Refs. [53–56]) see: J. Kaczmarczyk, J. Spałek, Phys. Rev. B 79, 214519 (2009)
J. Jȩdrak, J. Spałek, Phys. Rev. B 81 (2010), in press. Those extensions are relevant in e.g. spin-polarized (magnetic or in applied magnetic field) or superconducting states. In the present paper only the paramagnetic state is discussed
W.J. Hehre, R.F. Stewart, J.A. Pople, J. Chem. Phys. 51, 2657 (1969)
J. Fernández Rico, J.J. Fernández, R. López, G. Ramirez, Int. J. Quant. Chem. 78, 83 (2000)
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Spałek, J., Kurzyk, J., Podsiadły, R. et al. Extended Hubbard model with the renormalized Wannier wave functions in the correlated state II: quantum critical scaling of the wave function near the Mott-Hubbard transition. Eur. Phys. J. B 74, 63–74 (2010). https://doi.org/10.1140/epjb/e2010-00077-6
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DOI: https://doi.org/10.1140/epjb/e2010-00077-6