2006
DOI: 10.1103/physrevlett.97.136401
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Breakup of the Fermi Surface Near the Mott Transition in Low-Dimensional Systems

Abstract: We investigate the Mott transition in weakly coupled one-dimensional (1D) fermionic chains. Using a generalization of dynamical mean field theory, we show that the Mott gap is suppressed at some critical hopping t c2 ? . The transition from the 1D insulator to a 2D metal proceeds through an intermediate phase where the Fermi surface is broken into electron and hole pockets. The quasiparticle spectral weight is strongly anisotropic along the Fermi surface, both in the intermediate and metallic phases. We argue … Show more

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Cited by 68 publications
(73 citation statements)
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“…This is related to the occurrence of Fermi arcs and lines of zeros of the Greens function 80 as noticed in Ref. 43,44,81. This phenomena was first noticed microscopic studies of coupled ladders 85,86 and related proposals also appeared in recent phenomenological models of high Tc's [82][83][84] .…”
Section: Cluster One Particle Greens Function Cluster Self Enermentioning
confidence: 71%
“…This is related to the occurrence of Fermi arcs and lines of zeros of the Greens function 80 as noticed in Ref. 43,44,81. This phenomena was first noticed microscopic studies of coupled ladders 85,86 and related proposals also appeared in recent phenomenological models of high Tc's [82][83][84] .…”
Section: Cluster One Particle Greens Function Cluster Self Enermentioning
confidence: 71%
“…Recently the question whether a Mott insulator and a band insulator are fundamentally different has been raised 1,2,3,4,5,6,7,8 . To study this question, we consider the simplest model which allows, by tuning one parameter, to obtain a Mott insulator as well as a band insulator phase.…”
Section: Introductionmentioning
confidence: 99%
“…On the theory side it has been established that the system can be considered as 1D two leg ladder [18][19][20] very close to the (quarter-filled) Mott transition [21,22]. Hence, from a very fundamental perspective, we face not only the problem of dimensional cross-over [23][24][25] but also a weakly doped (quarter-filled) Mott-insulator. This makes the problem even more challenging, but also much more exciting, since the many-body excitations (and spectral gaps) in the vicinity of the Mott state are currently hotly debated issues [26][27][28][29].…”
Section: Introductionmentioning
confidence: 99%