2009
DOI: 10.1080/14786430902810498
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Correlation and confinement induced itinerant ferromagnetism in chain structures

Abstract: International audienceUsing a positive semidefinite operator technique one deduces exact ground states for a zig-zag hexagon chain described by a non-integrable Hubbard model with on-site repulsion. Flat bands are not present in the bare band structure, and the operators $\hat B^{\dagger}_{\mu,\sigma}$ introducing the electrons into the ground state, are all extended operators and confined in the quasi 1D chain structure of the system. Consequently, increasing the number of carriers, the $\hat B^{\dagger}_{\mu… Show more

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Cited by 13 publications
(12 citation statements)
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“…For this reason we use the method based on positive semidefinite operator properties whose applicability does not depend on dimensionality and integrability [13][14][15][16] . The method has been previously applied in conditions unimaginable before in the context of exact solutions in 1-3D, even in the presence of the disorder [17][18][19][20][21][22][23][24] .…”
Section: Introductionmentioning
confidence: 99%
“…For this reason we use the method based on positive semidefinite operator properties whose applicability does not depend on dimensionality and integrability [13][14][15][16] . The method has been previously applied in conditions unimaginable before in the context of exact solutions in 1-3D, even in the presence of the disorder [17][18][19][20][21][22][23][24] .…”
Section: Introductionmentioning
confidence: 99%
“…As Figs. (11,12) show, flat bands in the bare band structure are not present for non-zero values of allĤ 0 parameters. This fact can be directly and analytically verified in the following way.…”
Section: Discussionmentioning
confidence: 97%
“…To deduce exact ground states in such a case one uses a technique based on positive semidefinite operator properties whose applicability does not depend on dimensionality or integrability. The procedure itself has been described previously in details in several publications [16,17], provides results even in circumstances unexpected in the context of exact solutions as systems in two [18], or three [16] dimensions, disordered systems [19] or textures [20], being also intensively tested for chain structures [17,21,22] including hexagonal type of chains as well [23,24]. Using the method, one transforms the HamiltonianĤ in positive semidefinite form (i.e.Ĥ = nP n + E g , whereP n are positive semidefinite operators, while E g is a scalar) and looks for the most general wave vector |Ψ g with the property nP n |Ψ g = 0.…”
Section: Introductionmentioning
confidence: 98%