1998
DOI: 10.1016/s0550-3213(98)00256-9
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The Hubbard chain at finite temperatures: ab initio calculations of Tomonaga-Luttinger liquid properties

Abstract: We present a novel treatment of finite temperature properties of the onedimensional Hubbard model. Our approach is based on a Trotter-Suzuki mapping utilizing Shastry's classical model and a subsequent investigation of the quantum transfer matrix. We derive non-linear integral equations for three auxiliary functions which have a clear physical interpretation of elementary excitations of spin type and charge excitations in lower and upper Hubbard bands. This allows for a transparent analytical study of certain … Show more

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Cited by 90 publications
(168 citation statements)
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“…Since g(TCNQ − ) ≈ 2.00236, the free-electron value, χ(x) is directly related to Avogadro's number N A and the Bohr magneton µ B . Jüttner et al [38] obtained quantitative χ(x) for the Hubbard We find similar χ(x) for the EHM with U = 5t, the EEHM with U = 8t, γ = 0.2 and the PCM with U = 8t. Small V is conveniently approximated as a Hubbard model with an effective U e = U − V .…”
Section: Bow/cdw Boundarysupporting
confidence: 65%
“…Since g(TCNQ − ) ≈ 2.00236, the free-electron value, χ(x) is directly related to Avogadro's number N A and the Bohr magneton µ B . Jüttner et al [38] obtained quantitative χ(x) for the Hubbard We find similar χ(x) for the EHM with U = 5t, the EEHM with U = 8t, γ = 0.2 and the PCM with U = 8t. Small V is conveniently approximated as a Hubbard model with an effective U e = U − V .…”
Section: Bow/cdw Boundarysupporting
confidence: 65%
“…They are generically called chain models, some which having the property of integrability and to which the Bethe ansatz has been applied to solve them exactly at T = 0 and at finite T . Their thermodynamical properties are obtained through coupled integral equations which demand numerical analysis to be solved (as examples see references [10,11,12,13,14]). …”
Section: Discussionmentioning
confidence: 99%
“…5. Как отмечается в работах [7], [8], для мо-дели Хаббарда с конечным значением энергии отталкивания U двух электронов на одном узле без магнитного поля зависимость теплоемкости от температуры также имеет две точки максимума. Низкотемпературный пик связан со спиновыми воз-буждениями и достигается при температуре T ≈ J/k B .…”
Section: точное решение при T =unclassified