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arXiv:cond-mat/0303053 · Physical review. B, Condensed matter

Superconducting fluctuations in the Luther-Emery liquid

E. Orignac, Didier Poilblanc

Published Aug 14, 2003• 15 citations
arXivHTMLPDF

Abstract

The single-particle superconducting Green's functions of a Luther-Emery liquid is computed by bosonization techniques. Using a formulation introduced by Poilblanc and Scalapino [Phys. Rev. B 66, 052513 (2002)], an asymptotic expression of the superconducting gap is deduced in the long wavelength and small frequency limit. Due to superconducting phase fluctuations, the gap exhibits as a function of size L a ${(1/L)}^{{1/2K}_{\ensuremath{\rho}}}$ power-law decay as well as an interesting singularity at the spectral gap energy. Similarities and differences with the two-leg $t\ensuremath{-}J$ ladder are outlined.

DOI
10.1103/physrevb.68.052504

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The single-particle superconducting Green's functions of a Luther-Emery liquid is computed by bosonization techniques. Using a formulation introduced by Poilblanc and Scalapino [Phys. Rev. B 66, 052513 (2002)], an asymptotic expression of the superconducting gap is deduced in the long wavelength and small frequency limit. Due to superconducting phase fluctuations, the gap exhibits as a function of size L a (1/L)1/2K\ensuremathρ{(1/L)}^{{1/2K}_{\ensuremath{\rho}}}(1/L)1/2K\ensuremathρ​ power-law decay as well as an interesting singularity at the spectral gap energy. Similarities and differences with the two-leg t\ensuremath−Jt\ensuremath{-}Jt\ensuremath−J ladder are outlined.
Correlated-electron theories of superconductivity in layered cuprates often start from the premise of a gapped spin-liquid phase proximate to the superconducting state. This assumption is justified based on analytical and numerical demonstrations of a superconducting Luther-Emery phase in the doped 2-leg one-band Hubbard ladder, and the perceived analogy between coupled ladders and the two-dimensional CuO2{\mathrm{CuO}}_{2}CuO2​ layer. We demonstrate from accurate density matrix renormalization group studies the absence of the superconducting Luther-Emery phase in the doped 2-leg three-band ladder consisting of both copper and oxygen, even as the spin gap is large in the undoped three-band ladder. For realistic oxygen-oxygen hopping and Hubbard repulsion on the oxygen atoms, density-density rather than pairing correlations are dominant at long range. This result is equally valid whether or not the oxygens outside the ladder proper, over and above the rung and leg oxygens, are included in the computation. These results demonstrate the critical importance of oxygen orbitals, and raise disturbing questions about the applicability of many of the existing correlated-electron theories of superconductivity.
Correlated-electron theories of superconductivity in cuprates often start from the premise of a gapped spin-liquid phase proximate to the superconducting state. This assumption is based on, (i) demonstrations of a Luther-Emery phase with dominant superconducting correlations in the doped 2-leg one-band Hubbard ladder, and (ii) the perceived analogy between coupled ladders and the square lattice. We demonstrate from accurate density matrix renormalization group calculations the absence of the Luther-Emery phase in the doped 2-leg three-band ladder consisting of both copper and oxygen. For realistic oxygen-oxygen hopping and Hubbard repulsion on the oxygen atoms, the decay of the superconducting pair correlation with distance is almost indistinguishable from that of free fermions. Our results caste severe doubts on many of the existing correlated-electron theories of superconductivity.
A lightly doped single-band Hubbard model on a two-leg ladder exhibits a Luther-Emery phase, whereas the three-band Hubbard ladder behaves as a Luttinger liquid upon hole doping. To understand this discrepancy, we present a systematic density-matrix renormalization group study of the three-band Hubbard model on two-leg cylinders with further-neighbor particle hoppings. The inclusion of the longer-range hopping is motivated by the studies of the single-band Hubbard model in which the further-neighbor hopping terms are suggested to be crucial for the unconventional superconductivity. When the longer-range hopping parameters are small, the ground state is a Luttinger liquid having mutually commensurate superconducting, charge, and spin density wave correlations. Increasing the longer-range hopping drives a transition into a Luther-Emery phase with quasi-long-ranged superconducting and charge orders but short-ranged spin-spin correlations. By down-folding the three-band Hubbard model into an effective $t\text{\ensuremath{-}}{t}^{\ensuremath{'}}\text{\ensuremath{-}}J\text{\ensuremath{-}}{J}^{\ensuremath{'}}$ model, we find that in the Luther-Emery phase, both the nearest- and second-neighbor kinetic energies are enhanced due to an effective increase of copper-oxygen hybridization. Amplifying intercell oxygen orbital hopping mirrors the benefits of reducing the charge transfer energy, causing doped holes to favor oxygen orbitals and strengthening superconducting pairing.
We report a density-matrix renormalization group study of the lightly doped $t\text{\ensuremath{-}}J$ model on a four-leg cylinder with doped hole concentrations per site $\ensuremath{\delta}=5%\text{--}12.5%$. By keeping an unusually large number of states and long system sizes, we are able to accurately document the interplay between superconductivity, spin, and charge-density-wave orders. The long-distance behavior is consistent with that of a Luther-Emery liquid with a spin gap and power-law charge-density-wave and superconducting correlations. This is the widest $t\text{\ensuremath{-}}J$ or Hubbard system in which power-law superconducting correlations have been established.
Motivated by recent experiments on ultracold fermionic spin-1/2 6^66Li atoms in a Lieb lattice at various Hubbard repulsion UUU and filling fractions nnn (Lebrat et al., arXiv:2404.17555), we conduct a density matrix renormalization group (DMRG) analysis of the Hubbard model on a two-leg Lieb ladder. At half-filling, we find a ferrimagnetic Mott insulating ground state, consistent with Lieb's theorem. Away from half-filling, a state with finite total spin S⃗2≠0\vec{S}^2 \neq 0S2=0 and vanishing charge gap persists down to filling nc≈2/3n_c \approx 2/3nc​≈2/3. For lower, incommensurate fillings, the system is described by a Luttinger liquid with one charge and one spin mode. Intriguingly, in a narrow window near nc=2/3n_c = 2/3nc​=2/3, close to the onset of ferromagnetic order, we identify a superconducting Luther-Emery phase with dominant sxys_{xy}sxy​-wave pairing.