Doping and temperature dependence of the pseudogap and Fermi arcs in cuprates from dd-CDW short-range fluctuations in the context of the t-J model

At mean-field level the t-J model shows a phase diagram with close analogies to the phase diagram of hole doped cuprates. An order parameter associated with the flux or $d$ charge-density wave ($d$-CDW) phase competes and coexists with superconductivity at low doping showing characteristics identified with the observed pseudogap in underdoped cuprates. In addition, in the $d$-CDW state the Fermi surface is reconstructed toward pockets with low spectral weight in the outer part, resembling the arcs observed in angle-resolved photoemission spectroscopy experiments. However, the $d$-CDW requires broken translational symmetry, a fact that is not completely accepted. Including self-energy corrections beyond the mean, field we found that the self-energy can be written as two distinct contributions. One of these (called $\Sigma_{flux}$) dominates at low energy and originates from the scattering between carriers and $d$-CDW fluctuations in proximity to the $d$-CDW instability. The second contribution (called $\Sigma_{R\lambda}$) dominates at large energy and originates from the scattering between charge fluctuations under the constraint of non double occupancy. In this paper it is shown that $\Sigma_{flux}$ is responsible for the origin of low-energy features in the spectral function as a pseudogap and Fermi arcs. The obtained doping and temperature dependence of the pseudogap and Fermi arcs is similar to that observed in experiments. At low energy, $\Sigma_{R \lambda}$ gives an additional contribution to the closure of the pseudogap.Comment: 11 pages, 13 figure

Self-energy effects in cuprates and the dome-shaped behavior of the superconducting critical temperature

Hole doped cuprates show a superconducting critical temperature $T_c$ which follows an universal dome-shaped behavior as function of doping. It is believed that the origin of superconductivity in cuprates is entangled with the physics of the pseudogap phase. An open discussion is whether the source of superconductivity is the same that causes the pseudogap properties. The $t$-$J$ model treated in large-N expansion shows $d$-wave superconductivity triggered by non-retarded interactions, and an instability of the paramagnetic state to a flux phase or $d$-wave charge density wave ($d$-CDW) state. In this paper we show that self-energy effects near $d$-CDW instability may lead to a dome-shaped behavior of $T_c$. In addition, it is also shown that these self-energy contributions may describe several properties observed in the pseudogap phase. In this picture, although fluctuations responsible for the pseudogap properties leads to a dome-shaped behavior, they are not involved in pairing which is mainly non-retarded.Comment: 11 pages, 7 figures, accepted for publication in Phys. Rev.

Large-N expansion based on the Hubbard operator path integral representation and its application to the t-J model II. The case for finite JJ

We have introduced a new perturbative approach for $t-J-V$ model where Hubbard operators are treated as fundamental objects. Using our vertices and propagators we have developed a controllable large-N expansion to calculate different correlation functions. We have investigated charge density-density response and the phase diagram of the model. The charge correlations functions are not very sensitive to the value of $J$ and they show collective peaks (or zero sound) which are more pronounced when they are well separated (in energy) from the particle-hole continuum. For a given $J$ a Fermi liquid state is found to be stable for doping $\delta$ larger than a critical doping $\delta_c$. $\delta_c$ decreases with decreasing $J$. For the physical region of the parameters and, for $\delta< \delta_c$, the system enters in an incommensurate flux or DDW phase. The inclusion of the nearest-neighbors Coulomb repulsion $V$ leads to a CDW phase when $V$ is larger than a critical value $V_c$. The dependence of $V_c$ with $\delta$ and $J$ is shown. We have compared the results with other ones in the literature.Comment: 10 pages, 8 figures, to appear in Phys. Rev.

Spin exchange and superconductivity in a t−J′−Vt-J'-V model for two-dimensional quarter-filled systems

The effect of antiferromagnetic spin fluctuations on two-dimensional quarter-filled systems is studied theoretically. An effective $t-J'-V$ model on a square lattice which accounts for checkerboard charge fluctuations and next-nearest-neighbors antiferromagnetic spin fluctuations is considered. From calculations based on large-N theory on this model it is found that the exchange interaction, $J'$, increases the attraction between electrons in the d$_{xy}$ channel only, so that both charge and spin fluctuations work cooperatively to produce d$_{xy}$ pairing.Comment: 9 pages, 6 figure

Large-N expansion based on the Hubbard-operator path integral representation and its application to the t−Jt-J model

In the present work we have developed a large-N expansion for the $t-J$ model based on the path integral formulation for Hubbard-operators. Our large-N expansion formulation contains diagrammatic rules, in which the propagators and vertex are written in term of Hubbard operators. Using our large-N formulation we have calculated, for J=0, the renormalized $O(1/N)$ boson propagator. We also have calculated the spin-spin and charge-charge correlation functions to leading order 1/N. We have compared our diagram technique and results with the existing ones in the literature.Comment: 6 pages, 3 figures, Phys.Rev.B (in press

Path integrals for dimerized quantum spin systems

Dimerized quantum spin systems may appear under several circumstances, e.g\ by a modulation of the antiferromagnetic exchange coupling in space, or in frustrated quantum antiferromagnets. In general, such systems display a quantum phase transition to a N\'eel state as a function of a suitable coupling constant. We present here two path-integral formulations appropriate for spin $S=1/2$ dimerized systems. The first one deals with a description of the dimers degrees of freedom in an SO(4) manifold, while the second one provides a path-integral for the bond-operators introduced by Sachdev and Bhatt. The path-integral quantization is performed using the Faddeev-Jackiw symplectic formalism for constrained systems, such that the measures and constraints that result from the algebra of the operators is provided in both cases. As an example we consider a spin-Peierls chain, and show how to arrive at the corresponding field-theory, starting with both a SO(4) formulation and bond-operators.Comment: 20 pages, no figure

Formalismo cuántico en un modelo de interacción electromagnética de "anyons"

A partir del modelo de "gauge" clásico U(1) x U(1) para la interacción electromagnética de "anyons", se construye el formalismo cuántico. El modelo contiene dos campos de "gauge" U(1), el campo estadístico y el campo electromagnético, y puede ser acoplado tanto a un campo de materia bosónica como fermiónica. En el presente trabajo, se considera el segundo caso, es decir, un sistema de “anyons" fermiónicos en presencia de un campo electromagnético y se lleva a cabo la cuantificación canónica de acuerdo con el formalismo de Dirac. Se realiza también, la cuantificación del sistema a partir de la integral de camino y se obtiene la diagramática y las reglas de Feynman en el marco de la teoría perturbativaStarting from the U(1) x U(1) classical gauge model for the electromagnetic interaction of anyons, the quantum formalism is constructed. The model containing the statistical U(1) field and the electromagnetic field can be coupled to both, a commuting or an anticommuting matter field. We explicitly consider the second case, that is, a fermionic anyon system in the presence of an electromagnetic field and we carry out the canonical quantization by following the Dirac formalism. Later on, the path-integral approach is developed and the diagrammatic and Feynman rules, in the framework of the perturbation theory, are discussedFil: Foussats, Adriana Teresa. Universidad Nacional de Rosario - CONICET. Instituto de Física de Rosario (IFIR). Santa Fe. ArgentinaFil: Manavella, Edmundo Claudio. Universidad Nacional de Rosario - CONICET. Instituto de Física de Rosario (IFIR). Santa Fe. ArgentinaFil: Repetto, Carlos Enrique. Universidad Nacional de Rosario - CONICET. Instituto de Física de Rosario (IFIR). Santa Fe. ArgentinaFil: Zandrón, Oscar Pablo. Universidad Nacional de Rosario - CONICET. Instituto de Física de Rosario (IFIR). Santa Fe. ArgentinaFil: Zandrón, Oscar Sergio. Universidad Nacional de Rosario - CONICET. Instituto de Física de Rosario (IFIR). Santa Fe. Argentin