Two possible reasons for an instability with wave vector Q=(π, π) near the half-filling have been studied. The superexchange coupling of copper spins yields d-wave symmetry of the pseudogap. Nevertheless, the calculated critical temperature, T*, in this case is almost two times smaller than that observed experimentally in the bilayered cuprates. The phonon-mediated interaction (CDW scenario) provides the correct order of magnitude of T*. As the symmetries of the pseudogaps differ in both cases, T* does not increase when we switch them on simultaneously. © 1997 Plenum Publishing Corporation
The pseudogap phenomenon is most remarkable in the underdoped region of high-Tc cuprates. Since the ...
Self-consistent calculations of spin (charge) density wave order (SDW/CDW) parameters have been perf...
Self-consistent calculations of spin (charge) density wave order (SDW/CDW) parameters have been perf...
Two possible reasons for an instability with wave vector Q=(π, π) near the half-filling have been st...
Two possible reasons for an instability with wave vector Q=(π, π) near the half-filling have been st...
Two possible reasons for an instability with wave vector Q=(π, π) near the half-filling have been st...
Using the model of the singlet-correlated band the temperature dependence of d-wave superconducting ...
Using the model of the singlet-correlated band the temperature dependence of d-wave superconducting ...
Using the model of the singlet-correlated band the temperature dependence of d-wave superconducting ...
Using the model of the singlet-correlated band the temperature dependence of d-wave superconducting ...
Solutions of the integral equations for the pseudogap in the elementary excitation spectrum of curre...
Solutions of the integral equations for the pseudogap in the elementary excitation spectrum of curre...
Solutions of the integral equations for the pseudogap in the elementary excitation spectrum of curre...
Solutions of the integral equations for the pseudogap in the elementary excitation spectrum of curre...
The pseudogap phenomenon is most remarkable in the underdoped region of high-Tc cuprates. Since the ...
The pseudogap phenomenon is most remarkable in the underdoped region of high-Tc cuprates. Since the ...
Self-consistent calculations of spin (charge) density wave order (SDW/CDW) parameters have been perf...
Self-consistent calculations of spin (charge) density wave order (SDW/CDW) parameters have been perf...
Two possible reasons for an instability with wave vector Q=(π, π) near the half-filling have been st...
Two possible reasons for an instability with wave vector Q=(π, π) near the half-filling have been st...
Two possible reasons for an instability with wave vector Q=(π, π) near the half-filling have been st...
Using the model of the singlet-correlated band the temperature dependence of d-wave superconducting ...
Using the model of the singlet-correlated band the temperature dependence of d-wave superconducting ...
Using the model of the singlet-correlated band the temperature dependence of d-wave superconducting ...
Using the model of the singlet-correlated band the temperature dependence of d-wave superconducting ...
Solutions of the integral equations for the pseudogap in the elementary excitation spectrum of curre...
Solutions of the integral equations for the pseudogap in the elementary excitation spectrum of curre...
Solutions of the integral equations for the pseudogap in the elementary excitation spectrum of curre...
Solutions of the integral equations for the pseudogap in the elementary excitation spectrum of curre...
The pseudogap phenomenon is most remarkable in the underdoped region of high-Tc cuprates. Since the ...
The pseudogap phenomenon is most remarkable in the underdoped region of high-Tc cuprates. Since the ...
Self-consistent calculations of spin (charge) density wave order (SDW/CDW) parameters have been perf...
Self-consistent calculations of spin (charge) density wave order (SDW/CDW) parameters have been perf...