The superconducting gap, the critical temperature and the isotope coefficient in a superlattice of metallic quantum stripes is calculated as a function of the electron number density. We show that it is possible to design a particular artificial superlattice of quantum stripes that exhibits the curves of T(c) and of the isotope coefficient as a function of the charge density as in cuprate superconductors. The shape of the superlattice is designed in order to tune the chemical potential near the bottom of the third subband for an electron number density of rho similar to 5.810(-2) Angstrom(-2). The superconducting critical temperature shows a resonant amplification as a function of electron number density rho with a maximum at a critical value rho(c). The isotope coefficient shows a sharp drop from a regime where alpha > 0.5 at rho < rho(c) to a regime where alpha < 0.2 at rho greater than or equal to rho(c). The underdoped and overdoped regime in cuprate superconductors is associated with a transition from a quasi 1D behavior for rho > rho(c) to quasi 2D behavior for rho < rho(c) with opening of a pseudogap at rho similar to rho(c).
Vengono studiate le proprietà elettroniche e superconduttive di un superreticolo di strisce quantiche al limite atomico
Electronic and superconducting properties of a superlattice of quantum stripes at the atomic limit
Valletta A;
1997
Abstract
The superconducting gap, the critical temperature and the isotope coefficient in a superlattice of metallic quantum stripes is calculated as a function of the electron number density. We show that it is possible to design a particular artificial superlattice of quantum stripes that exhibits the curves of T(c) and of the isotope coefficient as a function of the charge density as in cuprate superconductors. The shape of the superlattice is designed in order to tune the chemical potential near the bottom of the third subband for an electron number density of rho similar to 5.810(-2) Angstrom(-2). The superconducting critical temperature shows a resonant amplification as a function of electron number density rho with a maximum at a critical value rho(c). The isotope coefficient shows a sharp drop from a regime where alpha > 0.5 at rho < rho(c) to a regime where alpha < 0.2 at rho greater than or equal to rho(c). The underdoped and overdoped regime in cuprate superconductors is associated with a transition from a quasi 1D behavior for rho > rho(c) to quasi 2D behavior for rho < rho(c) with opening of a pseudogap at rho similar to rho(c).I documenti in IRIS sono protetti da copyright e tutti i diritti sono riservati, salvo diversa indicazione.