Stripe-Induced High-Temperature Superconductivity in Cuprates

The single-particle spectral function of the strongly correlated electron system is composed of a coherent peak and incoherent hills on both sides. The non-resonant electronic scattering of the incoherent spectral function becomes the same in the \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$B_{\rm 1g}$\end{document} and \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$B_{\rm 2g}$\end{document} channels and also correlates to the optical conductivity. The mid-infrared hill in the optical conductivity has the same origin as the electronic Raman susceptibility induced by the hole hopping perpendicular to the stripe. The wide-energy Raman spectra in the hole-doped and electron-doped cuprates are different, because the hole-doped cuprates are in the stripe phase while the electron-doped ones are not.