Carrier-density-dependent momentum shift of the coherent peak and the LO phonon mode in p-type high-Tc superconductors
S. Sugai, H. Suzuki, Y. Takayanagi, T. Hosokawa, N. Hayamizu
DOI 10.1103/PhysRevB.68.184504 · Physical Review B
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Abstract
Systematic Raman scattering experiments were carried out in p-type superconductors YBCO, LSCO, Bi2212, and Bi2201. The superconducting coherent (pair-breaking) peak is anisotropic in k space not only in energy but also in existence itself. The position of the coherent peak in k space changes generally from (π/2,π/2) to (π,0), as carrier density increases, in correlation with the change of the low-energy electronic density of states. However, the change of the coherent peak in k space is more rapid than that of the electronic density of states, which suggests the existence of an additional pair-enhancing and pair-breaking mechanism. We found from two-phonon Raman scattering that the phonon mode with the strongest electron-phonon interactions changes from the breathing mode at (π,π) to the half-breathing mode at (π,0) in good correlation with the change of the coherent peak. It suggests that electron-phonon interactions play an important role to generate the superconductivity in the limited region of k space, even if magnetic interactions are the main origin of the superconductivity.
Source-reported materials — not catalogue approval
| Formula | Reported Tc (K) | Pressure (GPa) | Type |
|---|---|---|---|
| Bi2Sr2Ca0.8Y0.2Cu2O8 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 76 | Pressure not reported | unknown |
| Bi2Sr2Ca0.8Y0.2Cu2O8 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 86 | Pressure not reported | unknown |
| Bi2Sr2Ca0.9Y0.1Cu2O8 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 93 | Pressure not reported | unknown |
| Bi2Sr2CaCu2O8 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 82 | Pressure not reported | unknown |
| Bi2Sr1.2La0.8CuO6 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 9 | Pressure not reported | unknown |
| Bi2Sr1.3La0.7CuO6 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 23 | Pressure not reported | unknown |
| Bi2Sr1.5La0.5CuO6 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 32 | Pressure not reported | unknown |
| Bi1.74Pb0.38Sr1.88CuO6 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 21 | Pressure not reported | unknown |
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