Evidence that all high-temperature superconductors are p-type
Howard A. Blackstead, John D. Dow
DOI 10.1103/PhysRevB.55.6605 · Physical Review B
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Abstract
The ground charge state of Ce substituting for Nd+3 in Nd2 CuO4 is usually assumed to be Ce+4 , indicating that Ce is a donor which causes Nd2−z Cez CuO4 to be an n-type superconductor. Using the self-consistent bond/charge method, we show that the Ce ground state is Ce+3 , not Ce+4 , in ideal Nd2 CuO4 , implying that monatomic Ce dopants are isoelectronic centers, not n-type donors. The observed Ce doping of Nd2−z Cez CuO4 can be understood if an interstitial oxygen binds to the Ce, elevating its charge state to Ce+4 . This is a paired defect of Ce and oxygen, which dopes the host p-type, not n-type, because of oxygen's 2p holes. The condition that the interstitial oxygen does dope the host p-type translates into an approximate steric constraint that the ionic radius of the rare-earth ion R+3 must exceed that of Tb+3 for R2−z Cez CuO4 to superconduct. A similar situation occurs for the infinite-layer material Sr1−v Ndv CuO2 , where the Nd dopant is isoelectronic Nd+2 , not donor Nd+3 as assumed, unless an extra oxygen is adjacent to the Nd. The data are reviewed in light of these results, and show no convincing evidence either of particle-hole symmetry in doping, or of n-type doping of any high-temperature superconductor. Instead they hint that the superconductivity is associated with oxygen, rather than with any particle-hole-symmetric cuprate-plane phenomenon.
Source-reported materials — not catalogue approval
| Formula | Reported Tc (K) | Pressure (GPa) | Type |
|---|---|---|---|
| Nd2-zCezCuO4 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
| Sr1-vNdvCuO2 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
| Pr2-zThzCuO4 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 2 | Pressure not reported | unknown |
| Nd2-zThzCuO4 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 2 | Pressure not reported | unknown |
| Sm2-zThzCuO4 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 2 | Pressure not reported | unknown |
| Tm2-zCazCuO4 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
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