Physics – Condensed Matter – Superconductivity
Scientific paper
2002-09-12
Physics
Condensed Matter
Superconductivity
15 pages, 12 figures included, to appear in proceedings of SPIE Vol.#4811
Scientific paper
The lanthanide (Ln) copper oxides of the general chemical formula Ln2CuO4 take two different crystal structures: K2NiF4(T) and Nd2CuO4(T'). La2CuO4 takes the T structure by high-temperature bulk processes. The "thermal expansion mismatch" between the La-O and Cu-O bonds predicts that the T' phase of La2CuO4 can be stabilized at synthesis temperatures below 425 deg. Such low synthesis temperatures are difficult to access by bulk processes, but easy by thin-film processes. We have surveyed growth parameters in molecular beam epitaxy, and succeeded in the selective stabilization of T- and T'-La2CuO4. From our observations, it turns out that the growth temperature as well as the substrate play a crucial role in the selective stabilization: the T' structure is stabilized at low growth temperatures (< 600 deg.) and with substrates of a < 3.70 Ang or a > 3.90 Ang, while the T structure is stabilized at high growth temperatures (> 650 deg) or with substrates of a ~ 3.70 - 3.85 Ang. We have also been attempting hole (Ca, Sr, and Ba) and electron (Ce) doping into both of T- and T'-La2CuO4. In T-La2CuO4, hole doping produces the well-known LSCO and LBCO. Surprisingly, contrary to the empirical law, electron doping is also possible up to x ~ 0.06 - 0.08, although the films do not show superconductivity. In T'-La2CuO4, electron doping produces superconducting T'-(La,Ce)2CuO4 with Tc ~ 30 K, although hole doping has as yet been unsuccessful.
Greibe Tine
Naito Masashi
Sato Haruo
Tsukada Akio
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