Abstract
The T c variation of HgBa 2CuO 4+ δ (Hg-1201) and HgBa 2CuO 4F δ can be achieved by a change in the carrier concentration and by a compression of the structure under high pressure. Oxygenated and fluorinated series exhibit a cupola-shaped behavior for the T c vs. δ dependence, but the curves are shifted away from each other along the δ axis. NPD showed double amount of extra fluorine in comparison with extra oxygen for the oxygenated Hg-1201 phases with close T c's. An exchange of the extra oxygen by a double amount of fluorine causes a significant compression of the apical CuO bond distances, while the in-plane ones, as well as T c, do not vary. Fluorination of Hg-1223 resulted in a slight increase in T c in comparison with oxygenated material. The influence of the external pressure on the structure and T c of Hg-1201 strongly depends on the doping level. An increase in the extra oxygen content from underdoped to overdoped state results in the larger compression of the apical CuO and BaO Hg distances while the HgO 2 dumbbell as well as a distance between Ba and O from the (CuO 2) layers become practically pressure independent.
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