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Uniaxial pressure dependence of<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant="italic">T</mml:mi></mml:mrow><mml:mrow><mml:mi mathvariant="italic">c</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math>from high-resolution dilatometry of untwinned<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant="normal">La</mml:mi></mml:mrow><mml:mrow><mml:mn>2</mml:mn><mml:mi mathvariant="normal">−</mml:mi><mml:mi mathvariant="italic">x</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant="normal">Sr</mml:mi></mml:mrow><mml:mrow><mml:mi mathvariant="italic">x</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant="normal">CuO</mml:mi></mml:mrow><mml:mrow><mml:mn>4</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math>single crystals

F. GugenbergerC. MeingastGeorg RothK. GrubeV. BreitThomas WeberH. WühlS. UchidaInstitut für Nukleare Festkörperphysik and Institut für Technische Physik, Kernforschungszentrum Karlsruhe, P.O. Box 3640, 76021 Karlsruhe, GermanyYoshinobu NakamuraInstitut für Nukleare Festkörperphysik and Institut für Technische Physik, Kernforschungszentrum Karlsruhe, P.O. Box 3640, 76021 Karlsruhe, Germany
1994lv
ABI

Аннотация

We have carried out high-resolution dilatometry experiments on a series of high-quality single crystals of ${\mathrm{La}}_{2\mathrm{\ensuremath{-}}\mathit{x}}$${\mathrm{Sr}}_{\mathit{x}}$${\mathrm{CuO}}_{4}$ with various Sr content on both the under- and overdoped side of the ${\mathit{T}}_{\mathit{c}}$(x) phase diagram. A simple in situ technique was applied to prevent the usual twinning of the samples in the low-temperature orthorhombic (LTO) phase, which allows us to study the full anisotropy of the thermal expansion of the LTO phase. From the anomalies in the linear expansivities \ensuremath{\Delta}${\mathrm{\ensuremath{\alpha}}}_{\mathit{i}}$ (i=a,b,c) at ${\mathit{T}}_{\mathit{c}}$ we deduce all three uniaxial stress (${\mathit{dT}}_{\mathit{c}}$/${\mathit{dp}}_{\mathit{i}}$) and strain (${\mathit{dT}}_{\mathit{c}}$/d${\mathrm{\ensuremath{\varepsilon}}}_{\mathit{i}}$) dependences, which turn out to be large and almost cancel for hydrostatic pressure.

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