Details

Autor(en) / Beteiligte

• Kohsaka, Y.
• Hanaguri, T.
• Azuma, M.
• Takano, M.
• Davis, J. C.
• Takagi, H.

Titel

Visualization of the emergence of the pseudogap state and the evolution to superconductivity in a lightly hole-doped Mott insulator

Ist Teil von

• Nature physics, 2012-07, Vol.8 (7), p.534-538

Ort / Verlag

London: Nature Publishing Group UK

Erscheinungsjahr

2012

Quelle

Alma/SFX Local Collection

Beschreibungen/Notizen

• Scanning tunnelling microscopy images of the evolution of the pseudogap phase of a hole-doped cuprate superconductor suggest that it emerges in localized clusters that grow with increasing doping. Moreover, the eventual coalescence of these clusters coincides with the emergence of superconductivity. Superconductivity emerges from the cuprate antiferromagnetic Mott state with hole doping. The resulting electronic structure 1 is not understood, although changes in the state of oxygen atoms seem paramount 2 , 3 , 4 , 5 . Hole doping first destroys the Mott state, yielding a weak insulator 6 , 7 where electrons localize only at low temperatures without a full energy gap. At higher doping levels, the ‘pseudogap’, a weakly conducting state with an anisotropic energy gap and intra-unit-cell breaking of 90° rotational (C 4v ) symmetry, appears 3 , 4 , 8 , 9 , 10 . However, a direct visualization of the emergence of these phenomena with increasing hole density has never been achieved. Here we report atomic-scale imaging of electronic structure evolution from the weak insulator through the emergence of the pseudogap to the superconducting state in Ca 2− x Na x CuO 2 Cl 2 . The spectral signature of the pseudogap emerges at the lowest doping level from a weakly insulating but C 4v -symmetric matrix exhibiting a distinct spectral shape. At slightly higher hole density, nanoscale regions exhibiting pseudogap spectra and 180° rotational (C 2v ) symmetry form unidirectional clusters within the C 4v -symmetric matrix. Thus, hole doping proceeds by the appearance of nanoscale clusters of localized holes within which the broken-symmetry pseudogap state is stabilized. A fundamentally two-component electronic structure 11 then exists in Ca 2− x Na x CuO 2 Cl 2 until the C 2v -symmetric clusters touch at higher doping levels, and the long-range superconductivity appears.