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Letter

Nature 447, 569-572 (31 May 2007) | doi:10.1038/nature05881; Received 23 January 2007; Accepted 19 April 2007

Visualizing pair formation on the atomic scale in the high-Tc superconductor Bi2Sr2CaCu2O8+delta

Kenjiro K. Gomes1,3, Abhay N. Pasupathy1,3, Aakash Pushp1,3, Shimpei Ono2, Yoichi Ando2 & Ali Yazdani1

  1. Department of Physics, Joseph Henry Laboratories, Princeton University, Princeton, New Jersey 08544, USA
  2. Central Research Institute of Electric Power Industry, Komae, Tokyo 201-8511, Japan
  3. These authors contributed equally to this work.

Correspondence to: Ali Yazdani1 Correspondence and requests for materials should be addressed to A.Y. (Email: yazdani@princeton.edu).

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Pairing of electrons in conventional superconductors occurs at the superconducting transition temperature Tc, creating an energy gap Delta in the electronic density of states (DOS)1. In the high-Tc superconductors, a partial gap in the DOS exists for a range of temperatures above Tc (ref. 2). A key question is whether the gap in the DOS above Tc is associated with pairing, and what determines the temperature at which incoherent pairs form. Here we report the first spatially resolved measurements of gap formation in a high-Tc superconductor, measured on Bi2Sr2CaCu2O8+delta samples with different Tc values (hole concentration of 0.12 to 0.22) using scanning tunnelling microscopy. Over a wide range of doping from 0.16 to 0.22 we find that pairing gaps nucleate in nanoscale regions above Tc. These regions proliferate as the temperature is lowered, resulting in a spatial distribution of gap sizes in the superconducting state3, 4, 5. Despite the inhomogeneity, we find that every pairing gap develops locally at a temperature Tp, following the relation 2Delta/kBTp = 7.9 plusminus 0.5. At very low doping (less than or equal to0.14), systematic changes in the DOS indicate the presence of another phenomenon6, 7, 8, 9, which is unrelated and perhaps competes with electron pairing. Our observation of nanometre-sized pairing regions provides the missing microscopic basis for understanding recent reports10, 11, 12, 13 of fluctuating superconducting response above Tc in hole-doped high-Tc copper oxide superconductors.

  1. Department of Physics, Joseph Henry Laboratories, Princeton University, Princeton, New Jersey 08544, USA
  2. Central Research Institute of Electric Power Industry, Komae, Tokyo 201-8511, Japan
  3. These authors contributed equally to this work.

Correspondence to: Ali Yazdani1 Correspondence and requests for materials should be addressed to A.Y. (Email: yazdani@princeton.edu).

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