TY - JOUR
T1 - Mapping of the formation of the pairing gap in Bi2 Sr2 Ca2 CuO8 + δ
AU - Gomes, Kenjiro K.
AU - Pasupathy, Abhay N.
AU - Pushp, Aakash
AU - Parker, Colin
AU - Ono, Shimpei
AU - Ando, Yoichi
AU - Gu, Genda
AU - Yazdani, Ali
N1 - Funding Information:
We acknowledge the support through an NSF-DMR grant and NSF supported MRSEC program at Princeton Center for Complex Materials.
Copyright:
Copyright 2008 Elsevier B.V., All rights reserved.
PY - 2008/12
Y1 - 2008/12
N2 - High-resolution scanning tunneling microscopy has been used to study the formation of Cooper pairs in the cuprate superconductor Bi2 Sr2 CaCu2 O8 + δ. We measured the evolution of the tunneling gap as function of temperature (from 20 to 180 K) and doping (x = 0.12 - 0.22). Real space mapping of the density of states establish that the tunneling gap observed below the transition temperature (Tc) vanish inhomogenously in space, leading to the formation of a unique intermediate state, where nanoscale regions of pairing are present. Despite the inhomogeneity, we find that locally the gap spectrum evolves smoothly across Tc and, over a wide range of doping (x ≥ 0.16), the energy gap Δ vanishes at a temperature Tp, following a local criterion 2 Δ / kB Tp = 7.9 ± 0.5. Our observations suggest that at least in optimally doped and overdoped samples, all our measurements can be described with one single energy scale and that the gap measured above and below Tc must have the same origin. In the underdoped regime, this simple description fails to capture the temperature evolution of the local electronic states, indicating the presence of an additional phenomenon.
AB - High-resolution scanning tunneling microscopy has been used to study the formation of Cooper pairs in the cuprate superconductor Bi2 Sr2 CaCu2 O8 + δ. We measured the evolution of the tunneling gap as function of temperature (from 20 to 180 K) and doping (x = 0.12 - 0.22). Real space mapping of the density of states establish that the tunneling gap observed below the transition temperature (Tc) vanish inhomogenously in space, leading to the formation of a unique intermediate state, where nanoscale regions of pairing are present. Despite the inhomogeneity, we find that locally the gap spectrum evolves smoothly across Tc and, over a wide range of doping (x ≥ 0.16), the energy gap Δ vanishes at a temperature Tp, following a local criterion 2 Δ / kB Tp = 7.9 ± 0.5. Our observations suggest that at least in optimally doped and overdoped samples, all our measurements can be described with one single energy scale and that the gap measured above and below Tc must have the same origin. In the underdoped regime, this simple description fails to capture the temperature evolution of the local electronic states, indicating the presence of an additional phenomenon.
KW - C. Scanning tunneling microscopy
KW - D. Superconductivity
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U2 - 10.1016/j.jpcs.2008.06.136
DO - 10.1016/j.jpcs.2008.06.136
M3 - Article
AN - SCOPUS:57049178392
SN - 0022-3697
VL - 69
SP - 3034
EP - 3038
JO - Journal of Physics and Chemistry of Solids
JF - Journal of Physics and Chemistry of Solids
IS - 12
ER -