Author
Listed:
- Su-Di Chen
(Stanford University
Stanford University
SLAC National Accelerator Laboratory and Stanford University
University of California, Berkeley)
- Makoto Hashimoto
(SLAC National Accelerator Laboratory)
- Yu He
(Stanford University
Stanford University
SLAC National Accelerator Laboratory and Stanford University
Yale University)
- Dongjoon Song
(National Institute of Advanced Industrial Science and Technology
Institute for Basic Science)
- Jun-Feng He
(Stanford University
Stanford University
SLAC National Accelerator Laboratory and Stanford University
University of Science and Technology of China)
- Ying-Fei Li
(Stanford University
Stanford University
SLAC National Accelerator Laboratory and Stanford University)
- Shigeyuki Ishida
(National Institute of Advanced Industrial Science and Technology)
- Hiroshi Eisaki
(National Institute of Advanced Industrial Science and Technology)
- Jan Zaanen
(Leiden University)
- Thomas P. Devereaux
(SLAC National Accelerator Laboratory and Stanford University
Stanford University)
- Dung-Hai Lee
(University of California, Berkeley
Lawrence Berkeley National Laboratory)
- Dong-Hui Lu
(SLAC National Accelerator Laboratory)
- Zhi-Xun Shen
(Stanford University
Stanford University
SLAC National Accelerator Laboratory and Stanford University)
Abstract
In conventional superconductors, the phase transition into a zero-resistance and perfectly diamagnetic state is accompanied by a jump in the specific heat and the opening of a spectral gap1. In the high-transition-temperature (high-Tc) cuprates, although the transport, magnetic and thermodynamic signatures of Tc have been known since the 1980s2, the spectroscopic singularity associated with the transition remains unknown. Here we resolve this long-standing puzzle with a high-precision angle-resolved photoemission spectroscopy (ARPES) study on overdoped (Bi,Pb)2Sr2CaCu2O8+δ (Bi2212). We first probe the momentum-resolved electronic specific heat via spectroscopy and reproduce the specific heat peak at Tc, completing the missing link for a holistic description of superconductivity. Then, by studying the full momentum, energy and temperature evolution of the spectra, we reveal that this thermodynamic anomaly arises from the singular growth of in-gap spectral intensity across Tc. Furthermore, we observe that the temperature evolution of in-gap intensity is highly anisotropic in the momentum space, and the gap itself obeys both the d-wave functional form and particle–hole symmetry. These findings support the scenario that the superconducting transition is driven by phase fluctuations. They also serve as an anchor point for understanding the Fermi arc and pseudogap phenomena in underdoped cuprates.
Suggested Citation
Su-Di Chen & Makoto Hashimoto & Yu He & Dongjoon Song & Jun-Feng He & Ying-Fei Li & Shigeyuki Ishida & Hiroshi Eisaki & Jan Zaanen & Thomas P. Devereaux & Dung-Hai Lee & Dong-Hui Lu & Zhi-Xun Shen, 2022.
"Unconventional spectral signature of Tc in a pure d-wave superconductor,"
Nature, Nature, vol. 601(7894), pages 562-567, January.
Handle:
RePEc:nat:nature:v:601:y:2022:i:7894:d:10.1038_s41586-021-04251-2
DOI: 10.1038/s41586-021-04251-2
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