From a single-band metal to a high-temperature superconductor via two thermal phase transitions
Rui-Hua He, M. Hashimoto, H. Karapetyan, J. D. Koralek, J. P. Hinton,, J. P. Testaud, V. Nathan, Y. Yoshida, Hong Yao, K. Tanaka, W. Meevasana, R., G. Moore, D. H. Lu, S.-K. Mo, M. Ishikado, H. Eisaki, Z. Hussain, T. P., Devereaux, S. A. Kivelson, J. Orenstein, A. Kapitulnik

TL;DR
This study investigates the pseudogap phase in cuprate high-temperature superconductors, revealing a phase transition at T* and the coexistence of pseudogap and superconducting states through multiple experimental techniques.
Contribution
It provides a comprehensive multi-technique analysis of the pseudogap onset and its relation to superconductivity in cuprates, highlighting phase transition signatures.
Findings
Abrupt onset of a particle-hole asymmetric gap at T*
Detection of Kerr rotation indicating a phase transition
Superconducting features emerge near Tc, coexisting with pseudogap
Abstract
The nature of the pseudogap phase of cuprate high-temperature superconductors is a major unsolved problem in condensed matter physics. We studied the commencement of the pseudogap state at temperature T* using three different techniques (angle-resolved photoemission spectroscopy, polar Kerr effect, and time-resolved reflectivity) on the same optimally-doped Bi2201 crystals. We observed the coincident, abrupt onset at T* of a particle-hole asymmetric antinodal gap in the electronic spectrum, a Kerr rotation in the reflected light polarization, and a change in the ultrafast relaxational dynamics, consistent with a phase transition. Upon further cooling, spectroscopic signatures of superconductivity begin to grow close to the superconducting transition temperature (Tc), entangled in an energy-momentum-dependent fashion with the pre-existing pseudogap features, ushering in a ground state…
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