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13–17 Sept 2015
Freising
Europe/Berlin timezone

Electronic Raman Scattering in Cuprate Superconductors: The Pseudogap Story

16 Sept 2015, 08:30
40m
Freising

Freising

Invited Talk DyProSo2015 Main track Excitations of strongly correlated electron systems

Speaker

Prof. Alain SACUTO (Université Paris Diderot Paris 7)

Description

The pseudogap phase in cuprates remains hitherto a mysterious state of matter out of which the high-temperature superconductivity emerges. Discovered more than twenty five years ago [1], its indentification is still challenging although extensively studies have been carried out to elucidate its true nature [2,3]. In addition recent investigations in the underdoped side of the cuprate phase diagram have shown inside the pseudogap phase the existence of charge density wave order [4-6] which could be at the origin of the Fermi surface reconstruction in electron and hole pockets detected at high magnetic field by quantum oscillations [7,8] and transport measurements [9]. Instead of clarifying our understanding of the cuprate phase diagram, these recent investigations have revealed its unexpected complexity. In this context our purpose is to reveal by electronic Raman scattering, the signature of the normal state pseudogap and track its doping evolution through the cuprate phase diagram. We will demonstrate there exists a direct connection between Raman and transport measurements on the pseudogap. Although intensively studied in the underdoped regime, relatively less is known about the normal state pseudogap on the overdoped side, where it weakens and eventually disappears at a critical doping pc. Here, combining Raman spectroscopy on Bi-2212 over a large range of finely tuned doping with theoretical calculations, we determine pc=0.22 and we show that it coincides with a Lifshitz transition where the underlying hole-like active Fermi surface becomes electron-like [10]. Interestingly, the superconducting critical temperature Tc is unaffected by this transition. This demonstrates that the microscopic origins of the normal state pseudogap and the superconductivity are distinct. Only the former is tied to the change in the Fermi surface topology. [1] H. Alloul et al., PRL 63 1700, (1989); W. W. Warren et al., Phys. Rev. Lett. 62, 1193 (1989) [2] T. Timusk, T. and B. Statt, Rep. Prog. Phys.62 122, (1999) [3] J. L. Tallon, and J.W. Loram, Physica C 349, 53 (2001). [4] G. Ghiringhelli et al., Science 337 821,2012; M. Le Tacon et al. Nature Physics, 7(9):725,(2014). [5] J. Chang , Nature Phys. 8, 872, (2012) [6] T. Wu et al. Nature 477, 191, (2011) [7] S. Sebastian, Prog. Phys. 75 102501 (2012) [8] F. Laliberte et al. Nature Comm. 2, 432 (2011) [9] L. Taillefer Annu. Rev. Condens. Matter Phys. 1 51, (2010) [10] S. Benhabib, A. Sacuto, M. Civelli, I. Paul et al., Phys. Rev. Lett.114, 147001 (2015)

Primary author

Prof. Alain SACUTO (Université Paris Diderot Paris 7)

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