Change of carrier density at the pseudogap critical point of a cuprate superconductor

Abstract

The pseudogap is a central puzzle of cuprate superconductors. Its connection to the Mott insulator at low doping $p$ remains ambiguous and its relation to the charge order that reconstructs the Fermi surface at intermediate $p$ is still unclear. Here we use measurements of the Hall coefficient in magnetic fields up to 88 T to show that Fermi-surface reconstruction by charge order in YBa${}_2$Cu${}_3$O${}_y$ ends sharply at a critical doping $p=0.16$, distinctly lower than the pseudogap critical point at $p^{\ast }=0.19$. This shows that pseudogap and charge order are separate phenomena. We then find that the change of carrier density from $n=1+p$ in the conventional metal at high p to $n=p$ at low $p$ - a signature of the lightly doped cuprates - starts at $p^{\ast }$. This shows that pseudogap and antiferromagnetic Mott insulator are linked.

References in corpus (13)

• Direct observation of competition between superconductivity and charge density wave order in YBa2Cu3Oy
• Quantum oscillations and the Fermi surface in an underdoped high-Tc superconductor
• Resonant X-ray Scattering Study of Charge Density Wave Correlations in YBa${}_2$Cu${}_3$O${}_{6+x}$
• Lifshitz critical point in the cuprate superconductor YBa2Cu3Oy from high-field Hall effect measurements
• Charge density wave fluctuations in La2-xSrxCuO4 and their competition with superconductivity
• Competing charge, spin, and superconducting orders in underdoped YBa2Cu3Oy
• Quasiparticle mass enhancement approaching optimal doping in a high-Tc superconductor
• Phenomenology of the normal state in-plane transport properties of high-$T_c$ cuprates
• Pseudogap opening and formation of Fermi arcs as an orbital-selective Mott transition in momentum space
• Intrinsic Hall response of the CuO2 planes in a chain-plane-composite system of YBa2Cu3Oy
• Quantum Phase Transition in the Normal State of High-Tc Cuprates at Optimum Doping
• Density-wave instabilities of fractionalized Fermi liquids
• On the mass enhancement near optimal doping in high magnetic fields in the cuprates

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