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Naji, M. |
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Motta, Antonella |
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Aletan, Dirar |
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Mohamed, Tarek |
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Ertürk, Emre |
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Taccardi, Nicola |
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Kononenko, Denys |
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Petrov, R. H. | Madrid |
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Alshaaer, Mazen | Brussels |
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Bih, L. |
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Casati, R. |
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Muller, Hermance |
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Kočí, Jan | Prague |
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Šuljagić, Marija |
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Kalteremidou, Kalliopi-Artemi | Brussels |
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Azam, Siraj |
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Ospanova, Alyiya |
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Blanpain, Bart |
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Ali, M. A. |
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Popa, V. |
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Rančić, M. |
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Ollier, Nadège |
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Azevedo, Nuno Monteiro |
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Landes, Michael |
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Rignanese, Gian-Marco |
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Yamada, K.
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- 2023Tribological properties of 100% cellulose nanofiber (CNF) molding under dry- and boundary lubrication-conditions at CNF/steel contactscitations
- 2022Effects of temperature on expansion of concrete due to the alkali-silica reaction: A simplified numerical approach ; Efectos de la temperatura en la expansión del hormigón por la reacción álcali-sílice: una aproximación numérica simplificadcitations
- 2019The effect of titanate nanotube/Y2W3O12 hybrid fillers on mechanical and thermal properties of HDPE-based compositescitations
- 2016Critical doping for the onset of fermi-surface reconstruction by charge-density-wave order in the cuprate superconductor La2-xSrxCuO4citations
- 2013TRIP steel microstructure visualized by slow and very slow electronscitations
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article
Critical doping for the onset of fermi-surface reconstruction by charge-density-wave order in the cuprate superconductor La2-xSrxCuO4
Abstract
The Seebeck coefficient S of the cuprate superconductor La<sub>2-x</sub>Sr<sub>x</sub>CuO<sub>4</sub> (LSCO) was measured in magnetic fields large enough to access the normal state at low temperatures, for a range of Sr concentrations from x = 0.07 to x = 0.15. For x = 0.11, 0.12, 0.125, and 0.13, S/T decreases upon cooling to become negative at low temperatures. The same behavior is observed in the Hall coefficient R<sub>H</sub>(T). In analogy with other hole-doped cuprates at similar hole concentrations p, the negative S and R<sub>H</sub> show that the Fermi surface of LSCO undergoes a reconstruction caused by the onset of charge-density-wave modulations. Such modulations have indeed been detected in LSCO by x-ray diffraction in precisely the same doping range. Our data show that in LSCO this Fermi-surface reconstruction is confined to 0.085 < p < 0.15. We argue that in the field-induced normal state of LSCO, charge-density-wave order ends at a critical doping p<sub>CDW</sub> = 0.15 ± 0.005, well below the pseudogap critical doping p* ≃ 0.19.