| People | Locations | Statistics |
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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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Grilli, Marco
in Cooperation with on an Cooperation-Score of 37%
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Publications (7/7 displayed)
- 2023Signature of quantum criticality in cuprates by charge density fluctuationscitations
- 2023Signature of quantum criticality in cuprates by charge density fluctuationscitations
- 2023Superfluid response of two-dimensional filamentary superconductors
- 2022Quantum zero point electromagnetic energy difference between the superconducting and the normal phase in a high- superconducting metal bulk samplecitations
- 2022Quantum zero point electromagnetic energy difference between the superconducting and the normal phase in a high- T c superconducting metal bulk samplecitations
- 2020Doping-dependent competition between superconductivity and polycrystalline charge density wavescitations
- 2020Doping-dependent competition between superconductivity and polycrystalline charge density wavescitations
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article
Doping-dependent competition between superconductivity and polycrystalline charge density waves
Abstract
From systematic analysis of the high pulsed magnetic field resistance data of La2−x Srx CuO4 thin films, we extract an experimental phase diagram for several doping values ranging from the very underdoped to the very overdoped regimes. Our analy- sis highlights a competition between charge density waves and superconductivity which is ubiquitous between x = 0.08 and x = 0.19 and produces the previously observed double step transition. When suppressed by a strong magnetic field, superconductivity is resilient for two specific doping ranges centered around respectively x ≈ 0.09 and x ≈ 0.19 and the characteristic temperature for the onset of the competing charge den- sity wave phase is found to vanish above x = 0.19. At x = 1/8 the two phases are found to coexist exactly at zero magnetic field.