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Direct observation of competition between superconductivity and charge density wave order in YBa2Cu3O6.67
Direct observation of competition between superconductivity and charge density wave order in YBa2Cu3O6.67
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Direct observation of competition between superconductivity and charge density wave order in YBa2Cu3O6.67
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Direct observation of competition between superconductivity and charge density wave order in YBa2Cu3O6.67
Direct observation of competition between superconductivity and charge density wave order in YBa2Cu3O6.67
Journal Article

Direct observation of competition between superconductivity and charge density wave order in YBa2Cu3O6.67

2012
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Overview
X-ray diffraction experiments reveal that spatial charge ordering occurs in the pseudogap state of YBa 2 Cu 3 O 6.67 . Moreover, this charge ordered state competes with high-temperature superconductivity, and their relative strengths can be tuned using a magnetic field. Superconductivity often emerges in the proximity of, or in competition with, symmetry-breaking ground states such as antiferromagnetism or charge density waves 1 , 2 , 3 , 4 , 5 (CDW). A number of materials in the cuprate family, which includes the high transition-temperature (high- T c ) superconductors, show spin and charge density wave order 5 , 6 , 7 . Thus a fundamental question is to what extent do these ordered states exist for compositions close to optimal for superconductivity. Here we use high-energy X-ray diffraction to show that a CDW develops at zero field in the normal state of superconducting YBa 2 Cu 3 O 6.67 ( T c  = 67 K). This sample has a hole doping of 0.12 per copper and a well-ordered oxygen chain superstructure 8 . Below T c , the application of a magnetic field suppresses superconductivity and enhances the CDW. Hence, the CDW and superconductivity in this typical high- T c material are competing orders with similar energy scales, and the high- T c superconductivity forms from a pre-existing CDW environment. Our results provide a mechanism for the formation of small Fermi surface pockets 9 , which explain the negative Hall and Seebeck effects 10 , 11 and the ‘ T c plateau’ 12 in this material when underdoped.