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Magnetic phase diagram of underdoped YBa2Cu3Oy inferred from torque magnetization and thermal conductivity

Author(s): Yu, Fan; Hirschberger, Max; Loew, Toshinao; Li, Gang; Lawson, Benjamin J; et al

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dc.contributor.authorYu, Fan-
dc.contributor.authorHirschberger, Max-
dc.contributor.authorLoew, Toshinao-
dc.contributor.authorLi, Gang-
dc.contributor.authorLawson, Benjamin J-
dc.contributor.authorAsaba, Tomoya-
dc.contributor.authorKemper, JB-
dc.contributor.authorLiang, Tian-
dc.contributor.authorPorras, Juan-
dc.contributor.authorBoebinger, Gregory S-
dc.contributor.authorSingleton, John-
dc.contributor.authorKeimer, Bernhard-
dc.contributor.authorLi, Lu-
dc.contributor.authorOng, Nai Phuan-
dc.date.accessioned2018-07-20T15:09:19Z-
dc.date.available2018-07-20T15:09:19Z-
dc.date.issued2016-11-08en_US
dc.identifier.citationYu, Fan, Hirschberger, Max, Loew, Toshinao, Li, Gang, Lawson, Benjamin J, Asaba, Tomoya, Kemper, JB, Liang, Tian, Porras, Juan, Boebinger, Gregory S, Singleton, John, Keimer, Bernhard, Li, Lu, Ong, N Phuan. (2016). Magnetic phase diagram of underdoped YBa2Cu3Oy inferred from torque magnetization and thermal conductivity. PROCEEDINGS OF THE NATIONAL ACADEMY OF SCIENCES OF THE UNITED STATES OF AMERICA, 113 (12667 - 12672. doi:10.1073/pnas.1612591113en_US
dc.identifier.issn0027-8424-
dc.identifier.urihttp://arks.princeton.edu/ark:/88435/pr1wx0x-
dc.description.abstractStrong evidence for charge-density correlation in the underdoped phase of the cuprate YBa2Cu3Oy was obtained by NMR and resonant X-ray scattering. The fluctuations were found to be enhanced in strong magnetic fields. Recently, 3D charge-density-wave (CDW) formation with long-range order (LRO) was observed by X-ray diffraction in H> 15 T. To elucidate how the CDW transition impacts the pair condensate, we have used torque magnetization to 45 T and thermal conductivity kappa(xx) to construct the magnetic phase diagram in untwinned crystals with hole density p = 0.11. We show that the 3D CDW transitions appear as sharp features in the susceptibility and kappa(xx) at the fields H-K and H-p, which define phase boundaries in agreement with spectroscopic techniques. From measurements of the melting field H-m(T) of the vortex solid, we obtain evidence for two vortex solid states below 8 K. At 0.5 K, the pair condensate appears to adjust to the 3D CDW by a sharp transition at 24 T between two vortex solids with very different shear moduli. At even higher H (41 T), the second vortex solid melts to a vortex liquid which survives to fields well above 41 T. de Haas-van Alphen oscillations appear at fields 24-28 T, below the lower bound for the upper critical field Hc(2).en_US
dc.format.extent12667 - 12672en_US
dc.language.isoenen_US
dc.relation.ispartofPROCEEDINGS OF THE NATIONAL ACADEMY OF SCIENCES OF THE UNITED STATES OF AMERICAen_US
dc.rightsFinal published version. This is an open access article.en_US
dc.titleMagnetic phase diagram of underdoped YBa2Cu3Oy inferred from torque magnetization and thermal conductivityen_US
dc.typeJournal Articleen_US
dc.identifier.doidoi:10.1073/pnas.1612591113-
dc.date.eissued2016-10-24en_US
pu.type.symplectichttp://www.symplectic.co.uk/publications/atom-terms/1.0/journal-articleen_US

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