Author
Listed:
- Sungyu Park
(Institute for Basic Science)
- So Young Kim
(Institute for Basic Science
Pohang University of Science and Technology)
- Hyoung Kug Kim
(Pohang University of Science and Technology)
- Min Jeong Kim
(Institute for Basic Science
Pohang University of Science and Technology)
- Taeho Kim
(Institute for Basic Science
Pohang University of Science and Technology)
- Hoon Kim
(Institute for Basic Science
Pohang University of Science and Technology)
- Gyu Seung Choi
(Institute for Basic Science
Pohang University of Science and Technology)
- C. J. Won
(Pohang Accelerator Laboratory
Max Planck POSTECH/Korea Research Initiative)
- Sooran Kim
(Kyungpook National University)
- Kyoo Kim
(Korea Atomic Energy Research Institute (KAERI))
- Evgeny F. Talantsev
(Russian Academy of Sciences
Ural Federal University)
- Kenji Watanabe
(National Institute for Materials Science)
- Takashi Taniguchi
(National Institute for Materials Science)
- Sang-Wook Cheong
(Pohang Accelerator Laboratory
Max Planck POSTECH/Korea Research Initiative
Rutgers University)
- B. J. Kim
(Institute for Basic Science
Pohang University of Science and Technology)
- H. W. Yeom
(Institute for Basic Science
Pohang University of Science and Technology)
- Jonghwan Kim
(Institute for Basic Science
Pohang University of Science and Technology
Pohang University of Science and Technology)
- Tae-Hwan Kim
(Pohang University of Science and Technology
Max Planck POSTECH/Korea Research Initiative
Asia Pacific Center for Theoretical Physics (APCTP))
- Jun Sung Kim
(Institute for Basic Science
Pohang University of Science and Technology)
Abstract
Superconductivity in the vicinity of a competing electronic order often manifests itself with a superconducting dome, centered at a presumed quantum critical point in the phase diagram. This common feature, found in many unconventional superconductors, has supported a prevalent scenario in which fluctuations or partial melting of a parent order are essential for inducing or enhancing superconductivity. Here we present a contrary example, found in IrTe2 nanoflakes of which the superconducting dome is identified well inside the parent stripe charge ordering phase in the thickness-dependent phase diagram. The coexisting stripe charge order in IrTe2 nanoflakes significantly increases the out-of-plane coherence length and the coupling strength of superconductivity, in contrast to the doped bulk IrTe2. These findings clarify that the inherent instabilities of the parent stripe phase are sufficient to induce superconductivity in IrTe2 without its complete or partial melting. Our study highlights the thickness control as an effective means to unveil intrinsic phase diagrams of correlated van der Waals materials.
Suggested Citation
Sungyu Park & So Young Kim & Hyoung Kug Kim & Min Jeong Kim & Taeho Kim & Hoon Kim & Gyu Seung Choi & C. J. Won & Sooran Kim & Kyoo Kim & Evgeny F. Talantsev & Kenji Watanabe & Takashi Taniguchi & San, 2021.
"Superconductivity emerging from a stripe charge order in IrTe2 nanoflakes,"
Nature Communications, Nature, vol. 12(1), pages 1-8, December.
Handle:
RePEc:nat:natcom:v:12:y:2021:i:1:d:10.1038_s41467-021-23310-w
DOI: 10.1038/s41467-021-23310-w
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