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Camelback-shaped band reconciles heavy-electron behavior with weak electronic Coulomb correlations in superconducting TlNi2Se2

N. Xu, C. E. Matt, P. Richard, A. van Roekeghem, S. Biermann, X. Shi, S.-F. Wu, H. W. Liu, D. Chen, T. Qian, N. C. Plumb, M. Radović, Hangdong Wang, Qianhui Mao, Jianhua Du, Minghu Fang, J. Mesot, H. Ding, and M. Shi
Phys. Rev. B 92, 081116(R) – Published 24 August 2015

Abstract

Combining photoemission spectroscopy, Raman spectroscopy, and first-principles calculations, we characterize superconducting TlNi2Se2 as a material with weak electronic Coulomb correlations leading to a bandwidth renormalization of 1.4. We identify a camelback-shaped band, whose energetic position strongly depends on the selenium height. While this feature is universal in transition metal pnictides, in TlNi2Se2 it lies in the immediate vicinity of the Fermi level, giving rise to a pronounced van Hove singularity. The resulting heavy band mass resolves the apparent puzzle of a large normal-state Sommerfeld coefficient [H. Wang et al., Phys. Rev. Lett 111, 207001 (2013)] in this weakly correlated compound.

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  • Received 22 December 2014

DOI:https://doi.org/10.1103/PhysRevB.92.081116

©2015 American Physical Society

Authors & Affiliations

N. Xu1,2,*, C. E. Matt1,3, P. Richard4,5, A. van Roekeghem4,6, S. Biermann6,7,8, X. Shi1,4, S.-F. Wu4, H. W. Liu4, D. Chen4, T. Qian4, N. C. Plumb1, M. Radović1,9, Hangdong Wang10, Qianhui Mao10, Jianhua Du10, Minghu Fang10,11, J. Mesot1,2,3, H. Ding4,5, and M. Shi1,†

  • 1Swiss Light Source, Paul Scherrer Insitut, CH-5232 Villigen PSI, Switzerland
  • 2Institute of Condensed Matter Physics, École Polytechnique Fédérale de Lausanne, CH-1015 Lausanne, Switzerland
  • 3Laboratory for Solid State Physics, ETH Zürich, CH-8093 Zürich, Switzerland
  • 4Beijing National Laboratory for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China
  • 5Collaborative Innovation Center of Quantum Matter, Beijing, China
  • 6Centre de Physique Théorique, Ecole Polytechnique, CNRS-UMR7644, 91128 Palaiseau, France
  • 7Collège de France, 11 place Marcelin Berthelot, 75005 Paris, France
  • 8Kavli Institute for Theoretical Physics, University of California, Santa Barbara, California 93106, USA
  • 9SwissFEL, Paul Scherrer Institut, CH-5232 Villigen PSI, Switzerland
  • 10Department of Physics, Zhejiang University, Hangzhou 310027, China
  • 11Collaborative Innovation Center of Advanced Microstructures, Nanjing University, Nanjing 210093, China

  • *nan.xu@psi.ch
  • ming.shi@psi.ch

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Vol. 92, Iss. 8 — 15 August 2015

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