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Abstract
The electronic instabilities in CsV3Sb5 are believed to originate from the V 3d-electrons on the kagome plane, however the role of Sb 5p-electrons for 3-dimensional orders is largely unexplored. Here, using resonant tender X-ray scattering and high-pressure X-ray scattering, we report a rare realization of conjoined charge density waves (CDWs) in CsV3Sb5, where a 2 × 2 × 1 CDW in the kagome sublattice and a Sb 5p-electron assisted 2 × 2 × 2 CDW coexist. At ambient pressure, we discover a resonant enhancement on Sb L1-edge (2s→5p) at the 2 × 2 × 2 CDW wavevectors. The resonance, however, is absent at the 2 × 2 × 1 CDW wavevectors. Applying hydrostatic pressure, CDW transition temperatures are separated, where the 2 × 2 × 2 CDW emerges 4 K above the 2 × 2 × 1 CDW at 1 GPa. These observations demonstrate that symmetry-breaking phases in CsV3Sb5 go beyond the minimal framework of kagome electronic bands near van Hove filling.
The nature of unconventional charge density wave in kagome metals is currently under intense debate. Here the authors report the coexistence of the 2 × 2 × 1 charge density wave in the kagome sublattice and the Sb 5p-electron assisted 2 × 2 × 2 charge density waves in CsV3Sb5.
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Details
; Fabbris, G. 2
; Said, A. H. 2 ; Sun, J. P. 3
; Jiang, Yu-Xiao 4 ; Yin, J.-X. 5
; Pai, Yun-Yi 6
; Yoon, Sangmoon 7 ; Lupini, Andrew R. 8
; Nelson, C. S. 9
; Yin, Q. W. 10 ; Gong, C. S. 10 ; Tu, Z. J. 10 ; Lei, H. C. 10
; Cheng, J.-G. 3
; Hasan, M. Z. 4
; Wang, Ziqiang 11
; Yan, Binghai 12
; Thomale, R. 13
; Lee, H. N. 6
; Miao, H. 6
1 Oak Ridge National Laboratory, Materials Science and Technology Division, Oak Ridge, USA (GRID:grid.135519.a) (ISNI:0000 0004 0446 2659); The Hong Kong University of Science and Technology (Guangzhou), Advanced Materials Thrust, Guangzhou, China (GRID:grid.24515.37) (ISNI:0000 0004 1937 1450)
2 Argonne National Laboratory, Advanced Photon Source, Argonne, USA (GRID:grid.187073.a) (ISNI:0000 0001 1939 4845)
3 Chinese Academy of Sciences, Beijing National Laboratory for Condensed Matter Physics and Institute of Physics, Beijing, China (GRID:grid.9227.e) (ISNI:0000000119573309); University of Chinese Academy of Sciences, School of Physical Sciences, Beijing, China (GRID:grid.410726.6) (ISNI:0000 0004 1797 8419)
4 Princeton University, Laboratory for Topological Quantum Matter and Advanced Spectroscopy (B7), Department of Physics, Princeton, USA (GRID:grid.16750.35) (ISNI:0000 0001 2097 5006)
5 Southern University of Science and Technology, Laboratory for Quantum Emergence, Department of Physics, Shenzhen, China (GRID:grid.263817.9) (ISNI:0000 0004 1773 1790)
6 Oak Ridge National Laboratory, Materials Science and Technology Division, Oak Ridge, USA (GRID:grid.135519.a) (ISNI:0000 0004 0446 2659)
7 Oak Ridge National Laboratory, Materials Science and Technology Division, Oak Ridge, USA (GRID:grid.135519.a) (ISNI:0000 0004 0446 2659); Gachon University, Department of Physics, Seongnam, Republic of Korea (GRID:grid.256155.0) (ISNI:0000 0004 0647 2973)
8 Oak Ridge National Laboratory, Center for Nanophase Materials Sciences, Oak Ridge, USA (GRID:grid.135519.a) (ISNI:0000 0004 0446 2659)
9 Brookhaven National Laboratory, National Synchrotron Light Source II, Upton, USA (GRID:grid.202665.5) (ISNI:0000 0001 2188 4229)
10 Renmin University of China, Department of Physics and Beijing Key Laboratory of Opto-Electronic Functional Materials and Microdevices, Beijing, China (GRID:grid.24539.39) (ISNI:0000 0004 0368 8103)
11 Boston College, Department of Physics, Chestnut Hill, USA (GRID:grid.208226.c) (ISNI:0000 0004 0444 7053)
12 Weizmann Institute of Science, Department of Condensed Matter Physics, Rehovot, Israel (GRID:grid.13992.30) (ISNI:0000 0004 0604 7563)
13 University of Würzburg, Institute for Theoretical Physics, Würzburg, Germany (GRID:grid.8379.5) (ISNI:0000 0001 1958 8658)




