Abstract
Charge order in the kagome superconductor CsV3Sb5 exhibits a complex three-dimensional organization and intermediate-temperature anomalies whose bulk character has remained unsettled.We use orientation-dependent 51V NMR as a site-selective probe to determine the stacking of the charge density wave (CDW) state and its thermal evolution. Below TCDW≈94 K, the field-linear splitting of the 51V central transition together with the anisotropy of the Knight shift tensor identify an interlayer-modulated 3q CDW whose local environments are consistent with a four-layer 2 × 2 × 4 stacking with mixed trihexagonal/Star-of-David distortions, in agreement with synchrotron x-ray determinations. For comparison, RbV3Sb5 serves as a reference exhibiting a uniform trihexagonal 2 × 2 × 2 stacking, allowing us to isolate features unique to the 2 × 2 × 4 state in CsV3Sb5. With H0 ‖ c, the 51V quadrupolar satellites through the intermediate temperature scale near TCO≈65 K reorganize into two well-resolved electric-field-gradient manifolds that coexist over a finite interval; their relative spectral weights interchange on cooling while the total integrated satellite intensity remains conserved and νQ within each manifold is nearly temperature independent. The coexistence without critical broadening, together with conserved intensity, provides bulk evidence consistent with a first-order charge-order transition near TCO. Our measurements do not resolve whether this lower-temperature transition corresponds to a distinct in-plane order or a reorganization of the 3q state; rather, they delimit this window and provide bulk, site-resolved constraints that connect prior reported anomalies to a thermodynamic first-order transition.
| Original language | English |
|---|---|
| Pages (from-to) | 2351231-2351237 |
| Number of pages | 7 |
| Journal | Physical Review B |
| Volume | 112 |
| Issue number | 23 |
| DOIs | |
| State | Published - Dec 8 2025 |
Funding
We thank Stuart Brown, Riku Yamamoto, Tri Thanh Chau (University of California, Los Angeles), and Rong Cong (National High Magnetic Field Laboratory) for insightful discussions. X.W. and B.R.O. were supported by the U.S. Department of Energy, Office of Science, Office of Basic Energy Sciences, under Award No. DE-SC0025712. NMR measurements were performed at the National High Magnetic Field Laboratory, which is supported by the National Science Foundation under Cooperative Agreement No. DMR-2128556 and the State of Florida. A.C.S., B.R.O., and S.D.W. gratefully acknowledge support via the UC Santa Barbara NSF Quantum Foundry funded via the Q-AMASE-i program under award DMR-1906325. H.B. acknowledges the generous computing resources provided by the Sulis HPC service (EP/T022108/1), ARCHER2 UK National Computing Service, which was granted via HPC-CONEXS, the UK High-End Computing Consortium (EPSRC Grant No. EP/X035514/1).