Published April 11, 2024 | Version v1
Journal article

Magnetic phase diagram of Eu1xCaxCo2P2 determined using muon spin rotation and relaxation

  • 1. Institute of Materials Structure Science, High Energy Accelerator Research Organization (KEK), Tokai, Ibaraki 319-1106, Japan
  • 2. Materials and Life Science Experimental Facility (MLF) Division, J-PARC Center, Tokai, Ibaraki 319-1195, Japan
  • 3. Department of Materials Structure Science, The Graduate University for Advanced Studies (SOKENDAI), Tsukuba, Ibaraki 305-0801, Japan
  • 4. Department of Chemistry, Graduate School of Science, Kyoto University, Kyoto 606-8502, Japan
  • 5. The Institute for Solid State Physics, The University of Tokyo, Kashiwa, Chiba 277-8581, Japan
  • 6. Neutron Science and Technology Center, Comprehensive Research Organization for Science and Society (CROSS), Tokai, Ibaraki 319-1106, Japan
  • 7. Department of Applied Physics, KTH Royal Institute of Technology, SE-106 91 Stockholm, Sweden
  • 8. Physik-Institut, Universität Zürich, Winterthurerstrasse 190, CH-8057 Zürich, Switzerland
  • 9. Department of Physics and Astronomy, Uppsala University, Box 516, SE-75120 Uppsala, Sweden

Description

The present study investigated the magnetic nature of a solid solution system consisting of EuCo2P2 and CaCo2P2 using a muon spin rotation and relaxation (μ+SR) technique, which is sensitive to local magnetic environments. The former compound EuCo2P2 is known to enter an incommensurate helical antiferromagnetic (AF) phase below 66 K with neutrons, which was confirmed by the present μ+SR. The magnitude of the ordered Eu moments proposed with neutrons was found to be consistent with that estimated by μ+SR. Furthermore, the latter lattice-collapsed tetragonal phase compound CaCo2P2 is known to enter an A-type AF phase below 90 K, and μ+SR measurements on single crystals revealed the presence of a spin reorientation transition at around 40 K, below which the A-type AF order is likely to be completed. Although all Eu1xCaxCo2P2 compounds were found to enter a magnetic phase at low temperatures regardless of x, a static ordered state was formed only at the vicinity of the two end compounds, i.e., 0x0.4 and 0.9x1. Instead, a disordered state, i.e., a random spin-glass state, short-range ordered state, or highly fluctuating state was found in the x range between 0.4 and 0.9, even at the lowest measured temperature (2 K). Together with the magnetization data, our findings clarified the magnetic phase diagram of Eu1xCaxCo2P2, where a ferromagnetic exchange interaction between Co ions through the Eu2+ ion competes with a direct AF interaction among the Co ions, particularly in the x range between 0.57 and 0.9. This competition yielded multiple phases in Eu1xCaxCo2P2.

Additional details

Identifiers

DOI
10.1103/PhysRevB.109.144408;
Crossref Funder ID
10.13039/100012419; 10.13039/501100004359; 10.13039/501100001691;

Publishing Information

Journal Title
Physical Review B
Journal Volume
109
Journal Issue
14
Journal Page Range
11 pgs.
ISSN
1550-235X

Optional Information

Copyright
©2024 American Physical Society
Contract/Grant/Project number
M2177; 2022-06217; JP18KK0150; JP22H01761; JP22H03875; JP18H01863; JP20K21149; JP23H01840
Notes
Contact Email: juns@triumf.ca or j_sugiyama@cross.or.jp; Record automatically processed
Funding organization
TRIUMF; Vetenskapsrådet; Japan Society for the Promotion of Science