Our system is currently under heavy load due to increased usage. We're actively working on upgrades to improve performance. Thank you for your patience.
2016
DOI: 10.1016/j.jmmm.2015.12.093
|View full text |Cite
|
Sign up to set email alerts
|

Dilution effects in spin 7/2 systems. The case of the antiferromagnet GdRhIn5

Abstract: We report the structural and magnetic characterization of La-substituted Gd 1−x La x RhIn 5 (x ≤ 0.50) antiferromagnetic (AFM) compounds. The magnetic responses of pure GdRhIn 5 are well described by a S = 7/2 Heisenberg model. When Gd 3+ ions are substituted by La 3+ , the maximum of the susceptibility and the inflection point of the magnetic specific heat are systematically shifted to lower temperatures accompanied by a broadening of the transition. The data is qualitatively explained by a phenomenological m… Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1
1

Citation Types

2
14
0

Year Published

2017
2017
2023
2023

Publication Types

Select...
7
1

Relationship

0
8

Authors

Journals

citations
Cited by 26 publications
(16 citation statements)
references
References 35 publications
2
14
0
Order By: Relevance
“…In the dilute regime, Gd 3+ ions do not behave as free paramagnetic impurities, and drastically reduce the magnetic anisotropy of Kondo CeRhIn 5 at high temperatures. Although x c is above the 2D percolation limit found previously in Ce 1−x La x RhIn 5 (x c ∼ 0.4) [13], it is surprisingly close to the 3D percolation limit found in Gd 1−x La x RhIn 5 and cubic Ce 1−x La x In 3 (x c ∼ 0.65) [18], in agreement with the more isotropic magnetic response.…”
Section: Introductionsupporting
confidence: 88%
“…In the dilute regime, Gd 3+ ions do not behave as free paramagnetic impurities, and drastically reduce the magnetic anisotropy of Kondo CeRhIn 5 at high temperatures. Although x c is above the 2D percolation limit found previously in Ce 1−x La x RhIn 5 (x c ∼ 0.4) [13], it is surprisingly close to the 3D percolation limit found in Gd 1−x La x RhIn 5 and cubic Ce 1−x La x In 3 (x c ∼ 0.65) [18], in agreement with the more isotropic magnetic response.…”
Section: Introductionsupporting
confidence: 88%
“…Equation (20) scales worse than the absolute upper bound for the compact case calculated in (15). This is partly because more qubits are present in the unary case, often leading to more distance that must be travelled.…”
Section: Comparisons Between Unary and Compactmentioning
confidence: 93%
“…Most work in this area has focused on fermionic and spin- 1 2 particles, although there is a large set of relevant problems of scientific interest involving ensembles of d-level systems (i.e. qudits), including photonic [5], [6], vibrational [7]- [13], and spin-s [14], [15] degrees of freedom.…”
Section: Introductionmentioning
confidence: 99%
“…In order to consider spin Hamiltonians such as Heisenberg models 11,40 , we encode spin-s operators of arbitrary s, where the number of levels is d = 2s + 1. Matrix elements for transitions l j i l 0 h j are defined as follows 41…”
Section: Local Operatorsmentioning
confidence: 99%
“…Here we consider resource counts for simulating five physically and chemically relevant Hamiltonian systems. The Hamiltonians correspond to the shifted one-dimensional QHO, the Bose-Hubbard model 9,45,46 , multidimensional molecular Franck-Condon factors 17,18,47 , a spin-s transverse-field Heisenberg model 11,40 , and simulating Boson sampling 48 on a digital quantum computer. The former four systems consist of an arbitrary number of d-level particles.…”
Section: Composite Systemsmentioning
confidence: 99%