Doping-dependent bandwidth renormalization and spin-orbit coupling in (Sr1-xLax)2RhO4
Kyo-Hoon Ahn1, Kwan-Woo Lee, Jan Kuneš
1Department of Applied Physics, Graduate School, Korea University, Sejong 339-700, Korea.
Journal of Physics. Condensed Matter : an Institute of Physics Journal
|February 10, 2015
Summary
We studied the electronic structure of (Sr1-xLax)2RhO4. Electron doping weakens correlations, revealing it as a weakly correlated metal that becomes ferromagnetic due to Stoner instability.
Area of Science:
- Condensed matter physics
- Materials science
- Solid-state chemistry
Background:
- Investigating the electronic structure of correlated oxides is crucial for understanding their magnetic and conductive properties.
- Previous studies using LDA+U suggested significant correlation effects on spin-orbit splitting in (Sr1-xLax)2RhO4.
Purpose of the Study:
- To accurately determine the electronic structure of (Sr1-xLax)2RhO4.
- To clarify the role of electronic correlations and spin-orbit coupling in this material.
- To investigate the transition to ferromagnetic behavior with electron doping.
Main Methods:
- Combined density functional theory (DFT) and dynamical mean-field theory (DMFT).
- Accurate treatment of electronic correlations beyond static mean-field approximations.
Main Results:
- Electronic correlations do not significantly enhance spin-orbit splitting, contrary to LDA+U findings.
- The enhancement observed in LDA+U is an artifact of its static mean-field approximation.
- Electron doping (increasing x) reduces correlation effects, leading to increased quasi-particle bandwidth.
- (Sr1-xLax)2RhO4 is a weakly correlated metal.
- Stoner instability drives a transition to itinerant in-plane ferromagnetism around x=0.2.
Conclusions:
- DMFT provides a more accurate description of the electronic structure than LDA+U for this system.
- Electronic correlations play a less dominant role than previously thought.
- The material exhibits a doping-induced magnetic phase transition.
Related Concept Videos
¹H NMR: Interpreting Distorted and Overlapping Signals
1.8K
Spin systems where the difference in chemical shifts of the coupled nuclei is greater than ten times J are called first-order spin systems. These nuclei are weakly coupled, and their chemical shifts and coupling constant can generally be estimated from the well-separated signals in the spectrum.
As Δν decreases and the signals move closer, the doublets appear increasingly distorted. The intensities of the inner lines increase at the cost of those of the outer lines as the signals are...
As Δν decreases and the signals move closer, the doublets appear increasingly distorted. The intensities of the inner lines increase at the cost of those of the outer lines as the signals are...
1.8K
Spin–Spin Coupling Constant: Overview
1.7K
In bromoethane, the three methyl protons are coupled to the two methylene protons that are three bonds away. In accordance with the n+1 rule, the signal from the methyl protons is split into three peaks with 1:2:1 relative intensities. The methylene protons appear as a quartet, with the relative intensities of 1:3:3:1.
Qualitatively, any spin plus-half nucleus polarizes the spins of its electrons to the minus-half state. Consequently, the paired electron in the hydrogen–carbon bond must...
Qualitatively, any spin plus-half nucleus polarizes the spins of its electrons to the minus-half state. Consequently, the paired electron in the hydrogen–carbon bond must...
1.7K
NMR Spectroscopy: Spin–Spin Coupling
3.9K
The spin state of an NMR-active nucleus can have a slight effect on its immediate electronic environment. This effect propagates through the intervening bonds and affects the electronic environments of NMR-active nuclei up to three bonds away; occasionally, even farther. This phenomenon is called spin–spin coupling or J-coupling. Coupling interactions are mutual and result in small changes in the absorption frequencies of both nuclei involved. While nuclei of the same element are involved...
3.9K
¹³C NMR: ¹H–¹³C Decoupling
2.2K
The probability of having two carbon-13 atoms next to each other is negligible because of the low natural abundance of carbon-13. Consequently, peak splitting due to carbon-carbon spin-spin coupling is not observed in spectra. However, protons up to three sigma bonds away split the carbon signal according to the n+1 rule, resulting in complicated spectra.
A broadband decoupling technique is used to simplify these complex, sometimes overlapping, signals. Broadband decoupling relies on a...
A broadband decoupling technique is used to simplify these complex, sometimes overlapping, signals. Broadband decoupling relies on a...
2.2K
Double Resonance Techniques: Overview
872
Double resonance techniques in Nuclear Magnetic Resonance (NMR) spectroscopy involve the simultaneous application of two different frequencies or radiofrequency pulses to manipulate and observe two distinct nuclear spins. One important application of double resonance is spin decoupling, which selectively suppresses coupling with one type of nucleus while observing the NMR signal from another nucleus, simplifying the spectrum and enhancing resolution.
Spin decoupling is usually achieved by...
Spin decoupling is usually achieved by...
872
Colors and Magnetism
14.9K
Color in Coordination Complexes
When atoms or molecules absorb light at the proper frequency, their electrons are excited to higher-energy orbitals. For many main group atoms and molecules, the absorbed photons are in the ultraviolet range of the electromagnetic spectrum, which cannot be detected by the human eye. For coordination compounds, the energy difference between the d orbitals often allows photons in the visible range to be absorbed and emitted, which is seen as colors by the human...
When atoms or molecules absorb light at the proper frequency, their electrons are excited to higher-energy orbitals. For many main group atoms and molecules, the absorbed photons are in the ultraviolet range of the electromagnetic spectrum, which cannot be detected by the human eye. For coordination compounds, the energy difference between the d orbitals often allows photons in the visible range to be absorbed and emitted, which is seen as colors by the human...
14.9K


