Related Experiment Video
Updated: Aug 9, 2026

09:38
Fabrication Procedures and Birefringence Measurements for Designing Magnetically Responsive Lanthanide Ion Chelating Phospholipid Assemblies
Published on: January 3, 2018
Lightly doped La2-xSrxCuO4 as a Lifshitz helimagnet
V Juricic1, M B Silva Neto, C Morais Smith
1Institute for Theoretical Physics, University of Utrecht, Leuvenlaan 4, 3584 CE Utrecht, The Netherlands.
Physical Review Letters
|April 12, 2006
Summary
Static magnetic correlations in lightly doped La2-xSrxCuO4 are explained by a dipolar frustration model. This model accounts for magnetic phase transitions and reconciles experimental observations in this cuprate material.
Area of Science:
- Condensed matter physics
- Materials science
- Magnetism
Background:
- La2-xSrxCuO4 is a cuprate superconductor with complex magnetic properties.
- Understanding static magnetic correlations is crucial for explaining its electronic behavior.
Purpose of the Study:
- To investigate static magnetic correlations in lightly doped La2-xSrxCuO4.
- To explain the stability of magnetic phases and reconcile experimental data.
Main Methods:
- Utilizing a dipolar frustration model for a canted antiferromagnet.
- Analyzing Dzyaloshinskii-Moriya and XY anisotropies.
Main Results:
- The canted Néel state is stable for doping x < 2% due to specific anisotropies.
- Higher doping induces an unstable helicoidal magnetic phase.
- The model successfully reconciles elastic neutron scattering, Raman, and magnetic susceptibility data.
Conclusions:
- The dipolar frustration model provides a unified framework for understanding magnetic correlations in La2-xSrxCuO4.
- The study elucidates the transition from canted antiferromagnetism to a helicoidal magnetic phase with increasing doping.
Related Concept Videos
Colors and Magnetism
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 eye.
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 eye.
Paramagnetism
Paramagnets are materials with unpaired electrons that possess a finite magnetic moment. In the absence of a magnetic field, these moments are randomly oriented, and thus the net moment is zero. Under an external field, a torque acting on the moments tends to align them along the field's direction. However, the random thermal motion of electrons produces a torque opposite to the external field and tries to disorient the moments. These two competing effects align only a few moments along the...
Diamagnetism
Materials consisting of paired electrons have zero net magnetic moments. However, when these materials are placed under an external magnetic field, the moments opposite to the field are induced. Such materials are called diamagnets. Diamagnetism is the response of the diamagnets when placed in an external magnetic field.
Diamagnetism was discovered by Anton Brugmans in 1778 when he observed that bismuth gets repelled by magnetic fields, thus theorizing that diamagnets get repelled by magnets.
Diamagnetism was discovered by Anton Brugmans in 1778 when he observed that bismuth gets repelled by magnetic fields, thus theorizing that diamagnets get repelled by magnets.
Ferromagnetism
Materials like iron, nickel, and cobalt consist of magnetic domains, within which the magnetic dipoles are arranged parallel to each other. The magnetic dipoles are rigidly aligned in the same direction within a domain by quantum mechanical coupling among the atoms. This coupling is so strong that even thermal agitation at room temperature cannot break it. The result is that each domain has a net dipole moment. However, some materials have weaker coupling, and are ferromagnetic at lower...
