Low Temperature Dynamic Polaron Liquid in a Manganite Exhibiting Colossal Magnetoresistance
1Stanford Institute for Materials and Energy Sciences (SIMES), 2575 Sand Hill Road, Menlo Park, California 94025, USA.
Physical Review Letters
|May 17, 2024
Summary
Polarons, charge carriers coupled to lattice distortions, transform from static to dynamic states in quantum materials. This study reveals a dynamic polaron liquid emerges in the metallic phase of La_{1.2}Sr_{1.8}Mn_{2}O_{7}.
Area of Science:
- Condensed Matter Physics
- Materials Science
- Quantum Materials
Background:
- Polarons, formed by electrons and lattice distortions, are common in insulators.
- The evolution of polarons during transitions to metallic and superconducting states is not well understood.
- Understanding these transitions is crucial for developing novel quantum materials.
Purpose of the Study:
- To investigate the behavior of polarons across the metal-to-insulator transition in La_{1.2}Sr_{1.8}Mn_{2}O_{7}.
- To elucidate the changes in electron-lattice coupling during this transition.
- To identify the polaronic state in the metallic phase of this quantum material.
Main Methods:
- Utilized resonant inelastic x-ray scattering (RIXS) to probe electron-lattice interactions.
- Studied the colossal magneto-resistive bi-layer manganite La_{1.2}Sr_{1.8}Mn_{2}O_{7}.
- Analyzed spectral weight redistribution across the metal-to-insulator transition.
Main Results:
- In the insulating state, observed harmonic emissions of a dispersionless oxygen phonon.
- In the metallic state, detected a shift of spectral weight to a high-energy continuum.
- Demonstrated a transition from static to dynamic lattice distortions, forming a dynamic polaron liquid.
Conclusions:
- The metal-to-insulator transition involves a significant change in electron-lattice coupling dynamics.
- A novel dynamic polaron liquid ground state exists in the metallic phase of La_{1.2}Sr_{1.8}Mn_{2}O_{7}.
- These findings offer new insights into polaron behavior in quantum materials.
Related Concept Videos
Ferromagnetism
2.4K
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...
2.4K
Paramagnetism
2.5K
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...
2.5K
Diamagnetism
2.4K
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....
2.4K
Magnetic Susceptibility and Permeability
1.1K
In linear magnetic materials, like paramagnets and diamagnets, magnetization is proportional to the magnetic field intensity. The constant of proportionality, a dimensionless number, is called magnetic susceptibility. The value of the susceptibility depends on the type of material.
When diamagnetic materials are placed under an external magnetic field, the moments opposite to the field are induced. Hence, the susceptibility for diamagnets has a minimal negative value of 10-5–10-6. Since...
When diamagnetic materials are placed under an external magnetic field, the moments opposite to the field are induced. Hence, the susceptibility for diamagnets has a minimal negative value of 10-5–10-6. Since...
1.1K
Types Of Superconductors
972
A superconductor is a substance that offers zero resistance to the electric current when it drops below a critical temperature. Zero resistance is not the only interesting phenomenon as materials reach their transition temperatures. A second effect is the exclusion of magnetic fields. This is known as the Meissner effect. A light, permanent magnet placed over a superconducting sample will levitate in a stable position above the superconductor. High-speed trains that levitate on strong...
972
Colors and Magnetism
11.6K
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...
11.6K


