Related Experiment Video
Updated: Jan 24, 2026

10:26
Transport of Surface-modified Carbon Nanotubes through a Soil Column
Published on: April 2, 2015
9.9K
Bad Metallic Transport in a Modified Hubbard Model
Connie H Mousatov1, Ilya Esterlis1, Sean A Hartnoll1
1Department of Physics, Stanford University, Stanford, California 94305, USA.
Physical Review Letters
|May 31, 2019
Summary
We present a new model for bad metals, revealing T-linear resistivity and violations of the Wiedemann-Franz law in strongly correlated materials. This research offers insights into anomalous transport phenomena.
Area of Science:
- Condensed Matter Physics
- Materials Science
- Quantum Mechanics
Background:
- Strongly correlated metals exhibit anomalous transport properties.
- T-linear resistivity above the Mott-Ioffe-Regel limit is a key characteristic.
Purpose of the Study:
- Introduce a tractable microscopic model for bad metals.
- Characterize electric, thermal, and thermoelectric transport in strongly correlated systems.
Main Methods:
- Modified the Hubbard model by incorporating a screened Coulomb interaction.
- Analyzed the electric, thermal, and thermoelectric transport properties.
Main Results:
- Observed T-linear resistivity above the Mott-Ioffe-Regel limit across the phase diagram.
- Demonstrated strong violation of the Wiedemann-Franz law.
- Found a large thermopower with potential sign changes.
Conclusions:
- The new model successfully captures anomalous transport in bad metals.
- The screened Coulomb interaction is crucial for understanding these phenomena.
- The findings have implications for designing novel electronic and thermoelectric materials.
Related Concept Videos
Bonding in Metals
52.2K
Metallic bonds are formed between two metal atoms. A simplified model to describe metallic bonding has been developed by Paul Drüde called the “Electron Sea Model”.
52.2K
Metallic Solids
20.5K
Metallic solids such as crystals of copper, aluminum, and iron are formed by metal atoms. The structure of metallic crystals is often described as a uniform distribution of atomic nuclei within a “sea” of delocalized electrons. The atoms within such a metallic solid are held together by a unique force known as metallic bonding that gives rise to many useful and varied bulk properties.
All metallic solids exhibit high thermal and electrical conductivity, metallic luster, and malleability....
All metallic solids exhibit high thermal and electrical conductivity, metallic luster, and malleability....
20.5K
Alkali Metals
24.3K
Group 1 elements are soft and shiny metallic solids. They are malleable, ductile, and good conductors of heat and electricity. The melting points of the alkali metals are unusually low for metals and decrease going down the group, while the density increases going down the group with the exception of potassium (Table 1).
Table 1: Properties of the alkali metals
Table 1: Properties of the alkali metals
24.3K
Facilitated Transport
146.9K
The chemical and physical properties of plasma membranes cause them to be selectively permeable. Since plasma membranes have both hydrophobic and hydrophilic regions, substances need to be able to transverse both regions. The hydrophobic area of membranes repels substances such as charged ions. Therefore, such substances need special membrane proteins to cross a membrane successfully. In facilitated transport, also known as facilitated diffusion, molecules and ions travel across a...
146.9K
Primary Active Transport
197.3K
In contrast to passive transport, active transport involves a substance being moved through membranes in a direction against its concentration or electrochemical gradient. There are two types of active transport: primary active transport and secondary active transport. Primary active transport utilizes chemical energy from ATP to drive protein pumps that are embedded in the cell membrane. With energy from ATP, the pumps transport ions against their electrochemical gradients—a direction...
197.3K
Secondary Active Transport
137.4K
One example of how cells use the energy contained in electrochemical gradients is demonstrated by glucose transport into cells. The ion vital to this process is sodium (Na+), which is typically present in higher concentrations extracellularly than in the cytosol. Such a concentration difference is due, in part, to the action of an enzyme “pump” embedded in the cellular membrane that actively expels Na+ from a cell. Importantly, as this pump contributes to the high concentration of...
137.4K

