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Hall Number of Strongly Correlated Metals
1Physics Department, Technion, 32000 Haifa, Israel.
Physical Review Letters
|August 25, 2018
Summary
Researchers derived an exact formula for the temperature-dependent Hall number in metals. This formula, applicable to fermions and bosons, surprisingly links this transport coefficient to equilibrium properties, simplifying calculations for complex materials.
Area of Science:
- Condensed matter physics
- Quantum mechanics
- Materials science
Background:
- The Hall number is a crucial transport coefficient in understanding electronic properties of materials.
- Calculating the Hall number, especially in strongly correlated systems, presents significant theoretical and computational challenges.
- Existing methods often struggle with arbitrary potentials and interactions, limiting applicability.
Purpose of the Study:
- To derive an exact formula for the temperature-dependent Hall number.
- To establish a connection between the Hall number and equilibrium susceptibilities.
- To demonstrate the formula's utility in complex systems like Mott phases.
Main Methods:
- Derivation of an exact analytical formula for the Hall number.
- Utilizing theoretical frameworks applicable to nonrelativistic fermions and bosons.
- Employing equilibrium susceptibilities as a key calculational component.
Main Results:
- An exact formula for the temperature-dependent Hall number is established.
- The formula demonstrates that the Hall number depends solely on equilibrium susceptibilities.
- The approach is shown to be more numerically tractable than direct conductivity calculations.
- The Hall sign near Mott phases of lattice bosons is successfully calculated.
Conclusions:
- The derived formula provides a powerful new tool for calculating the Hall number in diverse materials.
- Linking the Hall number to equilibrium susceptibilities simplifies theoretical investigations, particularly for strongly correlated systems.
- This work opens avenues for more efficient numerical studies of electronic transport phenomena.
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