News Release

Researchers create better algorithm for simulating particles in Fermi Sea

Peer-Reviewed Publication

North Carolina State University

A North Carolina State University physicist and his German colleagues have created a new, more precise algorithm for simulating particle interactions when a single impurity is introduced into a Fermi sea. The algorithm shows that when these particles interact, the transition from quasiparticle to bound molecule in a polarized two-dimensional system is smooth. The new method may have implications for understanding the behavior of impurities in a variety of systems.

The Fermi sea describes a collection of weakly interacting identical fermions such as electrons that have been cooled to a very low temperature. No two fermions within the sea have exactly the same quantum state. The ground state of the Fermi sea in this pure form is well understood. However, what happens when an impurity - such as a particle with a different spin - is introduced? How does that one particle affect the system as a whole?

"Let's say that all the particles in the sea are up-spin particles, and we introduce one down-spin particle," says NC State physicist Dean Lee, co-author on a paper describing the work. "Does this new particle form a molecular bond with one of the up-spin particles? How does the system react?"

Lee and his colleagues, lead author Shahin Bour and Ulf-G. Meissner from Bonn University and Hans-Werner Hammer from Darmstadt University, developed a lattice algorithm called impurity lattice Monte Carlo that samples the possible paths of the impurity in the Fermi sea. Monte Carlo methods are commonly used to simulate quantum mechanical systems. Impurity lattice Monte Carlo differs from other methods in that it treats the impurity particle explicitly, in a completely different manner from the other particles in the system.

According to the lattice results, the transition from single particle to bound molecule is smooth. "Physicists had theorized that there should be a clear critical value, or interaction strength, where the impurity would bond with another particle and become a molecule," Lee says, "but our simulations don't show that. Instead, we find that there's an interesting ambiguous state where the particles are interacting, but may or may not be a bound molecule. And when the transition does happen, it occurs smoothly as a function of interaction strength.

"What we're most excited about, though, are the future possibilities. We want to take the lattice into three-dimensional simulations, and introduce an impurity to a paired superfluid to see what effects that has on the system. We hope that our method can be used to address questions relevant to cold atoms, solid state systems and neutron stars."

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The research appears in Physical Review Letters. The research was supported by the U.S. Department of Energy (DE-FG02-03ER41260).

Note to editors: Abstract follows

"Ab initio lattice results for Fermi polarons in two dimensions"

Authors: Dean Lee, NC State University; Shahin Bour and Ulf-G. Meissner, Bonn University, Germany; H.-W. Hammer, Darmstadt Technical University, Darmstadt, Germany
Published: Online in Physical Review Letters

Abstract:

We investigate the attractive Fermi polaron problem in two dimensions using non-perturbative Monte Carlo simulations. We introduce a new Monte Carlo algorithm called the impurity lattice Monte Carlo method. This algorithm samples the path integral in a computationally efficient manner and has only small sign oscillations for systems with a single impurity. As a benchmark of the method, we calculate the universal polaron energy in three dimensions in the scale-invariant unitarity limit and find agreement with published results. We then present the first fully non-perturbative calculations of the polaron energy in two dimensions and density correlations between the impurity and majority particles in the limit of zero range interactions. We find evidence for a smooth crossover transition from fermionic quasiparticle to molecular state as a function of interaction strength.


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