Cold Atom Lab: Few-Body Physics

Background

NASA’s Cold Atom Laboratory (CAL) is the first ever of its kind. That is to say that this is the first atomic physics experiment ever to catch a ride on the International Space Station and live in a perpetual microgravity environment. Built by scientists and engineers at the Jet Propulsion Laboratory in Pasadena, CA, CAL is a user facility for five independent research teams. The Quantum Hydrodynamics Lab at USD is a member in one of these high profile research teams, the Ultracold Few-Body Physics Team, directing experiments on CAL in space (the flight team). Along with Nobel Laureate Prof. Eric Cornell at CU Boulder, Prof. Jose D’Incao at CU Boulder, and Prof. Peter Engels at Washington State University, Prof. Maren Mossman and company work to perform experiments that will help us to understand the physics of few-body systems. In particular, the Ultracold Few-Body Physics Team is interested in creating and investigating Efimov trimers, which are very fragile and weakly bound three-body systems that exists in regimes where two-body bound states are hard to find.

The most intriguing part of these Efimov bound states is that there is an infinite series of them at increasing interaction strength, aka as the interaction strength, or scattering length a, between the atoms is increased to a specific value, a_0, the ground Efimov state can be observed. Increasing the scattering length even more by a constant factor (for three identical bosons at zero temperature, this factor is universally calculated to be 22.7), another trimer is formed, called the first excited Efimov state! Going further, there is an infinite series of these trimer bound states formed at (22.7)^n times the position of the ground Efimov state, a_0. This behavior is called a universal geometric scaling law. What this means is that, no matter the isotope, if the ground Efimov state has atoms that are a_0 apart spatially, then the first excited state has atoms that are 22.7 times apart, and so on and so forth!

These delicate states have been observed in ground-based studies, but these types of studies also experience strong variations due to temperature and density effects! To observe the first excited Efimov state without runaway atom losses, one must create atoms that are at extremely low temperatures (< 1nK) and low densities (< 10^9 atoms/cm^3). This is where microgravity comes in! Not only does microgravity allow for extremely low densities by allowing atoms to expand freely without being lost to the bottom of the glass cell, microgravity allows us to perform a super awesome cooling technique, known as delta-kick cooling. In ground-based experiments, the center of mass of the atoms (once a trap is turned off) would be accelerating downward at a rate of 9.81 m/s^2 as the atoms expand. But in microgravity, the center of mass of the atoms stays in the same place relative to the apparatus. After a certain amount of time, the same spherical magnetic trap is applied to the atoms again, applying a force on the atoms that varies spatially: a strong force to the atoms far from the center of mass, moving out at higher speeds; and a weak force to the atoms near the center of the distribution, already at relatively low velocities. Pretty *cool*, huh?

For more information, check out JPL’s CAL website, or you can see this Nature News article from 2018, these intro videos (video 1) (video 2) from JPL, or this article from JPL about the recent update.