
NSF Org: |
PHY Division Of Physics |
Recipient: |
|
Initial Amendment Date: | September 2, 2016 |
Latest Amendment Date: | May 20, 2020 |
Award Number: | 1607335 |
Award Instrument: | Continuing Grant |
Program Manager: |
John D. Gillaspy
PHY Division Of Physics MPS Directorate for Mathematical and Physical Sciences |
Start Date: | September 1, 2016 |
End Date: | August 31, 2020 (Estimated) |
Total Intended Award Amount: | $174,797.00 |
Total Awarded Amount to Date: | $179,797.00 |
Funds Obligated to Date: |
FY 2017 = $44,266.00 FY 2018 = $45,327.00 FY 2020 = $5,000.00 |
History of Investigator: |
|
Recipient Sponsored Research Office: |
601 E MAIN ST COLLEGEVILLE PA US 19426-2513 (610)409-3005 |
Sponsor Congressional District: |
|
Primary Place of Performance: |
PO Box 1000 Collegeville PA US 19426-1000 |
Primary Place of
Performance Congressional District: |
|
Unique Entity Identifier (UEI): |
|
Parent UEI: |
|
NSF Program(s): | AMO Experiment/Atomic, Molecul |
Primary Program Source: |
01001718DB NSF RESEARCH & RELATED ACTIVIT 01001819DB NSF RESEARCH & RELATED ACTIVIT 01002021DB NSF RESEARCH & RELATED ACTIVIT |
Program Reference Code(s): |
|
Program Element Code(s): |
|
Award Agency Code: | 4900 |
Fund Agency Code: | 4900 |
Assistance Listing Number(s): | 47.049 |
ABSTRACT
The goals of this collaborative project are twofold: first, to understand and control the movement of energy among strongly connected groups of atoms, and second, to improve an experimental technique for measuring the energy distribution among these atoms. These general goals are present in many areas of science (for example, in the study of the transport of energy in metals) but they are often difficult to realize for the simple reason that solids are densely packed with atoms and typically opaque. This work will be done in an "ultracold gas" of atoms that are cooled so that they move slowly like the atoms in a solid, but are at low density. Collections of these atoms are transparent and can be probed and controlled with lasers. If the outer electrons in these atoms are excited to high energy levels, then the atoms can exchange energy in ways that are similar to other quantum systems. Using a combination of simulation and experimental imaging techniques, the transport of energy will be measured. In this way, the project aims to create and study atomic systems that will yield insight into both fundamental quantum mechanics and the behavior of materials. The second goal of this project concerns a widely used experimental technique in which the energy level of an electron is measured by using a rapidly increasing electric field to rip off, or ionize, the outermost electron from the atom. The stripped electron is accelerated to a detector and the resulting signal is characteristic of the electron's original energy level. However, the ionization process is complex and nearby energy levels produce signals which are indistinguishable. This project will precisely shape the electric field pulse so that the signals from closely spaced energy levels can be distinguished, making new experiments possible in many areas of atomic physics.
In this project, the valence electron of ultracold rubidium atoms in a magneto-optical trap is excited to a weakly bound state of high principle quantum number, or Rydberg state. Both the spatial distribution of the atoms and the internal states to which they are excited are precisely controlled. The atoms in such a sample exchange energy through a dipole-dipole interaction. Building upon earlier work implementing "state selective field ionization" with two parallel cylinders of atoms excited to two different Rydberg states, other geometries and state distributions will be explored. As the electron's amplitude traverses the many avoided crossings on the way to ionization it splits due to Landau-Zener transitions and spreads throughout many Stark levels, complicating the identification of the original electronic energy level. Previous attempts at manipulating the electron's path to ionization have focused on coarsely determining the slope of the electric field ramp. Since there are hundreds of avoided crossings on the way to ionization, a genetic algorithm will be used to design the electric field ramp. In addition, recent simulations have revealed the possibility of observing the anisotropic nature of the dipole-dipole interaction as well as Anderson localization.
PUBLICATIONS PRODUCED AS A RESULT OF THIS RESEARCH
Note:
When clicking on a Digital Object Identifier (DOI) number, you will be taken to an external
site maintained by the publisher. Some full text articles may not yet be available without a
charge during the embargo (administrative interval).
Some links on this page may take you to non-federal websites. Their policies may differ from
this site.
PROJECT OUTCOMES REPORT
Disclaimer
This Project Outcomes Report for the General Public is displayed verbatim as submitted by the Principal Investigator (PI) for this award. Any opinions, findings, and conclusions or recommendations expressed in this Report are those of the PI and do not necessarily reflect the views of the National Science Foundation; NSF has not approved or endorsed its content.
Rydberg atoms, in which the outermost electron has been excited to a very high energy level, can interact strongly by exchanging energy with each other. When they are slowed to ultracold temperatures, a few hundred millionths of a degree above absolute zero, it becomes possible to study and control these dipole-dipole interactions. In our work, a collaboration between the small liberal arts institutions Bryn Mawr College and Ursinus College, we use a combination of experimental and computational techniques to explore the quantum dynamics of Rydberg atom systems.
We achieved two primary goals with the work funded by this grant. First, we developed a genetic algorithm to control the ionization of the Rydberg electron which allows for the measurement of previously difficult-to-resolve atomic states. Second, we used this technique to make the first measurement of the time evolution of three- and four-body interactions among Rydberg atoms.
Selective field ionization is an important laboratory technique in atomic physics used to measure the distribution of energy states that a Rydberg electron occupies. A ramped electric field is used to sequentially ionize states from low to high binding energy. The arrival time of the ionized electron at a detector is then correlated with its original energy. While this simple picture provides a basic understanding of selective field ionization, it neglects complications introduced by shifts and interactions among energy states during ionization. The complicated details, as hundreds of energy levels converge and nearly cross on the way to ionization, are shown in Fig. 1. Unfortunately, some energy states overlap in their paths to ionization, making it difficult or impossible to tell them apart in arrival time.
We have developed a technique to control the electron's path to ionization by adding small wiggles to the linearly increasing electric field ramp. These perturbations can cause the electron to simultaneously take different paths, leading to quantum interference. By selectively enhancing some paths while suppressing others, a particular set of wiggles can make large adjustments to the arrival time of the electron.
The complexity of the ionization process makes it impossible to directly calculate the optimal perturbation to the field ionization ramp. We therefore developed a "genetic algorithm" that evolves the wiggles in an effort to best achieve the desired state separation. A genetic algorithm is an artificial intelligence technique, inspired by Darwinian evolution, in which the software attempts to achieve an outcome by trying many different solutions. Each solution is scored by how well it achieved the target goal and the most successful members are mated together to create a new generation of possible solutions. After a few dozen generations, the algorithm can evolve near optimal solutions to the problem.
We are interested in studying these particular energy levels because Rydberg atoms excited to these states can exchange energy with each other in rarely seen triplets or quadruplets. These three- and four-body interactions can be used for quantum gates or for studies of quantum dynamics. In particular, these interactions can model the behavior of more difficult to study solid state materials. Our new genetic algorithm technique allowed us to quantitatively measure the rate at which the atoms interacted with each other.
We measured and directly compared these rates for the two-, three-, and four-body cases as shown in Fig. 2. We built a computational model of the experiment and simulated it on a supercomputer. Our data revealed interesting features in the dynamics. For example, since each type of interaction depends differently on the density of the atomic sample, comparison of simulation to data could allow for an indirect measurement of the density. We also observed interesting thermodynamic behavior. Quantum systems that do not come to equilibrium, or thermalize, in the expected way could have much to teach us about quantum dynamics. We see hints in our data of such a failure to thermalize.
Our work trained many undergraduate students at our institutions, who participated in all aspects of this research: computational, experimental, presenting at conferences, and writing journal articles. More than half of our student researchers are from populations under-represented in the physical sciences. Most of them have gone on to careers or graduate school in STEM fields or are planning to upon graduation.
Last Modified: 11/16/2020
Modified by: Thomas Carroll
Please report errors in award information by writing to: awardsearch@nsf.gov.