
NSF Org: |
DMR Division Of Materials Research |
Recipient: |
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Initial Amendment Date: | July 31, 2014 |
Latest Amendment Date: | June 2, 2016 |
Award Number: | 1306897 |
Award Instrument: | Continuing Grant |
Program Manager: |
Daryl Hess
dhess@nsf.gov (703)292-4942 DMR Division Of Materials Research MPS Directorate for Mathematical and Physical Sciences |
Start Date: | August 1, 2014 |
End Date: | January 31, 2019 (Estimated) |
Total Intended Award Amount: | $270,000.00 |
Total Awarded Amount to Date: | $270,000.00 |
Funds Obligated to Date: |
FY 2015 = $90,000.00 FY 2016 = $90,000.00 |
History of Investigator: |
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Recipient Sponsored Research Office: |
500 S LIMESTONE LEXINGTON KY US 40526-0001 (859)257-9420 |
Sponsor Congressional District: |
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Primary Place of Performance: |
500 South Limestone, 109 Kinkead Lexington KY US 40526-0001 |
Primary Place of
Performance Congressional District: |
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Unique Entity Identifier (UEI): |
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Parent UEI: |
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NSF Program(s): | CONDENSED MATTER & MAT THEORY |
Primary Program Source: |
01001516DB NSF RESEARCH & RELATED ACTIVIT 01001617DB NSF RESEARCH & RELATED ACTIVIT |
Program Reference Code(s): |
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Program Element Code(s): |
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Award Agency Code: | 4900 |
Fund Agency Code: | 4900 |
Assistance Listing Number(s): | 47.049 |
ABSTRACT
NONTECHNICAL SUMMARY
This award supports theoretical research and education aimed to investigate novel states of electrons.
Electrons are generally thought to be indivisible which is true at room temperature and under the conditions under which solid state devices normally operate. Most important to this research are the quantum Hall states, which occur in a two-dimensional sheet of electrons, usually at an artificially engineered interface between semiconductors, cooled to temperatures less than one degree from absolute zero, and placed in an a very strong magnetic field perpendicular to the sheet. In the simplest such state the electron can be thought of as "split" into three objects known as composite fermions. Each composite fermion has a charge one-third that of the electron along with other exotic properties. The charge and other properties of the excitation depend on the particular state. Some of these states offer possible platforms for quantum computing.
Conventional, semiconductor quantum Hall states need extreme conditions. In the past decade a new way of potentially realizing such states has been proposed where the environment inside some materials can generate the equivalent of very strong internal magnetic fields. The PI aims to study both conventional quantum Hall states and these newly discovered possibilities, known as topological band materials.
The PI will investigate whether topological band materials can support states that have not been discovered before, even in traditional quantum Hall systems. A main goal of the research is to understand the properties of such states in an approximate analytical way where the underlying physics is clear. This will enable understanding the similarities and the differences between conventional quantum Hall states and those in topological band materials. The PI will also utilize this approach to investigate conventional quantum Hall materials subjected to elastic strain.
Any real material contains lattice imperfections, substituted atoms, and defects, collectively known as disorder. The PI will develop a controlled approach to investigate the role of disorder where experiments on some quantum Hall states suggest that the effect of disorder is important.
The PI will also contribute to the organization of Winter Schools in India and will participate in the reorganization of the University Honors Program which provides a mechanism for students to learn about many disciplines and benefit from experimental learning.
TECHNICAL SUMMARY
This award supports theoretical research and education aimed to investigate quantum Hall states and topological states in materials. It has recently been established that materials with strong spin-orbit coupling can form new types of insulators, known as topological insulators, because of the topological properties of the band structure. When such bands are full, they have a quantized Hall conductance. With partial filling and strong electron-electron interactions fractional quantum Hall-like states form.
The research has two major thrusts:
1. Investigating novel states in fractionally filled topological bands: The PI will use an analytical approach to investigate Composite Fermion states in topological bands. (a) Ground state energies for gapped states at the principal fractions and collective excitations will be computed in the Hamiltonian approach developed for the fractional quantum Hall effect. (b) Transitions between principal fraction states of different spin will be investigated using ground state energy crossings. (c) Two different possibilities for the half-filled state, an electron fluid and a Composite Fermion fluid, will be investigated. The nature of the phase transition and low-energy excitations near the phase transition will be studied. (d) Edge states of fractionally filled topological bands will be studied using a conserving approximation. This is relevant for determining whether the topological band materials have excitations other than those of conventional fractional quantum Hall states. (e) Two time-reversed copies of topological bands are a model of a time-reversal invariant topological insulator. Fractionally filled states of strongly interacting electrons will be studied in this model. (f) Tilted fields or strain in the conventional fractional quantum Hall effects produces an anisotropy which has been measured. The PI will develop an analytical theory of such anisotopic states, and potential phase transitions into nematic-like states.
2. Elucidating the role of quenched disorder in quantum Hall ferromagnets: The prototypical system is the filling 1 bilayer, where experimental observations pose numerous challenges to theory, and where disorder seems to be essential. (a) The PI and collaborators will, at the first stage, mimic the nonperturbative effects of disorder by imposing a strong periodic potential on the quantum Hall system. Hartree-Fock and effective low-energy theories will be used to determine the generation of topological charges in response to the potential. (b) Collective excitations will be computed to derive an experimental signature in light scattering of such states. (c) A low-energy field theory will be constructed near the phase transitions between different arrangements of topological charge. (d) Weak disorder will be put in at this stage and renormalization group techniques will be used to determine the low-energy long-wavelength behavior near the transitions.
The PI will also contribute to the organization of Winter Schools in India and will participate in the reorganization of the University Honors Program which provides a mechanism for students to learn about many disciplines and benefit from experimental learning.
PUBLICATIONS PRODUCED AS A RESULT OF THIS RESEARCH
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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.
The quantum Hall effects, discovered in 1980, showed us a real, macroscopic, system engineered from semiconductors in which a physically measurable quantity, the resistance, depends only on the fundamental constants of nature, namely, the charge of the electron, e, the speed of light, c, and Planck's constant, h. The process of exploring the ramifications of this phenomenon and extending it to other systems such as Graphene (a single sheet of graphite) continues to this day.
There are two key properties shared by all quantum Hall systems. They are topological states of quantum matter, and charge degrees of freedom are inert in the bulk, only visible at low energies at the boundary.
In this project, the PI and co-workers have proceeded in two very different directions. The first direction is to explore the way the quantum Hall effects generalize to systems based on graphene, particularly monolayer, bilayer, and tetralayer graphene. The second is to investigate a phenomenon that occurs at the edges of quantum Hall systems as the smoothness of the edge is varied, called edge reconstruction. Since the information we obtain from quantum Hall systems is largely from the edge, such reconstructions are directly observable under the right circumstances.
Graphene: Without a magnetic field, electrons in graphene behave like relativistic massless particles at low energies near charge neutrality. This produces a fundamental change in the energy level structure in the presence of a large magnetic field as compared to semiconductor systems. Another difference is that there are many more internal degrees of freedom in graphene-based systems than in semiconductor systems. These may include the valley, the layer, and the orbital degrees of freedom in multilayer graphene systems. This leads to multiple phase transitions as external parameters such as the strength of the magnetic field, or the strength of an electric field perpendicular to the graphene, are varied.
One of the first such phase transitions was detected in 2014 in monolayer graphene as the coupling of the magnetic field to the spin degree of freedom was varied. The PI and collaborators helped elucidate the nature of the edge conduction in the two phases on either side of the transition. It turns out the "quasiparticles" which carry the edge current are vortices of the order parameter. Since then, the PI and co-workers has proposed phase diagrams for bilayer and tetralayer graphene as well. These systems have even more internal degrees of freedom and richer phase diagrams.
Edge currents in quantum Hall systems are carried by "chiral" modes, which can travel only one way along an edge. The number, charge, and chirality of these modes are subject to two constraints which emerge from the topological nature of the bulk quantum Hall state. However, many configurations of edge modes are allowed even after fulfilling these constraints. A change from one configuration to another as the smoothness of the edge potential varies is called an edge reconstruction. This phenomenon has been investigated since the nineties. Recently, the PI and collaborators found a new type of edge reconstruction. The more common type is driven by electrostatics, while the new one is driven by spin-exchange. Our type of reconstruction can, under certain conditions. generate additional pairs of neutral modes which propagate in opposite directions. We believe this type of reconstruction is generic, and should occur in many quantum Hall systems. Recently, experimentalists have developed the capability to measure neutral modes by measuring how heat propagates at the edge, which makes our reconstructions observable.
Last Modified: 06/08/2019
Modified by: Ganpathy N Murthy
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