Postdoc and graduate student positions available! Send email to akollar@umd.edu
Postdoc and graduate student positions available! Send email to akollar@umd.edu
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Research Areas
Research Areas
The field of circuit QED has emerged as a rich platform for both quantum computation and quantum simulation. Lattices of coplanar waveguide (CPW) resonators realize artificial photonic materials in the tight-binding limit. Combined with strong qubit-photon interactions, these systems can be used to study dynamical phase transitions, many-body phenomena, and spin models in driven-dissipative systems. These waveguide cavities are uniquely deformable and can produce lattices and networks which cannot readily be obtained in other systems, including periodic lattices in a hyperbolic space of constant negative curvature, and the one-dimensional nature of CPW resonators leads to degenerate flat bands. In our lab, we build experimental implementations of these systems using superconducting circuits.
Flat Bands
Flat Bands
The one-dimensional nature of CPW lattice sites and their inherent deformability leads naturally to the implementation of line graphs with degenerate flat bands. Qubits coupled to these systems will mediate photon-photon interactions within the flat bands. They will also experience novel electromagnetic environments depending on their detuning with respect to the band structure. The resulting photonic bound states have new and controllable forms which give rise to new types of effective spin-spin interactions, including frustrated short-range antiferromagentism in the flat bands.
A. J. Kollár, M. Fitzpatrick, P. Sarnak, A.A. Houck, Line-Graph Lattices: Euclidean and Non-Euclidean Flat Bands and Implementations in Circuit QED, arXiv:1902.02794v1 (2019).
N. M. Sundaresan, R. Lundgren, G. Zhu, A. V. Gorshkov, and A. A. Houck, “Interacting Qubit-Photon Bound States with Superconducting Circuits,” Phys. Rev. X 9, 011021 (2019).
J. S. Douglas, H. Habibian, C.-L. Hung, A. V. Gorshkov, H. J. Kimble, and D. E. Chang, “Quantum many-body models with cold atoms coupled to photonic crystals,” Nat. Phys. 9, 326 (2012).
N. M. Sundaresan, R. Lundgren, G. Zhu, A. V. Gorshkov, and A. A. Houck, “Interacting Qubit-Photon Bound States with Superconducting Circuits,” Phys. Rev. X 9, 011021 (2019).
J. S. Douglas, H. Habibian, C.-L. Hung, A. V. Gorshkov, H. J. Kimble, and D. E. Chang, “Quantum many-body models with cold atoms coupled to photonic crystals,” Nat. Phys. 9, 326 (2012).
Hyperbolic Lattices
Hyperbolic Lattices
Curvature is fundamental aspect of general relativity, but negatively curved 2D hyperbolic manifolds cannot be isometrically imbedded in 3D Euclidean space. The natural deformability of CPW resonators allows for the implementation of table-top hyperbolic lattices with high curvature. Incorporating qubits into these devices, we can start to examine quantum mechanics in this unique environment.
A. J. Kollár, M. Fitzpatrick, P. Sarnak, A.A. Houck, Line-Graph Lattices: Euclidean and Non-Euclidean Flat Bands and Implementations in Circuit QED, arXiv:1902.02794v1 (2019).
A. J. Kollár, M. Fitzpatrick, A. A. Houck, Hyperbolic Lattices in Circuit Quantum Electrodynamics, Nature 571, 45-49 (2019), arXiv:1802.09549.
A. A. Houck, H. E. Türeci, and J. Koch, “On-chip quantum simulation with superconducting circuits,” Nat. Phys. 8, 292 (2012).
A. J. Kollár, M. Fitzpatrick, A. A. Houck, Hyperbolic Lattices in Circuit Quantum Electrodynamics, Nature 571, 45-49 (2019), arXiv:1802.09549.
A. A. Houck, H. E. Türeci, and J. Koch, “On-chip quantum simulation with superconducting circuits,” Nat. Phys. 8, 292 (2012).
Interacting Chains
Interacting Chains
In the absence of fine tuning and many-body localization, large strongly-interacting closed systems are expected to self thermalize. Networks of qubits and resonators can be used to examine this behavior in the presence of drives and controllable dissipation set by qubit lifetimes and resonator coupling strengths.
M. Fitzpatick, N. M. Sundaresan, A. C. Y. Li, J. Koch, and A. A. Houck, “Observation of a Dissipative Phase Transition in a One-Dimensional Circuit QED Lattice,” Phys. Rev. X 7, 011016 (2017).
Raferty, J., D. Sadri, S. Schmidt, H. E. Türeci, A. A. Houck. Observation of a Dissipation-Induced Classical to Quantum Transition. Physical Review X 4, 031043 (2014).
A. A. Houck, H. E. Türeci, and J. Koch, “On-chip quantum simulation with superconducting circuits,” Nat. Phys. 8, 292 (2012).
Raferty, J., D. Sadri, S. Schmidt, H. E. Türeci, A. A. Houck. Observation of a Dissipation-Induced Classical to Quantum Transition. Physical Review X 4, 031043 (2014).
A. A. Houck, H. E. Türeci, and J. Koch, “On-chip quantum simulation with superconducting circuits,” Nat. Phys. 8, 292 (2012).
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