Induced Self-Stabilization in Fractional Quantum Hall States of Light
Recent progress in nanoscale quantum optics and superconducting qubits has made the creation of strongly correlated, and even topologically ordered, states of photons a real possibility. Many of these states are gapped and exhibit anyon excitations, which could be used for a robust form of quantum i...
| Hlavní autoři: | , , |
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| Médium: | Journal article |
| Jazyk: | English |
| Vydáno: |
American Physical Society
2014
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| _version_ | 1826284803880648704 |
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| author | Kapit, E Hafezi, M Simon, S |
| author_facet | Kapit, E Hafezi, M Simon, S |
| author_sort | Kapit, E |
| collection | OXFORD |
| description | Recent progress in nanoscale quantum optics and superconducting qubits has made the creation of strongly correlated, and even topologically ordered, states of photons a real possibility. Many of these states are gapped and exhibit anyon excitations, which could be used for a robust form of quantum information processing. However, while numerous qubit array proposals exist to engineer the Hamiltonian for these systems, the question of how to stabilize the many-body ground state of these photonic quantum simulators against photon losses remains largely unanswered. We here propose a simple mechanism that achieves this goal for Abelian and non-Abelian fractional quantum Hall states of light. Our construction uses a uniform two-photon drive field to couple the qubits of the primary lattice with an auxiliary "shadow" lattice, composed of qubits with a much faster loss rate than the qubits of the primary quantum simulator itself. This coupling causes hole states created by photon losses to be rapidly refilled, and the system's manybody gap prevents further photons from being added once the strongly correlated ground state is reached. The fractional quantum Hall state (with a small, transient population of quasihole excitations) is thus the most stable state of the system, and all other configurations will relax toward it over time. The physics described here could be implemented in a circuit QED architecture, and the device parameters needed for our scheme to succeed are in reach of current technology.We also propose a simple six-qubit device, which could easily be built in the near future, that can act as a proof of principle for our scheme. |
| first_indexed | 2024-03-07T01:19:20Z |
| format | Journal article |
| id | oxford-uuid:8fcf0a9d-6cfc-4e3c-b06a-8bf8c05607f3 |
| institution | University of Oxford |
| language | English |
| last_indexed | 2024-03-07T01:19:20Z |
| publishDate | 2014 |
| publisher | American Physical Society |
| record_format | dspace |
| spelling | oxford-uuid:8fcf0a9d-6cfc-4e3c-b06a-8bf8c05607f32022-03-26T23:06:57ZInduced Self-Stabilization in Fractional Quantum Hall States of LightJournal articlehttp://purl.org/coar/resource_type/c_dcae04bcuuid:8fcf0a9d-6cfc-4e3c-b06a-8bf8c05607f3EnglishSymplectic Elements at OxfordAmerican Physical Society2014Kapit, EHafezi, MSimon, SRecent progress in nanoscale quantum optics and superconducting qubits has made the creation of strongly correlated, and even topologically ordered, states of photons a real possibility. Many of these states are gapped and exhibit anyon excitations, which could be used for a robust form of quantum information processing. However, while numerous qubit array proposals exist to engineer the Hamiltonian for these systems, the question of how to stabilize the many-body ground state of these photonic quantum simulators against photon losses remains largely unanswered. We here propose a simple mechanism that achieves this goal for Abelian and non-Abelian fractional quantum Hall states of light. Our construction uses a uniform two-photon drive field to couple the qubits of the primary lattice with an auxiliary "shadow" lattice, composed of qubits with a much faster loss rate than the qubits of the primary quantum simulator itself. This coupling causes hole states created by photon losses to be rapidly refilled, and the system's manybody gap prevents further photons from being added once the strongly correlated ground state is reached. The fractional quantum Hall state (with a small, transient population of quasihole excitations) is thus the most stable state of the system, and all other configurations will relax toward it over time. The physics described here could be implemented in a circuit QED architecture, and the device parameters needed for our scheme to succeed are in reach of current technology.We also propose a simple six-qubit device, which could easily be built in the near future, that can act as a proof of principle for our scheme. |
| spellingShingle | Kapit, E Hafezi, M Simon, S Induced Self-Stabilization in Fractional Quantum Hall States of Light |
| title | Induced Self-Stabilization in Fractional Quantum Hall States of Light |
| title_full | Induced Self-Stabilization in Fractional Quantum Hall States of Light |
| title_fullStr | Induced Self-Stabilization in Fractional Quantum Hall States of Light |
| title_full_unstemmed | Induced Self-Stabilization in Fractional Quantum Hall States of Light |
| title_short | Induced Self-Stabilization in Fractional Quantum Hall States of Light |
| title_sort | induced self stabilization in fractional quantum hall states of light |
| work_keys_str_mv | AT kapite inducedselfstabilizationinfractionalquantumhallstatesoflight AT hafezim inducedselfstabilizationinfractionalquantumhallstatesoflight AT simons inducedselfstabilizationinfractionalquantumhallstatesoflight |