Microwave dielectric properties of LiNbO$_{\mathbf{3}}$ and AlN at millikelvin temperatures and single-photon power
ORAL
Abstract
Electro-optic materials are paramount to achieving efficient and
reliable signal transduction in the quantum regime.
It is of great interest to investigate the performance of these materials
at the quantum level and at cryogenic temperatures to assess their compatibility
with superconducting circuit-based quantum systems. This work presents a
detailed study of the electric properties of bulk, single-crystal LiNbO$_{3}$ and AlN at cryogenic
temperatures and at the single photon level. We characterize the
materials' dielectric loss tangent and dielectric tensor throughout a wide range of
electromagnetic power levels between temperatures from 35 to 700 mK. Our findings indicate that
both materials' loss tangent behavior is consistent with the two-level system model up
to a certain power threshold, beyond which it increases logarithmically with power. This suggests that
two-level system loss mechanisms dominate at the single-photon level, while additional loss mechanisms
become apparent at higher powers and temperatures.
reliable signal transduction in the quantum regime.
It is of great interest to investigate the performance of these materials
at the quantum level and at cryogenic temperatures to assess their compatibility
with superconducting circuit-based quantum systems. This work presents a
detailed study of the electric properties of bulk, single-crystal LiNbO$_{3}$ and AlN at cryogenic
temperatures and at the single photon level. We characterize the
materials' dielectric loss tangent and dielectric tensor throughout a wide range of
electromagnetic power levels between temperatures from 35 to 700 mK. Our findings indicate that
both materials' loss tangent behavior is consistent with the two-level system model up
to a certain power threshold, beyond which it increases logarithmically with power. This suggests that
two-level system loss mechanisms dominate at the single-photon level, while additional loss mechanisms
become apparent at higher powers and temperatures.
*This material is based upon work supported by the U.S. Department ofEnergy, Office of Science, National Quantum Information Science ResearchCenters, Superconducting Quantum Materials and Systems Center (SQMS)under contract number DE-AC02-07CH11359. The authors also acknowledge support from the DOE Office of Science Early Career Research Program.
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Presenters
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Alessandro Reineri
- Illinois Institute of Technology