Electrostatic tuning of mechanical and microwave resonances in 3D superconducting radio frequency cavities

We implement a non-contact, external method of simultaneously fine-tuning a mechanical resonator and a superconducting radio frequency (SRF) cavity using a capacitor formed between a silicon nitride membrane and a copper electrode at cryogenic temperatures. The silicon nitride membrane forms a varia...

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Main Authors: Jacob M. Pate, Luis A. Martinez, Johnathon J. Thompson, Raymond Y. Chiao, Jay E. Sharping
Format: Article
Language:English
Published: AIP Publishing LLC 2018-11-01
Series:AIP Advances
Online Access:http://dx.doi.org/10.1063/1.5055887
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spelling doaj-470bd9ada3934b0e8d19357ce0eecf522020-11-25T02:34:21ZengAIP Publishing LLCAIP Advances2158-32262018-11-01811115223115223-710.1063/1.5055887082811ADVElectrostatic tuning of mechanical and microwave resonances in 3D superconducting radio frequency cavitiesJacob M. Pate0Luis A. Martinez1Johnathon J. Thompson2Raymond Y. Chiao3Jay E. Sharping4School of Natural Sciences, University of California Merced, Merced, California 95343, USASchool of Natural Sciences, University of California Merced, Merced, California 95343, USASchool of Natural Sciences, University of California Merced, Merced, California 95343, USASchool of Natural Sciences, University of California Merced, Merced, California 95343, USASchool of Natural Sciences, University of California Merced, Merced, California 95343, USAWe implement a non-contact, external method of simultaneously fine-tuning a mechanical resonator and a superconducting radio frequency (SRF) cavity using a capacitor formed between a silicon nitride membrane and a copper electrode at cryogenic temperatures. The silicon nitride membrane forms a variable boundary condition for the SRF cavity thereby creating the optomechanical cavity. By controlling the DC voltage applied between an external electrode and the silicon nitride membrane we are capable of tuning the resonance frequency internal to the SRF cavity up to 25 kHz for a cavity with loaded quality factor of 2.5 million, corresponding to six cavity linewidths. At the same time we observe the electrostatic frequency shift of the membrane. This approach has the unique benefit of avoiding any dielectric insertion or added gaps due to a moving end-wall thereby limiting the loss of the cavity. Furthermore, this design avoids applied pressure typically used with piezoelectric devices in accelerator cavities. This work seeks to have strong impact in tuning high-Q cavities due to its ability to maintain low losses.http://dx.doi.org/10.1063/1.5055887
collection DOAJ
language English
format Article
sources DOAJ
author Jacob M. Pate
Luis A. Martinez
Johnathon J. Thompson
Raymond Y. Chiao
Jay E. Sharping
spellingShingle Jacob M. Pate
Luis A. Martinez
Johnathon J. Thompson
Raymond Y. Chiao
Jay E. Sharping
Electrostatic tuning of mechanical and microwave resonances in 3D superconducting radio frequency cavities
AIP Advances
author_facet Jacob M. Pate
Luis A. Martinez
Johnathon J. Thompson
Raymond Y. Chiao
Jay E. Sharping
author_sort Jacob M. Pate
title Electrostatic tuning of mechanical and microwave resonances in 3D superconducting radio frequency cavities
title_short Electrostatic tuning of mechanical and microwave resonances in 3D superconducting radio frequency cavities
title_full Electrostatic tuning of mechanical and microwave resonances in 3D superconducting radio frequency cavities
title_fullStr Electrostatic tuning of mechanical and microwave resonances in 3D superconducting radio frequency cavities
title_full_unstemmed Electrostatic tuning of mechanical and microwave resonances in 3D superconducting radio frequency cavities
title_sort electrostatic tuning of mechanical and microwave resonances in 3d superconducting radio frequency cavities
publisher AIP Publishing LLC
series AIP Advances
issn 2158-3226
publishDate 2018-11-01
description We implement a non-contact, external method of simultaneously fine-tuning a mechanical resonator and a superconducting radio frequency (SRF) cavity using a capacitor formed between a silicon nitride membrane and a copper electrode at cryogenic temperatures. The silicon nitride membrane forms a variable boundary condition for the SRF cavity thereby creating the optomechanical cavity. By controlling the DC voltage applied between an external electrode and the silicon nitride membrane we are capable of tuning the resonance frequency internal to the SRF cavity up to 25 kHz for a cavity with loaded quality factor of 2.5 million, corresponding to six cavity linewidths. At the same time we observe the electrostatic frequency shift of the membrane. This approach has the unique benefit of avoiding any dielectric insertion or added gaps due to a moving end-wall thereby limiting the loss of the cavity. Furthermore, this design avoids applied pressure typically used with piezoelectric devices in accelerator cavities. This work seeks to have strong impact in tuning high-Q cavities due to its ability to maintain low losses.
url http://dx.doi.org/10.1063/1.5055887
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