Tuning high-Q superconducting resonators by magnetic field reorientation
Superconducting resonators interfaced with paramagnetic spin ensembles are used to increase the sensitivity of electron spin resonance experiments and are key elements of microwave quantum memories. Certain spin systems that are promising for such quantum memories possess “sweet spots” at particular...
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Online Access: | http://dx.doi.org/10.1063/1.5129032 |
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doaj-b651a38a6db44149a7c6fd9f2b83b18f2020-11-25T02:05:43ZengAIP Publishing LLCAIP Advances2158-32262019-12-01912125225125225-510.1063/1.5129032Tuning high-Q superconducting resonators by magnetic field reorientationChristoph W. Zollitsch0James O’Sullivan1Oscar Kennedy2Gavin Dold3John J. L. Morton4London Centre for Nanotechnology, University College London, 17-19 Gordon Street, London WCH1 0AH, United KingdomLondon Centre for Nanotechnology, University College London, 17-19 Gordon Street, London WCH1 0AH, United KingdomLondon Centre for Nanotechnology, University College London, 17-19 Gordon Street, London WCH1 0AH, United KingdomLondon Centre for Nanotechnology, University College London, 17-19 Gordon Street, London WCH1 0AH, United KingdomLondon Centre for Nanotechnology, University College London, 17-19 Gordon Street, London WCH1 0AH, United KingdomSuperconducting resonators interfaced with paramagnetic spin ensembles are used to increase the sensitivity of electron spin resonance experiments and are key elements of microwave quantum memories. Certain spin systems that are promising for such quantum memories possess “sweet spots” at particular combinations of magnetic fields and frequencies, where spin coherence times or linewidths become particularly favorable. In order to be able to couple high-Q superconducting resonators to such specific spin transitions, it is necessary to be able to tune the resonator frequency under a constant magnetic field amplitude. Here, we demonstrate a high-quality, magnetic field resilient superconducting resonator, using a 3D vector magnet to continuously tune its resonance frequency by adjusting the orientation of the magnetic field. The resonator maintains a quality factor of >105 up to magnetic fields of 2.6 T, applied predominantly in the plane of the superconductor. We achieve a continuous tuning of up to 30 MHz by rotating the magnetic field vector, introducing a component of 5 mT perpendicular to the superconductor.http://dx.doi.org/10.1063/1.5129032 |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Christoph W. Zollitsch James O’Sullivan Oscar Kennedy Gavin Dold John J. L. Morton |
spellingShingle |
Christoph W. Zollitsch James O’Sullivan Oscar Kennedy Gavin Dold John J. L. Morton Tuning high-Q superconducting resonators by magnetic field reorientation AIP Advances |
author_facet |
Christoph W. Zollitsch James O’Sullivan Oscar Kennedy Gavin Dold John J. L. Morton |
author_sort |
Christoph W. Zollitsch |
title |
Tuning high-Q superconducting resonators by magnetic field reorientation |
title_short |
Tuning high-Q superconducting resonators by magnetic field reorientation |
title_full |
Tuning high-Q superconducting resonators by magnetic field reorientation |
title_fullStr |
Tuning high-Q superconducting resonators by magnetic field reorientation |
title_full_unstemmed |
Tuning high-Q superconducting resonators by magnetic field reorientation |
title_sort |
tuning high-q superconducting resonators by magnetic field reorientation |
publisher |
AIP Publishing LLC |
series |
AIP Advances |
issn |
2158-3226 |
publishDate |
2019-12-01 |
description |
Superconducting resonators interfaced with paramagnetic spin ensembles are used to increase the sensitivity of electron spin resonance experiments and are key elements of microwave quantum memories. Certain spin systems that are promising for such quantum memories possess “sweet spots” at particular combinations of magnetic fields and frequencies, where spin coherence times or linewidths become particularly favorable. In order to be able to couple high-Q superconducting resonators to such specific spin transitions, it is necessary to be able to tune the resonator frequency under a constant magnetic field amplitude. Here, we demonstrate a high-quality, magnetic field resilient superconducting resonator, using a 3D vector magnet to continuously tune its resonance frequency by adjusting the orientation of the magnetic field. The resonator maintains a quality factor of >105 up to magnetic fields of 2.6 T, applied predominantly in the plane of the superconductor. We achieve a continuous tuning of up to 30 MHz by rotating the magnetic field vector, introducing a component of 5 mT perpendicular to the superconductor. |
url |
http://dx.doi.org/10.1063/1.5129032 |
work_keys_str_mv |
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