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Naji, M. |
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Motta, Antonella |
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Aletan, Dirar |
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Mohamed, Tarek |
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Ertürk, Emre |
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Taccardi, Nicola |
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Kononenko, Denys |
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Petrov, R. H. | Madrid |
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Alshaaer, Mazen | Brussels |
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Bih, L. |
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Casati, R. |
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Muller, Hermance |
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Kočí, Jan | Prague |
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Šuljagić, Marija |
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Kalteremidou, Kalliopi-Artemi | Brussels |
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Azam, Siraj |
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Ospanova, Alyiya |
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Blanpain, Bart |
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Ali, M. A. |
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Popa, V. |
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Rančić, M. |
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Ollier, Nadège |
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Azevedo, Nuno Monteiro |
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Landes, Michael |
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Rignanese, Gian-Marco |
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Steppke, Alexander
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Publications (5/5 displayed)
- 2023Microstructuring YbRh2Si2 for resistance and noise measurements down to ultra-low temperaturescitations
- 2022Microstructuring YbRh2Si2 for resistance and noise measurements down to ultra-low temperaturescitations
- 2022Microstructuring YbRh 2 Si 2 for resistance and noise measurements down to ultra-low temperaturescitations
- 2010Pulsed laser deposition of niobium thin films for in-situ device fabrication and their superconducting propertiescitations
- 2008Planar high-Tc superconducting quantum interference device gradiometer for simultaneous measurements of two magnetic field gradientscitations
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article
Planar high-Tc superconducting quantum interference device gradiometer for simultaneous measurements of two magnetic field gradients
Abstract
Here, we present a planar superconducting quantum interference device (SQUID) structure consisting of four SQUIDs connected to antenna structures for simultaneous measurements of two magnetic field components. Using YBa2Cu3O7−x thin film technology, we are able to prepare gradiometer structures on strontium titanate (SrTiO3) tetracrystals containing two crossing 30° grain boundaries. This allows the production of four SQUID loops onto one substrate which can fulfill the high demands of symmetry inside the antenna structures. In our arrangement, the SQUID loops can act as independent field sensors which allow a measurement of two independent magnetic field gradient components.