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| 001 | 187426 | ||
| 005 | 20240610121126.0 | ||
| 024 | 7 | _ | |a 10.1109/TASC.2014.2365098 |2 doi |
| 024 | 7 | _ | |a 1051-8223 |2 ISSN |
| 024 | 7 | _ | |a 1558-2515 |2 ISSN |
| 024 | 7 | _ | |a WOS:000216431900001 |2 WOS |
| 037 | _ | _ | |a FZJ-2015-01091 |
| 041 | _ | _ | |a English |
| 082 | _ | _ | |a 530 |
| 100 | 1 | _ | |a Faley, Michael |0 P:(DE-Juel1)130633 |b 0 |e Corresponding Author |
| 245 | _ | _ | |a Integration Issues of Graphoepitaxial High-Tc SQUIDs Into Multichannel MEG Systems |
| 260 | _ | _ | |a New York, NY |c 2015 |b IEEE |
| 336 | 7 | _ | |a Journal Article |b journal |m journal |0 PUB:(DE-HGF)16 |s 1424179234_8551 |2 PUB:(DE-HGF) |
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| 336 | 7 | _ | |a article |2 DRIVER |
| 520 | _ | _ | |a We have analyzed the possibility to construct multichannel magnetoencephalography (MEG) systems based on high-Tc direct current superconducting quantum interference devices (DC SQUIDs) with graphoepitaxial step edge Josephson junctions. A new layout of multilayer high-Tc superconducting flux transformers was tested and a new type of high-Tc DC SQUID magnetometer intended for MEG systems was realized. These magnetometers have a vacuum-tight capsule of outer diameter 24 mm and a magnetic field resolution of ∼4 fT/√Hz at 77 K. Crosstalk between adjacent sensors was estimated and measured for in-plane and axial configurations. The vibration-free cooling of sensors, minimization of the sensor-to-object distance and optimization of the sensor positions as well as the gantry design are discussed. Our findings may have implications for the next generation of non-invasive imaging techniques that will be used to understand human brain function. |
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| 700 | 1 | _ | |a Gerasimov, I. A. |0 P:(DE-HGF)0 |b 1 |
| 700 | 1 | _ | |a Faley, O. M. |0 P:(DE-HGF)0 |b 2 |
| 700 | 1 | _ | |a Chocholacs, H. |0 P:(DE-Juel1)140455 |b 3 |u fzj |
| 700 | 1 | _ | |a Dammers, J. |0 P:(DE-Juel1)131757 |b 4 |u fzj |
| 700 | 1 | _ | |a Eich, E. |0 P:(DE-Juel1)140456 |b 5 |u fzj |
| 700 | 1 | _ | |a Boers, F. |0 P:(DE-Juel1)131752 |b 6 |u fzj |
| 700 | 1 | _ | |a Shah, N. J. |0 P:(DE-Juel1)131794 |b 7 |u fzj |
| 700 | 1 | _ | |a Sobolev, A. S. |0 P:(DE-HGF)0 |b 8 |
| 700 | 1 | _ | |a Slobodchikov, V. Yu. |0 P:(DE-HGF)0 |b 9 |
| 700 | 1 | _ | |a Maslennikov, Yu. V. |0 P:(DE-HGF)0 |b 10 |
| 700 | 1 | _ | |a Koshelets, V. P. |0 P:(DE-HGF)0 |b 11 |
| 700 | 1 | _ | |a Dunin-Borkowski, Rafal |0 P:(DE-Juel1)144121 |b 12 |
| 773 | _ | _ | |a 10.1109/TASC.2014.2365098 |g Vol. 25, no. 3, p. 1 - 5 |0 PERI:(DE-600)2025387-4 |n 3 |p 1601605 |t IEEE transactions on applied superconductivity |v 25 |y 2015 |x 1051-8223 |
| 856 | 4 | _ | |u http://ieeexplore.ieee.org/stamp/stamp.jsp?arnumber=6936876 |
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