TY - JOUR
T1 - RF pulse triggered superconducting switches
AU - Hiebl, Alois
AU - Numssen, Kai
AU - Kinder, Helmut
AU - Weck, Werner
AU - Müller, Anton
AU - Schölderle, Hermann
N1 - Funding Information:
Manuscript received August 5, 2002. This work was supported in part by Bayerische Forschungsstiftung. A. Hiebl, K. Numssen, and H. Kinder are with Technische Universität München, D-85748 Garching, Germany (e-mail: [email protected]). W. Weck, A. Müller, and H. Schölderle are with Magnet Motor, D-82319 Starnberg, Germany (e-mail: [email protected]). Digital Object Identifier 10.1109/TASC.2003.812936 Fig. 1. Typical measurement. The dc trigger pulse marks the duration of the RF pulse coupled into the superconductor. Right at its beginning (t = 1 ms), a small dc voltage jump is observed which increases with time until switching into the normal state occurs.
PY - 2003/6
Y1 - 2003/6
N2 - In recent years, we have studied the possibility of using YBCO thin films not only for passive switching, as in resistive fault current limiters, but also as actively switchable devices at high power levels and millisecond time scales. As a trigger, we previously used heat pulses which were launched from the backside of the substrate. This requires relatively high trigger power, however. More recently, we have used RF pulses which are directly applied to the superconducting strip itself. The RF magnetic field was applied by various types of coils at frequencies in the MHz range. The samples were prepared by thermal co-evaporation on sapphire substrates in the form of strips with dimensions 10 mm × 42 mm. They were submersed in liquid nitrogen and biased by a dc current. Simultaneously with the leading edge of the RF pulse, we observe the onset of a dc voltage drop along the superconductor which continues to increase during some milliseconds until the YBCO film eventually switches into the normal state. We have measured the switching time as a function of bias current, RF field direction, and RF power. The latter is considerably less than the heat pulse power required for our previous trigger method. The optimum field direction turned out to be perpendicular to the film.
AB - In recent years, we have studied the possibility of using YBCO thin films not only for passive switching, as in resistive fault current limiters, but also as actively switchable devices at high power levels and millisecond time scales. As a trigger, we previously used heat pulses which were launched from the backside of the substrate. This requires relatively high trigger power, however. More recently, we have used RF pulses which are directly applied to the superconducting strip itself. The RF magnetic field was applied by various types of coils at frequencies in the MHz range. The samples were prepared by thermal co-evaporation on sapphire substrates in the form of strips with dimensions 10 mm × 42 mm. They were submersed in liquid nitrogen and biased by a dc current. Simultaneously with the leading edge of the RF pulse, we observe the onset of a dc voltage drop along the superconductor which continues to increase during some milliseconds until the YBCO film eventually switches into the normal state. We have measured the switching time as a function of bias current, RF field direction, and RF power. The latter is considerably less than the heat pulse power required for our previous trigger method. The optimum field direction turned out to be perpendicular to the film.
KW - Active switch
KW - Fault current limiter
KW - YBCO thin films
UR - http://www.scopus.com/inward/record.url?scp=0042975007&partnerID=8YFLogxK
U2 - 10.1109/TASC.2003.812936
DO - 10.1109/TASC.2003.812936
M3 - Conference article
AN - SCOPUS:0042975007
SN - 1051-8223
VL - 13
SP - 1879
EP - 1881
JO - IEEE Transactions on Applied Superconductivity
JF - IEEE Transactions on Applied Superconductivity
IS - 2 II
T2 - 2002 Applied Superconductivity Conference
Y2 - 4 August 2002 through 9 August 2002
ER -