TY - JOUR
T1 - Material aspects for preparing HTS quasiparticle injection devices
AU - Schneider, C.W.
AU - Moerman, R.
AU - Roesthuis, F.J.G.
AU - Wichern, R.G.
AU - Gerritsma, G.J.
AU - Rogalla, H.
PY - 1997
Y1 - 1997
N2 - Quasiparticle (QP) injection devices based on HTS could play an important role in future superconducting applications if material aspects can be better controlled. One reason why this kind of device received little attention in the past is the lack of an appropriate barrier for QP tunnelling. In a series of experiments, we used different barriers to test if they are suitable, i.e. if a current and possibly a voltage gain can be achieved. We improved the performance of planar YBCO/natural barrier/Au devices and a current gain of more than 6 at 40 K was observed. Most devices, however, showed signs of heating effects. Another barrier material was SrTiO3 with layers of 5-6 nm thickness. Current-voltage characteristics showed that the barriers were continuous and we observed current gains of up to 3 at 60 K. PrBa2 Cu3O7-x is an interesting candidate if one could overcome the problem of resonant inelastic tunnelling for QP. In a series of experiments we demonstrated that, even for 3 Mn thin PBCO barriers on a- and c-axis oriented YBa2Cu3O7-x, most devices showed at best a current gain of 1. However, we have indications that a current gain of 10 could be possible with unity voltage gain
AB - Quasiparticle (QP) injection devices based on HTS could play an important role in future superconducting applications if material aspects can be better controlled. One reason why this kind of device received little attention in the past is the lack of an appropriate barrier for QP tunnelling. In a series of experiments, we used different barriers to test if they are suitable, i.e. if a current and possibly a voltage gain can be achieved. We improved the performance of planar YBCO/natural barrier/Au devices and a current gain of more than 6 at 40 K was observed. Most devices, however, showed signs of heating effects. Another barrier material was SrTiO3 with layers of 5-6 nm thickness. Current-voltage characteristics showed that the barriers were continuous and we observed current gains of up to 3 at 60 K. PrBa2 Cu3O7-x is an interesting candidate if one could overcome the problem of resonant inelastic tunnelling for QP. In a series of experiments we demonstrated that, even for 3 Mn thin PBCO barriers on a- and c-axis oriented YBa2Cu3O7-x, most devices showed at best a current gain of 1. However, we have indications that a current gain of 10 could be possible with unity voltage gain
U2 - 10.1109/77.621802
DO - 10.1109/77.621802
M3 - Article
VL - 7
SP - 2730
EP - 2733
JO - IEEE transactions on applied superconductivity
JF - IEEE transactions on applied superconductivity
SN - 1051-8223
IS - 2
ER -