TY - JOUR
T1 - Superconducting tunnel-junction refrigerator
AU - Melton, Robert Graham
AU - Paterson, James L.
AU - Kaplan, S. B.
PY - 1980/1/1
Y1 - 1980/1/1
N2 - The dc current through an S1-S2 tunnel junction, with 2 greater than 1, when biased with eV<1+2, will lower the energy in S1. This energy reduction will be shared by the phonons and electrons. This device is shown to be analogous to a thermoelectric refrigerator with an effective Peltier coefficient *1e. Tunneling calculations yield the cooling power Pc, the electrical power Pe supplied by the bias supply, and the cooling efficiency =PcPe. The maximum cooling power is obtained for eV=(2-1) and t1=T1Tc10.9. Estimates are made of the temperature difference T2-T1 achievable in Al-Pb and Sn-Pb junctions with an Al2O3 tunneling barrier. The performance of this device is shown to yield a maximum cooling efficiency 1(2-1) which can be compared with that available in an ideal Carnot refrigerator of =T1(T2-T1). The development of a useful tunnel-junction refrigerator requires a tunneling barrier with an effective thermal conductance per unit area several orders of magnitude less than that provided by the Al2O3 barrier in the Al-Pb and Sn-Pb systems.
AB - The dc current through an S1-S2 tunnel junction, with 2 greater than 1, when biased with eV<1+2, will lower the energy in S1. This energy reduction will be shared by the phonons and electrons. This device is shown to be analogous to a thermoelectric refrigerator with an effective Peltier coefficient *1e. Tunneling calculations yield the cooling power Pc, the electrical power Pe supplied by the bias supply, and the cooling efficiency =PcPe. The maximum cooling power is obtained for eV=(2-1) and t1=T1Tc10.9. Estimates are made of the temperature difference T2-T1 achievable in Al-Pb and Sn-Pb junctions with an Al2O3 tunneling barrier. The performance of this device is shown to yield a maximum cooling efficiency 1(2-1) which can be compared with that available in an ideal Carnot refrigerator of =T1(T2-T1). The development of a useful tunnel-junction refrigerator requires a tunneling barrier with an effective thermal conductance per unit area several orders of magnitude less than that provided by the Al2O3 barrier in the Al-Pb and Sn-Pb systems.
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U2 - 10.1103/PhysRevB.21.1858
DO - 10.1103/PhysRevB.21.1858
M3 - Article
AN - SCOPUS:0038942355
SN - 2469-9950
VL - 21
SP - 1858
EP - 1867
JO - Physical Review B-Condensed Matter
JF - Physical Review B-Condensed Matter
IS - 5
ER -