1999
DOI: 10.1023/a:1007780925567
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Cited by 17 publications
(16 citation statements)
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“…At low temperature, it is equivalent to a single junction whose Josephson energy is modulated with a 2e period by the gate charge coupled to the island formed between the two junctions. This modulation can be exploited for low-noise-temperature electrometry [23], provided that the device supercurrent is measured like in the present experiment. The SCPT could operate at high frequencies since intrinsic bandwidths up to 120 and 250 MHz have been demonstrated for arrays with 100 and 30 SQUIDs, respectively [24].…”
mentioning
confidence: 97%
“…At low temperature, it is equivalent to a single junction whose Josephson energy is modulated with a 2e period by the gate charge coupled to the island formed between the two junctions. This modulation can be exploited for low-noise-temperature electrometry [23], provided that the device supercurrent is measured like in the present experiment. The SCPT could operate at high frequencies since intrinsic bandwidths up to 120 and 250 MHz have been demonstrated for arrays with 100 and 30 SQUIDs, respectively [24].…”
mentioning
confidence: 97%
“…This device is an electrometer, dual to the DC SQUID amplifier [154,155] shown in (g). The QPST is similar to a single Cooper-pair transistor (SCPT) [156]; however, it could have a much higher sensitivity than an SCPT, which is limited by the charging energy of the JJs (by how small one can make the junction capacitance). The QPST is instead limited by the kinetic capacitance C k , whose ultimate limit is the series capacitance of the wires, which can be much smaller.…”
Section: Appendix F Flux-charge Duality and Lumped-element Supercondmentioning
confidence: 99%
“…1) is topologically a single-contact rf SQUID whose Josephson junction is replaced by a single-Cooper-pair transistor. 19,20,21,22 The latter consists of two mesoscopic junctions with Josephson energies E J1 , E J2 and capacitances C 1 , C 2 , coupled by a small island. The Hamiltonian of the charge-phase qubit in the eigenstate basis within the two-level approximation (E CP ≫ ε J (δ)) and the small-inductance limit reads as 2,19,20…”
Section: System Of Charge-phase Qubit and Tank Circuitmentioning
confidence: 99%
“…In general case, at arbitrary ratio of the Josephson and charging energies ε J (δ)/E CP (while the two-level approximation (1) is determined by ε J (δ)/E CP ≪ 1) the energy spectrum and eigenfunctions of the charge-phase qubit are given, respectively, by the Bloch bands E n (q, δ) and the Bloch wave functions |q, δ; n (n = 0, 1, 2... is the band index and q = en g the quasicharge) that are numerical solutions of Schrödinger equation with Hamiltonian containing all the charge states and periodic Josephson potential. 19,22 Then the lowest two energy levels n = 0, 1 form the basis of the charge-phase qubit, so…”
Section: System Of Charge-phase Qubit and Tank Circuitmentioning
confidence: 99%