1991
DOI: 10.2978/jsas.3.97
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DC SQUID RF amplifiers.

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1991
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Cited by 2 publications
(3 citation statements)
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“…In the high frequency range, the parasitic capacitance C p between the input coil and SQUID loop increases, and this makes the transfer of input flux into SQUID loop difficult. By placing the input coil inside the SQUID hole, the parasitic capacitance can be reduced much, but the multi-turn coil inside the SQUID hole reduces the mutual inductance with the SQUID loop, resulting in reduction of the amplifier gain [3,4].…”
Section: Configuration Of Squid Rf Amplifiermentioning
confidence: 99%
“…In the high frequency range, the parasitic capacitance C p between the input coil and SQUID loop increases, and this makes the transfer of input flux into SQUID loop difficult. By placing the input coil inside the SQUID hole, the parasitic capacitance can be reduced much, but the multi-turn coil inside the SQUID hole reduces the mutual inductance with the SQUID loop, resulting in reduction of the amplifier gain [3,4].…”
Section: Configuration Of Squid Rf Amplifiermentioning
confidence: 99%
“…Exlernal RF pump influence on DC SauID I-V curve We studied experimentally the influence of external microwave irradiation at irequencies of i6, 26 and 75 GHz on I-V curves of integrated four-loop DC SQUIDS(Tarasov et al 1991).Figure 1shows typical curves for different values of magnetic flux caused by input coil current bias. I-V curves of DCSOUID with external irradiation at 16 GHz (a), 36 GHz (6) and 75 GHz (c).…”
mentioning
confidence: 99%
“…We studied experimentally the influence of external microwave irradiation at irequencies of i6, 26 and 75 GHz on I-V curves of integrated four-loop DC SQUIDS (Tarasov et al 1991). Figure 1 shows typical curves for different values of magnetic flux caused by input coil current bias.…”
mentioning
confidence: 99%