Zugriffsnummer 16263
Dokumenttyp Konferenzartikel in Zeitschrift
Sprache Englisch
Titel High-Tc and low-Tc dc SQUID electronics
Autor(in); Institution
Drung, Dietmar; 7.13, Kryosensorik, PTB-Berlin
Quelle/Jahr Superconductor Science and Technology: 16 (2003), 1320 - 1336
ISSN 0953-2048
URL
Verlag Bristol [u.a.]: IOPP
Konferenzangaben International Superconductive Electronics Conference 2003 ; (ISEC 2003), Sydney, 07-11, July, 2003, Australia
Freie Schlagworte SQUID ; flux-locked loop ; additional positive feedback ; relaxation oscillation SQUID ; digital SQUID ; bias reversal ; Smith predictor
Zusammenfassung Superconducting quantum interference devices (SQUIDs) are commonly operated in a flux-locked loop (FLL). The SQUID electronics amplifies the small SQUID signal to an acceptable level without adding noise, and it linearizes the transfer function of the SQUID in order to provide sufficient dynamic range. In this paper, the fundamentals of SQUID readout are reviewed including a discussion of preamplifier noise. The basic FLL concepts, direct readout and flux modulation readout, are discussed both with dc bias and bias reversal. Alternative readout concepts such as additional positive feedback (APF), two-stage SQUIDs, SQUID series arrays, relaxation oscillation SQUIDs and digital SQUIDs are briefly described. The FLL dynamics are discussed on the basis of a simple model with finite loop delay. It is shown that with optimized SQUID electronics a system bandwidth of ≈ 18 Mhz and a corresponding slew rate of ≈ 8 Φ sub.0 µs.sup-1. are possible. A novel FLL scheme insolving a Smith predictor is presented which allows one to increase the FLL bandwidth to about 100 MHz. The theoretical predictions are experimentally checked using a high-speed SQUID electronics prototype with a small-signal bandwidth of 300 MHz. Methods for increasing the dynamic range of SQUID systems are described: flux-quanta counting and dynamic field compensation (DFC). With DFC,the residual magnetic field at the SQUID can be kept close to zero even if the device ismoved in the Earth's field. Therefore, the noise level of a high-Tc magnetometer measured inside a magnetically shielded room (60 fT Hz -½ with a 1/f corner at 2 Hz) remained unchanged after moving the device in the magnetic field outside the room (60 µT dc plus 0.8 µT peak-to-peak power line interference).

Zitierung

Drung, D. (2003). High-Tc and low-Tc dc SQUID electronics. Superconductor Science and Technology, 16, 1320–1336.

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