Low-frequency Nuclear Quadrupole Resonance with Dc SQUID

Low-frequency Nuclear Quadrupole Resonance with Dc SQUID PDF Author: Jih-Wen Chang
Publisher:
ISBN:
Category :
Languages : en
Pages : 328

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Low-frequency Nuclear Quadrupole Resonance with Dc SQUID

Low-frequency Nuclear Quadrupole Resonance with Dc SQUID PDF Author: Jih-Wen Chang
Publisher:
ISBN:
Category :
Languages : en
Pages : 328

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Low-frequency Nuclear Quadrupole Resonance with a Dc SQUID.

Low-frequency Nuclear Quadrupole Resonance with a Dc SQUID. PDF Author:
Publisher:
ISBN:
Category :
Languages : en
Pages : 149

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Conventional pure nuclear quadrupole resonance (NQR) is a technique well suited for the study of very large quadrupolar interactions. Numerous nuclear magnetic resonance (NMR) techniques have been developed for the study of smaller quadrupolar interactions. However, there are many nuclei which have quadrupolar interactions of intermediate strength. Quadrupolar interactions in this region have traditionally been difficult or unfeasible to detect. This work describes the development and application of a SQUID NQR technique which is capable of measuring intermediate strength quadrupolar interactions, in the range of a few hundred kilohertz to several megahertz. In this technique, a dc SQUID (Superconducting QUantum Interference Device) is used to monitor the longitudinal sample magnetization, as opposed to the transverse magnetization, as a rf field is swept in frequency. This allows the detection of low-frequency nuclear quadrupole resonances over a very wide frequency range with high sensitivity. The theory of this NQR technique is discussed and a description of the dc SQUID system is given. In the following chapters, the spectrometer is discussed along with its application to the study of samples containing half-odd-integer spin quadrupolar nuclei, in particular boron-11 and aluminum-27. The feasibility of applying this NQR technique in the study of samples containing integer spin nuclei is discussed in the last chapter. 140 refs., 46 figs., 6 tabs.

DC Squids as Radio-frequency Amplifiers and Application to the Detection of Nuclear Quadrupole Resonance

DC Squids as Radio-frequency Amplifiers and Application to the Detection of Nuclear Quadrupole Resonance PDF Author: Claude Hilbert
Publisher:
ISBN:
Category :
Languages : en
Pages : 248

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Low Frequency Magnetic Resonance with a Dc SQUID

Low Frequency Magnetic Resonance with a Dc SQUID PDF Author: Chuck Connor
Publisher:
ISBN:
Category :
Languages : en
Pages : 290

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Low-frequency NMR and NQR with a Dc SQUID Amplifier

Low-frequency NMR and NQR with a Dc SQUID Amplifier PDF Author: Nong-Qiang Fan
Publisher:
ISBN:
Category :
Languages : en
Pages : 214

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I. Low-frequency NMR and NQR Using a Dc SQUID

I. Low-frequency NMR and NQR Using a Dc SQUID PDF Author: Marcia Ann Ziegeweid
Publisher:
ISBN:
Category :
Languages : en
Pages : 280

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Application of a Dc SQUID to Rf Amplification

Application of a Dc SQUID to Rf Amplification PDF Author:
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Category :
Languages : en
Pages :

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Superconducting QUantum Interference Devices (SQUIDs) have been used for more than a decade for the detection of magnetic resonance. Until recently, these devices had mostly been confined to operation in the audiofrequency range, so that experiments have been restricted to measurements of resonance at low frequencies, or of changes in the static susceptibility of a sample induced by rf irradiation at the resonant frequency. However, the recent extension of the operating range of low noise dc SQUIDs to radiofrequencies (rf) allows one to detect magnetic resonance directly at frequencies up to several hundred megahertz. In this paper, we begin by summarizing the properties of dc SQUIDs as tuned rf amplifers. We then describe first, the development of a SQUID system for the detection of pulsed nuclear quadrupole resonance (NQR) at about 30 MHz and second, a novel technique for observing magnetic resonances in the absence of any externally applied rf fields.

DC SQUID Spectrometers for Nuclear Electric Quadrupole and Low Field Nuclear Magnetic Resonance Spectroscopy

DC SQUID Spectrometers for Nuclear Electric Quadrupole and Low Field Nuclear Magnetic Resonance Spectroscopy PDF Author: Dinh Minh That Ton
Publisher:
ISBN:
Category :
Languages : en
Pages : 256

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Nuclear Magnetic Resonance with Dc SQUID (Super-conducting QUantum Interference Device) Preamplifiers

Nuclear Magnetic Resonance with Dc SQUID (Super-conducting QUantum Interference Device) Preamplifiers PDF Author:
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Category :
Languages : en
Pages :

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Sensitive radio-frequency (rf) amplifiers based on dc Superconducting QUantum Interface Devices (SQUIDS) are available for frequencies up to 200 MHz. At 4.2 K, the gain and noise temperature of a typical tuned amplifier are 18.6 +- 0.5 dB and 1.7 +- 0.5 K at 93 MHz. These amplifiers are being applied to a series of novel experiments on nuclear magnetic resonance (NMR) and nuclear quadrupole resonance (NQR). The high sensitivity of these amplifiers was demonstrated in the observation of ''nuclear spin noise'', the emission of photons by 35Cl nuclei in a state of zero polarization. In the more conventional experiments in which one applies a large rf pulse to the spins, a Q-spoiler, consisting of a series array of Josephson junctions, is used to reduce the Q of the input circuit to a very low value during the pulse. The Q-spoiler enables the circuit to recover quickly after the pulse, and has been used in an NQR experiment to achieve a sensitivity of about 2 x 1016 nuclear Bohr magnetons in a single free precession signal with a bandwidth of 10 kHz. In a third experiment, a sample containing 35Cl nuclei was placed in a capacitor and the signal detected electrically using a tuned SQUID amplifier and Q-spoiler. In this way, the electrical polarization induced by the precessing Cl nuclear quadrupole moments was detected: this is the inverse of the Stark effect in NQR. Two experiments involving NMR have been carried out. In the first, the 30 MHz resonance in 119Sn nuclei is detected with a tuned amplifier and Q-spoiler, and a single pulse resolution of 1018 nuclear Bohr magnetons in a bandwidth of 25 kHz has been achieved. For the second, a low frequency NMR system has been developed that uses an untuned input circuit coupled to the SQUID. The resonance in 195Pt nuclei has been observed at 55 kHz in a field of 60 gauss. 23 refs., 11 figs.

The New Superconducting Electronics

The New Superconducting Electronics PDF Author: H. Weinstock
Publisher: Springer Science & Business Media
ISBN: 940111918X
Category : Technology & Engineering
Languages : en
Pages : 460

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This volume is based on the proceedings of the NATO-sponsored Advanced Studies Institute (ASn on The New Superconducting Electronics (held 9-20 August 1992 in Waterville Valley, New Hampshire USA). The contents herein are intended to provide an update to an earlier volume on the same subject (based on a NATO ASI held in 1988). Four years seems a relatively short time interval, and our title itself, featuring The New Superconducting Electronics, may appear somewhat pretentious. Nevertheless, we feel strongly that the ASI fostered a timely reexamination of the technical progress and application potential of this rapid-paced field. There are, indeed, many new avenues for technological innovation which were not envisioned or considered possible four years ago. The greatest advances by far have occurred with regard to oxide superconductors, the so-called high transition-temperature superconductors, known in short as HTS. These advances are mainly in the ability to fabricate both (1) high-quality, relatively large-area films for microwave filters and (2) multilayer device structures, principally superconducting-normal-superconducting (SNS) Josephson junctions, for superconducting-quantum-interference-device (SQUID) magnetometers. Additionally, we have seen the invention and development of the flux-flow transistor, a planar three-terminal device. During the earlier ASI only the very first HTS films with adequate critical-current density had just been fabricated, and these were of limited area and had high resistance for microwave current.