Transmission line probe for nmr

Abstract

A probe for an NMR device is disclosed in which a saddle coil is disposed on one side of a flexible insulating material, and an additional conductor is disposed on the opposite side. The additional conductor and the conductors of the saddle coil create a capacitance across the insulating material. This capacitance acts with the inductance of the saddle coil such that the probe itself forms a transmission line. The probe is thus inherently broadband and requires no tuning. It also presents a constant impedance, thus facilitating impedance matching to an NMR spectrometer. In a preferred embodiment, a chip resistor is disposed on the flexible insulating material, terminating the transmission line.

Description

STATEMENT REGARDING FEDERALLY SPONSORED RESEARCH[0001]The U.S. Government has a paid-up license in this invention and the right in limited circumstances to require the patent owner to license others on reasonable terms as provided for by the terms of PHY-0457039 awarded by the National Science Foundation.DESCRIPTION OF ATTACHED APPENDIX[0002]Not ApplicableBACKGROUND OF THE INVENTION[0003]1. Field of Invention[0004]The present invention relates generally to the field of nuclear magnetic resonance (NMR), and more specifically to an NMR probe wherein the probe itself constitutes a transmission line.[0005]2. Prior Art[0006]The nuclear magnetic resonance phenomenon occurs in atomic nuclei having an odd number of protons or neutrons. Due to the spin of the protons and neutrons, each such nucleus exhibits a magnetic moment, such that, when a sample composed of such nuclei is placed in a static, homogeneous magnetic field, B0, a greater number of nuclear magnetic moments align with the fiel...

AI Technical Summary

Problems solved by technology

This limits the range of magnetic fields and/or nuclear species to which a conventional probe is sensitive without changing the frequency to which the resonant circuit is tuned.

In many applications of NMR this bandwidth limitation poses substantial difficulties.

It is particularly problematic in studies where it is desirable to vary the B0 field over a wide range of magnitudes, in studies of quadrupolar nuclei (which contain very broad resonances), in studies of multiple nuclear species, or whenever physical access to the tuning elements of the probe is limited.

It will be thus further apparent that the limitation in bandwidth is related to the presence of a resonant circuit.

This is often a time consu

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