John Clarke - Berkeley CA, Nathan Kelso - Albany CA, SeungKyun Lee - Berkeley CA, Michael Moessle - Berkeley CA, Whittier Myers - Berkeley CA, Robert McDermott - Santa Barbara CA, Bernard Haken - Enschede, Alexander Pines - Berkeley CA, Andreas Trabesinger - Zurich,
Nuclear magnetic resonance (NMR) signals are detected in microtesla fields. Prepolarization in millitesla fields is followed by detection with an untuned dc superconducting quantum interference device (SQUID) magnetometer. Because the sensitivity of the SQUID is frequency independent, both signal-to-noise ratio (SNR) and spectral resolution are enhanced by detecting the NMR signal in extremely low magnetic fields, where the NMR lines become very narrow even for grossly inhomogeneous measurement fields. Additional signal to noise benefits are obtained by use of a low noise polarization coil, comprising litz wire or superconducting materials. MRI in ultralow magnetic field is based on the NMR at ultralow fields. Gradient magnetic fields are applied, and images are constructed from the detected NMR signals.