2007 APS March Meeting
Volume 52, Number 1
Monday–Friday, March 5–9, 2007;
Denver, Colorado
Session V3: Detection & Applications of NMR and MRI at Microtesla Magnetic Fields
11:15 AM–2:15 PM,
Thursday, March 8, 2007
Colorado Convention Center
Room: Korbel 2A-3A
Sponsoring
Unit:
DCMP
Chair: John Clarke, University of California, Berkeley
Abstract ID: BAPS.2007.MAR.V3.2
Abstract: V3.00002 : Low Field Nuclear Magnetic Resonance (NMR) using SQUIDs
11:51 AM–12:27 PM
Preview Abstract
Abstract
Author:
Martin Burghoff
(Physikalisch-Technische Bundesanstalt)
Using a high resolution SQUID system in a magnetically highly
shielded room,
we measured the precession of 1H nuclei of liquid benzene,
distilled water,
and chloroform in magnetic fields around a microTesla. We found
that the NMR
lines of these liquids are in the range of a few hundred
milliHertz and
increase linearly with the detection field over a Larmor
frequency range of
two orders of magnitude. The slope is attributed to the
inhomogeneity of the
detection field and enables the extrapolation of the natural line
width to
zero magnetic field. For this limit, where any molecular motion
is fast with
respect to the Larmor frequency, the natural resonance line
widths of
benzene, chloroform and distilled water were determined to be 120
mHz, 150
mHz, and 170 mHz, respectively.
In low magnetic fields, chemical shift and homonuclear coupling
become
negligible. All that remains as a source of a spectral structure
is pure
J-coupling between nuclei of different gyromagnetic ratio. We
studied pure
J-coupling between methylene protons and fluorine nuclei of
trifluorethanol
and between methyl protons and phosphorus in trimethylphosphate
at detection
fields from 0.5 microTesla to 4 microTesla. This corresponds to a
variation
of d=J(H,F)/(f(H)-f(F)) from 8 to 1 and of d=J(H,P)/(f(H)-f(P))
from 0.8 to
0.08, respectively. At very low fields, i.e. at d=8, the spectra of
trifluorethanol exhibited only one single resonance line with an
irregular
structure. With increasing field, more and more individual lines
were
revealed. For trimethylphosphate, d=0.08 represents the
transition to the
weak coupling regime.
In addition, we employed a 304 SQUID vector magnetometer system
for the
recording of the magnetic field generated by water protons in two
adjacent
sample tubes precessing about a magnetic field of a microTesla.
From the
spatially resolved data, positions and moments of the samples were
calculated, yielding a reconstructed moving image of the two
precessing
magnetic dipoles.
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2007.MAR.V3.2