DocumentCode
1120610
Title
4C1 - Nonlinear effects in an NMR experiment
Author
Pommier, J. ; Benoit, H.
Author_Institution
Institut d́Electronique Fondamentale Lab. associé au C.N.R.S., des Sciences, Orsay, France
Volume
2
Issue
9
fYear
1966
fDate
9/1/1966 12:00:00 AM
Firstpage
388
Lastpage
390
Abstract
We have studied multiple-photon transition in a low-field nuclear magnetic resonance (NMR) experiment. It is well known that a saturation of the NMR occurs when using a sufficiently high alternating magnetic field which induces multiple-photons transitions. We show theoretically that these multiphoton transitions are accompanied by an harmonic generation. For a
-photon transition, this generation occurs mostly on the
th and (
)th harmonic. For an irradiating field
t of pulsation ω such that
where H0 is the steady field and θ is the angle between H0 and H1 the amplitudes
and
of these components are given by
,
. We have verified these equations in a low-field NMR experiment (
Gs/s), polarizing first a flowing liquid in a high magnetic field. The liquid then flows in a modified Bloch spectrometer. The receiving coil is still perpendicular to the steady field but it is possible to adjust the angle θ between the axis of the emission coils (H1 field) and the steady-field H0 . Using a synchronous detection at the output of the receiving coil on the pulsation
, or
, we have directly detected multiphoton transistions. The above equations have been verified for
to
. There are slight discrepancies at high excitation which may be explained taking into account a large saturation.
-photon transition, this generation occurs mostly on the
th and (
)th harmonic. For an irradiating field
t of pulsation ω such that
where H
and
of these components are given by
,
. We have verified these equations in a low-field NMR experiment (
Gs/s), polarizing first a flowing liquid in a high magnetic field. The liquid then flows in a modified Bloch spectrometer. The receiving coil is still perpendicular to the steady field but it is possible to adjust the angle θ between the axis of the emission coils (H
, or
, we have directly detected multiphoton transistions. The above equations have been verified for
to
. There are slight discrepancies at high excitation which may be explained taking into account a large saturation.Keywords
Angular velocity; Coils; Detectors; Electromagnetic wave polarization; Equations; Frequency conversion; Nuclear magnetic resonance; Resonant frequency; Transmitters; Water conservation;
fLanguage
English
Journal_Title
Quantum Electronics, IEEE Journal of
Publisher
ieee
ISSN
0018-9197
Type
jour
DOI
10.1109/JQE.1966.1074071
Filename
1074071
Link To Document