Increasing 14N NQR signal by 1H– 14N level crossing with small magnetic fields
NQR detection of materials, such as TNT, is hindered by the low signal-to-noise ratio at low NQR frequencies. Sweeping small (0–26 mT) magnetic fields to shift the 1H NMR frequency relative to the 14N NQR frequencies can provide a significant increase of the 14N NQR signal-to-noise ratio. Three effe...
Gespeichert in:
Veröffentlicht in: | Journal of magnetic resonance (1997) 2005-11, Vol.177 (1), p.118-128 |
---|---|
Hauptverfasser: | , , , , |
Format: | Artikel |
Sprache: | eng |
Schlagworte: | |
Online-Zugang: | Volltext |
Tags: |
Tag hinzufügen
Keine Tags, Fügen Sie den ersten Tag hinzu!
|
Zusammenfassung: | NQR detection of materials, such as TNT, is hindered by the low signal-to-noise ratio at low NQR frequencies. Sweeping small (0–26
mT) magnetic fields to shift the
1H NMR frequency relative to the
14N NQR frequencies can provide a significant increase of the
14N NQR signal-to-noise ratio. Three effects of
1H–
14N level crossing are demonstrated in diglycine hydrochloride and TNT. These effects are (1) transferring
1H polarization to one or more of the
14N transitions, including the use of an adiabatic flip of the
1H polarization during the field sweep, (2) shortening the effective
14N
T
1 by the interaction of
1H with the
14N transitions, (3) “level transfer” effect where the third
14N (spin 1) energy level or other
14N sites with different NQR frequency are used as a reservoir of polarization which is transferred to the measured
14N transition by the
1H. The
14N NQR signal-to-noise ratio can be increased by a factor of 2.5 for one
14N site in diglycine hydrochloride (and 2.2 in TNT), even though the maximum
1H frequency used in this work, 1116
kHz, is only 30% larger than the measured
14N frequencies (834
kHz for diglycine hydrochloride and 843
kHz for TNT). |
---|---|
ISSN: | 1090-7807 1096-0856 |
DOI: | 10.1016/j.jmr.2005.07.016 |