By producing a train of absorption or dispersion signals (continuous‐wave magnetic resonance) or free induction decays (pulsed magnetic resonance) it is possible to save time in spin‐lattice relaxation measurements due to the fact that it is not necessary to wait for equilibrium magnetization before initiating the train. The relaxation time may be calculated from the train according to a simple rapidly converging iteration.

Topics
Nuclear magnetic resonance
1.
D. C.
Look
 and
D. R.
Locker
,
Phys. Rev. Lett.
20
,
987
(
1968
).
Google Scholar
Crossref
Search ADS
 
2.
W. C.
Smith
 and
D. R.
Torgeson
,
Rev. Sci. Instrum.
40
,
583
(
1969
).
Google Scholar
Crossref
Search ADS
 
3.
D. R.
Locker
 and
D. C.
Look
,
J. Appl. Phys.
39
,
6119
(
1968
).
Google Scholar
Crossref
Search ADS
 
4.
D. C.
Look
 and
D. R.
Locker
,
J. Chem. Phys.
50
,
2269
(
1969
).
Google Scholar
Crossref
Search ADS
 
5.
M.
Santini
,
Nuovo Cimento
16
,
232
(
1960
).
Google Scholar
Crossref
Search ADS
 
6.
Interested persons may obtain the computer program (FORTRAN IV, XTRAN, or CAL) from the authors.
This content is only available via PDF.
© 1970 The American Institute of Physics.
1970
The American Institute of Physics
You do not currently have access to this content.