EasyManua.ls Logo

Bruker BioSpin Solid State NMR - Table 17.5. Values of |R-P| for Various Spins I and Orders P

Default Icon
328 pages
Print Icon
To Next Page IconTo Next Page
To Next Page IconTo Next Page
To Previous Page IconTo Previous Page
To Previous Page IconTo Previous Page
Loading...
226 (327) BRUKER BIOSPIN User Manual Version 002
Basic MQ-MAS
and D shift positions for two sites with large and small d
iso
and large and small
δ
qis
and with large and small
δ
iso
and small and large
δ
qis
are plotted, respectively.
This behavior is independent of the spin quantum number and of the order p of
the experiment. Higher quantum order experiments are possible for half integer
spin quantum numbers >3/2, however, corresponding pulse programs are not pro
-
vided in the pulse program library. They can easily be derived from the 3Q pulse
program by changing the phase cycle. In the 3-pulse sequence (mp3qzqf) e.g.
ph2 should be changed for the 5Q experiment to:
ph2 = 0 0 36 36 72 72 108 108 144 144 180 180 216 216 252 252 288 288
324 324
An 18° phase increment of the phase ph1 of the first pulse is required for States or
States-TPPI phase sensitive acquisition. For a full phase cycle a multiple of 20
scans must be used.
For the 4-pulse sequence (mp3qzfil) the phases should be changed to:
ph1 = 0 36 72 108 144 180 216 252 288 324
ph2 = 0*40 90*40 180*40 270*40
ph3 = 0
ph4 = 0*10 90*10 180*10 270*10
receiver = {0 180}*5 {90 270}*5 {180 0}*5 {270 90}*5 {180 0}*5 {270 90}*5{0
180}*5 {90 270}*5.
Again an 18° phase increment of the first pulse for States or States-TPPI phase
sensitive detection in F1 is needed. Thus a full phase cycle can be performed with
a multiple of 160 scans.
The usefulness of such a 5Q experiment is limited, and there are several draw-
backs: Firstly, the sensitivity is much inferior to the 3Q experiment because of the
lower transition probability and a less efficient excitation. Secondly, the shift range
(in ppm) in the indirect dimension is much smaller when a rotor synchronized ex
-
periment is performed. The factors R-p are listed in Table 17.5.. The shift posi-
tions in the MQ dimension in a sheared spectrum are the same for all orders p
and therefore, no additional information can be expected. However, the observed
line widths are slightly reduced in the higher order experiments so in special cas
-
es some enhancement of resolution can provide additional information.
The spectral width in the MQ dimension of the sheared spectrum is given by spin-
ning speed / R-p in a rotor synchronized experiment. A 5Q experiment e.g.
gives a 7.08/1.42 = 5 times smaller spectral range in the indirect dimension than a
3Q experiment.
Table 17.5. Values of |R-p| for Various Spins I and Orders p
Spin I R(p=3) |R-p| (p=±3) |R-p| (p=±5) |R-p| (p=±7) |R-p| (p=±9)
3/2 -7/9 3.78 - - -
5/2 19/12 1.42 7.08 - -
7/2 101/45 0.76 3.78 10.58 -
9/2 91/36 0.47 2.36 6.61 14.17

Table of Contents

Related product manuals