Hi,
I'm currently using simulation to study magnetisation transfer. I've been using SIMPSON but for a system of 6 spins (3x13C, 1x15N and 2x1H) my laptop simply could not compute, so I thought I would try to transfer to SPINEVOLUTION for bigger spin system. It's quite a simple pulse sequence, but in SPINEV the FID pattern appeared to be 2Dish. I feel like I'm missing something. Here is the SIMPSON pulse program for just 2 channels:
reset
for {set i 0} {$i < 3} {incr i} {
set phase [expr $i*360.0/3.0]
pulse $t90 $pwr $phase 0 0
pulse [expr 4.0*$t90] $pwr [expr $phase+180.0] 0 0
pulse [expr 3.0*$t90] $pwr $phase 0 0
}
store 1
reset
pulseid $th $par(rf) 0 $par(rf) 90
store 2
for {set j 0} {$j < $par(np)} {incr j} {
reset
prop 1 $j
prop 2
prop 1 $j
acq
}
Here is my interpretation of it in SPINEVOLUTION:
CHN 1
timing(usec) (2.5 10 7.5 2.5 10 7.5 2.5 10 7 .5)40D1B (0.5)1D1A (2.5 10 7.5 2.5 10 7.5 2.5 10 7.5)40D1B
power(kHz) 100 100 100 100 100 100 100 100 100 500 100 100 100 100 100 100 100 100 100
phase(deg) 0 180 0 120 300 120 240 60 240 0 0 180 0 120 300 120 240 60 240
freq_offs(kHz) 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0
CHN 2
timing(usec) (60) (0.5) (60)
power(kHz) 0 500 0
phase(deg) 0 90 0
freq_offs(kHz) 0 0 0
From what I understand of it, the spinevolution pulse sequence should be
A
BAB
BBABB
BBBABBB
...
like stated in SIMPSON. but I this surely wouldn't give an oscillating FID.
The initial magnetisation is in channel one and we observe nuclei in channel two. If someone could have a look and tell me what I've been missing much would be appreciated. I've been using SPINEV for years but only for very minor applications such as echo, angles. This pulse should be similar to REDOR and somehow I just couldn't quite figure out what is wrong. I'm sure there is something very simple explanation...
Thanks for all your help.
Regards,
Vivien