Difference between revisions of "Noesyhsqc.m"
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| − | Phase-sensitive NOESY-HSQC sequence | + | {{DISPLAYTITLE:noesyhsqc.m}} __NOTOC__ |
| + | Phase-sensitive NOESY-HSQC sequence described in: | ||
| − | + | https://doi.org/10.1021/bi00441a004 | |
| + | |||
| + | https://doi.org/10.1016/0022-2364(90)90227-Z | ||
| + | |||
| + | https://doi.org/10.1002/9780470034590.emrstm0563 | ||
| + | |||
| + | https://doi.org/10.1016/j.jmr.2014.04.002 | ||
| − | using the bidirectional propagation method described in | + | using the bidirectional propagation method described in the last of these references. The sequence is hard-wired to {F1,F2,F3}={1H,15N,1H} with carbon decoupled throughout. |
| − | + | ==Syntax== | |
| − | + | fid=noesyhsqc(spin_system,parameters,H,R,K) | |
| − | + | ==Parameters== | |
| − | + | parameters.npoints - a vector of three integers giving the | |
| − | relaxation superoperator | + | number of points in the three temporal |
| − | + | dimensions, ordered as [t1 t2 t3]. | |
| + | |||
| + | parameters.sweep - a vector of three real numbers giving | ||
| + | the sweep widths in the three frequen- | ||
| + | cy dimensions, ordered as [f1 f2 f3]. | ||
| + | |||
| + | parameters.J - J-coupling for the HSQC stage magneti- | ||
| + | sation transfer, Hz. | ||
| + | |||
| + | parameters.tmix - NOESY stage mixing time, seconds. | ||
| + | |||
| + | H - Hamiltonian matrix, received from context function | ||
| + | |||
| + | R - relaxation superoperator, received from context function | ||
| + | |||
| + | K - kinetics superoperator, received from context function | ||
| − | + | ==Outputs== | |
| − | that are used in the | + | fid - a structure with four fields: fid.pos_pos, fid.pos_neg, |
| − | + | fid.neg_pos, fid.neg_neg that are used in the subsequ- | |
| + | ent States quadrature processing | ||
| − | + | ==Examples== | |
| − | + | An example NOESY-HSQC simulation for ubiquitin may be found in examples/nmr_proteins/noesyhsqc_ubiquitin_theo.m file; the output appears below. | |
| − | |||
| − | + | [[File:noesyhsqc.png]] | |
| − | |||
| − | |||
| − | + | ==Notes== | |
| − | + | The sequence starts with a pure Lz on protons at the moment and assumes that the relaxation superoperator is not thermalised - the relaxation destination is the zero state. | |
| − | + | The first citation is the NOESY-HMQC precursor to this NOESY-HSQC implementation. | |
| − | + | ==See also== | |
| − | + | [[noesy.m]], [[hsqc.m]], [[hnco.m]], [[protein.m]], [[nuclacid.m]], [[hcanh.m]], [[hcch_cosy.m]], [[hnca.m]], [[hncaco.m]], [[hncoca.m]], [[Built-in_experiments]] | |
| + | |||
| + | ''Version 2.4, authors: [[Luke Edwards]], [[Ilya Kuprov]]'' | ||
Latest revision as of 10:11, 30 August 2026
Phase-sensitive NOESY-HSQC sequence described in:
https://doi.org/10.1021/bi00441a004 https://doi.org/10.1016/0022-2364(90)90227-Z https://doi.org/10.1002/9780470034590.emrstm0563 https://doi.org/10.1016/j.jmr.2014.04.002
using the bidirectional propagation method described in the last of these references. The sequence is hard-wired to {F1,F2,F3}={1H,15N,1H} with carbon decoupled throughout.
Syntax
fid=noesyhsqc(spin_system,parameters,H,R,K)
Parameters
parameters.npoints - a vector of three integers giving the
number of points in the three temporal
dimensions, ordered as [t1 t2 t3].
parameters.sweep - a vector of three real numbers giving
the sweep widths in the three frequen-
cy dimensions, ordered as [f1 f2 f3].
parameters.J - J-coupling for the HSQC stage magneti-
sation transfer, Hz.
parameters.tmix - NOESY stage mixing time, seconds.
H - Hamiltonian matrix, received from context function
R - relaxation superoperator, received from context function
K - kinetics superoperator, received from context function
Outputs
fid - a structure with four fields: fid.pos_pos, fid.pos_neg,
fid.neg_pos, fid.neg_neg that are used in the subsequ-
ent States quadrature processing
Examples
An example NOESY-HSQC simulation for ubiquitin may be found in examples/nmr_proteins/noesyhsqc_ubiquitin_theo.m file; the output appears below.
Notes
The sequence starts with a pure Lz on protons at the moment and assumes that the relaxation superoperator is not thermalised - the relaxation destination is the zero state.
The first citation is the NOESY-HMQC precursor to this NOESY-HSQC implementation.
See also
noesy.m, hsqc.m, hnco.m, protein.m, nuclacid.m, hcanh.m, hcch_cosy.m, hnca.m, hncaco.m, hncoca.m, Built-in_experiments
Version 2.4, authors: Luke Edwards, Ilya Kuprov
