Difference between revisions of "Ct hsqc.m"

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     fid=ct_hsqc(spin_system,parameters,H,R,K)
 
     fid=ct_hsqc(spin_system,parameters,H,R,K)
  
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==Arguments==
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==Parameters==
  
 
     parameters.sweep              [F1 F2] sweep widths, Hz
 
     parameters.sweep              [F1 F2] sweep widths, Hz

Revision as of 18:48, 5 June 2026

Constant-time phase-sensitive HSQC pulse sequence.

Syntax

    fid=ct_hsqc(spin_system,parameters,H,R,K)

Parameters

    parameters.sweep              [F1 F2] sweep widths, Hz

    parameters.npoints            [F1 F2] numbers of points

    parameters.spins              {F1 F2} nuclei (e.g. '13C','1H')

    parameters.decouple_f2        nuclei to decouple in F2, e.g. 
                                  {'15N','13C'}

    parameters.decouple_f1        nuclei to decouple in F1, e.g. 
                                  {'1H','13C'}

    parameters.J                  working scalar coupling, Hz

    H  - Hamiltonian matrix, received from context function

    R  - relaxation superoperator, received from context function

    K  - kinetics superoperator, received from context function

Outputs

    fid.pos,fid.neg -  two components of the States quadrature 
                       signal.

Examples

Below is the output of examples/nmr_liquids/ct_hsqc_strychnine.m example file.

Ct hsqc strychnine.png

Notes

Natural abundance simulations should make use of the isotope dilution functionality. See dilute.m function.

See also

Liquid state NMR experiments

Version 2.5, authors: Matt Walker, Ilya Kuprov