Difference between revisions of "Overtone a.m"

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Overtone signal acquisition experiment inthe frequency domain. Syntax:
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Frequency domain overtone acquisition.
  
          spectrum=overtone_a(spin_system,parameters,H,R,K)
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==Syntax==
  
where H is the hamiltonian commutation superoperator, R is the relaxation
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    spectrum=overtone_a(spin_system,parameters,H,R,K)
superoperator and K is the chemical kinetics superoperator. The following
 
parameters are required:
 
  
    parameters.sweep          vector with two elements giving
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==Description==
                              the spectrum frequency extents
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The function performes frequency-domain acquisition at the overtone frequency. Because time-domain overtone spectroscopy is difficult (see http://dx.doi.org/10.1039/C4CP03994G for details, this mode of acquisition is preferable in practice).
                              in Hz around the overtone frequency
 
  
    parameters.npoints        number of points in the spectrum
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==Arguments==
  
    parameters.rho0           initial state
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    parameters.sweep        -  vector with two elements giving the spectrum frequency extents
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                                in Hz around the overtone frequency
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    parameters.npoints      -  number of points in the spectrum
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    parameters.rho0         -  initial state
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    parameters.coil        -  detection state
  
    parameters.coil            detection state
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    H                      -  Hamiltonian commutation superoperator
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    R                      -  unthermalised relaxation superoperator
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    K                      -  chemical kinetics superoperator
  
Relaxation must be present in the system dynamics, or the matrix
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==Returns==
inversion operation below would fail to converge. The relaxation
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The function returns the populations of the detection state at the frequencies specified.
matrix should *not* be thermalized.
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==Examples==
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==Notes==
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Relaxation must be present in the system dynamics, or the matrix inverse-times-vector operation performed by the frequency domain detection module would fail to converge. The relaxation superoperator should ''not'' be thermalised.
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==See also==
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[[overtone_cp.m]], [[overtone_dante.m]], [[overtone_hmqc.m]], [[overtone_pa.m]], [[slowpass.m]]
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''Revision 3284, authors: [[Ilya Kuprov]]''

Revision as of 16:51, 16 August 2016

Frequency domain overtone acquisition.

Syntax

    spectrum=overtone_a(spin_system,parameters,H,R,K)

Description

The function performes frequency-domain acquisition at the overtone frequency. Because time-domain overtone spectroscopy is difficult (see http://dx.doi.org/10.1039/C4CP03994G for details, this mode of acquisition is preferable in practice).

Arguments

    parameters.sweep        -  vector with two elements giving the spectrum frequency extents
                               in Hz around the overtone frequency

    parameters.npoints      -  number of points in the spectrum

    parameters.rho0         -  initial state

    parameters.coil         -  detection state
    H                       -  Hamiltonian commutation superoperator

    R                       -  unthermalised relaxation superoperator 

    K                       -  chemical kinetics superoperator

Returns

The function returns the populations of the detection state at the frequencies specified.

Examples

Notes

Relaxation must be present in the system dynamics, or the matrix inverse-times-vector operation performed by the frequency domain detection module would fail to converge. The relaxation superoperator should not be thermalised.

See also

overtone_cp.m, overtone_dante.m, overtone_hmqc.m, overtone_pa.m, slowpass.m


Revision 3284, authors: Ilya Kuprov