Difference between revisions of "Topdnp steady.m"

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{{DISPLAYTITLE:topdnp_steady.m}} __NOTOC__
 
{{DISPLAYTITLE:topdnp_steady.m}} __NOTOC__
 +
 
Time-optimised pulsed DNP experiment from: https://doi.org/10.1126/sciadv.aav6909 (a steady state version). Syntax (call from powder context): dnp=topdnp_steady(spin_system,parameters,H,R,K).
 
Time-optimised pulsed DNP experiment from: https://doi.org/10.1126/sciadv.aav6909 (a steady state version). Syntax (call from powder context): dnp=topdnp_steady(spin_system,parameters,H,R,K).
  
 
==Syntax==
 
==Syntax==
  
    dnp=topdnp_steady(spin_system,parameters,H,R,K)
+
dnp=topdnp_steady(spin_system,parameters,H,R,K)
  
 
==Arguments==
 
==Arguments==
  
        H - Hamiltonian matrix, received from
+
H - Hamiltonian matrix, received from
 
             context function
 
             context function
 
         R - relaxation superoperator, received
 
         R - relaxation superoperator, received
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==Outputs==
 
==Outputs==
  
        dnp                    - steady state observable on the de-
+
dnp                    - steady state observable on the de-
                                  tection state vector as a function
+
                              tection state vector as a function
                                  of microwave resonance offset
+
                              of microwave resonance offset
 +
 
 +
shebha-anandhi.jegadeesan@uni-konstanz.de
 +
ilya.kuprov@weizmann.ac.il
 +
guinevere.mathies@uni-konstanz.de
  
 
==Examples==
 
==Examples==
 +
 
See examples in the Spinach distribution relevant to this function.
 
See examples in the Spinach distribution relevant to this function.
  
 
==Notes==
 
==Notes==
 +
 
This page was generated from the function header in the Spinach repository.
 
This page was generated from the function header in the Spinach repository.
  
 
==See also==
 
==See also==
 +
 
* [[noveldnp.m]]
 
* [[noveldnp.m]]
 
* [[Built-in_experiments]]
 
* [[Built-in_experiments]]

Revision as of 15:06, 5 April 2026


Time-optimised pulsed DNP experiment from: https://doi.org/10.1126/sciadv.aav6909 (a steady state version). Syntax (call from powder context): dnp=topdnp_steady(spin_system,parameters,H,R,K).

Syntax

dnp=topdnp_steady(spin_system,parameters,H,R,K)

Arguments

H - Hamiltonian matrix, received from

            context function
        R - relaxation superoperator, received
            from context function, must be ther-
            malised to some finite temperature
        K - kinetics superoperator, received
            from context function
        parameters.irr_powers   - microwave amplitude (aka electron
                                  nutation frequency), Hz
        parameters.coil         - detection state vector
        parameters.pulse_dur    - pulse duration, seconds
        parameters.delay_dur    - delay duration, seconds
        parameters.nloops       - number of XiX/TPPM DNP blocks,
                                  must be an integer power of 2
        parameters.shot_spacing - delay between microwave irradiation
                                  periods, seconds
        parameters.addshift     - shift of the centre of the field
                                  profile, Hz
        parameters.el_offs      - microwave resonance offsets, a vector
                                  of frequencies in Hz

Outputs

dnp - steady state observable on the de-

                              tection state vector as a function
                              of microwave resonance offset
shebha-anandhi.jegadeesan@uni-konstanz.de
ilya.kuprov@weizmann.ac.il
guinevere.mathies@uni-konstanz.de

Examples

See examples in the Spinach distribution relevant to this function.

Notes

This page was generated from the function header in the Spinach repository.

See also


Version 2.11, authors: Shebha Anandhi Jegadeesan, Ilya Kuprov, Guinevere Mathies