NMRCOUPLING subkeys

The available switches within a NMRCOUPLING/END block control the computation of the NSSCCs. By default, the program will evaluate the FC coupling contribution for the first nucleus being the perturbing nucleus and all remaining nuclei responding.

Please note that the ordering of atoms in CPL is generally different from the ADF input. The ordering of atoms is the one being stored in TAPE21 and it is grouped by fragment types. In case you are in doubt about the ordering of atoms, you can run CPL for a few seconds. It will print a list of atoms with their coordinates. The ordering is currently the same as required the NMR program in the ADF program system. On the other hand, note that for the subkeys ATOMPERT and ATOMRESP the number of the atoms refer to the input ordering in the ADF calculation.

Available subkeys are:

NMRCOUPLING
 NUCLEI {npert nresp1 nresp2}
 ATOMPERT {npert1 npert2 npert3}
 ATOMRESP {nresp1 nresp2 nresp3}
 GAMMA {nnuc gamma}
 DSO
 PSO
 SD
 FC
 SCF {ITERATIONS=25 | NOCYCLE | CONVERGE=1e-4 }
 XALPHA
 CONTRIBUTIONS {1E19} {LMO, SFO, LMO2, SFO2}
END

NUCLEI {npert nresp1 nresp2}
Use nucleus no. npert as the perturbing nucleus, and nuclei nresp1, nresp2, etc as responding nuclei. You can supply more than one NUCLEI keys, in which case CPL evaluates the first-order MOs for each perturbing nucleus that is specified and computes the NSSCCs between all specified responding nuclei. For each NUCLEI line in the input, CPL has to perform an SCF cycle. Note: for the numbers of the atoms the internal CPL numbering should be used.

ATOMPERT {npert1 npert2 npert3}
ATOMRESP {nresp1 nresp2 nresp3}
ATOMPERT: use nucleus no. npert1, npert2, etc. as the perturbing nuclei. ATOMRESP: use nucleus no. nresp1, nresp2, etc. as the perturbing nuclei. You can supply more than one ATOMPERT and (or) ATOMRESP key. CPL computes the NSSCCs for all pairs of combinations of perturbing atoms and responding atoms. For each perturbing atom CPL has to perform an SCF cycle, which is the expensive part in the calculation. Note: the numbers refer to the input ordering in the ADF calculation. Use the subkey NUCLEI to specify the nuclei according to the internal CPL numbers of the atoms.

GAMMA {nnuc gamma}
Input a non-default magneto-gyric ratio of g = gamma for nucleus no. nnuc, in units of rad/(T s). Note that one should include the the typical 107 factor. CPL normally uses the g value of the most abundant NMR active isotope for a nucleus of a given charge by default. With the GAMMA keyword you can override this value or supply a value if CPL does not know about it. A list of g's that is used in the computation is printed in the output. You have to provide the GAMMA key for each nucleus you want to specify.

DSO
Compute the diamagnetic orbital term for each NSSCC that is requested (not default)

PSO
Compute the paramagnetic orbital term for each NSSCC (not default)

SD
Compute the SD term for each NSSCC. This is only default for spin-orbit ADF runs. The output will contain the sum of the FC and SD contributions. Please note that requesting this option results in a greatly increased computational cost in scalar or non-relativistic runs. The option NOSD will turn the SD computation off in spin-orbit runs and has no effect otherwise.

FC
Compute the FC contribution to the NSSCCs. This is the default option. Please note that it is currently not possible to compute the SD term without the FC term. Consult the 'practical aspects' section for instructions how to estimate the FC/SD cross term. The option NOFC will disable both the FC and SD computation.

SCF options
Settings related to the SCF cycle that is carried out by CPL. Valid options are (with default values if applicable):

ITERATIONS 25
maximum number of iterations
NOCYCLE
perform no cycle, equivalent to ITERATIONS 0
CONVERGE 1e-4
convergence criterion, an input of e corresponds approximately to a convergence of log(-e) digits, i.e. the results will be converged to about four significant digits by default. The measurement for the convergence is based on the sum S of the magnitudes of all occupied-virtual matrix elements of the induced first-order exchange potential. Note that the actual convergence criterion being used in the computation is e times S of the first cycle, i.e. the convergence criterion is set relative to the initial value of S.

XALPHA
Use first-order Xalpha potential instead of VWN potential. This will usually decrease the accuracy for couplings involving hydrogen, and does not have a large effect for couplings between heavier nuclei (not default). The key is mainly intended to ensure compatibility with our previously published results.

CONTRIBUTIONS {1e19} {LMO, SFO, LMO2, SFO2}
Print contributions from individual orbitals to the FC and OP term of the NSSCCs that are larger in magnitude than a certain threshold. The threshold refers to the reduced coupling constant K in SI units (not default). Additionally, an analysis in terms of Boys localized MOs (see User's Guide and SFOs. At present, either each key LMO, SFO, LMO2, SFO2 can be used individually, or grouped as {LMO, SFO2} or {SFO2, LMO}. If you need all analyses or different combinations, it is recommended to restart the CPL calculation from TAPE13, and to specify 0 iterations in the SCF. This way, the only additional computational cost should be the analysis itself.

The equation and an application for the analyses due to the LMO and SFO keys is described in the papers Autschbach, J.; Igna, C. D.; Ziegler, T., A theoretical investigation of the apparently irregular behavior of Pt-Pt spin-spin coupling constants. J. Am. Chem. Soc. 2003, 125, 1028-1032, and Guennic, B. L.; Matsumoto, K.; Autschbach, J., On the NMR properties of platinum thallium bonded complexes: Analysis of relativistic density functional theory results. Magn. Res. Chem. 2004, 42, S99-S116. The other analysis is based on the same equation as in Khandogin, J.; Ziegler, T., A density functional study of nuclear magnetic resonance spin-spin coupling constants in transition metal systems. Spectrochim. Acta 1999, A 55, 607-624.

In order for the LMO-based analyses to work, the MO -> LMO transformation matrix needs to be stored on TAPE21. In the ADF input, you can achieve this with the option "STORE" to the LOCORB key, i.e.

LOCORB STORE
 ... options
END

 

Copyright      Terms of Use      Privacy Policy
Search:
Home
About
News
Sitemap
Contact
Why ADF?
Brochure
Demos
Trial Version
How to buy
Downloads
FAQ
Newsletters
Documentation
Community