Abstract:
The nuclear magnetic shieldings of Si, Ge, and Sn in MH4−nYn (M = Si, Ge, Sn; Y = F, Cl, Br, I and n = 1–4) molecular systems are highly influenced by the substitution of one or more hydrogens by heavy-halogen atoms. We applied the linear response elimination of small components (LRESC) formalism to calculate those shieldings and learn whether including only a few of the leading relativistic correction terms is sufficient to be able to quantitatively reproduce the full relativistic value. It was observed that the nuclear magnetic shieldings change as the number of heavy halogen substituents and their weights vary, and the pattern of σ(M) generally does not exhibit the normal halogen dependence (NHD) behavior that can be seen in similar molecular systems containing carbon atoms. We also analyzed each relativistic correction afforded by the LRESC method and split them in two: core-dependent and ligand-dependent contributions; we then looked for the electronic mechanisms involved in the different relativistic effects and in the total relativistic value. Based on this analysis, we were able to study the electronic mechanism involved in a recently proposed relativistic effect, the “heavy atom effect on vicinal heavy atom” (HAVHA), in more detail. We found that the main electronic mechanism is the spin–orbit or σp T(3) correction, although other corrections such as σp S(1) and σp S(3) are also important. Finally, we analyzed proton magnetic shieldings and found that, for molecules containing Sn as the central atom, σ(H) decreases as the number of heavy halogen substituents (of the same type: either F, Cl, or Br) increases, albeit at different rates for different halogens. σ(H) only increase as the number of halogen substituents increases if the halogen is iodine. © 2014, Springer-Verlag Berlin Heidelberg.
Registro:
Documento: |
Artículo
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Título: | Core-dependent and ligand-dependent relativistic corrections to the nuclear magnetic shieldings in MH4−nYn (n = 0–4; M = Si, Ge, Sn, and Y = H, F, Cl, Br, I) model compounds |
Autor: | Maldonado, A.F.; Aucar, G.A.; Melo, J.I. |
Filiación: | Physics Department, Natural and Exact Science Faculty, Northeastern University of Argentina, Corrientes, Argentina Institute of Modelling and Innovation on Technology, IMIT, Corrientes, Argentina Dpto. Fisica, Facultad de Ciencias Exactas y Naturales, Univ. Buenos Aires and IFIBA-Conicet, Buenos Aires, Argentina
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Palabras clave: | LRESC; NMR; Polarization propagators; Relativistic effects; germanium; halogen; hydrogen; iodine; lead; ligand; proton; silicon; tin; Article; atom; electron; excitation; magnetic field; magnetism; nuclear magnetic resonance spectroscopy; polarization; proton nuclear magnetic resonance |
Año: | 2014
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Volumen: | 20
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Número: | 9
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DOI: |
http://dx.doi.org/10.1007/s00894-014-2417-z |
Título revista: | Journal of Molecular Modeling
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Título revista abreviado: | J. Mol. Model.
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ISSN: | 16102940
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CODEN: | JMMOF
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CAS: | germanium, 7440-56-4; hydrogen, 12385-13-6, 1333-74-0; iodine, 7553-56-2; lead, 7439-92-1, 13966-28-4; proton, 12408-02-5, 12586-59-3; silicon, 7440-21-3; tin, 14314-35-3, 7440-31-5
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Registro: | https://bibliotecadigital.exactas.uba.ar/collection/paper/document/paper_16102940_v20_n9_p_Maldonado |
Referencias:
- Edlund, U., Lejon, T., Pyykkö, P., Venkatachalam, T.K., Buncel, E., (1987) J Am Chem Soc, 109, p. 5982. , COI: 1:CAS:528:DyaL2sXltlCgu7o%3D
- Pyykkö, P., Görling, A., Rösch, N., (1987) Mol Phys, 61, p. 195
- Kaupp, M., Malkina, O.L., Malkin, V.G., Pyykkö, P., (1998) Chem Eur J, 4, p. 118. , COI: 1:CAS:528:DyaK1cXmtlCmtg%3D%3D
- Melo, J.I., Ruiz deAzúa, M.C., Giribet, C.G., Aucar, G.A., Provasi, P.F., (2004) J Chem Phys, 121, p. 6798. , COI: 1:CAS:528:DC%2BD2cXotVKmsb8%3D
- Kaupp, M., Schwerdtfeger, P., Relativistic effects on NMR chemical shifts (Chapter 9) (2004) Relativistic electronic structure theory, part 2: Applications, 2, pp. 552-597. , Elsevier, Amsterdam:
- Lantto, P., Romero, R.H., Gomez, S.S., Aucar, G.A., Vaara, J., (2006) J Chem Phys, 125, p. 184113
- Vaara, J., (2007) Phys Chem Chem Phys, 9, p. 5399. , COI: 1:CAS:528:DC%2BD2sXhtFCgsr7L
- Maldonado, A.F., Aucar, G.A., (2009) Phys Chem Chem Phys, 11, p. 5615. , COI: 1:CAS:528:DC%2BD1MXotFWmsLk%3D
- Autschbach, J., Zheng, S., (2009) Annu Rep NMR Spectrosc, 67, p. 1. , COI: 1:CAS:528:DC%2BD1MXhsFaru7fP
- Kantola, A.M., Lantto, P., Vaara, J., Jokisaari, J., (2010) Phys Chem Chem Phys, 12, p. 2679. , COI: 1:CAS:528:DC%2BC3cXislWktr8%3D
- Arcisauskaite, V., Melo, J.I., Hemmingsen, L., Sauer, S.P.A., (2011) J Chem Phys, 135, p. 044306
- Roukala, J., Maldonado, A.F., Vaara, J., Aucar, G.A., Lantto, P., (2011) Phys Chem Chem Phys, 13, p. 21016. , COI: 1:CAS:528:DC%2BC3MXhsFaiurfN
- Melo, J.I., Maldonado, A.F., Aucar, G.A., (2012) J Chem Phys, 137, p. 214319
- Melo, J.I., Maldonado, A.F., Aucar, G.A., (2011) Theor Chem Accounts, 129, p. 483. , COI: 1:CAS:528:DC%2BC3MXmtVGktbs%3D
- Melo, J.I., Ruiz deAzúa, M.C., Giribet, C.G., Aucar, G.A., Romero, R.H., (2003) J Chem Phys, 118, p. 471. , COI: 1:CAS:528:DC%2BD38XpvVejurY%3D
- Manninen, P., Lantto, P., Vaara, J., Ruud, K., (2003) J Chem Phys, 119, p. 2623. , COI: 1:CAS:528:DC%2BD3sXlsFKgtr8%3D
- Manninen, P., Ruud, K., Lantto, P., Vaara, J., (2005) J Chem Phys, 122, p. 114107
- Rodriguez-Fortez, A., Alemany, P., Ziegler, T., (1999) J Phys Chem A, 103, p. 8288
- Maldonado, A.F., Aucar, G.A., (2014) J Phys Chem A
- Gomez, S.S., Maldonado, A.F., Aucar, G.A., (2005) J Chem Phys, 123, p. 214108
- Visscher, L., Enevoldsen, T., Saue, T., Jensen, H.J.A., Oddershede, J., (1999) J Comput Chem, 20, p. 1262. , COI: 1:CAS:528:DyaK1MXlt1GhsL0%3D
- Jameson, C.J., (1998) Multinuclear NMR, , Plenum, New York:
- Kaupp, M., Kaupp, M., Bühl, M., Malkin, V.G., Interpretation of NMR chemical shifts (Chapter 18) (2004) Calculation of NMR and EPR parameters: theory and applications, pp. 293-306. , Wiley-VCH, Weinheim:
- Fukawa, S., Hada, M., Fukuda, R., Tanaka, S., Nakatsuji, H., (2001) J Comput Chem, 22, p. 528. , COI: 1:CAS:528:DC%2BD3MXisVSnur8%3D
- Aucar, G.A., Romero, R.H., Maldonado, A.F., (2010) Int Rev Phys Chem, 29, p. 1. , COI: 1:CAS:528:DC%2BC3cXjt1yhu78%3D
- Saue, T., Visscher, L., Bast, R., Jensen, H.J.A., Dyall, K.G., Ekstrom, U., Eliav, E., Yamamoto, S., (2010) DIRAC10, , http://dirac.chem.sdu.dk, University of Southern Denmark, Odense:
- Kagakkai, N.B., (1984) Kagaku benran, , 3rd edn. Maruzen, Tokyo
- Sadlej, A.J., (1991) Theor Chim Acta, 79, p. 123. , COI: 1:CAS:528:DyaK3MXktlGrurs%3D
- Maldonado, A.F., Gimenez, C.A., Aucar, G.A., (2012) Chem Phys, 395, p. 75. , COI: 1:CAS:528:DC%2BC38XitF2ksLk%3D
- Maldonado, A.F., Gimenez, C.A., Aucar, G.A., (2012) J Chem Phys, 136, p. 224110
- Aidas, K., Angeli, C., Bak, K.L., Bakken, V., Bast, R., Boman, L., Christiansen, O., Ågren, H., The Dalton quantum chemistry program system (2013) WIREs Comput Mol Sci, 4, pp. 269-284
- Kaneko, H., Hada, M., Nakajima, T., Nakatsuji, H., (1996) Chem Phys Lett, 261, p. 1. , COI: 1:CAS:528:DyaK28XlvFKnsbw%3D
Citas:
---------- APA ----------
Maldonado, A.F., Aucar, G.A. & Melo, J.I.
(2014)
. Core-dependent and ligand-dependent relativistic corrections to the nuclear magnetic shieldings in MH4−nYn (n = 0–4; M = Si, Ge, Sn, and Y = H, F, Cl, Br, I) model compounds. Journal of Molecular Modeling, 20(9).
http://dx.doi.org/10.1007/s00894-014-2417-z---------- CHICAGO ----------
Maldonado, A.F., Aucar, G.A., Melo, J.I.
"Core-dependent and ligand-dependent relativistic corrections to the nuclear magnetic shieldings in MH4−nYn (n = 0–4; M = Si, Ge, Sn, and Y = H, F, Cl, Br, I) model compounds"
. Journal of Molecular Modeling 20, no. 9
(2014).
http://dx.doi.org/10.1007/s00894-014-2417-z---------- MLA ----------
Maldonado, A.F., Aucar, G.A., Melo, J.I.
"Core-dependent and ligand-dependent relativistic corrections to the nuclear magnetic shieldings in MH4−nYn (n = 0–4; M = Si, Ge, Sn, and Y = H, F, Cl, Br, I) model compounds"
. Journal of Molecular Modeling, vol. 20, no. 9, 2014.
http://dx.doi.org/10.1007/s00894-014-2417-z---------- VANCOUVER ----------
Maldonado, A.F., Aucar, G.A., Melo, J.I. Core-dependent and ligand-dependent relativistic corrections to the nuclear magnetic shieldings in MH4−nYn (n = 0–4; M = Si, Ge, Sn, and Y = H, F, Cl, Br, I) model compounds. J. Mol. Model. 2014;20(9).
http://dx.doi.org/10.1007/s00894-014-2417-z