Performance of GESC and LRESC models for heavy-atom nuclear magnetic shieldings
- Autores
- Zapata Escobar, Andy Danian; Melo, Juan Ignacio; Aucar, Gustavo Adolfo
- Año de publicación
- 2025
- Idioma
- inglés
- Tipo de recurso
- artículo
- Estado
- versión publicada
- Descripción
- Some models have been developed recently to calculate and analyze the electronic origin of the nuclear magnetic shielding tensor. We present here the most recent results of calculations performed with the Geometric Elimination of the Small Component (GESC) model, which represents a partial improvement of the Linear Response Elimination of the Small Component (LRESC) model, particularly concerning diamagnetic contributions. We have found that the accuracy of the diamagnetic contributions obtained with the GESC model is higher than the one obtained with the LRESC model for any molecular system. The difference between the LRESC (σLRESCd) and the four-component (σpp) methods is mainly due to the Fermi contact mechanism (σFC,LRESC). In the case of the GESC model, the contribution of such electronic mechanism is lowered by a factor of 5/7 with respect to σ pp. Furthermore, the next important mechanism that contributes to the differences between σdLRESC and σpp is known as DiaK (σDiaK), being its values close to half of that due to σFC,LRESC. We analyze here the electronic mechanisms involved in the NMR shielding of halogen atoms of the following family of compounds: HX, IX, and AtX, where X = H, F, Cl, Br, I, At, and the shielding of the central atoms in the following family of molecules: Sn4−iXi and PbH4−iXi with i = 1–4 and X = H, F, Cl, Br, I. The calculations were performed at the LRESC-HF/DFT and GESC-HF/DFT levels of theory together with four-component DHF.
Fil: Zapata Escobar, Andy Danian. Consejo Nacional de Investigaciones Científicas y Técnicas. Centro Científico Tecnológico Conicet - Nordeste. Instituto de Modelado e Innovación Tecnológica. Universidad Nacional del Nordeste. Facultad de Ciencias Exactas Naturales y Agrimensura. Instituto de Modelado e Innovación Tecnológica; Argentina
Fil: Melo, Juan Ignacio. Consejo Nacional de Investigaciones Científicas y Técnicas. Oficina de Coordinación Administrativa Ciudad Universitaria. Instituto de Física de Buenos Aires. Universidad de Buenos Aires. Facultad de Ciencias Exactas y Naturales. Instituto de Física de Buenos Aires; Argentina
Fil: Aucar, Gustavo Adolfo. Consejo Nacional de Investigaciones Científicas y Técnicas. Centro Científico Tecnológico Conicet - Nordeste. Instituto de Modelado e Innovación Tecnológica. Universidad Nacional del Nordeste. Facultad de Ciencias Exactas Naturales y Agrimensura. Instituto de Modelado e Innovación Tecnológica; Argentina - Materia
-
LRESC
GESC
Shielding
Polarization Propagator - Nivel de accesibilidad
- acceso abierto
- Condiciones de uso
- https://creativecommons.org/licenses/by-nc-sa/2.5/ar/
- Repositorio
.jpg)
- Institución
- Consejo Nacional de Investigaciones Científicas y Técnicas
- OAI Identificador
- oai:ri.conicet.gov.ar:11336/278357
Ver los metadatos del registro completo
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Performance of GESC and LRESC models for heavy-atom nuclear magnetic shieldingsZapata Escobar, Andy DanianMelo, Juan IgnacioAucar, Gustavo AdolfoLRESCGESCShieldingPolarization Propagatorhttps://purl.org/becyt/ford/1.3https://purl.org/becyt/ford/1Some models have been developed recently to calculate and analyze the electronic origin of the nuclear magnetic shielding tensor. We present here the most recent results of calculations performed with the Geometric Elimination of the Small Component (GESC) model, which represents a partial improvement of the Linear Response Elimination of the Small Component (LRESC) model, particularly concerning diamagnetic contributions. We have found that the accuracy of the diamagnetic contributions obtained with the GESC model is higher than the one obtained with the LRESC model for any molecular system. The difference between the LRESC (σLRESCd) and the four-component (σpp) methods is mainly due to the Fermi contact mechanism (σFC,LRESC). In the case of the GESC model, the contribution of such electronic mechanism is lowered by a factor of 5/7 with respect to σ pp. Furthermore, the next important mechanism that contributes to the differences between σdLRESC and σpp is known as DiaK (σDiaK), being its values close to half of that due to σFC,LRESC. We analyze here the electronic mechanisms involved in the NMR shielding of halogen atoms of the following family of compounds: HX, IX, and AtX, where X = H, F, Cl, Br, I, At, and the shielding of the central atoms in the following family of molecules: Sn4−iXi and PbH4−iXi with i = 1–4 and X = H, F, Cl, Br, I. The calculations were performed at the LRESC-HF/DFT and GESC-HF/DFT levels of theory together with four-component DHF.Fil: Zapata Escobar, Andy Danian. Consejo Nacional de Investigaciones Científicas y Técnicas. Centro Científico Tecnológico Conicet - Nordeste. Instituto de Modelado e Innovación Tecnológica. Universidad Nacional del Nordeste. Facultad de Ciencias Exactas Naturales y Agrimensura. Instituto de Modelado e Innovación Tecnológica; ArgentinaFil: Melo, Juan Ignacio. Consejo Nacional de Investigaciones Científicas y Técnicas. Oficina de Coordinación Administrativa Ciudad Universitaria. Instituto de Física de Buenos Aires. Universidad de Buenos Aires. Facultad de Ciencias Exactas y Naturales. Instituto de Física de Buenos Aires; ArgentinaFil: Aucar, Gustavo Adolfo. Consejo Nacional de Investigaciones Científicas y Técnicas. Centro Científico Tecnológico Conicet - Nordeste. Instituto de Modelado e Innovación Tecnológica. Universidad Nacional del Nordeste. Facultad de Ciencias Exactas Naturales y Agrimensura. Instituto de Modelado e Innovación Tecnológica; ArgentinaAmerican Institute of Physics2025-12info:eu-repo/semantics/articleinfo:eu-repo/semantics/publishedVersionhttp://purl.org/coar/resource_type/c_6501info:ar-repo/semantics/articuloapplication/pdfapplication/pdfhttp://hdl.handle.net/11336/278357Zapata Escobar, Andy Danian; Melo, Juan Ignacio; Aucar, Gustavo Adolfo; Performance of GESC and LRESC models for heavy-atom nuclear magnetic shieldings; American Institute of Physics; Journal of Chemical Physics; 163; 22; 12-2025; 1-140021-9606CONICET DigitalCONICETenginfo:eu-repo/semantics/altIdentifier/url/https://pubs.aip.org/jcp/article/163/22/224131/3374705/Performance-of-GESC-and-LRESC-models-for-heavyinfo:eu-repo/semantics/altIdentifier/doi/10.1063/5.0306490info:eu-repo/semantics/openAccesshttps://creativecommons.org/licenses/by-nc-sa/2.5/ar/reponame:CONICET Digital (CONICET)instname:Consejo Nacional de Investigaciones Científicas y Técnicas2026-01-08T13:05:55Zoai:ri.conicet.gov.ar:11336/278357instacron:CONICETInstitucionalhttp://ri.conicet.gov.ar/Organismo científico-tecnológicoNo correspondehttp://ri.conicet.gov.ar/oai/requestdasensio@conicet.gov.ar; lcarlino@conicet.gov.arArgentinaNo correspondeNo correspondeNo correspondeopendoar:34982026-01-08 13:05:55.353CONICET Digital (CONICET) - Consejo Nacional de Investigaciones Científicas y Técnicasfalse |
| dc.title.none.fl_str_mv |
Performance of GESC and LRESC models for heavy-atom nuclear magnetic shieldings |
| title |
Performance of GESC and LRESC models for heavy-atom nuclear magnetic shieldings |
| spellingShingle |
Performance of GESC and LRESC models for heavy-atom nuclear magnetic shieldings Zapata Escobar, Andy Danian LRESC GESC Shielding Polarization Propagator |
| title_short |
Performance of GESC and LRESC models for heavy-atom nuclear magnetic shieldings |
| title_full |
Performance of GESC and LRESC models for heavy-atom nuclear magnetic shieldings |
| title_fullStr |
Performance of GESC and LRESC models for heavy-atom nuclear magnetic shieldings |
| title_full_unstemmed |
Performance of GESC and LRESC models for heavy-atom nuclear magnetic shieldings |
| title_sort |
Performance of GESC and LRESC models for heavy-atom nuclear magnetic shieldings |
| dc.creator.none.fl_str_mv |
Zapata Escobar, Andy Danian Melo, Juan Ignacio Aucar, Gustavo Adolfo |
| author |
Zapata Escobar, Andy Danian |
| author_facet |
Zapata Escobar, Andy Danian Melo, Juan Ignacio Aucar, Gustavo Adolfo |
| author_role |
author |
| author2 |
Melo, Juan Ignacio Aucar, Gustavo Adolfo |
| author2_role |
author author |
| dc.subject.none.fl_str_mv |
LRESC GESC Shielding Polarization Propagator |
| topic |
LRESC GESC Shielding Polarization Propagator |
| purl_subject.fl_str_mv |
https://purl.org/becyt/ford/1.3 https://purl.org/becyt/ford/1 |
| dc.description.none.fl_txt_mv |
Some models have been developed recently to calculate and analyze the electronic origin of the nuclear magnetic shielding tensor. We present here the most recent results of calculations performed with the Geometric Elimination of the Small Component (GESC) model, which represents a partial improvement of the Linear Response Elimination of the Small Component (LRESC) model, particularly concerning diamagnetic contributions. We have found that the accuracy of the diamagnetic contributions obtained with the GESC model is higher than the one obtained with the LRESC model for any molecular system. The difference between the LRESC (σLRESCd) and the four-component (σpp) methods is mainly due to the Fermi contact mechanism (σFC,LRESC). In the case of the GESC model, the contribution of such electronic mechanism is lowered by a factor of 5/7 with respect to σ pp. Furthermore, the next important mechanism that contributes to the differences between σdLRESC and σpp is known as DiaK (σDiaK), being its values close to half of that due to σFC,LRESC. We analyze here the electronic mechanisms involved in the NMR shielding of halogen atoms of the following family of compounds: HX, IX, and AtX, where X = H, F, Cl, Br, I, At, and the shielding of the central atoms in the following family of molecules: Sn4−iXi and PbH4−iXi with i = 1–4 and X = H, F, Cl, Br, I. The calculations were performed at the LRESC-HF/DFT and GESC-HF/DFT levels of theory together with four-component DHF. Fil: Zapata Escobar, Andy Danian. Consejo Nacional de Investigaciones Científicas y Técnicas. Centro Científico Tecnológico Conicet - Nordeste. Instituto de Modelado e Innovación Tecnológica. Universidad Nacional del Nordeste. Facultad de Ciencias Exactas Naturales y Agrimensura. Instituto de Modelado e Innovación Tecnológica; Argentina Fil: Melo, Juan Ignacio. Consejo Nacional de Investigaciones Científicas y Técnicas. Oficina de Coordinación Administrativa Ciudad Universitaria. Instituto de Física de Buenos Aires. Universidad de Buenos Aires. Facultad de Ciencias Exactas y Naturales. Instituto de Física de Buenos Aires; Argentina Fil: Aucar, Gustavo Adolfo. Consejo Nacional de Investigaciones Científicas y Técnicas. Centro Científico Tecnológico Conicet - Nordeste. Instituto de Modelado e Innovación Tecnológica. Universidad Nacional del Nordeste. Facultad de Ciencias Exactas Naturales y Agrimensura. Instituto de Modelado e Innovación Tecnológica; Argentina |
| description |
Some models have been developed recently to calculate and analyze the electronic origin of the nuclear magnetic shielding tensor. We present here the most recent results of calculations performed with the Geometric Elimination of the Small Component (GESC) model, which represents a partial improvement of the Linear Response Elimination of the Small Component (LRESC) model, particularly concerning diamagnetic contributions. We have found that the accuracy of the diamagnetic contributions obtained with the GESC model is higher than the one obtained with the LRESC model for any molecular system. The difference between the LRESC (σLRESCd) and the four-component (σpp) methods is mainly due to the Fermi contact mechanism (σFC,LRESC). In the case of the GESC model, the contribution of such electronic mechanism is lowered by a factor of 5/7 with respect to σ pp. Furthermore, the next important mechanism that contributes to the differences between σdLRESC and σpp is known as DiaK (σDiaK), being its values close to half of that due to σFC,LRESC. We analyze here the electronic mechanisms involved in the NMR shielding of halogen atoms of the following family of compounds: HX, IX, and AtX, where X = H, F, Cl, Br, I, At, and the shielding of the central atoms in the following family of molecules: Sn4−iXi and PbH4−iXi with i = 1–4 and X = H, F, Cl, Br, I. The calculations were performed at the LRESC-HF/DFT and GESC-HF/DFT levels of theory together with four-component DHF. |
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2025 |
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2025-12 |
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info:eu-repo/semantics/article info:eu-repo/semantics/publishedVersion http://purl.org/coar/resource_type/c_6501 info:ar-repo/semantics/articulo |
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article |
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publishedVersion |
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http://hdl.handle.net/11336/278357 Zapata Escobar, Andy Danian; Melo, Juan Ignacio; Aucar, Gustavo Adolfo; Performance of GESC and LRESC models for heavy-atom nuclear magnetic shieldings; American Institute of Physics; Journal of Chemical Physics; 163; 22; 12-2025; 1-14 0021-9606 CONICET Digital CONICET |
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http://hdl.handle.net/11336/278357 |
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Zapata Escobar, Andy Danian; Melo, Juan Ignacio; Aucar, Gustavo Adolfo; Performance of GESC and LRESC models for heavy-atom nuclear magnetic shieldings; American Institute of Physics; Journal of Chemical Physics; 163; 22; 12-2025; 1-14 0021-9606 CONICET Digital CONICET |
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eng |
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eng |
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American Institute of Physics |
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American Institute of Physics |
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