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Related Concept Videos

Spin–Spin Coupling: Three-Bond Coupling (Vicinal Coupling)01:22

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Vicinal or three-bond coupling is commonly observed between protons attached to adjacent carbons. Here, nuclear spin information is primarily transferred via electron spin interactions between adjacent C‑H bond orbitals. This generally favors the antiparallel arrangement of spins, so 3J values are usually positive.
The extent of coupling depends on the C‑C bond length, the two H‑C‑C angles, any electron-withdrawing substituents, and the dihedral angle between the...
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Spin–Spin Coupling: Two-Bond Coupling (Geminal Coupling)01:20

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Two NMR-active nuclei bonded to a central atom can be involved in geminal or two-bond coupling. Geminal coupling is commonly seen between diastereotopic protons in chiral molecules and unsymmetrical alkenes, among others.
The central atom need not be NMR-active because its electrons are affected by the electron polarization of the spin-active atoms. However, spin information is transmitted less effectively than in one-bond coupling, and 2J values are usually weaker than 1J values. The energy of...
1.1K
Spin–Spin Coupling: One-Bond Coupling01:17

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1.0K
Coupling interactions are strongest between NMR-active nuclei bonded to each other, where spin information can be transmitted directly through the pair of bonding electrons. While nuclei polarize their electrons to the opposite spins, the bonding electron pair has opposite spins. Configurations with antiparallel nuclear spins are expected to be lower in energy. When coupling makes antiparallel states more favorable, J is considered to have a positive value. The one-bond coupling constant, 1J,...
1.0K
Spin–Spin Coupling Constant: Overview01:08

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1000
In bromoethane, the three methyl protons are coupled to the two methylene protons that are three bonds away. In accordance with the n+1 rule, the signal from the methyl protons is split into three peaks with 1:2:1 relative intensities. The methylene protons appear as a quartet, with the relative intensities of 1:3:3:1.
Qualitatively, any spin plus-half nucleus polarizes the spins of its electrons to the minus-half state. Consequently, the paired electron in the hydrogen–carbon bond must...
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NMR Spectroscopy: Spin–Spin Coupling01:08

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1.6K
The spin state of an NMR-active nucleus can have a slight effect on its immediate electronic environment. This effect propagates through the intervening bonds and affects the electronic environments of NMR-active nuclei up to three bonds away; occasionally, even farther. This phenomenon is called spin–spin coupling or J-coupling. Coupling interactions are mutual and result in small changes in the absorption frequencies of both nuclei involved. While nuclei of the same element are involved...
1.6K
¹H NMR: Long-Range Coupling01:27

¹H NMR: Long-Range Coupling

1.9K
The coupling interactions of nuclei across four or more bonds are usually weak, with J values less than 1 Hz. While these are usually not observed in spectra, the presence of multiple bonds along the coupling pathway can result in observable long-range coupling.
In alkenes, spin information is communicated via σ–π overlap, as seen in allylic (four-bond) and homoallylic (five-bond) couplings. These coupling interactions are stronger when the σ bond is parallel to the alkene...
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Vibrational Spectra of a N719-Chromophore/Titania Interface from Empirical-Potential Molecular-Dynamics Simulation, Solvated by a Room Temperature Ionic Liquid
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Comparison among several vibronic coupling methods.

Amanda D Torres1, Carlos E V de Moura2, Ricardo R Oliveira1

  • 1Instituto de Química, Universidade Fedral do Rio de Janeiro, Avenida Athos da Silveira Ramos, 149, Centro de Tecnologia, Rio de Janeiro, 21941-909, Rio de Janeiro, Brazil.

Journal of Molecular Modeling
|August 11, 2022
PubMed
Summary
This summary is machine-generated.

This study compares four vibronic coupling methods for photoabsorption, finding the nuclear ensemble (NE) method best describes formaldehyde's forbidden transition. The direct vibronic coupling (DVC) method quantifies specific vibrational modes, while adiabatic Hessian (AH) and vertical gradient (VG) offer computational savings.

Keywords:
DFTFormaldehydeSpectroscopyVibronic couplingVibronic spectrum

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Area of Science:

  • Computational Chemistry
  • Theoretical Spectroscopy
  • Quantum Mechanics

Background:

  • Accurately modeling vibronic coupling is crucial for understanding photoabsorption spectra.
  • The symmetry-forbidden n → π* transition in formaldehyde serves as a benchmark for evaluating theoretical methods due to its sensitivity to vibronic effects.

Purpose of the Study:

  • To compare the performance of four distinct computational approaches for calculating vibronic coupling in photoabsorption.
  • To assess the accuracy and computational efficiency of the nuclear ensemble (NE), direct vibronic coupling (DVC), adiabatic Hessian (AH), and vertical gradient (VG) methods.

Main Methods:

  • Simulated photoabsorption spectra using four methods: NE, DVC, AH, and VG.
  • Analysis of vibrational mode contributions to the transition using DVC.
  • Comparison of computational cost and accuracy for each method.

Main Results:

  • The nuclear ensemble method provided the most accurate spectral description for the formaldehyde n → π* transition.
  • Direct vibronic coupling identified mode 1 (C=O out-of-plane bending) as the primary contributor, with modes 6 and 2 also significant.
  • NE and DVC yielded comparable results, while AH and VG offered computational advantages, with VG being the least demanding.

Conclusions:

  • Each method possesses unique strengths for simulating vibronic coupling in photoabsorption.
  • NE offers superior spectral accuracy, DVC provides insights into vibrational mode contributions, and AH/VG present computationally efficient alternatives.
  • The choice of method depends on the desired balance between accuracy, detailed analysis, and computational resources.