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Related Concept Videos

¹H NMR: Long-Range Coupling01:27

¹H NMR: Long-Range Coupling

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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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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...
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¹H NMR: Interpreting Distorted and Overlapping Signals01:02

¹H NMR: Interpreting Distorted and Overlapping Signals

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Spin systems where the difference in chemical shifts of the coupled nuclei is greater than ten times J are called first-order spin systems. These nuclei are weakly coupled, and their chemical shifts and coupling constant can generally be estimated from the well-separated signals in the spectrum.
As Δν decreases and the signals move closer, the doublets appear increasingly distorted. The intensities of the inner lines increase at the cost of those of the outer lines as the signals are...
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The Pauli Exclusion Principle03:06

The Pauli Exclusion Principle

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The arrangement of electrons in the orbitals of an atom is called its electron configuration. We describe an electron configuration with a symbol that contains three pieces of information:
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Spin–Spin Coupling: One-Bond Coupling01:17

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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,...
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NMR Spectroscopy: Spin–Spin Coupling01:08

NMR Spectroscopy: Spin–Spin Coupling

3.6K
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...
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Generation and Coherent Control of Pulsed Quantum Frequency Combs
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Density Matrix Embedding: A Strong-Coupling Quantum Embedding Theory.

Gerald Knizia1, Garnet Kin-Lic Chan1

  • 1Department of Chemistry, Princeton University, Princeton, New Jersey 08544, United States.

Journal of Chemical Theory and Computation
|November 21, 2015
PubMed
Summary
This summary is machine-generated.

Density Matrix Embedding Theory (DMET) now handles complex chemical systems. This quantum embedding method accurately models strongly correlated fragments, even single atoms, overcoming limitations of traditional approaches.

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Area of Science:

  • Quantum Chemistry
  • Computational Physics
  • Materials Science

Background:

  • Traditional embedding methods struggle with strongly correlated quantum systems.
  • Handling open quantum systems and strong environmental coupling presents significant challenges.
  • Existing techniques often rely on empirical approximations for strong interactions.

Purpose of the Study:

  • To extend Density Matrix Embedding Theory (DMET) beyond lattice models to the full chemical Hamiltonian.
  • To develop a rigorous quantum embedding method capable of treating arbitrary, strongly coupled fragments.
  • To provide a robust alternative to empirical approaches for complex quantum systems.

Main Methods:

  • Extension of DMET to incorporate the full chemical Hamiltonian.
  • Development of a rigorous quantum bath to model fragment-environment entanglement.
  • Application to strongly correlated hydrogen ring and grid models.

Main Results:

  • DMET successfully models strongly correlated hydrogen models, including challenging ring and grid systems.
  • The method accurately describes the symmetric dissociation of a 4x3 hydrogen atom grid.
  • Effective treatment of fragments as small as single hydrogen atoms was demonstrated.

Conclusions:

  • DMET provides a rigorous and accurate approach for embedding fragments in complex quantum systems.
  • The extended DMET overcomes limitations of traditional embedding and quantum chemistry methods.
  • This work enables new avenues for studying strongly coupled, strongly correlated systems fragment by fragment.