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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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Cationic Chain-Growth Polymerization: Mechanism00:57

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The cationic polymerization mechanism consists of three steps: initiation, propagation, and termination. In the initiation step of the polymerization process, the π bond of a monomer gets protonated by the Lewis acid catalyst, which is formed from boron trifluoride and water. The protonation of the π bond generates a carbocation stabilized by the electron‐donating group. In the propagation step, the π bond of the second monomer acts as a nucleophile and attacks the...
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π Electron Effects on Chemical Shift: Aromatic and Antiaromatic Compounds01:14

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In aromatic compounds, such as benzene, the circulation of (4n + 2) π-electrons sets up a diamagnetic or diatropic ring current around the perimeter of the molecule. This current induces a magnetic field that opposes the external field inside the ring and reinforces it on the outside. The protons in benzene are deshielded and exhibit high chemical shifts in the range 6.5–8.5 ppm. The shielding effect at the center of the ring is evident in complex aromatic molecules, such as...
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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.
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Radical Chain-Growth Polymerization: Mechanism01:09

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The radical chain-growth polymerization mechanism consists of three steps: initiation, propagation, and termination of polymerization. The polymerization initiates when a free radical generated from the radical initiator adds to the unsaturated bond in the monomer. The unpaired electron of the free radical and one π electron in the unsaturated bond creates a σ bond between the free radical and the monomer. As a result, the other π electron in the unsaturated bond converts this species into...
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Ziegler–Natta Chain-Growth Polymerization: Overview01:17

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Ziegler–Natta polymerization is another form of addition or chain‐growth polymerization used for synthesizing linear polymers over branched polymers. The catalyst used for polymerization is the Ziegler–Natta catalyst, named after Karl Ziegler and Giulio Natta, who developed it in 1953. This catalyst is an organometallic complex of titanium tetrachloride and triethyl aluminum, with the active form of the catalyst being an alkyl titanium compound. Using the Ziegler–Natta...
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Nonadiabatic dynamics with quantum nuclei: simulating charge transfer with ring polymer surface hopping.

Soumya Ghosh1, Samuele Giannini, Kevin Lively

  • 1Department of Physics and Astronomy, University College London, Gower Street, London WC1E 6BT, UK. soumya.ghosh@theochem.rub.de.

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We developed a new computational method combining fragment orbital-based surface hopping (FOB-SH) with ring-polymer molecular dynamics (RPMD) to accurately simulate charge transport, including nuclear quantum effects.

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Area of Science:

  • Computational Chemistry
  • Quantum Dynamics
  • Materials Science

Background:

  • Simulating electronic processes like charge transport requires accounting for non-adiabatic electronic and nuclear quantum effects, especially at low temperatures.
  • Existing methods like fragment orbital-based surface hopping (FOB-SH) treat nuclei classically, limiting accuracy for quantum nuclear phenomena.

Purpose of the Study:

  • To extend FOB-SH by incorporating nuclear quantum effects using ring-polymer molecular dynamics (RPMD).
  • To evaluate three distinct RPMD-based approaches for simulating charge transfer dynamics.

Main Methods:

  • Developed and applied three flavors of FOB-SH combined with RPMD: RPSH with bead approximation (RPSH-BA), RPSH with weighted bead approximation (RPSH-wBA), and the isomorphic Hamiltonian method (SH-RP-iso).
  • Investigated hole transfer in a molecular dimer model, analyzing detailed balance, internal consistency, and temperature/driving force dependence.

Main Results:

  • RPSH-BA underestimated excited state populations, while RPSH-wBA overestimated them.
  • The SH-RP-iso method demonstrated satisfactory accuracy and predicted a flattening of the rate vs. driving force dependence in the Marcus inverted regime at low temperatures.
  • Observed experimental trends were reproduced by the SH-RP-iso method.

Conclusions:

  • The combination of FOB-SH with the SH-RP-iso method is a promising approach for accurately simulating charge transport in molecular materials and biological systems.
  • This method effectively includes zero-point motion and tunneling, crucial for understanding low-temperature electronic processes.