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Atomic Nuclei: Nuclear Relaxation Processes01:23

Atomic Nuclei: Nuclear Relaxation Processes

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In the absence of an external magnetic field, nuclear spin states are degenerate and randomly oriented. When a magnetic field is applied, the spins begin to precess and orient themselves along (lower energy) or against (higher energy) the direction of the field. At equilibrium, a slight excess population of spins exists in the lower energy state. Because the direction of the magnetic field is fixed as the z-axis,  the precessing magnetic moments are randomly oriented around the z-axis.
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¹H NMR: Long-Range Coupling01:27

¹H NMR: Long-Range Coupling

2.0K
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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Magnetic Field due to Moving Charges01:23

Magnetic Field due to Moving Charges

9.3K
A stationary charge creates and interacts with the electric field, while a moving charge creates a magnetic field.
Consider a point charge moving with a constant velocity. Like the electric field, the magnetic field at any point is directly proportional to the magnitude of the charge and inversely proportional to the square of the distance between the source point and the field point. However, unlike the electric field, the magnetic field is always perpendicular to the plane containing the line...
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Inductive Effects on Chemical Shift: Overview01:27

Inductive Effects on Chemical Shift: Overview

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The protons in unsubstituted alkanes are strongly shielded with chemical shifts below 1.8 ppm. Methine, methylene, and methyl protons appear at approximately 1.7, 1.2 and 0.7 ppm, while the proton signal from methane appears at 0.23 ppm. An electronegative substituent, such as chlorine, withdraws the electron density from the protons, increasing their chemical shift. Progressive substitution of the hydrogens in methane by chlorine shifts the proton signals increasingly downfield, to 3.05 ppm in...
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Spin–Spin Coupling: Two-Bond Coupling (Geminal Coupling)01:20

Spin–Spin Coupling: Two-Bond Coupling (Geminal Coupling)

1.2K
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

1.1K
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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Related Experiment Video

Updated: Sep 19, 2025

Cooling an Optically Trapped Ultracold Fermi Gas by Periodical Driving
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Traveling chimera states by weak temporal couplings.

Wenbin Mao1, Guoshen Liang1, Zonghua Liu1

  • 1East China Normal University, School of Physics and Electronic Science, Shanghai 200241, People's Republic of China.

Physical Review. E
|June 19, 2025
PubMed
Summary

A neural model reveals how pacemaker loops influence brain rhythms during rest. It demonstrates sensitive switching between chimera states, offering insights into rapid brain state transitions.

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Area of Science:

  • Neuroscience
  • Computational Neuroscience
  • Complex Systems

Background:

  • Self-sustained oscillations in brain rhythms are crucial, with pacemaker loops playing a key role.
  • The precise function of pacemaker loops in the resting state, characterized by multi-scaled slow-wave activity and dynamic state switching, remains unclear.

Purpose of the Study:

  • To investigate the role of pacemaker loops in generating complex dynamics within the resting state of the brain.
  • To explore how network coupling influences brain rhythm dynamics and state transitions.

Main Methods:

  • Development of a neural model simulating a pacemaker loop-like network with weak temporal electrical coupling.
  • Analysis of emergent dynamics, including disorder, traveling chimera states, chimera states, and synchronization.
  • Introduction and application of an index Q to quantify local order parameter fluctuations.

Main Results:

  • The model generates diverse dynamic patterns: disorder, traveling chimera, chimera, and synchronization.
  • A sensitive switching phenomenon between traveling chimera and chimera states was observed.
  • Index Q confirmed a new regularity related to local order parameter fluctuations, dependent on parameter matching.
  • The traveling chimera state demonstrated robustness against variations in temporal coupling.

Conclusions:

  • Pacemaker loop networks can exhibit complex dynamics relevant to brain resting states.
  • The observed sensitive switching may explain rapid transitions between brain rhythms.
  • The index Q provides a novel measure for understanding network fluctuations and underlying regularities.