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¹H NMR: Interpreting Distorted and Overlapping Signals01:02

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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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Atomic Nuclei: Nuclear Spin State Overview01:03

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NMR-active nuclei have energy levels called 'spin states' that are associated with the orientations of their nuclear magnetic moments. In the absence of a magnetic field, the nuclear magnetic moments are randomly oriented, and the spin states are degenerate. When an external magnetic field is applied, the spin states have only 2 + 1 orientations available to them. A proton with = ½ has two available orientations. Similarly, for a quadrupolar nucleus with a nuclear spin value of one, the...
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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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Spin–Spin Coupling Constant: Overview01:08

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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 Spectrometers: Radiofrequency Pulses and Pulse Sequences01:17

NMR Spectrometers: Radiofrequency Pulses and Pulse Sequences

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A pulse is a short burst of radio waves distributed over a range of frequencies that simultaneously excites all the nuclei in the sample. Upon passing a radio frequency pulse along the x-axis, the nuclei absorb energy corresponding to their Larmor frequencies and achieve resonance. This shifts the net magnetization vector from the z-axis toward the transverse plane. This angle of rotation of the magnetization vector, or the flip angle, is proportional to the duration and intensity of the pulse.
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Photoluminescence: Fluorescence and Phosphorescence01:23

Photoluminescence: Fluorescence and Phosphorescence

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Photoluminescence is a process where a molecule absorbs light energy and re-emits it in the form of light. This phenomenon occurs when a substance absorbs photons, promoting its electrons to higher energy level excited states, followed by a relaxation process in which the electrons return to their original ground state energy levels and emit light. Photoluminescence is widely observed in various materials, including semiconductors, and organic and inorganic compounds.
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Related Experiment Video

Updated: May 2, 2026

Direct Imaging of Laser-driven Ultrafast Molecular Rotation
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Fluctuations in Spin Dynamics Excited by Pulsed Light.

Tetsuya Sato1, Shinichi Watanabe2,3, Mamoru Matsuo4,5,6,7

  • 1Institute for Solid State Physics, The University of Tokyo, 5-1-5 Kashiwanoha, Kashiwa 277-8581, Japan.

Physical Review Letters
|March 28, 2025
PubMed
Summary

This study explores nonequilibrium spin fluctuations in ferromagnets after light pulses. A new Fano factor reveals spin transfer dynamics, paving the way for spin noise spectroscopy.

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Area of Science:

  • Condensed Matter Physics
  • Quantum Optics

Background:

  • Understanding spin dynamics in magnetic materials is crucial for developing advanced technologies.
  • Nonequilibrium phenomena in ferromagnets are not fully understood, especially after external perturbations like light pulses.

Purpose of the Study:

  • To theoretically investigate nonequilibrium spin fluctuations in a ferromagnet induced by a light pulse.
  • To develop a method for analyzing spin transfer dynamics in nonequilibrium states.

Main Methods:

  • Utilized a Lindblad equation consistent with the Landau-Lifshitz-Gilbert equation.
  • Computed the autocorrelation function of magnetization.
  • Introduced a Fano factor to quantify nonequilibrium spin fluctuations.

Main Results:

  • The autocorrelation function of magnetization contains both thermal and nonequilibrium components.
  • The Fano factor effectively characterizes the transfer of spin units to the environment.
  • Demonstrated the utility of the Fano factor in analyzing nonequilibrium spin dynamics.

Conclusions:

  • The study provides a theoretical framework for understanding light-induced nonequilibrium spin fluctuations.
  • The proposed Fano factor offers a novel tool for probing spin relaxation dynamics.
  • Findings pave the way for nonequilibrium spin noise spectroscopy.