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Phase Transitions02:31

Phase Transitions

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Whether solid, liquid, or gas, a substance's state depends on the order and arrangement of its particles (atoms, molecules, or ions). Particles in the solid pack closely together, generally in a pattern. The particles vibrate about their fixed positions but do not move or squeeze past their neighbors. In liquids, although the particles are closely spaced, they are randomly arranged. The position of the particles are not fixed—that is, they are free to move past their neighbors to...
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Properties of Transition Metals02:58

Properties of Transition Metals

29.7K
Transition metals are defined as those elements that have partially filled d orbitals. As shown in Figure 1, the d-block elements in groups 3–12 are transition elements. The f-block elements, also called inner transition metals (the lanthanides and actinides), also meet this criterion because the d orbital is partially occupied before the f orbitals.
29.7K
Cooperative Allosteric Transitions01:58

Cooperative Allosteric Transitions

8.7K
Cooperative allosteric transitions can occur in multimeric proteins, where each subunit of the protein has its own ligand-binding site. When a ligand binds to any of these subunits, it triggers a conformational change that affects the binding sites in the other subunits; this can change the affinity of the other sites for their respective ligands. The ability of the protein to change the shape of its binding site is attributed to the presence of a mix of flexible and stable segments in the...
8.7K
Spin–Spin Coupling Constant: Overview01:08

Spin–Spin Coupling Constant: Overview

1.5K
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...
1.5K
NMR Spectroscopy: Spin–Spin Coupling01:08

NMR Spectroscopy: Spin–Spin Coupling

3.0K
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...
3.0K
Spin–Spin Coupling: One-Bond Coupling01:17

Spin–Spin Coupling: One-Bond Coupling

1.5K
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,...
1.5K

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Updated: Jan 26, 2026

Switchable Acoustic and Optical Resolution Photoacoustic Microscopy for In Vivo Small-animal Blood Vasculature Imaging
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Switchable Acoustic and Optical Resolution Photoacoustic Microscopy for In Vivo Small-animal Blood Vasculature Imaging

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Manipulating Spin Transition To Achieve Switchable Multifunctions.

Yin-Shan Meng1, Tao Liu1

  • 1State Key Laboratory of Fine Chemicals , Dalian University of Technology , 2 Linggong Road , Dalian 116024 , P. R. China.

Accounts of Chemical Research
|April 12, 2019
PubMed
Summary

Photoinduced spin transitions in metal ions enable reversible control over magnetic, dielectric, and fluorescence properties. This research highlights advances in creating smart materials with tunable functions for next-generation devices.

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Area of Science:

  • Materials Science
  • Chemistry
  • Physics

Background:

  • Spin transition in metal ions alters electron configurations, impacting material functions.
  • Photoinduced spin transitions offer precise control over material properties for advanced applications.
  • Challenges include achieving reversible switching and effective coupling between photoresponsive and functional units.

Purpose of the Study:

  • To review recent advances in using photoinduced spin transitions to tune material properties.
  • To highlight strategies for developing reversible spin-crossover (SCO) and metal-to-metal charge transfer (MMCT).
  • To explore the integration of SCO and MMCT units for multifunctional smart materials.

Main Methods:

  • Investigated photoinduced reversible SCO and MMCT phenomena.
  • Utilized metallocyanate building blocks to assemble SCO and MMCT units into chains.
  • Examined the influence of intermolecular interactions, such as π···π interactions, on MMCT.

Main Results:

  • Demonstrated photoswitchable tuning of magnetic properties, including single-chain magnet behavior.
  • Achieved reversible switching of molecular polarity and dielectric properties via electron transfer.
  • Observed colossal positive and negative thermal expansion, enabling phototunable nanomotor strategies.
  • Showcased modulation of fluorescence properties through energy transfer control.

Conclusions:

  • Photoinduced spin transitions are effective actuators for tuning diverse material functions.
  • Successful integration of SCO and MMCT units leads to materials with switchable magnetic, dielectric, and optical properties.
  • Future research holds promise for novel photoswitchable materials with applications in advanced devices.