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Related Concept Videos

Ionic Crystal Structures02:42

Ionic Crystal Structures

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Ionic crystals consist of two or more different kinds of ions that usually have different sizes. The packing of these ions into a crystal structure is more complex than the packing of metal atoms that are the same size.
Most monatomic ions behave as charged spheres, and their attraction for ions of opposite charge is the same in every direction. Consequently, stable structures for ionic compounds result (1) when ions of one charge are surrounded by as many ions as possible of the opposite...
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¹H NMR Chemical Shift Equivalence: Enantiotopic and Diastereotopic Protons00:58

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Replacing each alpha-hydrogen in chloroethane by bromine (or a different functional group) yields a pair of enantiomers. Such protons are called prochiral or enantiotopic and are related by a mirror plane. Enantiotopic protons are chemically equivalent in an achiral environment. Because most proton NMR spectra are recorded using achiral solvents, enantiotopic hydrogens yield a single signal.
In chiral compounds such as 2-butanol, replacing the methylene hydrogens at C3 produces a pair of...
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VSEPR Theory and the Effect of Lone Pairs04:01

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Effect of Lone Pairs of Electrons on Molecule Geometry
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Crystal Field Theory - Tetrahedral and Square Planar Complexes02:46

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Tetrahedral Complexes
Crystal field theory (CFT) is applicable to molecules in geometries other than octahedral. In octahedral complexes, the lobes of the dx2−y2 and dz2 orbitals point directly at the ligands. For tetrahedral complexes, the d orbitals remain in place, but with only four ligands located between the axes. None of the orbitals points directly at the tetrahedral ligands. However, the dx2−y2 and dz2 orbitals (along the Cartesian axes) overlap with the ligands less than the dxy,...
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Chirality at Nitrogen, Phosphorus, and Sulfur02:30

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Chirality is most prevalent in carbon-based tetrahedral compounds, but this important facet of molecular symmetry extends to sp3-hybridized nitrogen, phosphorus and sulfur centers, including trivalent molecules with lone pairs. Here, the lone pair behaves as a functional group in addition to the other three substituents to form an analogous tetrahedral center that can be chiral.
A consequence of chirality is the need for enantiomeric resolution. While this is theoretically possible for all...
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Chirality02:25

Chirality

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Chirality is a term that describes the lack of mirror symmetry in an object. In other words, chiral objects cannot be superposed on their mirror images. For example, our feet are chiral, as the mirror image of the left foot, the right foot, cannot be superposed on the left foot.
Chiral objects exhibit a sense of handedness when they interact with another chiral object. For example, our left foot can only fit in the left shoe and not in the right shoe. Achiral objects — objects that have...
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Chiral Phonons in 2D Halide Perovskites.

Mike Pols1, Geert Brocks1,2, Sofía Calero1

  • 1Materials Simulation & Modelling, Department of Applied Physics and Science Education, Eindhoven University of Technology, 5600 MB Eindhoven, The Netherlands.

Nano Letters
|June 16, 2025
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Summary

Chiral phonons in 2D halide perovskites carry angular momentum, driving spin and heat currents. This study confirms their presence, revealing insights into chirality-induced spin selectivity and spin Seebeck effects in these semiconductors.

Keywords:
angular momentumchiralitydensity functional theorymachine-learning force fieldsmetal halide perovskitesphonons, chiral phonons

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Area of Science:

  • Condensed Matter Physics
  • Materials Science
  • Spintronics

Background:

  • Chiral phonons in crystal structures exhibit circular polarization and carry angular momentum.
  • Two-dimensional (2D) halide perovskites are semiconductors with potential for chiral structures.
  • Phenomena like chirality-induced spin selectivity (CISS) and the spin Seebeck effect are observed in chiral 2D perovskites, but mechanisms are unclear.

Purpose of the Study:

  • To investigate the role of chiral phonons in 2D halide perovskites.
  • To elucidate the underlying mechanisms of CISS and spin Seebeck effects in these materials.

Main Methods:

  • Density functional theory (DFT) calculations.
  • On-the-fly machine-learning force fields trained against DFT.
  • Phonon chirality analysis.

Main Results:

  • Confirmed the presence of chiral phonons in 2D halide perovskites.
  • Identified low-energy phonons from the inorganic framework as the primary source of chirality.
  • Demonstrated that chiral phonons generate significant angular momentum under temperature gradients.

Conclusions:

  • Chiral phonons are key to understanding spin and thermal transport in chiral 2D perovskites.
  • These materials offer a platform for exploring phononic, electronic, spintronic, and thermal property interplay.
  • Further research into chiral phonon dynamics can unlock novel spintronic and thermoelectric applications.