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IR Absorption Frequency: Hybridization01:21

IR Absorption Frequency: Hybridization

1.1K
Hydrocarbons such as alkanes, alkenes, and alkynes show characteristic C–H stretching absorption bands. These IR stretching frequencies depend on the hybridization of the involved carbon atom and can be explained in terms of the s character of each hybridized atomic orbital.
Among the sp, sp2, and sp3 hybridized orbitals, sp orbitals have the maximum s character (50%). Consequently, the electrons are held more closely to the nucleus, resulting in stronger and shorter C–H bonds that...
1.1K
IR Absorption Frequency: Delocalization01:04

IR Absorption Frequency: Delocalization

1.2K
Electron delocalization refers to the distribution of electrons across multiple atoms within a molecule rather than being confined to a single atom or bond. This phenomenon is common in systems with conjugated bonds—structures where alternating single and double bonds allow π-electrons to move freely across the network. The movement of electrons stabilizes the molecule and can affect various chemical properties, including vibrational frequencies observed in IR spectroscopy.
In IR...
1.2K
Electron Paramagnetic Resonance (EPR) Spectroscopy: Organic Radicals01:17

Electron Paramagnetic Resonance (EPR) Spectroscopy: Organic Radicals

3.0K
Ideally, an unpaired electron shows a single peak in the EPR spectrum due to the transition between the two spin energy states. However, coupling interactions can occur between the spins of the unpaired electron and any neighboring spin-active nuclei. This hyperfine coupling results in hyperfine splitting, where the EPR signal is split into multiplets. The signals split into 2nI + 1 peaks, where n is the number of equivalent nuclei and I is the nuclear spin. These splitting patterns provide...
3.0K
¹H NMR: Interpreting Distorted and Overlapping Signals01:02

¹H NMR: Interpreting Distorted and Overlapping Signals

1.3K
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...
1.3K
Spin–Spin Coupling Constant: Overview01:08

Spin–Spin Coupling Constant: Overview

1.2K
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...
1.2K
¹³C NMR: ¹H–¹³C Decoupling01:04

¹³C NMR: ¹H–¹³C Decoupling

1.4K
The probability of having two carbon-13 atoms next to each other is negligible because of the low natural abundance of carbon-13. Consequently, peak splitting due to carbon-carbon spin-spin coupling is not observed in spectra. However, protons up to three sigma bonds away split the carbon signal according to the n+1 rule, resulting in complicated spectra.
A broadband decoupling technique is used to simplify these complex, sometimes overlapping, signals. Broadband decoupling relies on a...
1.4K

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Related Experiment Video

Updated: Nov 25, 2025

High Resolution Phonon-assisted Quasi-resonance Fluorescence Spectroscopy
10:40

High Resolution Phonon-assisted Quasi-resonance Fluorescence Spectroscopy

Published on: June 28, 2016

7.8K

Anharmonicity-Driven Rashba Cohelical Excitons Break Quantum Efficiency Limitation.

Chang Woo Myung1, Kwang S Kim1,2

  • 1Center for Superfunctional Materials, Department of Chemistry, Ulsan National Institute of Science and Technology (UNIST), 50 UNIST-gil, Ulsan, 44919, Korea.

Advanced Materials (Deerfield Beach, Fla.)
|December 18, 2020
PubMed
Summary
This summary is machine-generated.

Lead halide perovskites (LHPs) overcome the 25% internal quantum efficiency (IQE) limit in LEDs. A novel mechanism utilizing Rashba-Dresselhaus spin-orbit coupling (RD-SOC) enables bright excitons, achieving near 50% IQE.

Keywords:
anharmonic disorderexcitonslead halide perovskiteslight-emitting diodesquantum efficiencies

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Area of Science:

  • Solid State Physics
  • Materials Science
  • Quantum Chemistry

Background:

  • Closed-shell LEDs are limited to 25% internal quantum efficiency (IQE) due to optically inactive triplet excitons.
  • Lead halide perovskites (LHPs) offer a potential pathway to surpass this efficiency limitation.

Purpose of the Study:

  • To explore a novel emission mechanism in LHPs (APbX3) that circumvents the IQE limits of conventional LEDs.
  • To elucidate the role of broken inversion symmetry and spin-orbit coupling in LHP emission.

Main Methods:

  • Theoretical investigation using many-body theory.
  • First-principles calculations.
  • Analysis of anharmonicity and stereochemistry in LHPs.

Main Results:

  • Anharmonicity in LHPs breaks inversion symmetry, inducing Rashba-Dresselhaus spin-orbit coupling (RD-SOC).
  • This RD-SOC leads to the formation of bright cohelical and dark antihelical excitons.
  • The optically active cohelical exciton is identified as the lowest excited state in both organic and inorganic LHPs.

Conclusions:

  • RD-SOC in LHPs enables efficient light emission by utilizing anharmonicity.
  • This mechanism allows LHPs to achieve an ideal IQE approaching 50%, significantly exceeding the 25% limit of closed-shell LEDs.